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Optical Amplifiers and Their Applications

Output Photon Number Distribution of Erbium-Doped Fiber Amplifiers

G. Saplakoglu, M. CELIK

Published Jan 1, 1992• 2 citations
Publisher

Abstract

Erbium-doped fiber amplifiers (EDFA) are gaining increasing importance in the lightwave communications arena due mainly to their low insertion loss and easy manufacturability. Consequently there is significant motivation in obtaining the photon number distribution at the output of an EDFA taking finite bandwith and line shape of the signal lasers into account. In this paper the photon number distribution at the output of an EDFA resulting from an input wave packet having an arbitrary photon number distribution is evaluated. Previously the output photon number distribution was derived [1] for input fields having Poisson photon number distributions, i.e. for coherent sate input fields. Our treatment is more general in the sense that the input field can be in an arbitrary quantum sate. This generality will enable researchers to evaluate EDFA photon number distributions resulting from non-monochromatic incident fields [for example laser sources with phase and/or intensity noise] simply by using the appropriate input photon number distributions in the equations that will be derived below [see for example [2] for several photon number distributions corresponding to various laser line shapes].

DOI
10.1364/oaa.1992.thc2

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Erbium-doped fiber amplifiers (EDFA) are gaining increasing importance in the lightwave communications arena due mainly to their low insertion loss and easy manufacturability. Consequently there is significant motivation in obtaining the photon number distribution at the output of an EDFA taking finite bandwith and line shape of the signal lasers into account. In this paper the photon number distribution at the output of an EDFA resulting from an input wave packet having an arbitrary photon number distribution is evaluated. Previously the output photon number distribution was derived [1] for input fields having Poisson photon number distributions, i.e. for coherent sate input fields. Our treatment is more general in the sense that the input field can be in an arbitrary quantum sate. This generality will enable researchers to evaluate EDFA photon number distributions resulting from non-monochromatic incident fields [for example laser sources with phase and/or intensity noise] simply by using the appropriate input photon number distributions in the equations that will be derived below [see for example [2] for several photon number distributions corresponding to various laser line shapes].
"Doping a part of the optical fiber core by (Er3+ ) ions in presence of external pumping power will lead to form the erbium-doped fiber amplifier (EDFA).The performance of this optical amplifier depends on (the power and the wavelength of the pumping laser, the power and wavelength of the input signal, amplifier length, ion concentration). These parameters will affect the characteristics of EDFA such as amplifier gain, gain saturation, noise figure and output power. However, these characteristics can be determined by solving the EDFA propagation and rate equations. The solution of these equations of two-level laser medium can be done numerically. In this paper, we are proposed a novel method to solve these equations. The reconstructed results are perfectly coincided the well known numerical results.
Characteristics of noise in erbium doped fiber amplifier (EDFA) are theoretically analyzed and experimentally verified. Four discreet energy models are used for erbium ion transition. Spatially varying photon number for traveling optical field was defined in a spatially divided segment with finite length, whose length is decided by property of the spontaneous emission. Quantitative evaluation of the Langevin noise sources becomes possible by this model. The amplified spontaneous emission was included in terms of discrete longitudinal mode, which is defined for whole length of the EDFA. It was found that the relative intensity noise (RIN) in the EDFA hardly changes with noise frequency in the region higher than several kHz. The phase noise in EDFA also hardly changes with the noise frequency. The frequency noise of the signal light in the EDFA increases proportional to squared value of the noise frequency. The amount of RIN and the phase noise decrease in higher input optical power. Good correspondence between theoretical and experimental results was obtained.
We studied the quantum-statistical properties of pulse amplification in erbium-doped fiber amplifiers (OFAs), including saturation of the atomic population inversion and pump depletion. We use a fully quantum theory to describe the atom-field interaction as wed as the light propagation. The generating function of the output photon number distribution (PND) is determined as a function of time during the course of the pulse, with an arbitrary input PND assumed. For input light with Poisson PND, the output PND is shown to be the Laguerre distribution with parameter 1 at all times smaller than the coherence time /spl tau//sub c/, even in the presence of nonlinear effects. An expression for the photon count moment generating function is found for counting times T/spl Gt//spl tau//sub c/. The mean pulse shape is shown to be altered by the nonlinear amplification. The variance is similarly altered, and the excess amplifier noise is greater at the leading side of the pulse.>
Doping a part of the optical fiber core by (Er3+ ) ions in presence of external pumping power will lead to form the erbium-doped fiber amplifier (EDFA).The performance of this optical amplifier depends on (the power and the wavelength of the pumping laser, the power and wavelength of the input signal, amplifier length, ion concentration). These parameters will affect the characteristics of EDFA such as amplifier gain, gain saturation, noise figure and output power. However, these characteristics can be determined by solving the EDFA propagation and rate equations. The solution of these equations of two-level laser medium can be done numerically. In this paper, we are proposed a novel method to solve these equations. The reconstructed results are perfectly coincided the well known numerical results.
A version of an erbium doped fiber amplifier (EDFA) application scheme designed to increase the efficiency of the simultaneous quantum key distribution session and transmission of information by classical channels in a single optical fiber is explored.A theoretical study of the possibility to use EDFA in the explored way was conducted by numerical simulation methods.The mathematical model is based on the EDFA dynamics equations and the equations that determine the secure key generation rate in case of the subcarrier-wave quantum key distribution.A method for determining the optimal parameters of the scheme under study is described and the evaluation of the feasibility of using EDFA in the explored way is performed.A comparative analysis of the subcarrier-wave quantum key distribution system performance when integrated into an optical network is made in terms of the secure key generation rate for the cases when EDFA is either used or not.The results obtained demonstrate high efficiency of the scheme under study, i.e., the maximum achievable distance of the secure key distribution is increased while maintaining the efficiency of the information transmission.