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Physical Review Letters

Fresnel Light Drag in a Coherently Driven Moving Medium

M. Artoni, Iacopo Carusotto, Giuseppe Carlo La Rocca, F. Bassani

Published Mar 19, 2001• 24 citations
Publisher

Abstract

We theoretically study how the phase of a light plane wave propagating in a resonant medium under electromagnetically induced transparency (EIT) is affected by the uniform motion of the medium. For cuprous oxide (Cu2O), where EIT can be implemented through a typical pump-probe configuration, the resonant probe beam experiences a phase shift (Fresnel-Fizeau effect) that may vary over a wide range of values, positive or negative, and even vanishing, due to the combined effects of the strong frequency dispersion and anisotropy both induced by the pump. The use of such a coherently driven dragging medium may improve by at least 1 order of magnitude the sensitivity at low velocity in optical drag experiments.

DOI
10.1103/physrevlett.86.2549

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We theoretically study how the phase of a light plane wave propagating in a resonant medium under electromagnetically induced transparency (EIT) is affected by the uniform motion of the medium. For cuprous oxide (Cu2O), where EIT can be implemented through a typical pump-probe configuration, the resonant probe beam experiences a phase shift (Fresnel-Fizeau effect) that may vary over a wide range of values, positive or negative, and even vanishing, due to the combined effects of the strong frequency dispersion and anisotropy both induced by the pump. The use of such a coherently driven dragging medium may improve by at least 1 order of magnitude the sensitivity at low velocity in optical drag experiments.
A light beam normally incident upon an uniformly moving dielectric medium is, in general, subject to bendings due to a transverse Fresnel-Fizeau light drag effect. In most familiar dielectrics, the magnitude of this bending effect is very small and hard to detect. Yet, the effect can be dramatically enhanced in strongly dispersive media where slow group velocities in the m/s range have been recently observed taking advantage of the electromagnetically induced transparency effect. In addition to the usual downstream drag that takes place for positive group velocities, we discuss a significant anomalous upstream drag which is expected to occur for negative group velocities. Furthermore, for sufficiently fast speeds of the medium, higher-order dispersion terms are found to play an important role and to be responsible for light propagation along curved paths or the restoration of the time and space coherence of an incident noisy beam. The physics underlying this class of slow-light effects is thoroughly discussed.
Abstract The Fresnel light dragging effect has remained a subject of significant interest for over two centuries, describing the modification of light propagation in a moving medium. This effect is strongly influenced by the dispersive properties of the medium and is commonly manifested through the phase shift of transmitted light, which varies with the velocity of the medium. In this work, we investigate the phase shift induced by varying the velocity of a moving microcavity. Our results show that a phase shift of approximately 10 m rad is obtained at a velocity of 2 m/s, which increases to about 40 m rad as the velocity reaches 10 m/s. Additionally, the motion of the microcavity significantly affects the transmission of the probe field, leading to measurable perturbations that depend on the induced phase shift. Specifically, the perturbation increases from 0.004 at 2 m/s to 0.02 at 10 m/s. These findings demonstrate that increasing the velocity of the medium enhances the light dragging effect, resulting in a greater modification of light propagation compared to its behavior in a vacuum. This study provides valuable insight into the control of light–matter interaction in dynamic optical systems and its potential applications in advanced photonic technologies.
A moving dielectric medium can displace the optical path of light passing through it, a phenomenon known as the Fresnel-Fizeau optical drag effect. The resulting displacement is proportional to the medium's velocity. In this paper, we report on the observation of an anomalous optical drag effect, where the displacement is still proportional to the medium's speed but along the direction opposite to the medium's movement. We conduct an optical drag experiment under conditions of electromagnetically induced transparency and observe the transition from normal, to null, to anomalous optical drag by modification of the two-photon detuning.
The Fresnel-Fizeau effect of transverse drag, in which the trajectory of a light beam changes due to the transverse motion of the optical medium, is usually extremely small and hard to detect. We observe transverse drag in a moving hot-vapor cell, utilizing slow light due to electromagnetically induced transparency (EIT). The drag effect is enhanced by a factor 3.6 × 10 5 , corresponding to the ratio between the light speed in vacuum and the group velocity under EIT conditions. We study the contribution of the thermal atomic motion, which is much faster than the mean medium velocity, and identify the regime where its effect on the transverse drag is negligible.
As one of the most influential experiments on the development of modern macroscopic theory from Newtonian mechanics to Einstein's special theory of relativity, the phenomenon of light dragging in a moving medium has been discussed and observed extensively in different types of systems. To have a significant dragging effect, the long duration of light travelling in the medium is preferred. Here we demonstrate a light-dragging experiment in an electromagnetically induced transparent cold atomic ensemble and enhance the dragging effect by at least three orders of magnitude compared with the previous experiments. With a large enhancement of the dragging effect, we realize an atom-based velocimeter that has a sensitivity two orders of magnitude higher than the velocity width of the atomic medium used. Such a demonstration could pave the way for motional sensing using the collective state of atoms in a room temperature vapour cell or solid state material.
Abstract We address the coherent regulation of Fizeau's light dragging effect in a five-level atomic medium using the exploitation of joint strong control and weak probing fields. The strength of Fizeau's light dragging, as well as the phase velocity and group index, exhibit a strong reliance upon the detuning of the probing type field and the associated Rabi type frequencies of the control fields. The maximum coefficient for Fizeau's light dragging is determined to be ± 500. This phenomenon significantly affects the phase along with the group velocities and induces a phase shift in light pulses propagating through the medium. Besides, the phase shift with maximum strength of light pulse in the medium is found to be ± 0.08 radians. Finally, it is important to note that our findings hold practical implications for applications such as interferometry, imaging coding, and the development of cloaking devices.