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Title: The X-ray Pump–Probe instrument at the Linac Coherent Light Source

Abstract

The X-ray Pump–Probe instrument achieves femtosecond time-resolution with hard X-ray methods using a free-electron laser source. It covers a photon energy range of 4–24 keV. A femtosecond optical laser system is available across a broad spectrum of wavelengths for generating transient states of matter. The instrument is designed to emphasize versatility and the scientific goals encompass ultrafast physical, chemical and biological processes involved in the transformation of matter and transfer of energy at the atomic scale.

Authors:
 [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [1];  [2];  [1]
+ Show Author Affiliations
  1. SLAC National Accelerator Lab., Menlo Park, CA (United States). Linac Coherent Light Source (LCLS).
  2. Paul Scherrer Inst. (PSI), Villigen (Switzerland)
Publication Date:
Research Org.:
SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States)
Sponsoring Org.:
USDOE Office of Science (SC)
OSTI Identifier:
1208881
Alternate Identifier(s):
OSTI ID: 1502967
Grant/Contract Number:  
AC03-76SF00515
Resource Type:
Accepted Manuscript
Journal Name:
Journal of Synchrotron Radiation (Online)
Additional Journal Information:
Journal Name: Journal of Synchrotron Radiation (Online); Journal Volume: 22; Journal Issue: 3; Journal ID: ISSN 1600-5775
Publisher:
International Union of Crystallography
Country of Publication:
United States
Language:
English
Subject:
43 PARTICLE ACCELERATORS; FEL; X-ray; pump-probe; time-resolved

Citation Formats

Chollet, Matthieu, Alonso-Mori, Roberto, Cammarata, Marco, Damiani, Daniel, Defever, Jim, Delor, James T., Feng, Yiping, Glownia, James M., Langton, J. Brian, Nelson, Silke, Ramsey, Kelley, Robert, Aymeric, Sikorski, Marcin, Song, Sanghoon, Stefanescu, Daniel, Srinivasan, Venkat, Zhu, Diling, Lemke, Henrik T., and Fritz, David M. The X-ray Pump–Probe instrument at the Linac Coherent Light Source. United States: N. p., 2015. Web. doi:10.1107/S1600577515005135.
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Chollet, Matthieu, Alonso-Mori, Roberto, Cammarata, Marco, Damiani, Daniel, Defever, Jim, Delor, James T., Feng, Yiping, Glownia, James M., Langton, J. Brian, Nelson, Silke, Ramsey, Kelley, Robert, Aymeric, Sikorski, Marcin, Song, Sanghoon, Stefanescu, Daniel, Srinivasan, Venkat, Zhu, Diling, Lemke, Henrik T., & Fritz, David M. The X-ray Pump–Probe instrument at the Linac Coherent Light Source. United States. https://doi.org/10.1107/S1600577515005135
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Chollet, Matthieu, Alonso-Mori, Roberto, Cammarata, Marco, Damiani, Daniel, Defever, Jim, Delor, James T., Feng, Yiping, Glownia, James M., Langton, J. Brian, Nelson, Silke, Ramsey, Kelley, Robert, Aymeric, Sikorski, Marcin, Song, Sanghoon, Stefanescu, Daniel, Srinivasan, Venkat, Zhu, Diling, Lemke, Henrik T., and Fritz, David M. Tue . "The X-ray Pump–Probe instrument at the Linac Coherent Light Source". United States. https://doi.org/10.1107/S1600577515005135. https://www.osti.gov/servlets/purl/1208881.
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@article{osti_1208881,
title = {The X-ray Pump–Probe instrument at the Linac Coherent Light Source},
author = {Chollet, Matthieu and Alonso-Mori, Roberto and Cammarata, Marco and Damiani, Daniel and Defever, Jim and Delor, James T. and Feng, Yiping and Glownia, James M. and Langton, J. Brian and Nelson, Silke and Ramsey, Kelley and Robert, Aymeric and Sikorski, Marcin and Song, Sanghoon and Stefanescu, Daniel and Srinivasan, Venkat and Zhu, Diling and Lemke, Henrik T. and Fritz, David M.},
abstractNote = {The X-ray Pump–Probe instrument achieves femtosecond time-resolution with hard X-ray methods using a free-electron laser source. It covers a photon energy range of 4–24 keV. A femtosecond optical laser system is available across a broad spectrum of wavelengths for generating transient states of matter. The instrument is designed to emphasize versatility and the scientific goals encompass ultrafast physical, chemical and biological processes involved in the transformation of matter and transfer of energy at the atomic scale.},
doi = {10.1107/S1600577515005135},
journal = {Journal of Synchrotron Radiation (Online)},
number = 3,
volume = 22,
place = {United States},
year = {Tue Apr 21 00:00:00 EDT 2015},
month = {Tue Apr 21 00:00:00 EDT 2015}
}
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Journal Article:
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Publisher's Version of Record
https://doi.org/10.1107/S1600577515005135
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Figures / Tables:

Figure 1 Figure 1: Overview of the XPP instrument layout. Distances are indicated in meters from the center of the diffractometer. S&D are slits and non-destructive intensity diagnostics, DCM is a large-offset double-crystal monochromator, CCM is a channel-cut monochromator, TT is a timetool measuring the arrival time of the optical laser inmore » reference to the X-rays, M1 and M2 are silicon mirrors that can be used to deflect the beam in the vertical direction and can also provide harmonic rejection, L-IN is the laser in-coupling for the optical laser, D is a diagnostic. Components located downstream of the dashed line can be translated into the main LCLS line and allow the XPP instrument to take advantage of the full power and properties of the fundamental. The gray line is the LCLS main line, whereas the black one is offset 600 mm horizontally by the DCM. The sample at the XPP instrument is located approximately 200 m downstream of the undulators.« less
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