<?xml version="1.0"?>
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<title>LCLS News</title>
<link>http://lcls.slac.stanford.edu</link>
<description>Latest news and announcements about the Linac Coherent Light Source project at the SLAC National Accelerator Laboratory.</description>
<language>en-us</language>
<copyright>Copyright 2009 SLAC National Accelerator Laboratory</copyright>
<image>
<url>http://lcls.slac.stanford.edu/images/lclsLogo.gif</url>
<title>LCLS</title>
<link>http://lcls.slac.stanford.edu</link>
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<title>Nov 18 4 pm Seminar: First pump-probe experiment at LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=173</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/173_150.jpg" alt="LCLS-PULSE Logo" /><br />LCLS-PULSE seminar "First pump-probe experiment at LCLS", Dr. Ryan Coffee, November 18, 2009, 4:00-5:00 PM, Bldg 137, Room 322.<br /><br />The LCLS free-electron x-ray laser is the first coherent radiation source capable of saturating K-shell photoionization for second row elements.  Our experiment was the first opportunity to study multiple core-hole processes in aligned molecules.  We used the tight focus of the LCLS in the High Field Physics instrument to create double-core vacancies in nitrogen molecules.  By first pulsing the molecules with a stack of 8 IR laser pulses with relative delays of about 15 fs, we used a ~100 fs duration nearly square-top pulse to impulsively align the nitrogen molecules.  This alignment allowed us to measure an angle dependence of the Auger relaxation of the doubly K-vacant molecule.  Furthermore, we were able to select only single interactions within the duration of the xFEL pulse by running the LCLS at 20 pC bunch charge and at shorter bunch compression.  We also observed the IR laser induced pre-dissociation of x-ray induced N_2^2+ and in fact this signal allowed us to rapidly find spatio-temporal overlap of the IR laser and the x-ray pulses.<br /><br />For more information, contact Yiping or Haidan LCLS-PULSE seminar organizers.<br /><br />Yiping Feng<br />LCLS, Photon Division, X-ray Science Department SLAC National Accelerator Laboratory<br />2575 Sand Hill Road, Building 280A/Room 288 Menlo Park, CA 94025<br /><br />(650) 926-2890 - Office<br />(408) 888-9827 - Cell<br />(650) 926-3615 - Fax]]></description>
<pubDate>Wed, 18 Nov 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=173</guid>
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<title>May-September Outline Posted </title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=170</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/170_150.jpg" alt="" /><br />The AMO instrument was commissioned during the fall of 2009. For the second round of commissioning/operations scheduled for May-September 2010, AMO experiments are scheduled as well as commissioning for the SXR and XPP instruments. User-assisted commissioning experiments for SXR are also scheduled. <br /><br />In general, activities are scheduled to begin on Thursday, following machine development and repair days each Tuesday and Wednesday. To facilitate planning and preparation, an <a href="http://www-ssrl.slac.stanford.edu/lcls/users/schedules.html">outline has been posted</a> to the user site showing the activities planned by week. <br /><br />The length and order of shifts within each week is still to be determined, dependent on machine and instrument development. Ideally, beam time will be allocated in alternating shifts (~12 hours each), but some 24 hour shifts may be required. The final schedule will be distributed with this detail as soon as it is available.<br /><br />To help users plan proposed experiments for the next call (due April 1st), please check the LCLS website for <a href="http://www-ssrl.slac.stanford.edu/lcls/users/logistics.html#policies">updated policies</a>, as well as news about the latest operating parameters.<br /> <br />Currently we are limited to a spectral range down to 750 eV, and we will guarantee this spectral range for experiments scheduled in Spring and Fall 2010. We are also developing operations at lower energies, down to 510 eV. We cannot guarantee it at this time (subject to Radiation Physics review and approval), but we are confident enough to solicit proposals for the Fall 2010.  <br /><br />The minimum pulse duration in standard operation is ~ 70 femtoseconds FWHM. We have developed lower current operation which is now available for users. In this low current moded pulse lengths have been shown to be less than 20 femtoseconds. We believe the pulses are much shorter (for reference see http://www-public.slac.stanford.edu/sciDoc/docMeta.aspx?slacPubNumber=slac-pub-13642) and solicit proposals to measure this. <br /><br />The maximum repetition rate of the X-ray flashes is expected to be 60 Hz and we are working on moving to 120 Hz.  <br /><br />]]></description>
<pubDate>Fri, 13 Nov 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=170</guid>
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<title>107 Proposals Received for November Call for LCLS Proposals</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=141</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/141_150.jpg" alt="" /><br />The third LCLS Call for Proposals ended on Wednesday, November 4 at 4 pm. This deadline was extended for an additional day after demand during the last few hours before the deadline temporarily overloaded our servers. We apologize for the delay and urge users to plan ahead and submit their proposals well in advance of the next deadline which is Thursday, April 1, 2010. <br /><br />This last call resulted in 107 new proposals: 16 for AMO, 32 for SXR, and 59 for XPP. Proposals are now being processed to ensure completeness, then they will be forwarded to the LCLS Proposal Reviewer Panel (PRP) who will identify and coordinate  external referees. The PRP will rank the proposals when they meet in Feburary 2010. <br /><br />User assisted commissioning experiments scheduled for the current initial start up run, which ends December 17, 2009 are posted on the web at http://www-ssrl.slac.stanford.edu/lcls/users/schedules.html<br /><br />The schedule for the next round of user assisted commissioning experiments is being finalized and should be announced shortly. These commissioning experiments should begin ~May 6 and continue through September 14, 2010.<br /><br />To help users plan proposed experiments for the next call (due April 1st), please check the LCLS website for updated policies, see http://www-ssrl.slac.stanford.edu/lcls/users/logistics.html#policies  as well news about the latest operating parameters.<br /> <br />Currently we are limited to a spectral range down to 750 eV, and we will guarantee this spectral range for experiments scheduled in Spring and Fall 2010. We are also developing operations at lower energies, down to 510 eV. We cannot guarantee it at this time (subject to Radiation Physics review and approval), but we are confident enough to solicit proposals for the Fall 2010.  <br /><br />The minimum pulse duration in standard operation is ~ 70 femtoseconds FWHM. We have developed lower current operation which is now available for users. In this low current moded pulse lengths have been shown to be less than 20 femtoseconds. We believe the pulses are much shorter (for reference see http://www-public.slac.stanford.edu/sciDoc/docMeta.aspx?slacPubNumber=slac-pub-13642) and solicit proposals to measure this. <br /><br />The maximum repetition rate of the X-ray flashes is expected to be 60 Hz and we are working on moving to 120 Hz. <br /><br />]]></description>
<pubDate>Wed, 11 Nov 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=141</guid>
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<title>Live from the Main Control Center: The LCLS Real Time Display</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=172</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/172_150.jpg" alt="" /><br />]]></description>
<pubDate>Tue, 10 Nov 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=172</guid>
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<title>Behind Every Great LCLS User, Outstanding Beam Operations</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=171</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/171_150.jpg" alt="" /><br />]]></description>
<pubDate>Tue, 10 Nov 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=171</guid>
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<title>NEW LCLS Parameters Update</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=86</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/86_150.jpg" alt="" /><br />Currently we are limited to a spectral range down to 750 eV, and we will guarantee this spectral range for experiments scheduled in Spring and Fall 2010. We are also developing operations at lower energies, down to 510 eV. We cannot guarantee it at this time (subject to Radiation Physics review and approval), but we are confident enough to solicit proposals for the Fall 2010.  <br /><br />The minimum pulse duration in standard operation is ~ 70 femtoseconds FWHM. We have developed lower current operation which is now available for users. In this low current moded pulse lengths have been shown to be less than 20 femtoseconds. We believe the pulses are much shorter (for reference see http://www-public.slac.stanford.edu/sciDoc/docMeta.aspx?slacPubNumber=slac-pub-13642) and solicit proposals to measure this. <br /><br />The maximum repetition rate of the X-ray flashes is expected to be 60 Hz and we are working on moving to 120 Hz. <br /><br />We will provide updates on additional parameters as they become available.     <br />]]></description>
<pubDate>Tue, 03 Nov 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=86</guid>
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<title>Election Results Annnounced for LCLS Users' Organiztation Executive Committee</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=72</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/72_150.jpg" alt="LCLS-PULSE Logo" /><br />Election results were announced at the LCLS Users' Meeting on October 20, 2009. Congratulations to Todd Ditmire (AMO), Jan Luning (SXR), Oleg Shpyrko (XCS) and Martin Meedom Nielsen (XPP) who were elected to join existing members of the LCLS Users' Executive Committee (LCLS UEC):<br /><br />Dick Lee, LLNL Matter in Extreme Conditions (MEC) - CHAIR<br />Anton Barty, LLNL Coherent X-ray Imaging (CXI) <br />Thomas Earnest, LBNL Coherent X-ray Imaging (CXI) <br />Phil Heimann, LBNL Soft X-ray Science (SXR) <br />Hyotcherl Ihee, KAIST X-ray Pump-Probe (XPP) <br />Art J Nelson, LLNL Matter in Extreme Conditions (MEC) <br />Mark Sutton, McGill U. X-ray Correlation Spectroscopy (XCS) <br />Linda Young, ANL Atomic, Molecular and Optical Science (AMO) <br />Cathy Knotts, SLAC LCLS/SSRL Liaison (Ex Officio) <br />Katherine Kantardjieff, CSU Fullerton, Crystallography (Ex Officio, SSRL UOEC Chair) <br /><br />http://www-conf.slac.stanford.edu/ssrl-lcls/2009/LCLS_UOECelection.asp]]></description>
<pubDate>Sun, 01 Nov 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=72</guid>
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<title>Christoph Bostedt at the AMO</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=168</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/168_150.jpg" alt="Video by Calla Cofield and Brad Plummer." /><br />]]></description>
<pubDate>Wed, 28 Oct 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=168</guid>
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<title>SSRL/LCLS Users' Meeting Wraps Up</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=167</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/167_150.jpg" alt="Monday's first plenary session in Panofsky Auditorium. (Photo by Lauren Knoche.)" /><br />]]></description>
<pubDate>Wed, 21 Oct 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=167</guid>
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<title>LCLS: The World's Largest Laser Writer?</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=166</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/166_150.jpg" alt="The letters "LCLS" were etched during LCLS instrument commissioning. (Image: LCLS scientific team.)" /><br />]]></description>
<pubDate>Mon, 19 Oct 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=166</guid>
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<title>LCLS Users Test X-ray Laser's Effects on Atoms, Molecules Next</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=160</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/160_150.jpg" alt="Visiting scientists from The Ohio State University with LCLS colleagues. (Photo: Nicholas Bock.)" /><br />]]></description>
<pubDate>Thu, 15 Oct 2009 15:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=160</guid>
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<title>Seminar: Mapping the conformations of biological assemblies</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=159</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/159_150.jpg" alt="LCLS-PULSE Logo" /><br />LCLS-PULSE seminar "Mapping the conformations of biological assemblies", Dr. Abbas Ourmazd, University of Wisconsin Milwaukee, October 14, 2009, 4:00-5:00 PM, Bldg 137, Room 322.<br /><br />The LCLS offer a powerful route to recovering the structure of individual biomolecules from random diffraction snapshots of series of identical molecules.  However, biological molecules can assume a variety of conformations.  Mapping the conformational heterogeneity of macromolecules presents a formidable challenge to X-ray crystallography, single-molecule coherent diffraction, and cryo-electron microscopy.  This has severely limited our knowledge of the conformations assumed by biological systems and their role in biological function, even though they are known to be important.  We propose a new approach to determining to high resolution the three-dimensional conformations of biological entities such as molecules, macromolecular assemblies, and ultimately cells, with existing and emerging experimental techniques.  This approach may also enable one to circumvent current limits due to radiation damage and solution purification.<br /><br />For more information, contact Yiping or Haidan LCLS-PULSE seminar organizers.<br /><br />Yiping Feng<br />LCLS, Photon Division, X-ray Science Department SLAC National Accelerator Laboratory<br />2575 Sand Hill Road, Building 280A/Room 288 Menlo Park, CA 94025<br /><br />(650) 926-2890 - Office<br />(408) 888-9827 - Cell<br />(650) 926-3615 - Fax]]></description>
