qRIXS Capabilities
qRIXS Capabilities for Run 27
qRIXS is a dedicated instrument designed to investigate correlated-electron condensed matter systems using a broad range of time-resolved spectroscopy techniques. It will be available for general user proposals in the Run 26 call, operating at the anticipated 120 Hz repetition rate.
The qRIXS instrument supports a variety of experimental modalities, including time-resolved resonant inelastic X-ray scattering (tr-RIXS), transient X-ray absorption, diffraction, and reflectivity. Optical excitation from the terahertz (THz) to ultraviolet (UV) regime is enabled by the Carbide laser system, operating at its fundamental wavelength of 1030 nm.
In general, due to the low repetition rate of LCLS-I, time-resolved RIXS experiments will not be offered unless an exceptionally strong scientific justification is provided.
The following capabilities will be supported:
- Sample positioning on an in-vacuum diffractometer, 6 degrees of freedom, sphere of confusion <50 microns
- At the moment only bulk samples and thin films on substrates will be considered
- A load-lock chamber
- Sample cooling with base temperature ~ 25 K
- Diagnostic paddle for calibration targets, spatio-temporal overlap, etc.
- Laser in- and out- coupling (in co-linear configuration)
- Detectors optimized for x-ray absorption and diffraction
- Arrival time monitor located ~1.5 m from the interaction point
qRIXS operations in Run 27 will be focused on standard user experiments. In preparation for these efforts the following tables summarize the expected x-ray and laser capabilities for the Cu accelerator and CARBIDE laser system.
Performance Parameters for Run 27
X-ray Parameters | Laser Parameters | ||
|---|---|---|---|
Repetition rate (Hz) | 120 | Repetition rate (Hz) | 120 |
Energy Range (eV) | 250 - 1100 | Wavelength (nm) | 1030 and up to 4th harmonic, MIR (1.3-16 um tunable), THz |
Spot Size (um), H x V | 10 x 10, min 1000 max | Pulse Duration (fs) | <50 @ 1030 nm (via the spectral broadening developed in-house), <300 @ MIR, discussion with Giacomo Coslovich is highly encouraged |
Energy per pulse (nJ) | ~10-100 nJ (high-resolution mode); ~1 μJ (low-resolution mode) | Energy per pulse (μJ) | Depending on the wavelength, discussion with Giacomo Coslovich is highly encouraged |
Pulse Duration (fs) | ~200 fs (high-resolution mode); ~50 fs (low-resolution mode) | Spot size (μm) | Adjustable between 100 and 500, discussion with Giacomo Coslovich is highly encouraged |
Beamline Resolving Power | >20,000 (for high-resolution mono grating) ~2000 (for high-throughput mono grating) | Polarization control | Horizontal and vertical, circular |
Combined Spectrometer resolving power | 10,000 @ 931 eV | Arrival time monitor precision (fs) | <20. The overall performance will depend on the machine parameters and instrument configuration, discussion with Giacomo Coslovich is highly encouraged |
Polarization | Linear horiz. |
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The following detectors will be provided to the users:
- Avalanche PhotoDiodes (APD) and Large area photodiodes. The APDs are single-photon sensitive fast detectors suitable for X-ray Absorption Spectroscopy (XAS) in Total Fluorescence Yield (TFY) mode, and for X-ray Diffraction. These detectors will be mounted on an in-vacuum rotatable stage (2-theta arm) and can be placed in the horizontal scattering plane.
- qRIXS spectrometer (Archon).
- The archon CCD pixel dimensions are 1200x4224 px. Dispersion is along the long axis.
- Modes available:
- 2D mode which is binned by 2px along the short axis, i.e. 600 x 4224 px at a frame rate of 1 Hz.
- 1D mode which is full vertical binning along the short axis, i.e. 1x4224 at a frame rate of 102 Hz.
- Depending on timely delivery, an in-vacuum 2D detector will be offered as well, with the following characteristics:
- 512 X 512 pixels
- 50 um pixel size
- 5 kHz full frame readout
This detector will also be mounted on the 2-theta arm
Users are encouraged to contact Apurva Mehta, mehta@slac.stanford.edu and Georgi Dakovski, dakovski@slac.stanford.edu for more information.
qRIXS contacts
Georgi Dakovski
qRIXS Instrument Lead Scientist
(650) 926-5703
dakovski@slac.stanford.edu
Lingjia Shen
Instrument Scientist
(650) 926-3087
lingjias@slac.stanford.edu
Daniel Jost
Instrument Scientist
jostd@slac.stanford.edu
Joshua J. Turner
Instrument Scientist
joshuat@slac.stanford.edu
Jake Koralek
Instrument Scientist
(650) 926-3335
koralek@slac.stanford.edu
Raybel Almeida
Area Manager
(650) 926-3370
rayalm@slac.stanford.edu
Giacomo Coslovich
Laser Scientist
(650) 926-5091
gcoslovich@slac.stanford.edu
Patrick Oppermann
Controls Engineer
(650) 926-2423
oppermann@slac.stanford.edu
Quentin Yougoubare
Mechanical Engineer
(650) 926-4128
qyou@slac.stanford.edu
Peter Nguyen
Science & Engineering Associate
(650) 926-4787
nguyenpk@slac.stanford.edu