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Phys. Rev. A 71, 013819 (2005) [15 pages]

Pulse transformation and time-frequency filtering with electromagnetically induced transparency

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R. N. Shakhmuratov1,2,3 and J. Odeurs1
1Instituut voor Kern- en Stralingsfysica, Katholieke Universiteit Leuven, Celestijnenlaan 200 D, B-3001 Leuven, Belgium
2Optique Nonlinéaire Théorique, Université Libre de Bruxelles, Campus Plaine Code Postal 231, B-1050 Bruxelles, Belgium
3Kazan Physical Technical Institute, Russian Academy of Sciences, 10∕7 Sibirsky trakt, Kazan 420029, Russia

Received 7 April 2004; revised 22 June 2004; published 28 January 2005

A simple analytical solution for the propagation of a weak Gaussian pulse in a dense absorptive medium with electromagnetically induced transparency is found. This solution is applied to the analysis of three regimes: (1) and (2) the pulse spectrum is narrower than the transparency window [which is narrow (1) or wide (2) with respect to the width of the absorption line] and (3) the pulse spectrum is broader than the transparency window. It is shown that the pulse maintains its area in all three regimes and maintains its Gaussian shape but narrows in spectrum in regime 1. In regime 2, the pulse begins to distort after a certain distance. In regime 3, the pulse is split into two parts. One part is an adiabatic part with a spectrum defined by the effective width of the transparency window for a thick medium and the other is an oscillating nonadiabatic part of short duration. The adiabatic part propagates slowly and the nonadiabatic part propagates with a velocity close to the speed of light. Thus in regime 3, the medium acts as a time-frequency filter, separating the narrow and wide spectrum components of the pulse in time at the output of the absorber.

© 2005 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.71.013819
DOI:
10.1103/PhysRevA.71.013819
PACS:
42.50.Gy, 42.50.Hz, 42.65.Tg, 42.65.Dr