<pubDate>Wed, 14 Oct 2009 11:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=159</guid>
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<title>From the Director of LCLS: Ramping Up User Science</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=161</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/161_150.jpg" alt="" /><br />]]></description>
<pubDate>Fri, 09 Oct 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=161</guid>
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<title>Crafting Coherence</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=164</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/164_150.jpg" alt="The Echo-7 experiment." /><br />]]></description>
<pubDate>Mon, 05 Oct 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=164</guid>
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<title>PHOTONIC FRONTIERS: Linac Coherent Light Source begins operation</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=158</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/158_150.jpg" alt="A dozen LCLS undulators (silver) installed along the undulator hall." /><br />]]></description>
<pubDate>Thu, 01 Oct 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=158</guid>
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<title>LCLS Launches User Science Today </title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=157</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/157_150.jpg" alt="The AMO instrument scientists with the first LCLS users in the instrument hutch." /><br />]]></description>
<pubDate>Thu, 01 Oct 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=157</guid>
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<title>Seminar: THz pulses from 4th generation lightsources: Perspectives for fully synchronized THz pump X-ray probe experiments</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=122</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/122_150.jpg" alt="LCLS-PULSE Logo" /><br />LCLS-PULSE seminar  "THz pulses from 4th generation lightsources: Perspectives for fully synchronized THz pump X-ray probe experiments", Dr. Michael Gensch, BESSY, Helmholtz-Center Berlin, Wednesday, September 23, 2009, 4:00-5:00 PM, Bldg 137, Room 322.<br /><br />For more information, contact Yiping or Haidan LCLS-PULSE seminar organizers.<br /><br />Yiping Feng<br />LCLS, Photon Division, X-ray Science Department SLAC National Accelerator Laboratory<br />2575 Sand Hill Road, Building 280A/Room 288 Menlo Park, CA 94025<br /><br />(650) 926-2890 - Office<br />(408) 888-9827 - Cell<br />(650) 926-3615 - Fax<br /> <br /><br /><br />]]></description>
<pubDate>Wed, 23 Sep 2009 23:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=122</guid>
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<title>First Test of New X-ray Laser Strips Neon Bare</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=155</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/155_150.jpg" alt="The main experimental chamber of the AMO instrument, the high-field physics end-station. " /><br />]]></description>
<pubDate>Fri, 18 Sep 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=155</guid>
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<title>Where the LCLS Ends: The SXR Beamline </title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=154</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/154_150.jpg" alt="" /><br />]]></description>
<pubDate>Tue, 15 Sep 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=154</guid>
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<title>Performance of a picosecond x-ray delay line unit at 8.39 keV</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=147</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/147_150.jpg" alt="Three-dimensional model of the delay line." /><br />A prototype device capable of splitting an x-ray pulse into two adjustable fractions, delaying one of them with the aim to perform x-ray photon correlation spectroscopy and pump–probe type studies, was designed, manufactured, and tested. The device utilizes eight perfect silicon crystals in vertical 90° scattering geometry. Its performance has been verified with 8.39 keV synchrotron radiation. The measured throughput of the device with a Si(333) premonochromator at 8.39 keV under ambient conditions is 0.6%. Time delays up to 2.62 ns have been achieved, detected with a time resolution of 16.7 ps. © 2009 Optical Society of America.]]></description>
<pubDate>Fri, 04 Sep 2009 22:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=147</guid>
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<title>LCLS Team Awarded FEL Prize, Certificate</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=144</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/144_150.jpg" alt="" /><br />Last week at the 31st Free Electron Laser Conference in Liverpool, United Kingdom, SLAC physicists David Dowell and Paul Emma were awarded the FEL Prize for their technical achievements with the Linac Coherent Light Source, and John Galayda accepted a certificate for the entire LCLS team, lauding their excellent work in creation and commissioning of the unprecedented machine. <br /><br />The FEL Committee awards one prize each year to a person or people whose work has advanced the field of free-electron laser science. After four years of construction, the LCLS team achieved the world's brightest short-pulse, hard X-ray laser light in April of this year. The LCLS worked perfectly on the first try. "It was exciting that such a machine started up so quickly," said Emma, who led the LCLS commissioning effort. <br /><br />Emma said that Dowell deserves much credit for this immediate success. Dowell designed the radio frequency electron gun that creates pulses of electrons to travel through the SLAC linac to the LCLS undulator magnets, where the very bright X-rays are created. <br /><br />The FEL prize, by tradition, recognizes outstanding technical research or design. In conjunction with this year's prize, John Galayda—director of construction for the LCLS project—received a special award certificate on behalf of the LCLS team. <br /><br />"The certificate was an acknowledgement by the FEL international organizing committee of the outstanding performance of the entire LCLS team," said Galayda. Conference Chairman Mike Poole, who presented the certificate, suggested that it be displayed in the Main Control Center. Galayda intends to make copies for LCLS contributors Lawrence Livermore National Laboratory and Argonne National Laboratory. <br /><br />This year's FEL prize breaks a trend that the FEL committee has followed for many years. "In most cases, the FEL prize has been given to exceptional theorists or visionaries who proposed new directions of the field," Emma said. "This is one of the first given to an operating machine." <br /><br />This prize recognizes LCLS as an important advancement in FEL science and therefore is a tribute to all who helped create this revolutionary new light source. "This is one of the first real team prizes," Emma said. "It really should go to all the people at SLAC who worked on the LCLS and demonstrated that this marvelous new light source works, and works well."  <br /><br />]]></description>
<pubDate>Wed, 02 Sep 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=144</guid>
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<title>Revealing the atomic dance</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=149</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/149_150.jpg" alt="The XPCS technique for observing equilibrium dynamics." /><br />]]></description>
<pubDate>Tue, 01 Sep 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=149</guid>
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<title>LCLS News: AMO Instrument Sees First Light</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=143</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/143_150.jpg" alt="" /><br />The Linac Coherent Light Source X-ray beam streamed into the Atomic, Molecular and Optical Science instrument for the first time. <br /><br />"The beam has been banging on the door of our hutch since Friday," AMO Instrument Scientist John Bozek said yesterday as researchers swarmed the instrument to make final adjustments. <br /><br />After insuring that all of the necessary controls, hardware, safety authorizations and radiation protection surveys were completed and in place, Bozek and his team opened the beam shutter at 8:14 p.m., letting in the beam and bathing the instrument in the world's brightest, shortest pulses of laser X-rays. <br /><br />The AMO team is now carefully aligning the instrument and will spend the next six weeks finalizing preparations for the first experiments, which will begin on October 1. <br /><br />"Everybody involved has done a great job and worked very hard," said Bozek. "We're all just thrilled to see the beam passing through the instrument for the first time!" <br />]]></description>
<pubDate>Tue, 18 Aug 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=143</guid>
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<title>From the Director of LCLS: From Dream to Reality</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=148</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/148_150.jpg" alt="LCLS Director: Joachim Stöhr" /><br />In 1999, a year before I joined SLAC, Keith Hodgson asked me to chair a committee with the charge to develop and document the scientific case for a new revolutionary light source at SLAC, proposed in 1992 by Claudio Pellegrini of UCLA. It had been named the Linac Coherent Light Source, or LCLS, in the Design Study Report published in 1998. Co-chaired by Gopal Shenoy from Argonne, the committee brainstormed about what to do with pulses of X-rays that were ultrashort and ultrastrong and had this special property called coherence. Many of us went through a rapid learning curve, exploring what such hot beams would do to a sample, what it meant that the pulses were a thousand times faster than before, and how to take advantage of the coherent nature of the X-rays. <br /><br />In essence, the committee was given the opportunity to dream up scientific opportunities afforded by an unprecedented X-ray laser with a wavelength magically shortened by more than 1000-fold compared to conventional lasers. The First Experiments document published in September 2000 proposed five experiments which were presented to the Basic Energy Science Advisory Committee of the Department of Energy on October 10, 2000. I remember worrying whether BESAC would find the experiments sufficiently exciting to give the green light for LCLS construction. <br /><br />Nine years later, the first experimental station will receive X-rays next week. After a commissioning period of the beam and the instrument, users will be given the opportunity in early October to explore their own dreams. These first studies will explore the very basic interactions of the LCLS X-rays with the simplest form of matter, atoms and molecules. The "sample" or "target" hit by the beam will be a volume of gas or a jet of gas which can be continuously replenished so that one does not have to worry about "beam damage"—that is, whether the previous X-ray pulse has changed the target. Typically, scientists will measure the properties (energy, intensity, arrival time) of the products (electrons, ions, photons) that are created by the beam-target interaction. The experiments are surprisingly similar in concept to those carried out throughout SLAC’s history with the linac beam hitting targets in end stations A and B. Yet while those high-energy physics experiments crashed electrons into targets and explored the ultimate building blocks and forces inside the tiny atomic nuclei, the LCLS experiments will address processes happening during the interactions of X-rays with the electronic clouds surrounding the nuclei. <br /><br />For example, one interesting question is whether one can make so-called "hollow atoms" by stripping atoms of its electrons from the inside out. In a simple picture, the electronic cloud surrounding the atomic core is structured like the spherical shells of an onion. Hollow atoms would resemble an onion whose brown skin is unchanged but where one or more of its inner shells is missing. Of course, such an object is unstable and will only exist for an instant of time before collapsing. But the collapse itself is of great interest. When electrons from the outer filled shells simultaneously jump into the inner empty shells, more than one photon or light particle may be emitted per atom and this process would be the foundation of an atomic X-ray laser. <br /><br />While LCLS itself has turned from dream to reality, the users are still anxiously awaiting the exploration of their scientific dreams. <br /><br />—Joachim Stöhr<br />  SLAC Today, August 14, 2009 <br /><br />]]></description>
<pubDate>Fri, 14 Aug 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=148</guid>
