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Reflective bistability in 1.55 μm laser diode amplifiers

Paradorn Pakdeevanich, M.J. Adams

Published Jan 1, 1998• 0 citations
Publisher

Abstract

Bistable laser amplifiers are attractive for potential application in optical switching because of very low input optical requirement, high extinction ratio and the presence of optical gain. Optical bistability (OB) arises from gain saturation and the associated nonlinear refraction combined with the effect of feedback in the laser cavity. We present the experimental results of bistable characteristics for the case of a 1.55 /spl mu/m symmetric Fabry-Perot (F-P) laser amplifier with uncoated facets. This paper reports a particularly rich variety of behaviour for reflected signals. Three main forms of hysteresis loops are observed on reflection. The hysteresis loop changes from anticlockwise to clockwise hysteresis in the optical input-output characteristic when the drive current or initial phase detuning is changed. The butterfly hysteresis loop is observed experimentally at optical input power as low as 260 /spl mu/W for a drive current equal to 90% of the lasing threshold. The dependence of the optical bistability on drive current, initial phase detuning and injected optical power has been investigated. In the bistable light output-initial phase detuning characteristic, the optimum frequency is shifted downward with an increase in the injected power or the drive current. All measurements are in good agreement with an analytical model.

DOI
10.1049/ic:19980915

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We present experimental measurements of bistable characteristics for the case of a 1.55-/spl mu/m symmetric Fabry-Perot laser amplifier with a particularly rich variety of behavior for reflected signals. Three main forms of hysteresis loops are observed on reflection. The hysteresis loop changes from anticlockwise to clockwise hysteresis in the optical output-input characteristic when the drive current or initial phase detuning is changed. A "butterfly" hysteresis loop is observed experimentally at an optical input power as low as 300 /spl mu/W for a drive current equal to 94% of the lasing threshold. The dependence of the reflective optical bistability on drive current, initial phase detuning, and injected optical pewter has been investigated for the first time in an uncoated 1.55-/spl mu/m amplifier. Measurements of the device voltage shifts on switching reveal hysteresis loops which match those in the corresponding optical powers and which indicate the amount of gain saturation and nonlinear refraction responsible for bistability. An analytical model is used to describe the observed reflective bistability and to give insight into the detailed physical mechanisms responsible.

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Applied Physics Letters•Feb 18, 1991•30 citations
Bistable laser amplifiers are attractive for potential application in optical switching because of very low input optical requirement, high extinction ratio and the presence of optical gain. Optical bistability (OB) arises from gain saturation and the associated nonlinear refraction combined with the effect of feedback in the laser cavity. We present the experimental results of bistable characteristics for the case of a 1.55 /spl mu/m symmetric Fabry-Perot (F-P) laser amplifier with uncoated facets. This paper reports a particularly rich variety of behaviour for reflected signals. Three main forms of hysteresis loops are observed on reflection. The hysteresis loop changes from anticlockwise to clockwise hysteresis in the optical input-output characteristic when the drive current or initial phase detuning is changed. The butterfly hysteresis loop is observed experimentally at optical input power as low as 260 /spl mu/W for a drive current equal to 90% of the lasing threshold. The dependence of the optical bistability on drive current, initial phase detuning and injected optical power has been investigated. In the bistable light output-initial phase detuning characteristic, the optimum frequency is shifted downward with an increase in the injected power or the drive current. All measurements are in good agreement with an analytical model.
We present experimental measurements of bistable characteristics for the case of a 1.55-/spl mu/m symmetric Fabry-Perot laser amplifier with a particularly rich variety of behavior for reflected signals. Three main forms of hysteresis loops are observed on reflection. The hysteresis loop changes from anticlockwise to clockwise hysteresis in the optical output-input characteristic when the drive current or initial phase detuning is changed. A "butterfly" hysteresis loop is observed experimentally at an optical input power as low as 300 /spl mu/W for a drive current equal to 94% of the lasing threshold. The dependence of the reflective optical bistability on drive current, initial phase detuning, and injected optical pewter has been investigated for the first time in an uncoated 1.55-/spl mu/m amplifier. Measurements of the device voltage shifts on switching reveal hysteresis loops which match those in the corresponding optical powers and which indicate the amount of gain saturation and nonlinear refraction responsible for bistability. An analytical model is used to describe the observed reflective bistability and to give insight into the detailed physical mechanisms responsible.
Laser diode amplifiers exhibit optical bistability when biased just below lasing threshold, and have applications as optical memory elements and optical switches, due to their very low switching energy (fJ) and presence of optical gain. While LDAs operated in transmission have received much attention, the reflection mode of operation has been largely neglected. In this paper we present a detailed experimental and numerical investigation of Fabry Perot LDA (FP-LDA) behavior under light injection when operated in reflection. We observe transitions from anticlockwise to clockwise hysteresis with changing bias level or incident wavelength detuning. Moreover, we also report the first experimental observation of X-shaped (or butterfly hysteresis) in this system. Our results are in very good agreement with calculation.>
We present what is to our knowledge the first study of optical bistability in Fabry-Perot laser-diode amplifiers that have asymmetric facet reflectivities. When operated in reflection, the light input-light output characteristics exhibit a transition from counterclockwise to clockwise hysteresis by way of an X-shaped or butterfly hysteresis. This transition can be achieved by a change in either the device bias or the phase detuning of the incident light. Our results are in good agreement with calculation.
In this paper, we observe experimentally the optical bistability induced by the side-mode injection power and wavelength detuning in a single mode Fabry—Pérot laser diode (SMFP-LD). Results show that the bistability characteristics of the dominant and injected modes are strongly dependent on the injected input optical power and wavelength detuning in an SMFP-LD. We observe three types of hysteresis loops: counterclockwise, clockwise, and butterfly hysteresis with various loop widths. In the case of a bistability loop caused by injection power, the transition from counterclockwise to clockwise in the hysteresis direction with the wavelength detuning from 0.028 nm to 0.112 nm is observed in a way of butterfly hysteresis for the dominant mode by increasing the wavelength detuning. The width of hysteresis loop, induced by wavelength detuning is also changed while the injection power is enhanced from −7 dBm to −5 dBm.
We demonstrate optically bistable (light switching light) operation in a room-temperature InGaAsP Fabry-Perot amplifier. The amplifier is an InGaAsP/InP laser structure biased at ~95% of its lasing threshold. It is switched with <3 μW of optical power provided by the mechanically chopped output of a quasi-single-mode InGaAsP/InP laser. The experimental apparatus is depicted in Fig, 1. A change in the refractive Index in the amplifier of only 5 × 10−4 is sufficient to cause switching. Input and output pulses from the nonlinear amplifier are shown in Fig. 2 when the source frequency is initially detuned by 14 GHz from the closest Fabry-Perot mode of the amplifier. Smaller switching powers are required at lesser detunings. The physical mechanism of the intensity-dependent change of the refractive index is thought to be the change in carrier density resulting from stimulated recombination of free carriers.