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Superluminous Laser Pulse in an Active Medium
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D. L. Fisher and T. Tajima
Physics Department, University of Texas, Austin
Received 24 May 1993
Physical conditions are obtained to make the propagation velocity of a laser pulse and thus the phase velocity of the excited wake be at any desired value, including that equal to or greater than the speed of light. The provision of an active-plasma laser medium with an appropriately shaped pulse allows not only replenishment of laser energy loss to the wake field but also acceleration of the group velocity of photons. A stationary solitary solution in the accelerated frame is obtained from our model equations and simulations thereof for the laser, plasma, and atoms.
PACS numbers: 52.40.Db, 42.50.Rh
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We propose the use of an active laser 1) medium to control the envelope propagation velocity of a laser pulse in a plasma 2) to any design velocity Ʋ env, including the speed of light or greater. Such a pulse is said to be superluminous. It is possible with appropriate construction of the laser pulse profile in the direction of propagation to " accelerate" the group velocity of that pulse. This is related to the process of self-induced transparency [1] and to the triple soliton solutions already obtained for a (nonactive) plasma system [2, 3]. Since the pulse can travel at the design speed with no change in its structure, the phase velocity of the accelerating field will also be at the design speed in an active-plasma medium. The preexcited active medium plays the role of a nonlinear amplifier, amplifying the front of the laser pulse and absorbing energy at the rear of the pulse in such a manner as to maintain its shape but at the same time increase the overall pulse speed. This apparent acceleration of the group velocity even beyond the speed of light does not violate the special theory of relativity as energy and information flow in fact do not exceed с. The leading edge of the pulse which is necessary for acceleration already contains information about the pulse and this information is extracted through the nonlinear amplification process. If the pulse is of finite length, the peak will travel only to the edge of the pulse (the edge travels with the pulse group velocity) with the design velocity and with the group velocity thereafter.
The process of effective acceleration of the photon group velocity and the recovery of laser energy loss by the active medium has applications in photonics and telecommunications as well as to wake-field accelerators. With application to acceleration [4]the increase of the phase velocity of the wake field could help overcome slippage between the particle bunch and accelerating field as the particle bunch outruns the accelerating field due to the difference between the phase velocity of the field and the particle velocity Ʋ ≈ с. Second, since the energy used to induce the wake comes from the active medium and not from the laser pulse, pump depletion [5] may be eliminated. The energy to induce the wake field originally comes from the active medium, leaving the structure of the pulse unchanged with the final energy density of the material reduced by the amount necessary to induce the wake field. Third, using a properly shaped active medium channel in the transverse direction, we should be able to replenish energy loss to diffraction and refraction, thereby optically guiding and effectively focusing the laser pulse.
Three conditions must be met to accelerate the pulse envelope to the design speed Ʋ env and retain a stationary structure. First is the resonance condition: The laser photon energy should approximately match that of the transition energy in the active medium. Here we consider the case of exact resonance, but small detuning might be both possible and desirable to minimize unwanted non-linear optical effects. Second the laser pulse duration must match the time scale of energy exchange between the active medium and laser pulse (reciprocal of the average Rabi frequency). Third a certain energy density in the active medium is necessary for the acceleration of the pulse envelope. Starting with the wave equation where A is the vector potential of the laser pulse, ⱷ is the potential for the plasma electric field, and the transverse component of polarization vector P contains only the active material dependent (atomic) response. None of the plasma effects are included in P; they enter through ⱷ and J. The index of refraction ŋ is for the nonactive portion of the material response (atomic). The form of the fields in one dimension for a laser of frequency ⱷ and wave number k0 are
where y = 1/V 1 - (v/c)2, U(z, t) and V(z, t) are the slowly varying real (electric dipole dispersion) and imaginary (absorption) components of the material polarization vector [1], and y(z, f) and a(z, t) are the slowly varying phase and envelope of the laser pulse.
References:
[1] S.L. McCall and E. L. Hahn, Phys. Rev. 183, 457 (1969).
[2] K. Mima et al., Phys. Rev. Lett. 57, 1421 (1986).
[3] C. McKinstrie and D.Dubois, Phys. Rev. Lett. 57, 2022 (1986).
[4] T.Tajima and J.M.Dawson, Phys. Rev. Lett 43, 267 (1979).
[5] W.Horton and T.Tajima, Phys. Rev. A.34, 4110 (1986).