2003
DOI: 10.1016/s0168-9002(03)00875-1
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FEL research and development at the SLAC sub-picosecond photon source, SPPS

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Cited by 30 publications
(12 citation statements)
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“…4. The detector was designed to be tested at the SPPS in Stanford, 34 which was, until its shutdown in 2006, a worldwide unique femtosecond x-ray source with a rather moderate photon number per pulse, on the order of 10 6 at the photon energy of 9.4 TABLE I. Total photoionization cross section and mean charge q created per absorbed photon as a function of photon energy ប for the rare gases helium to xenon.…”
Section: Gmds For Hard X-ray Felsmentioning
confidence: 99%
“…4. The detector was designed to be tested at the SPPS in Stanford, 34 which was, until its shutdown in 2006, a worldwide unique femtosecond x-ray source with a rather moderate photon number per pulse, on the order of 10 6 at the photon energy of 9.4 TABLE I. Total photoionization cross section and mean charge q created per absorbed photon as a function of photon energy ប for the rare gases helium to xenon.…”
Section: Gmds For Hard X-ray Felsmentioning
confidence: 99%
“…We describe here diffuse x-ray scattering measurements in which the structural dynamics of the liquid-state and the subsequent ablation process are directly measured with subpicosecond resolution. Measurements were performed at the Stanford linear accelerator center using the sub-picosecond pulse source, a precursor to future hard x-ray free electron lasers [13] and a spontaneous source of 9 keV x-rays with a pulse duration of 80 fs FWHM [14]. The setup is similar to the schematic shown in reference [15].…”
mentioning
confidence: 99%
“…Since the very first ultrafast structural experiments at SPPS [43,103,104], the brightness of XFELs has increased by about one million fold, allowing for the study of more complex systems and photoinduced phenomena such as protein dynamics in crystalline [105][106][107][108][109][110][111][112] and liquid phases, [113] bond formation in the [Au(CN) 2 -] 3 trimer in solution, [114,115] lattice dynamics in individual gold nanoparticles, [116] ultrafast melting of charge and orbital order in PCMO, [117] non-linear lattice dynamics [118] and CWD order in YBCO, [119] visualization of breathing modes in nanocrystals at extreme photoexcitation conditions, [120] photoinduced insulator-to-metal (IM) transitions, [121] warm dense matter physics, [122] and ultrafast crystallization [123] and melting [124] in shock-compressed crystals. Figure 9a-d shows time-resolved X-ray diffraction results obtained by Barends et al [107] at LCLS in the investigation of the ultrafast structural dynamics that follows CO photodissociation in Myoglobin-CO (MbCO).…”
Section: Time-resolved Fs-x-ray Crystallography and Scatteringmentioning
confidence: 99%
“…Thus, the application of intense fs-mid-IR lasers may bring the effective brightness of table-top fs-hard X-ray diffractometers to the level of~10 5 -10 6 photons/pulse (at sample position). This is about one order of magnitude below the flux achieved at the Sub-Picosecond Photon Source (SPPS) [43]. SPPS was a test facility that operated at the Stanford Linear Accelerator Center (SLAC) before the Linac Coherent Light Source (LCLS) became available in 2009 (see section below).…”
Section: Introduction To Fourth-generation Fs-hard X-ray Sources: X-rmentioning
confidence: 99%