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Journal of Physics Condensed Matter

Coherent response in the forward direction to the almost stepwise -pulse

E. A. Popov

Published Jul 15, 1996• 5 citations
Publisher

Abstract

The coherent response in the forward direction to the almost stepwise -pulse (hereafter one supposes that the pure stepwise -pulse is described by a step function) is theoretically analysed. In this way, first of all the analytical form of the -pulse has been obtained when remagnetization of the `magnetic shutter' takes place. The problem is solved by employing the semiclassical Maxwell - Bloch formalism. Then the time evolution of the coherent response to that -pulse is calculated when it propagates through a two-level resonant medium. Finally the theoretical results are used to describe the experiment quantitatively.

DOI
10.1088/0953-8984/8/29/021

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The coherent response in the forward direction to the almost stepwise -pulse (hereafter one supposes that the pure stepwise -pulse is described by a step function) is theoretically analysed. In this way, first of all the analytical form of the -pulse has been obtained when remagnetization of the `magnetic shutter' takes place. The problem is solved by employing the semiclassical Maxwell - Bloch formalism. Then the time evolution of the coherent response to that -pulse is calculated when it propagates through a two-level resonant medium. Finally the theoretical results are used to describe the experiment quantitatively.
An effective two-level Maxwell-Bloch formalism is developed to describe various time-dependent phenomena in a three-level V-type system. The Maxwell-Bloch equations govern the temporal evolution of a probe field while a strong driving field is applied on the adjacent transition. The main assumption adopted throughout the paper is that the spontaneous decay rate on the coherently driven transition exceeds the decay rate on the probe transition as well as inverse time variations of both pulses. It is shown that the probe pulse interacts with such a medium in a manner similar to that in a self-induced transparency. An amplification without inversion of a relatively short probe pulse while propagating through an optically thick atomic medium is analyzed.
The coherent propagation of two optical short pulses through a resonant medium consisting of two three-level atoms in the configuration is investigated. A self-consisting analytical solution without steady state or adiabatic approximations is presented. The electric field in the model studied consists of two co-propagating plane waves, each of which is in near resonance with a transition in the absorber. The density matrix of two three level atoms is studied. Also, the reduced density matrices are stated. The present approach for the semiclassical treatment of resonant coherent interactions in three-level atoms represents a generalization of the Maxwell- Bloch equations for a two-level system. The Maxwell-Bloch equations reduced to the non-linear pendulum equation. The solution shows that the two pulses can propagate simultaneously without loss under some conditions about the pulses and the medium. The propagation of the two pulses through the medium without any constrains approves the self -induced transparency (SIT) phenomenon.
The initial value problem for the propagation of a pulse through a resonant two-level optical medium is solved by the inverse scattering method. In general, an incident pulse decomposes not only into a special class of pulses to which the medium is transparent but also yields radiation which is absorbed by the medium. In this respect ``this problem'' has properties markedly different from other dispersive and reversible wave phenomena some of which are tractable by the inverse scattering method. Indeed, it is remarkable that in the present case the method still applies. In particular, we show that, while there are an infinite number of local conservation laws, the integrated densities, and in particular the energy, are only conserved for a very special class of initial conditions. The theoretical results obtained are in close agreement with all the qualitative features observed in the experiments on coherent pulse propagation. Finally, we also show that causality is preserved. Two new and novel features are introduced and briefly discussed. First, we show that if the homogeneous broadening effect is a function of position in the medium, the pulses may speed up and slow down accordingly, without losing their permanent identities. Second, we have found a new kind of solution mode corresponding to a proper eigenvalue of the scattering problem which is not a bound state.
We introduce a notion of ``matrix potential'' to nonlinear optical systems. In terms of a matrix potential ggg, we present a gauge-field-theoretic formulation of the Maxwell-Bloch equation that provides a semiclassical description of the propagation of optical pulses through resonant multilevel media. We show that the Bloch part of the equation can be solved identically through ggg and the remaining Maxwell equation becomes a second-order differential equation with a reduced set of variables due to the gauge invariance of the system. Our formulation clarifies the (non-Abelian) symmetry structure of the Maxwell-Bloch equations for various multilevel media in association with symmetric spaces G/HG/HG/H. In particular, we associate the nondegenerate two-level system for self-induced transparency with G/H=SU(2)/U(1)G/H=\mathrm{SU}(2)/\mathrm{U}(1)G/H=SU(2)/U(1) and three-level $\ensuremath{\Lambda}$ or VVV systems with G/H=SU(3)/U(2)G/H=\mathrm{SU}(3)/\mathrm{U}(2)G/H=SU(3)/U(2). We give a detailed analysis for the two-level case in the matrix potential formalism, and address various properties of the system including soliton numbers, effective potential energy, gauge and discrete symmetries, modified pulse area, conserved topological, and nontopological charges. The nontopological charge measures the amount of self-detuning of each pulse. Its conservation law leads to a different type of pulse stability analysis that explains earlier numerical results.
Based on the numerical solution of Maxwell-Bloch equations, we study the dynamics of coherent propagation of unipolar, half-cycle, attosecond light pulse in a three-level resonantly absorbing medium. A comparison with the propagation of such pulse in a two-level medium is performed. It is shown that the pulse, which behaves like a 4π-pulse in a two-level medium, in a three-level medium behaves like a 6π-pulse and splits into three sub-pulses propagating at different velocities in the medium. The investigated phenomenon allows for a more detailed understanding of the still insufficiently studied dynamics of coherent propagation of half-cycle pulses in a resonant medium.