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<title>SLAC to Receive Additional $21.8M in Recovery Act Funding for New Research Instruments</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=150</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/150_150.jpg" alt="SLAC National Accelerator Laboratory" /><br />The Department of Energy's SLAC National Accelerator Laboratory will receive $21.8 million in new funding from the American Recovery and Reinvestment Act. The funding will catalyze instrumentation construction and improvements at the laboratory's two light source research facilities, the Linac Coherent Light Source (LCLS) and the Stanford Synchrotron Radiation Lightsource (SSRL). <br /><br />The new funds secured by SLAC are part of the more than $327 million in Recovery Act funding announced by Energy Secretary Steven Chu this week, $220 million of which will go to the Department of Energy's national laboratories to support scientific research, instrumentation and laboratory infrastructure projects across the nation. <br /><br />"These new initiatives will help to create new jobs while allowing the U.S. to maintain its scientific leadership and economic competitiveness," said Secretary Steven Chu. "The projects provide vital funding and new tools for research aimed at strengthening America's energy security and tackling some of science's toughest challenges." <br /><br />With this final round of project funding, the Obama Administration has now approved the full $1.6 billion in Recovery Act funds allotted by Congress to the DOE Office of Science. In total, SLAC has been awarded $90 million in Recovery Act funding. <br /><br />Of the $21.8 million in new funding coming to the laboratory, $20 million will enable the construction of an experimental station for the study of matter in extreme conditions at the LCLS, SLAC's new X-ray laser. <br /><br />"The Matter in Extreme Conditions instrument enabled by the Recovery Act completes the suite of six scientific stations envisioned for the first phase of the LCLS," says Jo Stöhr, LCLS director. "It allows the scientific community to explore, with unprecedented detail, the properties and behavior of matter in extreme states." <br /><br />The MEC instrument has the unique capability of creating and probing new forms of short-lived states of matter that can exist during fusion processes, the evolution of stars and inside supernovae. Matter passing through such transient states may also be the precursor for new types of materials that have yet remained undiscovered. <br /><br />The remaining $1.8 million will be put toward experimental upgrades and equipment at the Stanford Synchrotron Radiation Lightsource. One million dollars will go toward a new experimental station which will allow scientists to study materials in the realistic conditions required for energy, environmental and technological applications. Example applications include the possibility of mimicking photosynthesis for light-induced energy production, studying the structure and role of water in biological systems, and revealing the components and chemistry of crude oil. The other $0.8 million will be for a needed upgrade of the liquid nitrogen cooling systems required to run the facility at planned higher performance. <br /><br />Piero Pianetta, acting SSRL director, says, "This takes us from the dreaming stage to the doing stage very quickly. It accelerates these parts of our program by several years." <br /><br />SLAC National Accelerator Laboratory is a multi-program laboratory exploring frontier questions in photon science, astrophysics, particle physics and accelerator research. Located in Menlo Park, California, SLAC is operated by Stanford University for the U.S. Department of Energy Office of Science.<br /><br />]]></description>
<pubDate>Fri, 07 Aug 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=150</guid>
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<title>LCLS Commissioning News: The LCLS achieved SASE FEL saturation at a fundamental wavelength of 1.5 Angstroms on April 14, 2009</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=138</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/138_150.jpg" alt="" /><br />]]></description>
<pubDate>Wed, 05 Aug 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=138</guid>
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<title>Hard X-ray Workshop: Taking the Unprecedented Even Farther</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=151</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/151_150.jpg" alt="Workshop participants take a break outside the Research Office Building. " /><br />With the launch of the LCLS just around the corner, scientists are already talking about ways to extend the capabilties of the world's first operating hard X-ray free electron laser, or FEL. <br /><br />This was the point of focus for researchers attending the workshop, Science Drivers for Hard X-Ray Upgrades to LCLS, held July 29-31, 2009 at SLAC. The workshop, which drew more than 70 participants from around the world, was organized for researchers to begin considering potential LCLS upgrades with a horizon covering the next 10 years. <br /><br />When the LCLS sees its first scientific user experiments beginning this fall, the X-ray FEL will operate at energies around 800 eV, and will reach energies as high as 8 keV by the end of next year. Scientists at the workshop discussed ways to increase the energy reach by more than a factor of four, focusing on energies up to 30 and perhaps as high as 50 keV. The access to higher energy X-rays would give scientists an even better look at the properties of matter and would drive research in energy science, materials science and biology. <br /><br />SLAC physicist Aymeric Robert, who was one of the organizers of the event, said that the workshop was a first step in establishing the scientific case for LCLS upgrades. <br /><br />"The LCLS was the first machine of its kind to be created, but now that it has had such a startling turn-on we are getting more demanding," he said with a grin. "This workshop was really the start for thinking about what to do next." <br />]]></description>
<pubDate>Tue, 04 Aug 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=151</guid>
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<title>Science Drivers for Hard X-Ray Upgrades to LCLS Workshop </title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=134</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/134_150.jpg" alt="" /><br />]]></description>
<pubDate>Wed, 29 Jul 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=134</guid>
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<title>LCLS Newsletter, Issue 2, July 2009</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=153</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/153_150.jpg" alt="" /><br />]]></description>
<pubDate>Mon, 20 Jul 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=153</guid>
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<title>A New Office Buliding for the LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=128</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/128_150.jpg" alt="" /><br />]]></description>
<pubDate>Fri, 19 Jun 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=128</guid>
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<title>From the Director: The LCLS Users are Coming!</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=131</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/131_150.jpg" alt="" /><br />]]></description>
<pubDate>Fri, 12 Jun 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=131</guid>
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<title>AMO Moves In</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=126</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/126_150.jpg" alt="" /><br />]]></description>
<pubDate>Wed, 03 Jun 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=126</guid>
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<title>From the Director: New ALDs in LCLS, SSRL and PPA and a new directorate in the Making</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=132</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/132_150.jpg" alt="" /><br />The individuals who serve at the associate laboratory director level at SLAC are an extraordinarily dedicated group. For the past two years, Steve Kahn has led the Particle Physics and Astrophysics Directorate through some of the most turbulent years at the laboratory. Dale Knutson has led the Linac Coherent Light Source Directorate for the last year, and brought additional leadership to the laboratory that is delivering success not only in LCLS, but also in the LCLS Ultrafast Science Instruments and other projects at the lab. <br /><br />Effective June 1, David MacFarlane has taken over from Steve as the PPA ALD. David has been at SLAC for three and a half years. We recruited him from UCSD and he has held a series of leadership positions at SLAC. David was BaBar spokesperson from 2004–2006; he was head of Experimental Particle Physics in PPA when I was PPA director, and additionally deputy director of PPA under Steve Kahn. He has recently also been taking a leading role in developing the ATLAS effort for PPA. <br /><br />Effective July 1, Jo Stohr will take over from Dale Knutson as the LCLS ALD. Jo came to SLAC in 2000 and has been director of the Stanford Synchrotron Radiation Lightsource since 2005. When I became lab director, I asked Jo to serve as the ALD for SSRL. Jo has been co-leading the joint light source efforts with Lawrence Berkeley National Laboratory for the past year. He now will bring his experience and broad expertise in light source science to LCLS. I am very grateful that Piero Pianetta has agreed to be the acting ALD for SSRL effective July 1. We will start an international search immediately to find a permanent SSRL ALD. <br /><br />Steve Kahn and Dale Knutson will not have much time to rest. Steve will be going back to a full time leadership role in the LSST. I have asked Dale to help with the formation of a new Accelerator Directorate which we hope to bring up in mid-summer. We are still discussing the structure and content of the Accelerator Directorate, but I feel strongly that as one of three "National Accelerator Laboratories" in the U.S. (the others are Fermi and Thomas Jefferson), I want to have accelerators more visible and more strongly represented in the laboratory organization. <br /><br />Please join me in thanking Steve, Dale, David, Jo and Piero for their dedication to the laboratory. All of these individuals are taking on major responsibilities for the health of the laboratory as a whole. Their dedication is inspiring for all of us. <br />]]></description>
<pubDate>Wed, 03 Jun 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=132</guid>
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<title>LCLS-PULSE Seminar: Nondiabatic Alignment Dynamics</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=124</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/124_150.jpg" alt="" /><br />]]></description>
<pubDate>Wed, 27 May 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=124</guid>
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<title>Where the LCLS Ends: The CXI Instrument</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=125</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/125_150.jpg" alt="" /><br />]]></description>
<pubDate>Tue, 26 May 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=125</guid>
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<title>LCLS-PULSE Seminar: X-ray Thomson Scattering Measurements in Shock-Compressed Matter</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=123</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/123_150.jpg" alt="lcls-pulse logo" /><br />]]></description>
<pubDate>Thu, 21 May 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=123</guid>
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<title>Second LCLS Call for Proposals</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=107</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/107_150.jpg" alt="The AMO and SXR hutches sit in the Near Experimental Hall" /><br /><i>Submit Proposals for Experiments with Soft X-rays at the AMO and SXR Stations Before May 15th</i><br /><br />SLAC National Accelerator Laboratory is currently building the world's first hard X-ray free-electron laser, the <a href="http://lcls.slac.stanford.edu">Linac Coherent Light Source</a> (LCLS), which will start operation in summer 2009. LCLS will produce intense, sub-picosecond pulses of spatially-coherent X-rays. In a flash of about 100 femtoseconds duration, LCLS will provide 10<sup>12</sup> X-ray photons, roughly as many photons as obtained in one second at today's best storage-ringbased synchrotron radiation facilities. LCLS X-rays will enable investigation of systems at the atomic and nano-scale under conditions where the matter is far from equilibrium, and actually undergoing real-time reactions.<br /><br />It is the goal of LCLS to attract a large number of users from diverse fields and to enable a broad set of important experiments that take advantage of the unique capabilities of LCLS. Five experimental stations are currently being constructed to serve the following scientific thrust areas:<br /><br />1. <a href="http://lcls.slac.stanford.edu/amo/">Atomic, molecular and optical science (AMO)</a><br /><br />2. <a href="http://lcls.slac.stanford.edu/sxr/">Investigation of materials with soft X-rays (SXR)</a><br /><br />3. <a href="http://lcls.slac.stanford.edu/xpp/">Diffraction studies of stimulated dynamics (XPP)</a> <br /><br />4. <a href="http://lcls.slac.stanford.edu/cxi/">Coherent imaging of non-periodic objects (CXI)</a><br /><br />5. <a href="http://lcls.slac.stanford.edu/xcs/">Coherent scattering of nano-scale fluctuations (XCS)</a><br /><br />In this second call for proposals, we invite the world's research community to submit scientific proposals for experiments to be carried out during the time period March – July 2010. During this period, only the two soft-X-ray experimental stations at LCLS will be operational: AMO and SXR. The available spectral range will be from 0.8 to 2 keV, and the maximum repetition rate of the Xray flashes is expected to be 60 Hz. <a href="https://oraweb7.slac.stanford.edu/apex/slacprod/f?p=188:1">Proposals must be submitted by May 15, 2009.</a><br /><br />Detailed descriptions of the instruments are available on the <a href="http://lcls.slac.stanford.edu/Instruments.aspx">LCLS User Web site</a>. <br /><br />Find up-to-date information on the AMO beamline at:  <br /><a href="http://lcls.slac.stanford.edu/amo/AMOTechOverview.aspx">http://lcls.slac.stanford.edu/amo/AMOTechOverview.aspx</a><br />Specific questions about the AMO station should be directed to John Bozek (jdbozek@slac.stanford.edu).<br /> <br />Find up-to-date information on the SXR beamline at: <br /><a href="http://lcls.slac.stanford.edu/sxr/SXRTechOverview.aspx">http://lcls.slac.stanford.edu/sxr/SXRTechOverview.aspx</a><br /><a href="http://lcls.slac.stanford.edu/sxr/SXRTechEndStations.aspx">http://lcls.slac.stanford.edu/sxr/SXRTechEndStations.aspx</a><br />For more information about the SXR instruments, contact Michael Rowen (rowen@slac.stanford.edu).<br /><br />Instructions for submitting proposals can be found on the <a href="https://oraweb7.slac.stanford.edu/apex/slacprod/f?p=188:1">LCLS Users Web Site</a>.<br /><i>Note: For security and privacy purposes, users need to register again and get new accounts/passwords (even if they already have accounts from past proposal submissions). </i><br /><br /><a href="https://oraweb7.slac.stanford.edu/apex/slacprod/f?p=188:1">Closing date to submit AMO or SXR Proposals: May 15, 2009</a>]]></description>
