qRIXS Capabilities
qRIXS Early Science Capabilities for Run 24
The qRIXS Instrument is a large-scale x-ray emission spectrometer, designed for cutting-edge time-resolved resonant inelastic x-ray scattering experiments on condensed matter systems. It consists of the Sample Chamber and a 6-meter long Spectrometer arm. The Chamber is also suitable for experiments focusing on X-ray Diffraction/Resonant Elastic X-ray Scattering, X-ray reflectivity, and X-ray Absorption Spectroscopy. The following capabilities will be provided:
- 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, ~ 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
- For this Run, experiments carried out at a fixed qRIXS spectrometer angle will be supported.
qRIXS operations in Run 24 will be focused on standard user experiments. Depending on the commissioning results in Run 23, we might schedule Early Science with the LCLS-II superconducting linac at the beginning of Run 24. The Early Science program will be led by the LCLS Materials Sciences Department. If you have interest in participating in the Early Science Program please consider sending a letter of intent to the Materials Sciences department head Apurva Mehta (mehta@slac.stanford.edu) who will coordinate this effort. The department head will work with the user community to develop an LCLS-led Early Science campaign. In preparation for these efforts the following tables summarize the expected x-ray and laser capabilities for the SC accelerator and CARBIDE laser system. The development team(s) will try to provide the largest array of possible capabilities. Please use these tables to guide your thinking on possible Early Science experiments.
Performance Parameters for Run 24
X-ray Parameters | Laser Parameters | ||
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Repetition rate (kHz) | 33 | Repetition rate (kHz) | Adjustable between 1 and 100 |
Energy Range (eV) | 250 - 1100 | Wavelength (nm) | 1030 and up to 4th harmonic, MIR (1.3-16 um tunable, available from CY2025) |
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 |
Energy per pulse (nJ) | >10 | Energy per pulse (μJ) | Depending on the repetition rate, discussion with Giacomo Coslovich is highly encouraged |
Pulse Duration (fs) | <200 | Spot size (μm) | Adjustable between 50 and 200 |
Beamline Resolving Power | >20,000 | 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. |
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 100 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.