1994
DOI: 10.1117/12.176131
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Picosecond detection and broadband mixing of near-infrared radiation by YBaCuO films

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1994
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“…In contrast, for NdGaO3 the boundary resistance is a "bottleneck" for the heat flow within several nanosecond time interval. More properly the relaxation of phonon temperature is governed by the phonon escape time: Tes ; = CpRbd (5) Here d is the film thickness, v the sound velocity, r the phonon transparency of te boundary between film and substrate, Rô is the thermal boundary resistance and c,, is the phonon specific heat. We think this process is essential during the first 5 ns of S-N transition for samples 1 of the transition.…”
Section: Tephmentioning
confidence: 99%
“…In contrast, for NdGaO3 the boundary resistance is a "bottleneck" for the heat flow within several nanosecond time interval. More properly the relaxation of phonon temperature is governed by the phonon escape time: Tes ; = CpRbd (5) Here d is the film thickness, v the sound velocity, r the phonon transparency of te boundary between film and substrate, Rô is the thermal boundary resistance and c,, is the phonon specific heat. We think this process is essential during the first 5 ns of S-N transition for samples 1 of the transition.…”
Section: Tephmentioning
confidence: 99%