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Acta Physica Sinica

MULTI-PHOTON SPECTRUM OF TRANSMITTED LIGHT FOR THE MIXED ABSORPTIVE-DISPERSIVE DRIVEN OPTICAL SYSTEM IN GOOD CAVITY CASE

In R

Published Jan 1, 1991• 0 citations
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Abstract

In this paper, the multi-photon spectrum of transmitted light for the mixed absorptive-dispersive optical system in good cavity case is discussed. Owing to the influence of detuning θ and △, not all the various peak values of the spectrum appear at the point of ω = ω_o, and the coefficient of different peak value is not the same. Therefore, the spectrum of transmitted light will show various characters, such as single peak, multi-peaks or asymmetric ones.

Related papers

MULTI-PHOTON SPECTRUM OF TRANSMITTED LIGHT FOR THE MIXED ABSORPTIVE-DISPERSIVE DRIVEN OPTICAL SYSTEM IN GOOD CAVITY CASE

ZHANG LIN, LIN REN-MING, 福建师范大学物理系,福州,350007

In this paper, the multi-photon spectrum of transmitted light for the mixed absorptive-dispersive optical system in good cavity case is discussed. Owing to the influence of detuning θ and △, not all the various peak values of the spectrum appear at the point of ω = ω0, and the coefficient of different peak value is not the same. Therefore, the spectrum of transmitted light will show various characters, such as single peak, multi-peaks or asymmetric ones.

Acta Physica Sinica•Jan 1, 1991•0 citations

MULTI-PHOTON SQUEEZING EFFECT FOR THE MIXED ABSORPTIVE-DISPERSIVE DRIVEN OPTICAL SYSTEM IN GOOD CAVITY CASE

ZHANG LIN, LIN REN-MING, 福建师范大学物理系,福州,350007

In this paper, the multi-photon field squeezing effects for the mixed absorptive-dispersive driven optical system in good cavity case is discussed. Under certain condition, for the single-photon case the squeezing effect of A1, one of the quadrature component of field, in the mixed systems is better than that in the pure absorptive systems. And for the two-photon case, the squeezing effect of A2, another quadrature component of field, may appear.

Acta Physica Sinica•Jan 1, 1990•1 citation

MULTI-PHOTON SQUEEZING EFFECT FOR THE MIXED ABSORPTIVE-DISPERSIVE DRIVEN OPTICAL SYSTEM IN GOOD CAVITY CASE

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Acta Physica Sinica•Jan 1, 1990•0 citations

THE MULTI-PHOTON QUANTUM STATITISCAL THEORY OF DRIVEN OPTICAL SYSTEMS (II)——BAD CAVITY CASE

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In this paper, the multi-photon FPE of driven optical systems are treated for bad cavity case. The semi-classical linear stability analysis are performed. The non-classical effects are discussed, and it is shown that in two-photon case the atom-atom correlation enhances the non-clasical effects. This is in opposite to the single-photon case, and different from the good cavity case. The two-photon spectrum of transmitted light and resonance fluorescense are obtained, where the Rabi frequency Ω∝y2 (y is the incident field).

Acta Physica Sinica•Jan 1, 1988•3 citations

THE MULTI-PHOTON QUANTUM STATISTICAL THEORY OF DRIVEN OPTICAL SYSTEMS (Ⅰ)——FOKKER-PLANCK EQUATION AND GOOD CAVITY CASE

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The systematic method of Fokker-Planck equation (FPE) for the generalized Wigner distribution is used to study the multi-photon transition process of a driven optical system. The general multi-photon FPE, the state equation and the spectrum of transmitted light in good cavity limit are obtained- The two-photon optical bistability spectrum of transmitted light is calculated and compared with single-photon case. It is shown that for multi-photon case, the atom -atom correlation is also negligible in the good cavity limit.

Acta Physica Sinica•Jan 1, 1988•1 citation

THE MULTI-PHOTON QUANTUM STATITISCAL THEORY OF DRIVEN OPTICAL SYSTEMS (II) BAD CAVITY CASE

In R

In this paper, the multi-photon FPE of driven optical systems are treated for bad cavity case. The semi-classical linear stability analysis are performed. The non-classical effects are discussed, and it is shown that in two-photon case the atom-atom correlation enhances the non-clasical effects. This is in opposite to the single-photon case, and different from the good cavity case. The two-photon spectrum of transmitted light and resonance fluorescense are obtained, where the Rabi frequency Ωocy2 (y is the incident field).

Acta Physica Sinica•Jan 1, 1988•0 citations
In this paper, the multi-photon spectrum of transmitted light for the mixed absorptive-dispersive optical system in good cavity case is discussed. Owing to the influence of detuning θ and △, not all the various peak values of the spectrum appear at the point of ω = ω_o, and the coefficient of different peak value is not the same. Therefore, the spectrum of transmitted light will show various characters, such as single peak, multi-peaks or asymmetric ones.
In this paper, the multi-photon FPE of driven optical systems are treated for bad cavity case. The semi-classical linear stability analysis are performed. The non-classical effects are discussed, and it is shown that in two-photon case the atom-atom correlation enhances the non-clasical effects. This is in opposite to the single-photon case, and different from the good cavity case. The two-photon spectrum of transmitted light and resonance fluorescense are obtained, where the Rabi frequency Ω∝y2 (y is the incident field).
The systematic method of Fokker-Planck equation (FPE) for the generalized Wigner distribution is used to study the multi-photon transition process of a driven optical system. The general multi-photon FPE, the state equation and the spectrum of transmitted light in good cavity limit are obtained- The two-photon optical bistability spectrum of transmitted light is calculated and compared with single-photon case. It is shown that for multi-photon case, the atom -atom correlation is also negligible in the good cavity limit.
In this paper, the multi-photon FPE of driven optical systems are treated for bad cavity case. The semi-classical linear stability analysis are performed. The non-classical effects are discussed, and it is shown that in two-photon case the atom-atom correlation enhances the non-clasical effects. This is in opposite to the single-photon case, and different from the good cavity case. The two-photon spectrum of transmitted light and resonance fluorescense are obtained, where the Rabi frequency Ωocy2 (y is the incident field).