- CXI - Coherent X-ray Imaging
- MEC - Matter in Extreme Conditions
- MFX - Macromolecular Femtosecond Crystallography
- XCS - X-ray Correlation Spectroscopy
- XPP - X-ray Pump Probe
- SLAC MeV-UED
- LCLS-II Instruments (L2SI)
- NEH 1.1. or TMO - Time-resolved AMO
- NEH 1.2 or Tender X-ray Instrument (TXI)
- NEH 2.2
- Instrument Maps
- Standard Configurations
Line-imaging VISAR (Velocity Interferometer System for Any Reflector) is a useful diagnostic for measuring shock wave velocity of matter in extreme conditions and is used in many laboratories as a tool to study high pressure, shock, and Z-pinch physics. MEC uses VISAR analysis to study shock waves propagating through materials subject to laser-driven plasma-induced shocks and is capable of measuring shock velocities on a nanosecond timescale. Here we describe MEC's experimental setup dedicated to studying VISAR data and our in-house data analysis code which allows users to analyze their data in-situ.
An overview of the theory and mathematical formalism of VISAR analysis can be viewed in the following document:
A presentation about the principles of VISAR analysis can be viewed in the following document:
The MEC experimental endstation can be seen in Fig. 1. An illustration of the original design of the VISAR setup as a part of the experimental endstation can be seen in Fig. 2. The current setup has been modified from its previous design such that the optics and streak cameras are now contained within a two-level enclosure.
A schematic diagram of the basic optical arrangement of needed for making a VISAR arrangement can be seen in Fig. 3. Following the arrows provides a flow-chart for how a VISAR measurement is made, starting from the fiber-coupled single-mode laser.
As portrayed in the above diagram, as a shock front collides with the object of interest, causing it to propagate forward, light emanating from the fiber-coupled single-mode laser is reflected off of the moving surface. The Doppler-shifted light of wavelength lambda is then directed toward an interferometer, where it is split into two separate beams. One of the beams is temporally delayed by the insertion of an etalon in its beam path, and then the two beams are recombined, resulting in a fringe pattern which is recorded by a streak camera. A shift in the fringe pattern corresponds to a phase shift, which can be used to calculate the breakout velocity of the object of interest.
The VISAR laser is an Nd:YAG injection-seeded laser with pulse shaping capabilities. It is driven at a wavelength of 532 nm with a pulse width of 100 ns and a pulse repetition frequency (PRF) of 10 Hz. The total possible output energy of the laser is 30 mJ, however usually no more than ~5 mJ is used so as to not damage the optical fiber that is used for transport. The output of the laser is fiber-optically coupled to the VISAR endstation, since the laser itself does not sit next to the setup (see Fig. 4). The multimode fiberguide used has a core diameter of 1 mm.
The fiber output at the MEC endstation is then directed toward the sample in the target chamber (TC), and the reflected light is then redirected back to the VISAR test setup where it is sent through an interferometer and recorded by the streak cameras. A schematic of this can be seen in the following diagram in Fig. 5.
Relay Imaging System
The sample on which the VISAR laser impinges is imaged back onto the slits of the streak cameras. Cylindrical lenses are used to have a different magnification in the direction parallel and perpendicular to the slits of the streak camera, to increase the contrast of the fringes and maintaining a high resolution for the phase measurement. The design of this imaging system, with the current magnification and Field of View can be seen in Fig. 6.
While the above setup stays the same for the most part, some changes can be made (i.e. swapping out one lens for one with a different focal length) to conform to the users' specifications. These changes should be discussed with the MEC Point of Contact (POC) and/or instrument scientists for the experiment.
MEC's VISAR analysis uses two Mach-Zehnder interferometers for the separate VISAR beds. Each bed has a an etalon of differing thickness, therefore the phase delay between the two beams in each interferometer will be slightly different, thus leading to differing fringe shifts. A 3D diagram of the Mach-Zehnder interferometers can be seen in Figs. 7 and 8.
The Mach-Zehnder interferometers include etalons with lengths <15 cm on motorized linear stages that can travel ~5 cm. The end mirror sits on a motorized stage that can tip, tilt, and translate as needed. Furthermore, they include a white light alignment station with a sensitivity of <2 microns, as well as a flip-up beamblock for remote target imaging and a flip-up reticle for remote CCD alignment check.
By comparing the two different free-surface velocity profiles obtained by the separate VISAR beds, one can find the correct number of 2pi fringe jumps to correct for such that the two free-surface velocities match up.
Optical Streak Cameras
A diagram of the optical streak camera used in MEC's VISAR analysis can be seen below in Fig. 9.
The optical streak cameras used to record the VISAR data are Hamamastu C7700s. They have a high dynamic range of 1500:1 and a temporal resolution of <100 ps depending on the sweep range (sweep windows: 0.5 ns, 1 ns, 5 ns,..., 1 ms). They can capture images in a single shot mode or with repetition frequencies up to 1 kHz. They are connected to output optics and a CCD/CCD control unit.
Currently no analysis program for the VISAR is supported by MEC (the old MECana program is obsolete and not supported any more). Users should bring their own analysis software, or include scientist with the required expertise in their collaboration.
MEC Contact Info
MEC Dept Head
Hae Ja Lee
MEC Area Manager
MEC Laser Area Manager
Control Room: (650) 926-7970
MEC Hutch: (650) 926-7974
Vestibule: (650) 926-7976