Nonreciprocal second harmonic generation in CuB<sub>2</sub>O<sub>4</sub>
ORAL
Abstract
In a matter with broken time-reversal and space-inversion symmetries, optical responses can differ for the photons propagating in the opposite directions. The so-called nonreciprocal optical effect has been observed ranging from GHz to X-ray. Especially, CuB2O4 is known to show huge nonreciprocal effects for the linear optical response, such as absorption, luminescence and refraction. In this study, we have investigated nonreciprocity of second harmonic generation. It is demonstrated that such gigantic nonreciprocal effects can show up for not only linear optical responses but also for nonlinear optical responses.
CuB2O4 shows nonreciprocal absorption at 1.405 eV, which corresponds to the intratomic transition of Cu2+ hole [1]. In addition, it has been reported that the large second harmonic signal appears at this transition [2]. Therefore, we expect nonreciprocal second harmonic generation at this photon energy. By carefully tuning the amplitude and phase of electric-dipole and magnetic-dipole transitions, we realize very large nonreciprocal signal reaching 97 %. The temperature dependence and magnetic-field dependence will also be discussed in the presentation.
[1] S. Toyoda et al., PRL 115, 267207 (2015)
[2] R. V. Pisarev et al., PRL 93, 037204 (2004)
CuB2O4 shows nonreciprocal absorption at 1.405 eV, which corresponds to the intratomic transition of Cu2+ hole [1]. In addition, it has been reported that the large second harmonic signal appears at this transition [2]. Therefore, we expect nonreciprocal second harmonic generation at this photon energy. By carefully tuning the amplitude and phase of electric-dipole and magnetic-dipole transitions, we realize very large nonreciprocal signal reaching 97 %. The temperature dependence and magnetic-field dependence will also be discussed in the presentation.
[1] S. Toyoda et al., PRL 115, 267207 (2015)
[2] R. V. Pisarev et al., PRL 93, 037204 (2004)
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Presenters
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Shingo Toyoda
RIKEN CEMS
Authors
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Shingo Toyoda
RIKEN CEMS
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Manfred Fiebig
ETH Zurich and RIKEN CEMS
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Taka-hisa Arima
Department of Advanced Materials Science, University of Tokyo, RIKEN CEMS and University of Tokyo, Univ of Tokyo-Kashiwanoha, Department of Advanced Material Science, The University of Tokyo
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Yoshinori Tokura
RIKEN, Center for Emergent Matter Science (CEMS), RIKEN, Japan, CEMS, RIKEN, RIKEN CEMS and University of Tokyo, Center for Emergent Matter Science (CEMS), RIKEN, RIKEN CEMS, Department of Applied Physics, The University of Tokyo, The University of Tokyo, Center for Emergent Matter Science, RIKEN, RIKEN Center for Emergent Matter Science
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Naoki Ogawa
RIKEN CEMS and JST-PRESTO, Center for Emergent Matter Science (CEMS), RIKEN