<pubDate>Fri, 15 May 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=107</guid>
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<title>LCLS  Special Seminar: Longitudinal Coherence Measurements at FLASH</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=121</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/121_150.jpg" alt="lcls" /><br />LCLS Seminar<br /><br />May 5, 2009<br />10:00 – 11:00 AM<br />Redwood Building (ROB) Bldg 48 Room B<br /><br />Longitudinal Coherence Measurements at FLASH<br /><br />William F. Schlotter<br />University of Hamburg<br />Institute for Experimental Physics<br /><br />ABSTRACT<br /><br />The availability of two XUV pulses with a variable delay opens a new window into the world of ultrafast dynamics.  In 2008 we constructed a wavefront division beamsplitter that uses a Mach Zehnder geometry to impart a tunable delay on XUV pulses of up to 6 ps with sub 200 attosecond scanning precision.<br /><br />In the time domain I will present first order autocorrelation measurements from the split and delay system for XUV pulses at FLASH*.  And in the frequency domain I will show single shot spectra from FLASH.  Together these measurements provide complementary insight into the longitudinal coherence of radiation from a self amplified spontaneous emission free electron laser. <br /><br /><br />To highlight potential applications of the delay line system, I will present a planned experiment to sequentially image ultrafast demagnetization induced by an optical pump on a ferromagnetic film.<br /><br /> <br /><br />*FLASH is a free electron laser in Hamburg, Germany operating at XUV wavelengths.<br /><br /><br />]]></description>
<pubDate>Tue, 05 May 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=121</guid>
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<title>New Era of Research Begins as World's First Hard X-ray Laser Achieves “First Light”</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=113</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/113_150.jpg" alt="The LCLS beam " /><br />]]></description>
<pubDate>Tue, 28 Apr 2009 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=113</guid>
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<title>LCLS-PULSE Seminar:  Tunable angular momentum and ultrafast magnetization dynamics in GdFeCo</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=115</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/115_150.jpg" alt="" /><br />On April, 29, Rabound University Nijmegen's Professor Andrei Kirilyuk will present "Tunable angular momentum and ultrafast magnetization dyanmics in GdFeCo" at 2:00 PM in the Cypress Room, Bldg. 40. <br /><br />]]></description>
<pubDate>Mon, 27 Apr 2009 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=115</guid>
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<title>From the Director of the LCLS Construction: My Thanks to the LCLS Collaboration and SLAC</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=118</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/118_150.jpg" alt="" /><br />]]></description>
<pubDate>Fri, 24 Apr 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=118</guid>
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<title>LCLS-PULSE Seminar: Soft X-Ray Scattering at Beamline 9-0-1 of the Advanced Light Source</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=112</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/112_150.jpg" alt="" /><br />]]></description>
<pubDate>Fri, 10 Apr 2009 14:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=112</guid>
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<title>LCLS-PULSE Seminar: Coherent X-ray Scattering for Nanostructures & Surface Dynamics</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=111</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/111_150.jpg" alt="" /><br />]]></description>
<pubDate>Thu, 09 Apr 2009 23:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=111</guid>
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<title>LCLS-PULSE Seminar: Commissioning Status</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=106</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/106_150.jpg" alt="Seminar" /><br />]]></description>
<pubDate>Thu, 02 Apr 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=106</guid>
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<title>Registration Open: Workshop on Matter in Extreme Conditions</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=108</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/108_150.jpg" alt="The proposed MEC endstation would support studies of materials in extreme environments." /><br />Interested scientists are invited to participate in the proposed Matter in Extreme Conditions endstation at SLAC's Linac Coherent Light Source, the world's first hard X-ray free electron laser. Next month, the workshop "<a href="http://www-conf.slac.stanford.edu/mec2009/default.asp?id=home">Matter in Extreme Conditions</a>" will provide opportunity to discuss the instrumentation needs of the community, as input to the endstation design.<br /><br />The LCLS is nearing completion with operations anticipated in late summer or early fall this year. The proposed MEC endstation would be dedicated to studies of matter in extreme conditions with a focus on high energy density science. The MEC workshop will take place April 13–15 in SLAC's Redwood Conference Room, Building 48. Registration is open, and available online through the <a href="http://www-conf.slac.stanford.edu/mec2009/default.asp?id=registration">Registration Web page</a>.<br /><br />]]></description>
<pubDate>Tue, 31 Mar 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=108</guid>
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<title>LCLS Undulators Installed and Ready for Beam</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=109</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/109_150.jpg" alt="LCLS team members stand by the newly installed undulators." /><br />]]></description>
<pubDate>Mon, 30 Mar 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=109</guid>
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<title>Seminar: LCLS-I and Beyond</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=104</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/104_150.jpg" alt="LCLS-PULSE Seminar: LCLS-I and Beyond" /><br />LCLS-PULSE SEMINAR:<br />LCLS-I and Beyond<br /><br />March 18, 2009<br />4:00 – 5:00 PM<br />Rm. 322, Bldg. 137<br /><br />Dr. Jerome B. Hastings<br />Professor of Photon Science<br />Linac Coherent Light Source<br />SLAC National Accelerator Lab<br /><br />Scientists at SLAC and other institutions have been thinking and modeling upgrades to LCLS. These range from near transform limited pulses to new undulators to polarization control. The properties of LCLS will be reviewed and these opportunities and the challenges they present will be described.]]></description>
<pubDate>Wed, 18 Mar 2009 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=104</guid>
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<title>SLAC Hosts First Meeting of LCLS Instrument Users</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=105</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/105_150.jpg" alt="LCLS Users Tour the Facility" /><br />]]></description>
<pubDate>Mon, 16 Mar 2009 15:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=105</guid>
</item>
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<title>Downtime for the LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=103</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/103_150.jpg" alt="" /><br />]]></description>
<pubDate>Wed, 04 Mar 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=103</guid>
</item>
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<title>Where the LCLS Ends: the XPP Instrument</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=102</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/102_150.jpg" alt="XPP Instrument Scientist David Fritz (center) with the XPP engineers." /><br />]]></description>
<pubDate>Tue, 03 Mar 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=102</guid>
</item>
<item>
<title>From the LCLS Directorate: Commissioning Status</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=101</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/101_150.jpg" alt="Dale Knutson" /><br />]]></description>
<pubDate>Mon, 02 Mar 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=101</guid>
</item>
<item>
<title>Where the LCLS Ends: The AMO Instrument</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=98</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/98_150.jpg" alt="John Bozek stands near a poster showing the AMO instrument." /><br />]]></description>
<pubDate>Wed, 11 Feb 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=98</guid>
</item>
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<title>Undulator Test Lights Up the LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=97</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2009/97_150.jpg" alt="" /><br />]]></description>
<pubDate>Tue, 03 Feb 2009 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=97</guid>
</item>
<item>
<title>First Electrons Stream Through the LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=96</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/96_150.jpg" alt="Physicists and operators in the LCLS control room" /><br />]]></description>
<pubDate>Mon, 15 Dec 2008 16:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=96</guid>
</item>
<item>
<title>Staff LCLS Tour</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=89</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/89_150.jpg" alt="SLAC's LCLS open house on Thursday, Dec. 4 " /><br />]]></description>
<pubDate>Mon, 08 Dec 2008 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=89</guid>
</item>
<item>
<title>LCLS Laser Heater Installed</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=88</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/88_150.jpg" alt="Inside the LCLS injector vault where the laser heater is installed." /><br />]]></description>
<pubDate>Tue, 02 Dec 2008 16:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=88</guid>
</item>
<item>
<title>Turner Construction Hands Off LCLS Site</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=87</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/87_150.jpg" alt="SLAC facilities staff members discuss the Turner-LCLS handover." /><br />]]></description>
<pubDate>Tue, 25 Nov 2008 16:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=87</guid>
</item>
<item>
<title>Sneak a Peek at the LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=85</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/85_150.jpg" alt="The LCLS Beam Transport Hall." /><br />All SLAC staff members are invited to take a sneak peek at the Linac Coherent Light Source on Thursday, December 4. Come revel in the engineering feat of more than 537 meters of tunnel and take in the impressive new equipment while chatting with LCLS scientists.<br /><br />The walking tour will begin in the Beam Transport Hall, work its way through the temperature-controlled Undulator Hall and the subterranean Near Experimental Hall, and end in the cavernous Far Experimental Hall, which was hewn from solid sandstone. (See the <a href="http://lcls.slac.stanford.edu/FacilityMap.aspx">LCLS Facility Map</a> for a full site overview.)<br /><br />The tour will last approximately 45 minutes and requires a steady 3/4-mile walk. Buses will depart from <a href="http://www2.slac.stanford.edu/maps/slacarea.html#gridMap">Parking Lot C</a> every 15 minutes between 9:00–11:00 a.m. and again between 2:00–4:00 p.m. to transport staff to the Beam Transport Hall. To join a tour group, simply sign up for a convenient time on the <a href="http://www-conf.slac.stanford.edu/lcls_tour/">tour registration Web page</a>. Registration will close at noon on Wednesday, December 3. ]]></description>
<pubDate>Mon, 24 Nov 2008 16:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=85</guid>
</item>
<item>
<title>Main Control Center Gets Ergonomic Update</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=84</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/84_150.jpg" alt="" /><br />]]></description>
<pubDate>Mon, 17 Nov 2008 20:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=84</guid>
</item>
<item>
<title>The LCLS in Pictures</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=71</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/71_150.jpg" alt="Inside the LCLS Beam Dump area. " /><br />]]></description>
<pubDate>Fri, 03 Oct 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=71</guid>
</item>
<item>
<title>Sensing the Energy: Calibrating the LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=68</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/68_150.jpg" alt="The LCLS total energy sensor, to be used during commissioning." /><br />]]></description>
<pubDate>Thu, 25 Sep 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=68</guid>
</item>
<item>
