Nv. Denisova et al., WEAK-PULSE TRANSPARENCY ENHANCEMENT IN AN OPTICALLY DENSE 3-LEVEL MEDIUM INDUCED BY A 2-PI PULSE IN A NEIGHBORING TRANSITION (V-SCHEME), Journal of experimental and theoretical physics, 86(1), 1998, pp. 39-48
The coherent V-configuration interaction between an optically dense re
sonantly-absorbing three-level medium (neon) and two ultrashort superr
adiance pulses with converging wave fronts is investigated experimenta
lly and theoretically. Both separate and combined propagation of pulse
s with wavelengths lambda(1) = 614.3 nm (strong field, theta(1) greate
r than or equal to pi) and lambda(3) = 594.5 nm (weak field, theta(3)
approximate to pi/20) are studied. For propagation of a separate stron
g-field pulse, supertransparency of the absorbing medium was observed,
which is associated with the generation of a soliton-like pulse at th
e difference frequency (Delta upsilon approximate to 1700 MHz) and the
dispersion-diffraction stabilization effect. Under these conditions a
weak-field pulse is completely absorbed. Combined propagation of the
pulses leads to novel effects. A below-threshold pulse (weak field) wa
s observed to pass through the absorber while interacting coherently w
ith a strong-field pulse at a neighboring transition. It is shown theo
retically that absorption of the weak pulse is reduced for two reasons
: first, as a result of incoherent transparency of the resonance trans
ition caused by emptying of the lower level by the field of the strong
pulse, and second, as a result of coherent transfer of polarization b
etween the upper levels via the two-photon processes. When the conditi
ons for combined propagation are met, the latter mechanism ensures inv
ersionless amplification of a weak pulse over a wide band of frequenci
es. In this case, the gain can even exceed the linear absorption coeff
icient in absolute value. A difference in propagation velocities of th
e weak and strong pulses was recorded experimentally, along with a shi
ft in the carrier frequency of the weak field towards the red (approxi
mate to 600 MHz). A mechanism for transfer of phase modulation from a
strong pulse to a weak pulse via the common lower level is discussed t
heoretically. (C) 1998 American Institute of Physics.