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physica status solidi (b)

Dynamical Effects in Increasing Absorption Optical Bistability of Thermal Origin

Martin Kretschmar, F. Henneberger, H. Rossmann, I. N. Haddad

Published Sep 1, 1987• 9 citations
Publisher
DOI
10.1002/pssb.2221430152

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Nonlinear Refraction and Increasing Absorption in HgCdTe Optical Bistability at Room Temperature: an Experimental Study

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Many authors have experimentally examined the nonlinearities of HgCdTe at resonance with the CO2 laser wavelength [1]. At room temperature non1inearities of electronic origin, arising from band filling, are weak because of Auger recombination and are masked by thermal effects. In this communication we extend the analysis of ref. 1 on thermally induced optical bistability at low power: we show, for the first time in HgCdTe, the appearance of clockwise hysteresis cycles in transmission as input power Pi is increased, due to nonlinear absorption. We can account for both absorptive and refractive nonlinear contributions by simultaneous monitoring of transmission and reflection. The Hg0.815Cd0.185Te plates (280 um in thickness, with doping pa =1*1016 cm-3, prepared and polished by Elettronica SpA) were placed without heatsinking in a thermally controlled environment. In Fig. 1 the transmitted (Pt) and reflected (Pr) power is shown as a function of Pi: the three data sets differ in cavity mistuning. The thermooptic effect was measured directly, by a close focus optical pyrometer, and indirectly by taking data at different thermal bath temperature T. The values of Pi at the hysteresis associated to a given cavity interference order (indicated with the symbols of Fig. 1c) drift with T (Fig. 2): the maximum induced temperature increase is inferred to be 30-35°C, with steps of 2.5-3.5°C at the switching points, and a value of dn/dT = -2.8*10-3 K-1 is deduced. Fig. 3 presents numerical results (to be compared with Fig. 1b) obtained parametrically solving the nonlinear Fabry Perot equations using the absorption measured after AR coating one sample face. This nonlinear absorption will be discussed in terms of a free carrier origin.

Topical Meeting on Optical Bistability (OB)•Jan 1, 1988•0 citations
This paper presents an approach to the intracavity interaction of electromagnetic waves with anharmonic lattice vibrations of ionic crystals. The nonlinear lattice dynamics and an expression for the nonlinear polarization are derived in terms of optical phonon modes. In the rotating-wave approximation the total coherent Hamiltonian of the system is derived. Using the corresponding equation of steady states, the increasing absorption optical bistability (IAOB), as a nonlinear effect, is demonstrated. The results show that optical nonlinearities due to the interaction of photons with various elementary excitations of bosonic type such as phonons and excitons may be the origin of IAOB, which is consistent with our previous works.
The switching dynamics of thermally induced optical bistability due to increasing absorption is investigated in thin CdS platelets, at room temperature. Fast and slow components can be observed during the switching process, they depend on the holding point intensity and on the switching pulse energy. It is shown that the transverse relaxation of the temperature in the sample influences this dynamics. The spectral shift of the band to band absorption edge, at the origin of the bistable behavior, is observed in a three beam experiment.
Many authors have experimentally examined the nonlinearities of HgCdTe at resonance with the CO2 laser wavelength [1]. At room temperature non1inearities of electronic origin, arising from band filling, are weak because of Auger recombination and are masked by thermal effects. In this communication we extend the analysis of ref. 1 on thermally induced optical bistability at low power: we show, for the first time in HgCdTe, the appearance of clockwise hysteresis cycles in transmission as input power Pi is increased, due to nonlinear absorption. We can account for both absorptive and refractive nonlinear contributions by simultaneous monitoring of transmission and reflection. The Hg0.815Cd0.185Te plates (280 um in thickness, with doping pa =1*1016 cm-3, prepared and polished by Elettronica SpA) were placed without heatsinking in a thermally controlled environment. In Fig. 1 the transmitted (Pt) and reflected (Pr) power is shown as a function of Pi: the three data sets differ in cavity mistuning. The thermooptic effect was measured directly, by a close focus optical pyrometer, and indirectly by taking data at different thermal bath temperature T. The values of Pi at the hysteresis associated to a given cavity interference order (indicated with the symbols of Fig. 1c) drift with T (Fig. 2): the maximum induced temperature increase is inferred to be 30-35°C, with steps of 2.5-3.5°C at the switching points, and a value of dn/dT = -2.8*10-3 K-1 is deduced. Fig. 3 presents numerical results (to be compared with Fig. 1b) obtained parametrically solving the nonlinear Fabry Perot equations using the absorption measured after AR coating one sample face. This nonlinear absorption will be discussed in terms of a free carrier origin.