<title>Girders Get the Green Light</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=65</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/65_150.jpg" alt="Undulator support girders are now being installed in the Undulator Hall." /><br />]]></description>
<pubDate>Thu, 18 Sep 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=65</guid>
</item>
<item>
<title>People Today: Mike Bogan</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=62</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/62_150.jpg" alt="" /><br />]]></description>
<pubDate>Wed, 10 Sep 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=62</guid>
</item>
<item>
<title>LCLS Efforts at Argonne Recognized</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=61</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/61_150.jpg" alt="Vacuum group Pacesetter Award recipients and colleagues." /><br />Several colleagues at Argonne National Laboratory in Chicago recently received special recognition for their contributions to the Linac Coherent Light Source. The LCLS collaborators received the Pacesetter Award, given each year to Argonne employees who demonstrate outstanding performance on a project.<br /><br />Argonne awarded this year's Pacesetter to 13 individuals for innovation in the development of undulator vacuum chambers, while beating a tight LCLS delivery schedule.<br /><br />From the official citation: "Through careful day-to-day planning, cooperative teamwork, and a high level of effort and focus, this team of individuals successfully delivered 33 undulator control racks close to five weeks ahead of schedule per the request of LCLS installation coordinators. There was no compromise of testing or quality control to meet this ambitious milestone. LCLS management was very impressed and grateful for this early delivery."<br /><br />Click <a href="http://today.slac.stanford.edu/feature/2008/lcls-pacesetter.asp">here</a> for photos of the recipients. ]]></description>
<pubDate>Mon, 08 Sep 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=61</guid>
</item>
<item>
<title>Building the LCLS: Monthly Update</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=67</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/67_150.jpg" alt="" /><br />Construction highlights for the Linac Coherent Light Source (LCLS) this month include:<br /><br />• Preparation for energizing the water handling systems in the Beam Transport Hall and Undulator Hall and throughout the facility.<br /><br />• Installation of sprinklers and ductwork in the Far Experimental Hall.<br /><br />• Electrical grounding installation in the Access Tunnel leading to the FEH. <br /><br />• Continued testing of the pressurized water systems throughout the facility<br /><br />• Applying the epoxy finish to the subbasement floor in the Near Experimental Hall<br /><br />• Mechanical, electrical and plumbing layout for the Far Experimental Hall and Access Tunnel<br /><br />• Installation of emergency lighting and cable trays in the beam dump<br /><br />• Domestic water and sanitary sewer tie-ins to the Access Tunnel on the northeast side of the Collider Hall<br /><br />• Installation and alignment of quadrupole magnets and the first sections of vacuum pipe in the Beam Transport Hall <br /><br />• Installation of an auxiliary cooling tower to enable continued startup and monitoring of the chilled water system in the Central Utilities Plant during shutdown of the main linac<br /><br />• Regrading of the "amphitheater" above the undulator hall, adjacent to building 3.1<br /><br />• Completion of piping insulation in the Central Utilities Plant<br /><br />• Domestic water and sanitary sewer installation in the Far Experimental Hall<br /><br />• HVAC training for Central Utilities Plant facilities support groups<br /><br />• Final installation of the elevator in the Near Experimental Hall]]></description>
<pubDate>Mon, 01 Sep 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=67</guid>
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<title>LUSI Project Completes Critical Decision 2 Review</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=58</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/58_150.jpg" alt="The XPP instrument." /><br />Congratulations to the scientists and engineers of the Linac Coherent Light Source Ultrafast Science Instrumentation project, or LUSI. The team last week successfully completed Department of Energy review for Critical Decision 2, or CD2. This is a huge milestone for the group and for the Linac Coherent Light Source collaboration as a whole, giving the green light to the instrument designs and cost estimates. <br /><br />"I'm sure the LUSI team feels pretty good right now. You’ve earned it," said LCLS director of construction John Galayda during the review closeout session last Thursday.<br /><br />SLAC Director Persis Drell thanked the DOE review panel and offered her congratulations to the LUSI team. "I'm really proud of how this has come together. The laboratory thanks you for your efforts."<br /><br />The three day review took place to evaluate the scientific program underlying the LUSI project, as well as the data collection, control and safety systems associated with the instruments. <br /><br />The LUSI project comprises an initial set of three instruments, to be built by 2012, for use with the LCLS: <a href="http://lcls/slac.stanford.edu/xcs">X-ray Correlation Spectroscopy</a>, <a href="http://lcls/slac.stanford.edu/xpp">X-ray Pump Probe</a>, and <a href="http://lcls/slac.stanford.edu/cxi">Coherent X-ray Imaging</a> instruments.  ]]></description>
<pubDate>Tue, 26 Aug 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=58</guid>
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<item>
<title>LCLS Injector Gun: The One-minute Overhaul</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=56</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/56_150.jpg" alt="Physicist Axel Brachmann with a vacuum transport chamber." /><br />]]></description>
<pubDate>Tue, 26 Aug 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=56</guid>
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<title>LCLS Progress Steps Up: First Vacuum Chambers in the Beam Transport Hall</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=55</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/55_150.jpg" alt="A two-person crew uses a laser to align components in the Beam Transport Hall. " /><br />]]></description>
<pubDate>Tue, 19 Aug 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=55</guid>
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<title>First LCLS Call for Proposals: Experiments With Soft X-rays at the AMO Station</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=54</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/54_150.jpg" alt="AMO high field physics end station" /><br /><div style="text-align:center;font-weight:bold;">Closing date: September 1, 2008</div><br /><br />The Stanford Linear Accelerator Center SLAC is currently building the world’s first hard X-ray free-electron laser, the Linac Coherent Light Source (LCLS), which will start operation in summer 2009. LCLS will produce intense, sub-picosecond pulses of spatially-coherent X-rays. In a flash of about 100 femtoseconds duration, LCLS will provide 1012 X-ray photons, roughly as many photons as obtained in one second at today’s best storage-ringbased synchrotron radiation facilities. LCLS X-rays will enable investigation of systems at the atomic and nano-scale under conditions where the matter is far from equilibrium, and actually undergoing real-time reactions.<br /><br /><p>Four experimental stations are currently being constructed to serve the following scientific thrust areas:<br /><ol><br /><li>Atomic, molecular and optical science (AMO)</li><br /><li>Coherent imaging of non-periodic objects (CXI)</li><br /><li>Coherent scattering of nano-scale fluctuations (XCS)</li><br /><li>Diffraction studies of stimulated dynamics (XPP)<br /><br />Two more stations are currently being planned to serve:</li><br /><li>High energy density science (HED)</li><br /><li>Investigation of materials with soft X-rays (SXR)</li><br /></ol><br /><br />It is the goal of LCLS to attract a large number of users from diverse fields and to enable a broad set of important experiments that take advantage of the unique capabilities of LCLS.<br /><br />LCLS will begin operation in the second half of 2009, providing X-rays in the spectral range 0.8 to 2 keV. The AMO experimental station will be ready for commissioning and first operation during this period. LCLS hereby invites the world’s research community to submit scientific proposals for experiments with soft X-rays at the AMO experimental station. Proposals for the first LCLS operation period (July-December 2009) must be submitted by September 1, 2008.<br /><br />The proposal process is described at the <a href="http://lcls.slac.stanford.edu/user/">LCLS User web site</a><br />(<a href="http://lcls.slac.stanford.edu/user/">http://lcls.slac.stanford.edu/user/</a>) (available by July 1st, 2008).<br /><br />During 2010 it is anticipated that the spectral range of the LCLS will be extended to 8 keV. A call for proposals for the first LCLS hard X-ray station, XPP, as well as for additional soft X-ray experiments, will be issued in early 2009.<br /><br /><p>Specific questions about the AMO station should be directed to John Bozek (<a href="mailto:jdbozek@SLAC.Stanford.EDU">jdbozek@slac.stanford.edu</a>).<br />]]></description>
<pubDate>Thu, 07 Aug 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=54</guid>
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<item>
<title>Building the LCLS: Monthly Update</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=45</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/45_150.jpg" alt="" /><br />Construction highlights for the Linac Coherent Light Source (LCLS) this week include:<br /><br />• Completing the power and lighting installations in the Near Experimental Hall Sub-Basement<br /><br />• Installing domestic water and sanitary sewer tie-ins in Building 750<br /><br />• Completing the wiring installation for Building 921<br /><br />• Preparation for energizing the water handling systems in the Beam Transport Hall and Undulator Hall and throughout the facility.<br /><br />• Installation of sprinklers and ductwork in the Far Experimental Hall.<br /><br />• Electrical grounding installation in the Access Tunnel leading to the FEH. ]]></description>
<pubDate>Fri, 01 Aug 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=45</guid>
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<item>
<title>Building the LCLS: An Image Gallery</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=48</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/48_150.jpg" alt="Inside the cavernous Far Experimental Hall." /><br />]]></description>
<pubDate>Fri, 25 Jul 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=48</guid>
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<title>FLASH Imaging Redux: Nano-Cinema is Born</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=47</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/47_150.jpg" alt="X-rays capture the action as a tiny silicon wafer explodes." /><br />]]></description>
<pubDate>Tue, 08 Jul 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=47</guid>
</item>
<item>
<title>Building the LCLS: Monthly Update</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=44</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/44_150.jpg" alt="" /><br /> Construction highlights for the Linac Coherent Light Source (LCLS) this week include:<br /><br />• Installation of light fixtures and electrical outlets in the Central Utilities Plant.<br /><br />• Excavation and installation of rebar for footing at the north end of the Central Utilities Plant.<br /><br />• Preparations to pour the final floor in the Access Tunnel.<br /><br />• Final preparation for energizing the Central Utilities Plant<br /><br />• Power, lighting and fire alarm installation inside the Beam Dump and Front End Enclosure, as well as road grading above the Beam Dump<br /><br />• Pouring the remainder of the finished floor inside the X-ray Tunnel<br /><br />• Final preparation for beneficial occupancy of the Beam Transport Hall<br /><br />• Paving of the parking lot around the Near Experimental Hall, installation of final baserock around the exterior<br /><br />• Energizing of systems within the Central Utilities Plant<br /><br />• Piping installation and finished floor concrete pour in the Far Experimental Hall<br /><br />• Preparations for finishing out the entrance to the Access Tunnel<br /><br />• Continued energization of systems in the Central Utilities Plant ]]></description>
<pubDate>Fri, 27 Jun 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=44</guid>
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<title>SLAC Welcomes Jochen Schneider to the LCLS Team</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=43</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/43_150.jpg" alt="Jochen Schneider" /><br />This month SLAC welcomes Jochen Schneider, the most recent addition to the Linac Coherent Light Source (LCLS) team. Schneider initially came to SLAC last January as a visiting professor. His appointment as new director of the Experimental Facilities Division for the LCLS marks a big step toward making the LCLS a scientific reality. <br /><br />"We've just had the first workshops for users, which worked out very nicely," Schneider said. "I think it's a very exciting time to get moving."<br /><br />Schneider has a long career with free electron laser research, having developed the research program for the Free electron Laser in Hamburg (FLASH) facility at the Deutsches Elektronen-Synchrotron laboratory (DESY) in Germany. Schneider now brings that expertise to SLAC to create the scientific research and user program for the LCLS. <br /><br />As director of the Experimental Facilities Division for the LCLS, Schneider's primary responsibility will be organizing the transition from LCLS construction to user operations. In June, the LCLS organization hosted the first two user workshops designed to help potential users prepare research proposals—the Atomic, Molecular and Optical and the X-ray Pump-Probe workshops. Schneider says the workshops are crucial for ensuring the LCLS begins producing science as soon as commissioning is complete.<br /><br />"I am thrilled that Jochen has accepted this responsibility," said SLAC Director Persis Drell. "He is an invaluable resource to the laboratory in this role and will be critical in helping us to ensure outstanding early science from LCLS when it turns on."<br /><br />]]></description>
