2011
DOI: 10.1063/1.3609862
|View full text |Cite
|
Sign up to set email alerts
|

Development of a compact fast CCD camera and resonant soft x-ray scattering endstation for time-resolved pump-probe experiments

Abstract: The designs of a compact, fast CCD (cFCCD) camera, together with a resonant soft x-ray scattering endstation, are presented. The cFCCD camera consists of a highly parallel, custom, thick, high-resistivity CCD, readout by a custom 16-channel application specific integrated circuit to reach the maximum readout rate of 200 frames per second. The camera is mounted on a virtual-axis flip stage inside the RSXS chamber. When this flip stage is coupled to a differentially pumped rotary seal, the detector assembly can … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
52
0

Year Published

2013
2013
2022
2022

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 71 publications
(52 citation statements)
references
References 36 publications
0
52
0
Order By: Relevance
“…Kirkpatrick-Baez optics were used to focus the beam to a spot size with a diameter less than 300 μm. Using the fast-CCD camera (fCCD) [18], we measured the (0q0) diffraction peak in the in-plane scattering geometry as a function of relative delay between collinear propagating x-ray pulses (π-polarized; 100 fs FWHM) and 800 nm (1.55 eV) pump pulses (~120 fs pulse duration; 118 μm 1/e 2 radius; ppolarized). Figure 2(a) shows how the diffraction peak intensity varies with time for absorbed pump fluences ranging from 2.6 to 18.4 mJ/cm 2 , where we have accounted for the reflectivity using dielectric function data from Bastjan et al [21].…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Kirkpatrick-Baez optics were used to focus the beam to a spot size with a diameter less than 300 μm. Using the fast-CCD camera (fCCD) [18], we measured the (0q0) diffraction peak in the in-plane scattering geometry as a function of relative delay between collinear propagating x-ray pulses (π-polarized; 100 fs FWHM) and 800 nm (1.55 eV) pump pulses (~120 fs pulse duration; 118 μm 1/e 2 radius; ppolarized). Figure 2(a) shows how the diffraction peak intensity varies with time for absorbed pump fluences ranging from 2.6 to 18.4 mJ/cm 2 , where we have accounted for the reflectivity using dielectric function data from Bastjan et al [21].…”
Section: Resultsmentioning
confidence: 99%
“…Optical pump, soft X-ray resonant diffraction probe experiments were performed at the Soft X-Ray (SXR) beamline of the Linac Coherent Light Source X-ray Free Electron Laser (LCLS FEL) [17], using the Resonant Soft X-ray Scattering endstation [18]. The (010) cut TbMnO3 single crystal was oriented such that the a axis was in the horizontal scattering plane.…”
Section: Resultsmentioning
confidence: 99%
“…Diffraction data were acquired using the RSXS endstation [30], equipped with a fast avalanche photodiode (integrating over the entire diffraction peak) and a two dimensional fast CCD camera both shielded from the optical pump laser by an Al window. Fig.…”
Section: Methodsmentioning
confidence: 99%
“…In the twodimensional topology, each pixel has its own dedicated readout. The most common one-dimensional detector is the chargecoupled device (CCD), and CCDs of various forms are in use at all XFELs [1][2][3]. CCDs accumulate charge in each pixel, and (noiselessly) transport that charge from pixel-to-pixel.…”
Section: Introductionmentioning
confidence: 99%
“…For single-shot experiments, where all of the photons arrive simultaneously, counting is not possible. 1 Integrating detectors, which integrate all charge received during a certain period, are thus the readout architecture for XFELs.…”
Section: Introductionmentioning
confidence: 99%