2012
DOI: 10.1063/1.3681254
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Normalization schemes for ultrafast x-ray diffraction using a table-top laser-driven plasma source

Abstract: We present an experimental setup of a laser-driven x-ray plasma source for femtosecond x-ray diffraction. Different normalization schemes accounting for x-ray source intensity fluctuations are discussed in detail. We apply these schemes to measure the temporal evolution of Bragg peak intensities of perovskite superlattices after ultrafast laser excitation.

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Cited by 49 publications
(41 citation statements)
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“…In order to characterize the response of the PZT film to ultrashort stress pulses we excited the SRO electrode with near infrared (800 nm) femtosecond light pulses (τ = 40 fs) and monitored the induced lattice dynamics by UXRD experiments at a laser-driven plasma xray source (PXS) [16,17] in a pump-probe scheme. The generated hard x-ray pulses (E = 8.05 keV (Cu K α ), τ = 150 fs) were collected by a Montel multilayer mirror and focused onto the sample with a convergence of 0.3…”
mentioning
confidence: 99%
“…In order to characterize the response of the PZT film to ultrashort stress pulses we excited the SRO electrode with near infrared (800 nm) femtosecond light pulses (τ = 40 fs) and monitored the induced lattice dynamics by UXRD experiments at a laser-driven plasma xray source (PXS) [16,17] in a pump-probe scheme. The generated hard x-ray pulses (E = 8.05 keV (Cu K α ), τ = 150 fs) were collected by a Montel multilayer mirror and focused onto the sample with a convergence of 0.3…”
mentioning
confidence: 99%
“…The primary intensity of the PXS is considered to be rather unstable when compared to standard x-ray tubes or synchrotron sources [120]. Short timescale pulse J1 A2 A4 A6 A8 A10 A12 A14 A16 A18 A20 A22 A24 A26 A28 A30 A32 C2 C4 C6 C8 C10 C12 C14 C16 C18 C20 C22 C24 C26 C28 C30 J1 A2 A4 A6 A8 A10 A12 A14 A16 A18 A20 A22 A24 A26 A28 A30 A32 C2 C4 C6 C8 C10 C12 C14 C16 C18 C20 C22 C24 C26 C28 C30 C32 IC11 …”
Section: Discussionmentioning
confidence: 99%
“…As detailed in appendix A.1.3, the primary intensity of the PXS is considered to be rather unstable compared to standard x-ray tubes or synchrotron sources [120]. While pulse to pulse uctuations can in principle be eliminated by averaging over many (N ≈ 10000) pulses at a laser repetition rate of 1kHz, long time scale intensity uctuations arising from mechanical unstabilities of the copper tape, increasing debris contamination and uncertainties in the positioning of the laser focus can only be eliminated from the data by a suitable monitor signal.…”
Section: · 10mentioning
confidence: 99%
“…Femtosecond x-ray diffraction experiments have provided detailed insight into the dynamics of semiconductor 45 and perovskite SLs, [77][78][79][80][81][82][83][84][85] in the latter including ultrafast motions along different anharmonically coupled lattice coordinates. 79 Here, we present results for the ferromagnetic SRO/STO superlattice structure introduced in Fig.…”
Section: A Real-space Atomic Motions and Vibrational Dynamicsmentioning
confidence: 99%