<pubDate>Tue, 24 Jun 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=43</guid>
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<title>First LCLS Users Attend Workshop at SLAC</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=37</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/37_150.jpg" alt="More than 50 prospective users attended the LCLS AMO Workshop at SLAC this week." /><br />This week, more than 50 prospective Linac Coherent Light Source (LCLS) users arrived at SLAC for a workshop focusing on the Atomic, Molecular and Optical (AMO) science instrument. The workshop was geared toward helping future LCLS users prepare proposals to conduct experiments once the LCLS and the AMO instrument comes online.<br /><br />The AMO instrument, which will be housed in the Near Experimental Hall, will be the first experimental LCLS endstation available to users. Scientists will use the AMO instrument to investigate how the simplest forms of matter—atoms, molecules and clusters of molecules—interact with the powerful X-ray pulses of the LCLS, and will yield clues to how such matter behaves on extremely fast timescales. ]]></description>
<pubDate>Tue, 03 Jun 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=37</guid>
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<title>Getting in Under the Ground Floor</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=36</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/36_150.jpg" alt="" /><br />What do you get when you combine 120 concrete trucks filled with more than 1,000 cubic yards of concrete, with 350,000 pounds of steel rebar? "Happy physicists," according to Linac Coherent Light Source (LCLS) Conventional Facilities Manager David Saenz.<br /><br />Yesterday morning, starting at sunrise, scores of concrete trucks rumbled onto the SLAC site to complete what is the last major pour for the LCLS civil construction. The trucks lined up throughout the day at the entrance to the access tunnel behind the Collider Hall to deliver 1,000 cubic yards of concrete to form a single slab floor for the Far Experimental Hall deep beneath SLAC's east hills.<br /><br />Pouring the massive floor as a single slab will give physicists an added degree of flexibility in reconfiguring experimental hutches in the future. Had the floor been poured in sections, the joints between the sections would allow the floor to shift and move in ways that could wreak havoc on the delicate alignment of the LCLS hardware.<br /><br />In the two days alone leading up to the pour, working round the clock, crews put over 190,000 pounds of steel rebar in place to form the rigid skeleton for the slab floor. The crews then spent Thursday delivering concrete through long hoses down the access tunnel, a process that took over 18 hours. ]]></description>
<pubDate>Fri, 30 May 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=36</guid>
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<title>From atom smashers to X-ray movies</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=34</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/34_150.jpg" alt="" /><br />]]></description>
<pubDate>Thu, 29 May 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=34</guid>
</item>
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<title>Building the LCLS: Monthly Update</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=35</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/35_150.jpg" alt="" /><br />Construction highlights from the Linac Coherent Light Source this week include:<br /><br /><br />- Assembling concrete forms adjacent to Building 3.1 in preparation for installation of concrete utility pads.<br /><br />- Installation of boiler exhaust stacks in the Central Utilities Plant.<br /><br />- Installation of cable trays and grounding connections in the Beam Dump and the Front End Enclosure. <br /><br />- Grading the section of PEP Ring Road above the Beam Dump.<br /><br />- Installing cable trays and electrical switchgear in the Front End Enclosure.<br /><br />- Pouring the roof deck and painting the floors of the sub-basement in the Near Experimental Hall.]]></description>
<pubDate>Fri, 23 May 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=35</guid>
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<title>From the Director: Lehman Lauds LCLS</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=31</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/31_150.jpg" alt="SLAC Director Persis Drell" /><br />The Office of Science semi-annually conducts reviews of its large major projects and this week it focused on the Linac Coherent Light Source (LCLS). Dan Lehman, the Director of the Office of Project Assessment in the Office of Science, leads this process and he arrived at SLAC with a large team of world-class scientists, engineers and management consultants to look over all aspects of the LCLS project.<br /><br />While preparation for any review, and especially a Lehman review, takes a lot of work, this is a very constructive process. All aspects of the project are reviewed, with a strong emphasis on organization and management. The review provides a reality check, and when issues are identified, it offers a broad experience base to help identify solutions. The emphasis on positive and constructive feedback is particularly helpful.<br /><br />This week's Lehman review was the best I have seen for the LCLS. The committee was very impressed by the progress since their visit last July. Worrisome technical issues have been nailed; civil construction is nearing completion; and completed tunnels and vast experimental halls are beginning to fill with accelerator hardware. In addition, the commissioning of the electron beam has been very successful and the electron bunch at the end of the linac meets the specifications needed to achieve X-ray free electron laser radiation production. As the committee noted in their closeout briefing, "John Galayda and his project team are to be commended for these achievements, especially in a climate of change and uncertainty."<br /><br />The entire LCLS team deserves an enormous amount of credit for all the accomplishments of the past 9 months, including our collaborators at our partner labs, Argonne and Lawrence Livermore national laboratories. I would particularly like to thank John Galayda for his dedication and hard work. I have to confess that I am more than a little jealous as the LCLS team now enters what I believe is one of the most exciting phases of the project. A little over a year from now, the project plans to deliver the first x-rays to the AMO experiment in the Near Hall and start the early science program for the first users. This next year will be thrilling for the entire lab! ]]></description>
<pubDate>Fri, 16 May 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=31</guid>
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<title>Argonne's Last Stand</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=29</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/29_150.jpg" alt="Mike Zurawel with the LCLS undulator pedestals in End Station A." /><br />Installation of the first undulator pedestals for the Linac Coherent Light Source (LCLS) is set to begin this week in the Undulator Hall. The final shipment of the stands arrived at SLAC last April from Argonne National Laboratory, where they were designed.<br /><br />In all, the LCLS will use two pedestals per undulator, for a total of 66. Each pedestal is carefully designed to dampen the effects of outside vibration. To reduce the influence of slight temperature variations, the pedestals are wrapped with fiberglass blankets and filled with specially prepared sand. A removable plate atop each pedestal carries a set of electric motors and cams designed to make very fine adjustments to the exact position of the undulator—a critical parameter for the LCLS to work.<br /><br />The pedestals are currently housed in End Station A as technicians make final preparations in advance of installation. "Installing the pedestals will be the easy part," says installation manager Mike Zurawel. Once the installation begins, he says, the biggest challenge will be integrating the various undulator systems and commissioning the control systems that keep all the pieces aligned and moving properly.<br /><br />Last week, Argonne lead engineer Geoff Pyle and a team of representatives came to SLAC for "Undulator Week," where collaborators brainstorm about solutions to challenges that crop up. "Argonne has been incredibly helpful helping us get the pedestals ready," Zurawel says. "Last week Geoff and I sat on the floor for an hour figuring out how to adjust the positioning shims. That was fun... it was like play." ]]></description>
<pubDate>Mon, 12 May 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=29</guid>
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<title>XPP Proposal Preparation Workshop, June 20-21, 2008</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=23</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/23_150.jpg" alt="Rendering of the XPP instrument" /><br />In preparation for the upcoming call for proposals to use the LCLS for XPP experiments, a workshop will be held at SLAC June 20-21, 2008 to inform future XPP users of the status of the LCLS and assist them with preparing their proposals for beam time.  Details of the XPP instrumentation and the performance parameters of the LCLS will be presented along with discussions of ideas and details of the expected proposal to successful experiment processes.  Please see <a href="http://www-conf.slac.stanford.edu/xpp">the workshop site</a> for more details and to register.]]></description>
<pubDate>Mon, 21 Apr 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=23</guid>
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<title>AMO Proposal Preparation Workshop, June 2-3, 2008</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=22</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/22_150.jpg" alt="3D rendering of the AMO instrument" /><br />In preparation for the upcoming call for proposals to use the LCLS for AMO experiments, a workshop will be held at SLAC June 2-3, 2008 to inform future AMO users of the status of the LCLS and assist them with preparing their proposals for beam time.  Details of the AMO instrumentation and the performance parameters of the LCLS will be presented along with discussions of ideas and details of the expected proposal to successful experiment processes.  Please see the <a href="http://www-conf.slac.stanford.edu/amo/2008/">AMO workshop website</a> for more details and to register.]]></description>
<pubDate>Fri, 11 Apr 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=22</guid>
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<title>March 2008 AMO Status</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=21</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/21_150.jpg" alt="3D rendering of the AMO instrument" /><br />The AMO end-station is in the final design process, with detailed drawings of the mechanical components being produced, commercial components specified and controls and data acquisition software being designed.  This process is expected to last until the summer when a review of the design will be held and procurement of components begin.]]></description>
<pubDate>Fri, 14 Mar 2008 19:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=21</guid>
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<title>Stand and Deliver</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=1</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/1_150.jpg" alt="LCLS construction team with a set of newly arrived support stands" /><br />Last week, trucks arrived with the first shipment of specially designed stands for Linac Coherent Light Source (LCLS) magnets and diagnostics to be installed in the Beam Transport Hall. This section of the LCLS, called the "linac-to-undulator," will connect the end of the linac to the undulator magnet arrays. Preparation for installing the stands is starting now as construction on the Beam Transport Hall nears completion.<br /><br />All together there are more than 200 stands, with the heaviest weighing over half a ton. But for now, only a handful of the stands are on site, and the vendor will store the rest until they are needed simply because of the sheer mass of steel involved. Tim Montagne, the LCLS team leader in charge of the design effort for the stands, said that as a first step toward readying the hardware for installation, a few of the stands were shipped for test fitting of all the representative large magnets.<br /><br />The stands themselves are engineered to virtually eliminate motion due to vibration from things like ventilation fans, circulating cooling water or nearby traffic. The specifications require that the magnets can move no more than 50 nanometers, a distance smaller than the size of a single virus.<br /><br />"What you're seeing represents about one year of work," said Montagne.]]></description>
<pubDate>Thu, 07 Feb 2008 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=1</guid>
