2018
DOI: 10.1063/1.4994041
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Attosecond transient absorption instrumentation for thin film materials: Phase transitions, heat dissipation, signal stabilization, timing correction, and rapid sample rotation

Abstract: We present an extreme ultraviolet (XUV) transient absorption apparatus tailored to attosecond and femtosecond measurements on bulk solid-state thin-film samples, specifically when the sample dynamics are sensitive to heating effects. The setup combines methodology for stabilizing sub-femtosecond time-resolution measurements over 48 h and techniques for mitigating heat buildup in temperature-dependent samples. Single-point beam stabilization in pump and probe arms and periodic time-zero reference measurements a… Show more

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Cited by 15 publications
(8 citation statements)
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References 40 publications
(36 reference statements)
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“…If the pump beam has a waist of 30 μm (≈100 μm FWHM), the time taken for the temperature to fall by 90% of the initial jump is 4 ms. This amount is significantly longer than the approximately 10-ns timescales required for bulk samples or thin films on a substrate, and it has been confirmed by heat-flow simulations in real experimental geometries [18]. The repetition rate of pump-probe experiments should then be much less than 250 Hz in order to avoid heat accumulation.…”
Section: Heating As a Source For Systematic Errorsmentioning
confidence: 77%
See 1 more Smart Citation
“…If the pump beam has a waist of 30 μm (≈100 μm FWHM), the time taken for the temperature to fall by 90% of the initial jump is 4 ms. This amount is significantly longer than the approximately 10-ns timescales required for bulk samples or thin films on a substrate, and it has been confirmed by heat-flow simulations in real experimental geometries [18]. The repetition rate of pump-probe experiments should then be much less than 250 Hz in order to avoid heat accumulation.…”
Section: Heating As a Source For Systematic Errorsmentioning
confidence: 77%
“…where α is the thermal diffusivity of the material, which is 2 × 10 −6 m 2 s −1 for VO 2 [18]. If the pump beam has a waist of 30 μm (≈100 μm FWHM), the time taken for the temperature to fall by 90% of the initial jump is 4 ms.…”
Section: Heating As a Source For Systematic Errorsmentioning
confidence: 99%
“…, is computed and averaged over 100 full time-delay scans. The slow drift of the pump-probe delay is stabilized over several hours using periodic reference measurements [14]. The XUV and NIR pulses are s-and p-polarized with respect to the sample surface, respectively [15].…”
mentioning
confidence: 99%
“…There are, however, a number of effective and proven strategies to enhancing the rate of in-plane thermal transport. For truly "free-standing" thin samples in the quasi-2D limit, a useful model to understand the tradeoffs is provided by the equation (Jager et al, 2018):…”
Section: Heat Dissipation and Limitations In Multi-shot Experimentsmentioning
confidence: 99%