2003
DOI: 10.1103/physreva.68.063802
|View full text |Cite
|
Sign up to set email alerts
|

Light amplification through collective atomic recoil motion modified by a harmonic potential

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
6
0

Year Published

2005
2005
2013
2013

Publication Types

Select...
4

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(6 citation statements)
references
References 20 publications
0
6
0
Order By: Relevance
“…Therefore, the steady-state CARLs were proposed and have been experimentally demonstrated [8][9], but, with a relative weak gain. In this paper, we report a result in order to give a more detailed theoretical analysis to a modified CARL system [10] which produces a CW laser output with a higher gain. In our previous scheme, the active cold atoms are trapped in a harmonic potential, which can be realized by loading the atoms into an optical lattice or an overall magnetic trap, instead of introducing a light molasses [9] [11] or adding a thermal collision/momentum damping mechanism to the atomic motion [6].…”
Section: Introduction and Simulation Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Therefore, the steady-state CARLs were proposed and have been experimentally demonstrated [8][9], but, with a relative weak gain. In this paper, we report a result in order to give a more detailed theoretical analysis to a modified CARL system [10] which produces a CW laser output with a higher gain. In our previous scheme, the active cold atoms are trapped in a harmonic potential, which can be realized by loading the atoms into an optical lattice or an overall magnetic trap, instead of introducing a light molasses [9] [11] or adding a thermal collision/momentum damping mechanism to the atomic motion [6].…”
Section: Introduction and Simulation Resultsmentioning
confidence: 99%
“…The coefficient (1 − e −κτ )/κ of Eq. (10) shows here that when the damping rate κ is small enough and the evolution time τ ≫ 1/κ, the intensity gain of the probe field will be extremely high in the neighborhood of ∆ 21 = nν, and thus results in a uniform discrete gain structure as shown in Fig.2 simulated directly on Eq.(2). Although the Raman gain condition will not be changed if the higher harmonic components of Eq.…”
Section: ∆20mentioning
confidence: 98%
“…For our current purpose the high-Q cavity provides a low noise detection, which not only enhances atom-cavity coupling but also increases the sensitivity of measurement by a factor of 1/(1−R), where R is the reflectivity of cavity mirror [46]. Further, these requirements of the system enable a usage of Bonifacio's collective atomic recoil laser (CARL) model [47] to introduce an extra trapping potential [35] for the micro-trap on atom chip. Describing the two-level atomic gas with the Pauli spin operator σ 0 and their internal transitions byσ ± , pump and probe modes byâ 2 ,â 1 , the system Hamiltonian is [35],…”
Section: Model and Mechanismmentioning
confidence: 99%
“…Further, these requirements of the system enable a usage of Bonifacio's collective atomic recoil laser (CARL) model [47] to introduce an extra trapping potential [35] for the micro-trap on atom chip. Describing the two-level atomic gas with the Pauli spin operator σ 0 and their internal transitions byσ ± , pump and probe modes byâ 2 ,â 1 , the system Hamiltonian is [35],…”
Section: Model and Mechanismmentioning
confidence: 99%
See 1 more Smart Citation