TY - JOUR
T1 - Enhancement of near-resonant degenerate four-wave-mixing signals by excitation of a coupled transition
AU - Wilson-Gordon, A. D.
AU - Friedmann, H.
PY - 1984
Y1 - 1984
N2 - It is shown that intense collisionless Rayleigh-type extraresonant signals in degenerate four-wave mixing (DFWM) can be obtained when the | a | b transition which produces the DFWM signal is coupled to another transition ( | a | d ) which is excited near-resonantly by an additional laser beam. Two effects contribute to the Rayleigh-type extraresonant signal at 2=1. The first effect is resonance-enhanced three-photon scattering (TPS), which leads to the population of state | b and consequently contributes a term in ba, the off-diagonal density-matrix element, which is characterized by the linewidth (1T1)ba, the inverse lifetime of the state | b . The second effect derives from the effective lifetime acquired by the ground state | a due to its strong coupling to state | d . This leads to a term in ba characterized by a linewidth 12(1T1)da, which is half the inverse lifetime of the state | d . When (1T1)da(1T1)ba, the TPS effect dominates and the extraresonant DFWM signal is narrow and intense. When (1T1)da(1T1)ba, the signal is less intense and interference between the two effects is evident.
AB - It is shown that intense collisionless Rayleigh-type extraresonant signals in degenerate four-wave mixing (DFWM) can be obtained when the | a | b transition which produces the DFWM signal is coupled to another transition ( | a | d ) which is excited near-resonantly by an additional laser beam. Two effects contribute to the Rayleigh-type extraresonant signal at 2=1. The first effect is resonance-enhanced three-photon scattering (TPS), which leads to the population of state | b and consequently contributes a term in ba, the off-diagonal density-matrix element, which is characterized by the linewidth (1T1)ba, the inverse lifetime of the state | b . The second effect derives from the effective lifetime acquired by the ground state | a due to its strong coupling to state | d . This leads to a term in ba characterized by a linewidth 12(1T1)da, which is half the inverse lifetime of the state | d . When (1T1)da(1T1)ba, the TPS effect dominates and the extraresonant DFWM signal is narrow and intense. When (1T1)da(1T1)ba, the signal is less intense and interference between the two effects is evident.
UR - http://www.scopus.com/inward/record.url?scp=35949019687&partnerID=8YFLogxK
U2 - 10.1103/physreva.30.1377
DO - 10.1103/physreva.30.1377
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:35949019687
SN - 1050-2947
VL - 30
SP - 1377
EP - 1385
JO - Physical Review A
JF - Physical Review A
IS - 3
ER -