1999
DOI: 10.1364/ol.24.001305
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Detection of ultrafast phenomena by use of a modified Sagnac interferometer

Abstract: We describe a time-division interferometer based on the Sagnac geometry for monitoring ultrafast changes in the real and the imaginary components of the refractive index as well as phase changes that are due to surface displacement. Particular advantages of this interferometer are its simple common-path design and operation at normal incidence with a microscope objective for both pumping and probing. Operation is demonstrated by detection of temperature changes and coherent phonon generation in a gold film.

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Cited by 114 publications
(80 citation statements)
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“…The present interferometer design is related to a timedomain Sagnac interferometer first developed for monitoring picosecond longitudinal acoustic pulses in solids 24 and then applied to SAW imaging. 5 Sagnac interferometers, inherently of common-path design with no moving parts, have the advantage of mechanical stability.…”
Section: A Optical Interferometermentioning
confidence: 99%
See 1 more Smart Citation
“…The present interferometer design is related to a timedomain Sagnac interferometer first developed for monitoring picosecond longitudinal acoustic pulses in solids 24 and then applied to SAW imaging. 5 Sagnac interferometers, inherently of common-path design with no moving parts, have the advantage of mechanical stability.…”
Section: A Optical Interferometermentioning
confidence: 99%
“…It is, however, in general also possible to work with much longer values of ␦ , timing the first probe pulse to always arrive before each pump pulse and the second probe pulse after; 24,[41][42][43] in this case one can approximate r 1 as a time-independent quantity. ͑Alternatively, if desired, the interval ␦ can be scanned.͒ The present interferometer design ͑configuration A͒ has the advantage that it is possible to adjust ␦ to an arbitrarily small value by simple axial displacement of mirrors M1 or M2.…”
Section: -3mentioning
confidence: 99%
“…These techniques make use of very short stress pulses, generated by thermoelastic deformation of the surface irradiated by an ultrashort optical pulse, that propagate across the specimen and are subsequently detected by another optical probing pulse after a controlled delay. The detection principle is usually the change in the specimen optical reflectivity (Thomsen et al 1986;Rossignol et al 2005;Vollmann et al 2002), although the change in the surface slope (OBD) (Wright and Kawashima 1992) and interferometric detection (Hurley and Wright 1999) have also been reported. The fine achievable temporal resolution (of the order of picoseconds), lateral resolution (of the order of micrometers), and the specific and expensive equipment needed make these techniques especially adequate for characterizing microstructures and thin films in laboratory, but not well-suited for macroscopic industrial inspection where the temporal and spatial scales are much larger.…”
Section: Laser Velocimetrymentioning
confidence: 99%
“…For the gold film and probe wavelength used, ⌬ is only sensitive to the out-of-plane surface motion. 14 We therefore express our data in terms of the calibrated difference in surface displacement ⌬u z ϭ ⌬ /4 recorded by the two probe pulses ͑that is effectively averaged over the probe beam spatial profile͒. This difference ⌬u z is proportional to the outward surface particle velocity v z ϭ‫ץ‬u z /‫ץ‬t, where v z Ϸ⌬u z / ͑since Ӷ2 / , where is the phonon angular frequency͒.…”
mentioning
confidence: 99%