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<title>The Underground Panoramas of SLAC</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=2</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/2_150.jpg" alt="The tunnel is prepped for the final breakthrough" /><br />The tunneling breakthrough into the Far Experimental Hall (FEH) of the Linac Coherent Light Source (LCLS) on January 14th was the culmination of months of planning and excavation work. Having begun nearly a year ago, the FEH cavern is nearly complete, with only the pouring of the concrete slab floor remaining. Once the floor is poured, construction of the experimental hutches can begin.<br /><br />The cavern, which measures 50 feet wide, 35 feet tall, and 230 feet long, was excavated in sectioned layers, starting from the top. Over the course of FEH excavation, as each bench was removed, tunneling subcontractor Tolga Togan of Affholder Incorporated documented the process with his camera to create this series of panoramas of the cavern and the road header at work.<br /><br /><a href="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan1_full.jpg"><img src="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan1_big.jpg" alt="Panorama" /></a><br />Working to finish the FEH top heading, which is the ceiling. The road header worked from top to bottom in layers to excavate the FEH. (Click on image for larger version.)<br /><br /><a href="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan2_full.jpg"><img src="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan2_big.jpg" alt="Panorama" /></a><br />Looking directly into the access tunnel, the FEH appears curved in this panorama. Each end is visible as the road header removes the next layer of earth. (Click on image for larger version.)<br /><br /><a href="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan3_full.jpg"><img src="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan3_big.jpg" alt="Panorama" /></a><br />Looking westward, with the access tunnel on the right, and the east end of the FEH out of frame. Removal of the second layer nears completion. (Click on image for larger version.)<br /><br /><a href="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan4_full.jpg"><img src="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan4_big.jpg" alt="Panorama" /></a><br />After removal of the last wall of earth (far left) one layer remains to reach the final floor of the FEH. (Click on image for larger version.)<br /><br /><a href="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan5_full.jpg"><img src="http://www-public.slac.stanford.edu/lcls/images/articleImages/2008/2_pan5_big.jpg" alt="Panorama" /></a><br />Excavation is now complete, and the site is prepped for the final breakthrough, which took place just after this shot. (Click on image for larger version.)]]></description>
<pubDate>Wed, 30 Jan 2008 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=2</guid>
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<title>More Magnetic Milestones in the MMF</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=3</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/3_150.jpg" alt="The first LCLS undulator to be mounted to its girder, undergoing coordinate measurement" /><br />Last week, undulator work in SLAC's Magnetic Measurement Facility (MMF) for the Linac Coherent Light Source (LCLS) entered a new chapter as workers for the first time mated an undulator with the girder to which it will eventually be mounted in the Undulator Hall (UH). This marks a further step toward the beginning of installation, scheduled to begin in the next few months as work on the UH nears completion.<br /><br />As one would expect of a machine as complex as the LCLS, pairing an undulator and girder is a bit more complicated that simply tightening a few bolts. Each undulator weighs 1,800 pounds, and the girders weigh 2,600 pounds—but despite that degree of heft, the interface between the two must be precise down to 20 microns, or one-fifth the width of a human hair. Verifying the precision machining of the girders, which will be mounted permanently to their stands in the UH, is critical to ensuring the undulators may be swapped as needed without having to dismantle the beam pipe. The beam pipe itself will also be secured to the undulator girders.<br /><br />"We're working very hard to certify the undulators conform to the optimal design specifications, and this is one more step toward completing that job," said Metrology Department team leader Eric Lundahl. "It's exciting to see the LCLS moving forward."]]></description>
<pubDate>Tue, 22 Jan 2008 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=3</guid>
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<title>From the Director of LCLS Construction: Okay, So We Build the LCLS and Turn It On—Then What?</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=4</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/4_150.jpg" alt="LCLS Director, John Galayda" /><br />When the Linac Coherent Light Source (LCLS) was first conceived in 1992, an x-ray free-electron laser was considered an expensive and technically high-risk endeavor to create a light source with unprecedented and indeed uncertain potential. Early SLAC reports describing the LCLS concept hint at its scientific potential, but not much more. The LCLS proposal had an advantage that would prove decisive. It took a lot of the cost risk away, because using the SLAC linac would cut several hundred million dollars off the size of the bet one had to make to find out what an x-ray free-electron laser (FEL) could do.<br /><br />Holding down the cost was considered important to keeping the LCLS proposal viable; every effort was made to re-use existing facilities. In 1996, the design made use of the Final Focus Test Beam facility to house the undulator magnets. A 24-meter long enclosure built onto the end of the Final Focus Test Beam (FFTB) was provided for x-ray experiments. The need for longer x-ray beamlines was recognized back then, and the 1996 Design Study Report included a concept for shooting LCLS x-rays to the eastern edge of the SLAC site through a very narrow tunnel.<br /><br />By 1995, however, the scientific potential for an x-ray free-electron laser was getting widespread recognition. The German physics lab DESY proposed a huge FEL facility attached to the TESLA linear collider at the 1996 Future Light Sources workshop in Grenoble, France. It became possible to "think big" about FELs. An expansion of the LCLS concept, to a bundle of four undulator x-ray sources, was written up in 2000.<br /><br />I arrived at SLAC in 2001. By this time the LCLS design had grown. What had been proposed as a single experiment in the Research Yard had become a large building capable of holding four experiment enclosures, and was called the "Near Hall." A "Far Experiment Hall" was located about where the real Near Experiment Hall is located today. In 2002, the Department of Energy (DOE) gave LCLS "Critical Decision 1" approval, thereby accepting the LCLS Conceptual Design. I had the opportunity to meet Ray Orbach, Director of the Office of Science, in September 2002, just before he signed off on CD-1. He asked me pointed questions about the LCLS: Was the design limited in some way? Was it a good long-term investment for the DOE? He made it very clear that he would be satisfied with nothing less than a FEL facility that would be the most advanced in the world—not just when it turned on, but for decades to come and when new competing facilities came on-line. His "criticisms" were music to my ears!<br /><br />I brought the message back to SLAC. The LCLS team got to work. With the enthusiastic support of Jonathan Dorfan and Keith Hodgson, we changed the layout of the LCLS facility to allow expansion to six or more "hard" x-ray FELs. This is the layout which is now being constructed. There is room in the LCLS tunnel for the second of these six undulator sources. The Near Experiment Hall is where the Far Experiment Hall used to be, and the Far Experiment Hall is the underground vault you saw in SLAC Today on Tuesday. The cost of the LCLS went up, but the DOE encouraged the new design as it developed in 2003–2004. We were off and running. The LCLS team and Stanford Synchrotron Radiation Laboratory (SSRL) researchers have published enough forefront ideas for new free-electron laser sources to keep us busy for another 20 years or more. There are concepts for expanding the LCLS beyond the earlier six-undulator layout. The DOE is fully aware of SLAC’s desire to start constructing a second undulator source in the existing LCLS tunnel. The ball is in our court; we must decide which of the many options for the second undulator we should propose.<br /><br />The SLAC linac, the centerpiece of its high-energy physics program since the construction of the lab, was the enabling asset that made it possible to hold down the price of the original LCLS concept. It turns out that the linac ensures that SLAC is capable of hosting the most advanced x-ray FELs that anyone has envisioned to date. The maximum energy of the SLAC linac, 50 GeV, is believed to be about the highest energy beam that one can possibly use to make an FEL work. As of today, we think that a strong case can be made for a world-leading FEL using a 30 GeV beam and there is no FEL proposal in the world that envisions so high an energy. Because of this energy reach, we have an inherent advantage in peak intensity at wavelengths from 50 Angstroms to 1 Angstrom—the size of an atom—and shorter. This gives us the ability to image very dense materials on ultrasmall size scales to a degree impossible anywhere else. The DOE was impressed with the preview of these capabilities presented to them recently by SLAC Director Persis Drell.<br /><br />When it turns on, the LCLS faces a very bright future as the world's top light source. I feel confident that we have met Ray Orbach’s challenge. The LCLS will not be "merely" the world's first "hard" x-ray FEL. SLAC is equipped to lead the world in this research area for years to come.]]></description>
<pubDate>Fri, 18 Jan 2008 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=4</guid>
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<title>LCLS Tunneling Achieves Major, Final Milestone</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=5</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2008/5_150.jpg" alt="John Galayda addresses onlookers just after tunneling crews punched through the final few feet" /><br />Yesterday morning a crowd of about 60 onlookers, bedecked in hard-hats and reflective vests, witnessed the final tunneling break through for construction of the Linac Coherent Light Source (LCLS) in the dimly lit cavern of the Far Experimental Hall (FEH). Crews working in the X-ray Transport Hall punched through the final few feet of earth and into the FEH in dramatic fashion—a crescendo of rumbling gathered until the spiked teeth of the road header gouged a gaping hole through the front wall of the FEH, devouring a sign strung across the spot for the occasion. A short time later, miners on the other side waved their congratulations to the group.<br /><br />Although much finishing work remains to complete the tunnels before LCLS hardware installation can begin, Monday's break through means that the entire LCLS tunnel complex is now physically connected.<br /><br />Department of Energy Site Office Deputy Manager Hanley Lee said that joining the tunnel and FEH is an important step not just for the LCLS, but for SLAC's future. "I know you probably wish you could have done it all by yourself," Lee said, addressing Director of LCLS Construction John Galayda, "but I know you had a pretty big team behind you to make this possible."<br /><br />"Today represents a very big milestone in the final steps toward completing the tunnels for the LCLS project," said SLAC Director Persis Drell. "It's a huge step toward a future program of LCLS science that will define this laboratory in a major way. I would particularly like to mention the professionalism of the SLAC staff, and to thank and acknowledge John Galayda—this, for John, is a very special day."<br /><br />Stay tuned to SLAC Today for a complete video account of the occasion. In the meantime, you can watch a teaser video from yesterday's proceedings (RealPlayer required). And don't forget, you can monitor the ongoing construction progress using the LCLS Dashboard and the two LCLS webcams.]]></description>
<pubDate>Tue, 15 Jan 2008 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=5</guid>
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<title>Underground After Sundown</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=6</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2007/6_150.jpg" alt="The Affholder Inc. second shift tunneling crew working on the LCLS" /><br />While most of SLAC sleeps, a select group remains hard at work, driving ahead construction progress on the Linac Coherent Light Source (LCLS). Since last spring, tunnel contractor Affholder Inc. has used double shifts to speed ahead tunneling progress, with the second shift on the clock from 4:00 p.m. to 2:00 a.m.<br /><br />The leaders of these two teams, Jose Franco and Jose Rios, each have decades of experience digging tunnels and have worked all over the United States. Each says that what stands out the most on Department of Energy projects is the emphasis on safety.<br /><br />"It's nice because I feel like they take care of us," says Franco, a resident of Los Angeles who also helped dig Fermilab's Tevatron tunnel in 2000. "It's very safe... everybody takes precaution."<br /><br />In all, about 15 miners and a handful of electricians and engineers make up the second-shift tunneling crews. When completed this spring, the tunneling portion of the LCLS construction will have lasted 20 months. Franco and Rios agree that the worst part of the job is time spent away from home. Rios, who usually lives in South Carolina, says California is beautiful, but expensive. However, both Franco and Rios concede they do save money on sunscreen.]]></description>
<pubDate>Wed, 12 Dec 2007 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=6</guid>
