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IEEE Journal of Quantum Electronics

Analysis of giant pulse amplification in Nd3+doped glass

R. Dumanchin, J. Farcy, M. Michon, P. Vincent

Published Feb 1, 1971• 17 citations
Publisher

Abstract

In a study of the mechanism of giant pulse amplification in Nd3+doped glass, the following measurements have been made: 1) energy extracted from an amplifier as a function of the input energy, 2) relative fluorescence intensity at 0.9μ in a slab, pumped by the emission of a ruby laser, and 3) gain variation after the transit of an intense, short, rectangular pulse. The experimental results have been compared to theoretical results from a model where both metastable and terminal levels are regarded as comprising two components. The unknown multiplicity of the lower component of the terminal level g11appears as a parameter. It is assumed that during the pulse duration, Boltzmann distribution is maintained between the components of each level. A finite terminal level lifetime τnmay be introduced in the model. Best agreement is obtained with the following values of the parameters: amplification cross section\sigma_{21}\simeq 1.8.10^{-20}cm2,g_{11} = 1or 2, and\tau_{11} \geq 100ns.

DOI
10.1109/jqe.1971.1076592

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•Aug 12, 2002•0 citations
In a study of the mechanism of giant pulse amplification in Nd3+doped glass, the following measurements have been made: 1) energy extracted from an amplifier as a function of the input energy, 2) relative fluorescence intensity at 0.9μ in a slab, pumped by the emission of a ruby laser, and 3) gain variation after the transit of an intense, short, rectangular pulse. The experimental results have been compared to theoretical results from a model where both metastable and terminal levels are regarded as comprising two components. The unknown multiplicity of the lower component of the terminal level g11appears as a parameter. It is assumed that during the pulse duration, Boltzmann distribution is maintained between the components of each level. A finite terminal level lifetime τnmay be introduced in the model. Best agreement is obtained with the following values of the parameters: amplification cross section\sigma_{21}\simeq 1.8.10^{-20}cm2,g_{11} = 1or 2, and\tau_{11} \geq 100ns.
Pulse-propagation phenomena of accumulated photon echo signals was investigated for the F3/24(1)–I9/24 transition of the Nd3+ ion doped with 20 ppm concentration in silicate glass fiber (core diameter of 6 μm) at 4.2 K using an 82 MHz mode-locked dye laser. The intensity of the transmitted probe pulses from the Nd3+ fiber was measured as a function of the Nd3+ fiber length. The fiber length for the maximum probe-pulse intensity induced by the pump pulses was determined to be 4 m when the pump pulses of 0.50 mW average power and the probe pulses of 0.25 mW average power were used. We derived the pulse area equations which take into account the coherent interaction between the pulses and the Nd3+ fiber. The fiber-length dependence of the signal intensity was explained well by the pulse area equations.
Several experiments on optically excited ruby are described. First, absorption transitions initiated from the metastable states,t\min{2}\max{3}2Eandt\min{2}\max{3}2T1, are investigated in the photon energy range from 5500 to 45 000 cm-1. The absorption spectrum of these excited states is determined in both\pi-and σ-polarizations and assignments for the observed absorption bands are achieved. Obtained results are compared with other experiments reported in the literature. Next, emission properties of pink ruby are studied in the region near theRlines. The emission spectrum is determined point by point by means of intense flash excitation. The observed weak bands are ascribed to theR'and phonon assistedRtransitions. Laser actions in these bands are discussed and experimental results on phonon terminated laser amplification are presented. An experiment using a giant pulse as an excitation source reveals that the transition time fromt\min{2}\max{3}2Etot\min{2}\max{3}2T1is shorter than a fraction of 1μs at room temperature.
Experimental and theoretical investigations were made of amplifying properties of an active neodymium glass fiber and a regenerative amplification regime was observed. It was found that the intensity gain of such a glass-fiber optical quantum amplifier increased exponentially on increase in the pump energy and corresponded to a regenerative regime. It was found that such a regenerative amplifier could operate on pulses above a certain minimum power. The experimental value of this minimum power was 10 mW. The maximum gain achieved in these experiments was 105 when the active length of the fiber was 40 cm.
"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.
In this work, we have investigated experimentally and theoretically the process of frequency upconversion at low temperatures in rare earth doped vitreous samples. A sample of chalcogenide glass doped with erbium ions (Er3+) was pumped with a laser source at 1.54 μm. We have observed, at room temperature, three different emission bands around 530 nm, 555 nm and 670 nm, originating from the excited state erbium levels 2H11/2, 4S3/2 and 4F9/2 to the 4I15/2 ground-state, respectively. A cryogenic system cooled the sample down to 4 K, and we have recorded many spectra in this range of temperature. We have observed relative increase in the intensity of the green fluorescence, which comes from the level 4S3/2, and also the vanishing emission of the 530 nm line around 210 K. For all emission lines, the frequency upconversion process has been accounted for with three photons absorbed from the pumping source, but saturation effects were observed above 10 mW of incident power. We have made a theoretical treatment of the experimental data and a numeric simulation, which has revealed that the observed behaviors are related to processes that involve step-wise photon absorption and phonon assisted nonradiative decay, both dependent on the temperature and phonon energy of the sample. We also present, in the third chapter, an analytic treatment of pulse propagation in nonlinear media. We have used a variational approach to predict the behavior of an optical pulse propagating in the vicinity of a two-photon resonance, where the third order nonlinearities may be enhanced and limits optical devices development. A possible solution for the problem is the propagation of a pulse with suitable profile and frequency chirp resulting in a balancing of the nonlinear effects.