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Journal of Radio Electronics

Propagation of a U-shaped radio pulse in a selectively amplifying medium

A.V. Kulikova, Nikolai S. Bukhman

Published Feb 1, 2024• 0 citations
Publisher

Abstract

General relations are obtained that govern the evolution of the leading edge of a signal propagating in a selectively amplifying medium. The propagation of a pulse with a rectangular envelope, the carrier frequency of which is close to the frequency of one of the spectral amplification lines of a selective (in frequency) amplifying medium, is considered. The time dependence of the envelope of the initially rectangular signal is studied for various values of the optical thickness of the substance layer for the Gaussian and Lorentzian contours of the spectral line. It is shown that in the case of a shift of the carrier frequency of the signal relative to the center of the spectral line, the interference of the primary and amplified signal can lead to very significant oscillations of the total signal in time.

DOI
10.30898/1684-1719.2024.2.2

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General relations are obtained that govern the evolution of the leading edge of a signal propagating in a selectively amplifying medium. The propagation of a pulse with a rectangular envelope, the carrier frequency of which is close to the frequency of one of the spectral amplification lines of a selective (in frequency) amplifying medium, is considered. The time dependence of the envelope of the initially rectangular signal is studied for various values of the optical thickness of the substance layer for the Gaussian and Lorentzian contours of the spectral line. It is shown that in the case of a shift of the carrier frequency of the signal relative to the center of the spectral line, the interference of the primary and amplified signal can lead to very significant oscillations of the total signal in time.
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Propagation of a short quasi-monochromatic electromagnetic (light or radio) signal (wave packet) is considered. The carrier frequency of the signal is close to the frequency of the absorption spectral line (or group of lines) of a medium, and the spectrum width is large relative to the width of this spectral line (or group of lines). Analytic formulas for the temporal dependence of the signal are derived and numerically confirmed for paths of various lengths. It is shown that the signal is substantially distorted long before it noticeably decays owing to absorption. The signal’s temporal dependence turns out to be rather universal with respect to the form factor of the spectral line, the optical thickness of the substance layer, and the initial temporal dependence of the signal.
The uniform asymptotic description of the propagation of an input rectangle-modulated harmonic signal of fixed angular frequency ${\mathrm{\ensuremath{\omega}}}_{\mathit{c}}$ and initial pulse width T into the half-space z>0 that is occupied by a single-resonance Lorentz medium is presented. The asymptotic description is developed by representing the input rectangular pulse as the difference between two Heaviside-unit-step-function-modulated signals that are separated in time by the initial pulse width T. This representation clearly shows that the resultant pulse distortion in the dispersive medium is primarily due to the Sommerfeld and Brillouin precursor fields that are associated with the leading and trailing edges of the input pulse. The dynamical pulse evolution with increasing propagation distance z>0 is completely described for both long and very short initial pulse widths T. In both cases it is shown that the pulse distortion becomes severe when the propagation distance z is such that the precursor fields associated with the trailing edge of the pulse interfere with the precursor fields associated with the leading edge. Finally, the asymptotic theory clearly shows that the main body of the pulse propagates with the signal velocity in the dispersive medium.
It is shown that in a selectively absorbing medium, the propagation velocity of a linearly frequency-modulated signal differs from its group velocity and depends on its modulation index, and the "modulation" addition to the group delay time reverses its sign when the sign of the modulation index changes. As a result, the propagation velocity of a linearly frequency-modulated signal can be superluminal at its subluminal group velocity and superluminal at its subluminal group velocity. When the center of the spectral line falls within the spectrum of a linearly frequency–modulated signal, a single linearly frequency-modulated signal is divided into two signals, one of which propagates at a speed higher than the group velocity (possibly higher than the vacuum light velocity), and the second is lower than the group velocity. The difference in the propagation speed of linearly frequency-modulated signals differing in the sign of the modulation index can lead to the fact that the initially amplitude-modulated signal, when propagating in a selectively absorbing medium, can be divided into several signals propagating at different speeds, and these signals, under certain conditions, can also be purely amplitude-modulated. Obviously, these effects can occur not only when a signal propagates in a selectively absorbing medium, but also when it is reflected from a selectively absorbing surface and propagated through linear filters in circuit theory.
We analytically study the linear propagation of arbitrarily shaped light pulses through an absorbing medium with a narrow transparency window or through a resonant amplifying medium. We point out that, under certain general conditions, the pulse acquires a nearly Gaussian shape, irrespective of its initial shape and of the spectral profile of the line. We explicitly derive in this case the pulse parameters, including its skewness, responsible for a deviation of the delay of the pulse maximum from the group delay. We illustrate our general results by analyzing the slow-light experiments having demonstrated the largest fractional pulse delays.