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<title>LCLS Team Takes Pictures of the Electron Beam</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=8</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2007/8_150.jpg" alt="A camera took this image of the LCLS beam's cross section" /><br />How do you take a picture of something as thin as a strand of hair that's moving at the speed of light?<br /><br />Like professionals who photograph wildlife or fussy babies, the Linac Coherent Light Source (LCLS) team is not daunted. They've adapted several technologies to take pictures of the LCLS electron beam.<br /><br />The pictures ensure that the beam still looks and behaves like it's supposed to after being created by the injector, accelerated, and bent by bunch compressors. For the commissioning work done last spring and summer, researchers used 14 devices installed along the injection line to help bring the electron beam up to spec for its downstream role in creating ultrafast, ultrashort x-ray pulses.<br /><br />Near the beam's source, where the beam is still low in energy, researchers are using scintillating crystals to capture the crosswise dimensions of the beam. The beam shoots through the crystals, transferring kinetic energy that makes the crystals emit light, which nearby cameras detect.<br /><br />After the beam gets accelerated to higher energies, physicists use a different method to picture the beam. They place a piece of aluminum foil hundreds of times thinner than kitchen foil in the beam pipe. The beam passes straight through, but the electromagnetic field that travels with the beam interacts with the foil, reflecting light to well-positioned digital cameras.<br /><br />The vacuum and mechanical manufacturing groups are adding more of these optical transition radiation (OTR) cameras to one of the areas where electron bunches get compressed.<br /><br />"We've had great success with this OTR diagnostic for measuring beam size," said LCLS physicist Henrik Loos.<br /><br />During the next commissioning run this winter, LCLS physicists and engineers will be working to understand and fix a problem that unexpectedly cropped up in one of the OTR devices. Under certain conditions, the electrons radiate collectively, belying the assumption that each electron radiates independently and distorting the measured image.<br /><br />When working well, the OTR pictures give valuable two-dimensional information on the transverse cross-section, or diameter of the beam.]]></description>
<pubDate>Wed, 21 Nov 2007 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=8</guid>
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<title>The LCLS Races Forward</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=9</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2007/9_150.jpg" alt="Inside the Near Experimental Hall crews are finishing out installation of utilities" /><br />Construction crews working on the Linac Coherent Light Source (LCLS) site are busier than ever these days. Last week, the Beam Transport Hall, which bisects the research yard, began receiving the final yards of concrete for the roof after being connected to the Undulator Hall. On the other side of the hill, the Central Utilities Plant (CUP) is taking shape next to the Near Experimental Hall. You can keep track of the action in real-time with the LCLS webcams.]]></description>
<pubDate>Mon, 12 Nov 2007 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=9</guid>
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<title>LUSI Moves Forward</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=10</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2007/10_150.jpg" alt="A cartoon of the planned X-ray Correlation Spectroscopy Instrument" /><br />As construction continues on the experimental halls that will receive the beam from the Linac Coherent Light Source (LCLS), the instruments that will go inside still exist only in the minds and computers of the designers. But in the past few months, those instruments are getting closer to reality.<br /><br />"Right now things are really picking up," says David Fritz, a scientist on the LCLS Ultrafast Science Instruments (LUSI) project.<br /><br />Having received approval of Critical Decision-1 from the Department of Energy (DOE) on Sept. 27, 2007, the project is fully staffed and is in the thick of project engineering and design.<br /><br />"The LCLS is a new type of machine," Fritz says. "Even simple components have to change to be used at LCLS. We're realizing this more and more every day."<br /><br />The LUSI project will continue through 2012, but sufficient instrumentation will be available by mid-2009 so that LCLS science can begin with LUSI instruments immediately after first light.<br /><br />The LUSI group is designing three instruments. The Coherent X-ray Imaging Instrument (CXI) will collect structural information on nanometer-sized objects with the goal to one day study individual biological molecules. Although current technologies require that a protein be crystallized before structural analysis, the CXI will not, allowing scientists to study many molecules that have otherwise remained inscrutable.<br /><br />The X-ray Pump-Probe Instrument (XPP) will use an optical laser to excite a sample that changes upon stimulation with light. The LCLS beam will then probe the changes by collecting and analyzing the scattered x-rays. For example, during photosynthesis chemicals respond to light so quickly that scientists have not been able to decipher the reaction.<br /><br />The X-ray Correlation Spectroscopy Instrument (XCS) will permit scientists to observe the natural motion or dynamics of matter in equilibrium. These equilibrium motions will be observed on times down to the duration of the LCLS beam, 100 femtoseconds. These studies will be applied to polymers, glasses, superconductors and much more.<br /><br />The next target for the LUSI team is to establish the baseline costs and the schedule and be ready for the next DOE review and milestone early in 2008.]]></description>
<pubDate>Tue, 06 Nov 2007 08:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=10</guid>
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<title>Surfing for Granite</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=11</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2007/11_150.jpg" alt="Ben Poling (left) and Ed Akerstrom with the six-ton granite block Akerstrom acquired on Craigslist." /><br />The Linac Coherent Light Source (LCLS) project is a collaboration that brings together components and equipment from dozens of suppliers. Last month, Craigslist.org joined that supply chain. Ed Akerstrom, a member of the LCLS undulator assembly team, scored a huge find—a six-ton block of granite—on the popular website and saved SLAC thousands of dollars in the process.<br /><br />Akerstrom, a machinist who regularly trolls Craigslist.org for deals on tools, found the 15-foot-long granite block by accident. Coincidentally, the seller was associated with a previous SLAC-approved supplier, making acquisition of the stone a lot easier.<br /><br />"He told me about his find on the phone," said Ben Poling, the undulator assembly team leader. "When he said they only wanted $300 for it, I figured he must have the dimensions wrong."<br /><br />Granite blocks of this size provide solid, ultra-stable platforms for mounting sensitive equipment. The team, now working in the Collider Hall, had been searching for such a block to use as part of a production line for pre-setting the beam pipe vacuum chambers before they are mounted to the undulator assemblies. Since its arrival, the block has been milled to surface precision that varies less than half of one thousandth of an inch, achieving what Poling terms "AA grade." A stone of this size and quality normally would cost more than $15,000, but thanks to Akerstrom's online acumen, the group spent a fraction of that.<br /><br />"It cost more to have the stone trucked over to SLAC," said Poling. Once it was finished, the total cost of shipping, mounting and resurfacing was less than $3000, according to Poling.<br /><br />With the new granite block in place, the assembly team can soon start piecing together the associated structures that will hold the undulator magnets. These massive assemblies will comprise 33 undulators divided among 11 individual cells made up of heavy support pedestals, quadrupole focusing magnets, beam position monitors and related components.<br /><br />The LCLS is designed such that many of its key systems, including the undulator magnets, can be fine-tuned as necessary without having to take down the machine. Recently, another key component in this fine-tuning system began arriving at SLAC. Called undulator support movers, these devices contain high-precision motors that can make minute adjustments on the fly to keep the undulators aligned to within a few microns.<br /><br />With a stream of such key components arriving by the week, the undulator assembly team will soon be ready to begin piecing together the undulator assemblies in advance of installation, scheduled to begin next year.]]></description>
<pubDate>Tue, 23 Oct 2007 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=11</guid>
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<title>LCLS on a Pedestal</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=12</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2007/12_150.jpg" alt="Rows of undulators rest in the Collider Hall." /><br />Last week, a team working with the Linac Coherent Light Source (LCLS) construction project repositioned dozens of undulator magnets to make room for pre-assembly of the undulator support pedestals. For months, the undulators have remained stored in wooden crates in the Collider Hall, and now the first stages leading to their installation next year are set to begin.<br /><br />"The most exciting thing for me is just seeing it all start to come together," said Ben Poling, leader of the group that will pre-assemble the undulator support systems. "I've been with this project since the beginning. It's really satisfying."<br /><br />Poling and colleagues are currently making room among the rows of crates for the coming parade of related equipment—vacuum chambers, quadrupole magnets and beam position monitors that the team will soon start piecing together. Assembling these structures calls for a dedicated workspace furnished with high-precision mock-ups—actual replicas of the final support stands—for aligning the components, which Poling's group is currently setting up in the Collider Hall. The undulators will only be installed once the pedestals are in place in the Undulator Hall. In all, the LCLS will use 33 undulators at one time, with seven serving as back-ups.]]></description>
<pubDate>Thu, 18 Oct 2007 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=12</guid>
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<title>From the Director: One Lab</title>
<link>http://lcls.slac.stanford.edu/Article.aspx?article_id=13</link>
<description><![CDATA[<img src="http://lcls.slac.stanford.edu/images/ArticleIcons/2007/13_150.jpg" alt="SLAC Director, Persis Drell" /><br />Pief Panofsky built a laboratory with a single purpose: to probe the fundamental structure of matter with the world’s largest electron accelerator. During his lifetime, the lab reinvented itself many times in order to stay on the frontiers of scientific discovery. Fields of science and the laboratory programs have advanced remarkably in 45 years, but the principles of outstanding science that Panofsky stood for have not changed.<br /><br />We now have a laboratory with a broader scientific mission and we are developing an organization that needs to optimally support that broader mission. My goal as acting director is to optimally position the laboratory to help make a smooth transition to the future scientific programs under a new lab director who will be coming in the spring.<br /><br />My motto for my time as acting director is: One Lab. What does one lab mean? On the science mission side, it means that as one lab we are developing and will articulate a long range vision for the lab of simultaneous excellence in a series of closely linked fields that attack the frontier questions of science. One Lab means that we all recognize the importance of articulating this coherent and integrated vision for the lab’s future scientific programs, and understand how the whole of our programs is much more than just the sum of its parts. This is what makes the lab truly great.<br /><br />On the mission support side, one lab means that the improvement initiative for the laboratory will optimize systems that support the scientific mission across the whole lab. We may find areas where more centralization than we have now is appropriate because it will result in efficiencies or better accountability. But one size does not always fit all, and some aspects of services will always have to be locally managed and tailored for individual programs.<br /><br />One lab means the same standards and expectations for safety performance in all areas of the lab. We have all signed up to Safety First. That means that when we go to do our work, we think of safety first: safety before budget, safety before schedule. We need to be implementing safety systems across the site in a consistent way.<br /><br />One lab means we have a respectful workplace where every employee, no matter what unit they work in, is treated in the same respectful way. Everyone at this site is contributing to the mission of the lab in an important way and should be treated as such.<br /><br />I have been asked, "Why not wait until the new director comes to start making changes?" Simply, Stanford President John Hennessy was very clear when he asked me to take on this job that his expectation of me is to move the lab forward at this time. As acting director, I cannot and will not make major changes in strategic direction at the lab, apart from those already underway, but in areas where we have changes that we know we have to make, I will move aggressively.<br /><br />The future of SLAC and the future of our science are of critical importance to me. I am confident that working together we will be successful during these challenging and very exciting times.]]></description>
<pubDate>Fri, 05 Oct 2007 07:00:00 GMT</pubDate>
<guid>http://lcls.slac.stanford.edu/Article.aspx?article_id=13</guid>
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