1993
DOI: 10.1063/1.110092
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High-frequency polarization self-modulation in vertical-cavity surface-emitting lasers

Abstract: Polarization self-modulation at frequencies up to 6 GHz is observed in a vertical-cavity surface-emitting laser. This self-oscillation is observed when a portion of the laser output power is injected back into the laser after having rotated its polarization by 90° with respect to the initial laser polarization state. Our experiment demonstrates a simple technique for generating an ultrahigh frequency optical clock. New applications in optical storage are also envisioned.

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Cited by 104 publications
(43 citation statements)
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“…1,4 Here, we consider the behavior of a VCSEL under polarization-changing optical feedback, simulating the experimental situation described in Ref. 1. The external cavity is formed by the VCSEL and a partial reflector, and a quarter-wave plate is inserted inside the cavity with its axes rotated by 45°with respect to the polarization basis states of the VCSEL.…”
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confidence: 99%
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“…1,4 Here, we consider the behavior of a VCSEL under polarization-changing optical feedback, simulating the experimental situation described in Ref. 1. The external cavity is formed by the VCSEL and a partial reflector, and a quarter-wave plate is inserted inside the cavity with its axes rotated by 45°with respect to the polarization basis states of the VCSEL.…”
mentioning
confidence: 99%
“…The polarization-state selection, the polarization dynamics, and the polarization switching in VCSELs can be changed by optical injection, 2 current modulation, 3 and by polarizationsensitive optical feedback. 1,4 Here, we consider the behavior of a VCSEL under polarization-changing optical feedback, simulating the experimental situation described in Ref. 1.…”
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confidence: 99%
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“…An optical feedback scheme that has received a lot of attention has been referred to as polarization-rotated (PR) feedback or orthogonal feedback [5][6][7][8][9][10][11][12][13][14]. In this scheme a 90-deg polarization-rotating device is placed in the external cavity, and thus, the associated linear orthogonal polarizations (in the following referred to as x and y) are mutually fed back: x-polarized light is reinjected into the laser as y-polarized light after a delay time τ , and vice versa.…”
Section: Introductionmentioning
confidence: 99%
“…The increase in the feedback/coupling strength typically destabilizes the otherwise steady dynamics to self-pulsation with a period either close to the laser relaxation oscillation frequency or to the feedback/coupling delay time [1]. The waveform can vary from sharp pulsing to harmonic to square wave (SW) depending on the system nonlinearity [2][3][4][5], on the sub-or super-critical nature of the underlying Hopf bifurcation [5,6], on the laser mode competition or on the coupling/feedback parameters [7][8][9][10][11][12][13][14][15]. An interesting combination of these parameters is found in a recent experiment, where two edge-emitting laser diodes are mutually coupled through their orthogonal polarization modes [16].…”
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confidence: 99%