2013
DOI: 10.1364/ol.38.002295
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Limits to superweak amplification of beam shifts

Abstract: The magnitudes of beam shifts (Goos-Hänchen and Imbert-Fedorov, spatial and angular) are greatly enhanced when a reflected light beam is postselected by an analyzer, by analogy with superweak measurements in quantum theory. Particularly strong enhancements can be expected close to angles at which no light is transmitted for fixed initial and final polarizations. We derive a formula for the angular and spatial shifts at such angles (which includes the Brewster angle), and we show that their maximum size is limi… Show more

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Cited by 42 publications
(40 citation statements)
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“…Since the adiabatic parameter was not too small in our experiment, we preformed additional calculations of time shifts, which take into account the second-derivative terms in the Taylor expansion of the transmission coefficient T ω ( ). These calculations are presented in the Supplementary Note 2, and the results are similar to the analogous beam-shift calculations by Götte and Dennis [48]. The refined dependences D t ν c ,γ ( ) are plotted in Fig.…”
Section: Resultssupporting
confidence: 76%
“…Since the adiabatic parameter was not too small in our experiment, we preformed additional calculations of time shifts, which take into account the second-derivative terms in the Taylor expansion of the transmission coefficient T ω ( ). These calculations are presented in the Supplementary Note 2, and the results are similar to the analogous beam-shift calculations by Götte and Dennis [48]. The refined dependences D t ν c ,γ ( ) are plotted in Fig.…”
Section: Resultssupporting
confidence: 76%
“…We note that, in this condition, the degree of asymmetry is smaller than the above case. In fact, in the case of elliptical polarization beam with its long axis along to the horizontal direction, there exists a relatively large spatial Imbert-Fedorov shift [38].…”
Section: Experimental Observation and Discussionmentioning
confidence: 99%
“…On the other hand, supposing that the preselected state |H is incident near the Brewster angle, the operator exp(−ik y δ H ) cannot be expanded as 1 − ik y δ H due to the strong coupling [47][48][49][50]. Therefore, the weak value A w in Eq.…”
Section: Theoretical Modelmentioning
confidence: 99%