1991
DOI: 10.1070/qe1991v021n09abeh004059
|View full text |Cite
|
Sign up to set email alerts
|

Optical pressure on atoms in a field of counterpropagating amplitude- and frequency-modulated waves which are in resonance with an atomic transition

Abstract: 3method depends on the decoupling of high order Green's functions. A comparison of the results of the different methods might reveal information about the mathematics of the decouphg, which is often obscure although the method is physically intuitive. This will be done at a later stage.Abstract. Relativistic corrections to P +H charge transfer are calculated. It is found that relativistic effects completely change the high energy behaviour, but that at the highest energies yet used (10 MeV) the corrections are… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
9
0

Year Published

2011
2011
2023
2023

Publication Types

Select...
4
2

Relationship

0
6

Authors

Journals

citations
Cited by 6 publications
(9 citation statements)
references
References 1 publication
0
9
0
Order By: Relevance
“…The use of counterpropagating amplitude-modulated light waves, leading to a stimulated light pressure on atoms, has been proposed as a viable method to achieve large force magnitudes F F rad over a wide velocity range v ⊥ Γ sp /k [34,35]. While the magnitude of the stimulated bichromatic force (BCF) can be explained using an intuitive resonant optical π-pulse interpretation [35,36], an understanding of the large velocity capture range requires a doubly-dressed atom picture [37]. In the simplest case, a two-level system interacts with collinearly superimposed bichromatic standing waves with equal intensities I BCF and symmetrically detuned by ±|δ Γ sp | from atomic resonance.…”
Section: B Coherent Optical Forcesmentioning
confidence: 99%
“…The use of counterpropagating amplitude-modulated light waves, leading to a stimulated light pressure on atoms, has been proposed as a viable method to achieve large force magnitudes F F rad over a wide velocity range v ⊥ Γ sp /k [34,35]. While the magnitude of the stimulated bichromatic force (BCF) can be explained using an intuitive resonant optical π-pulse interpretation [35,36], an understanding of the large velocity capture range requires a doubly-dressed atom picture [37]. In the simplest case, a two-level system interacts with collinearly superimposed bichromatic standing waves with equal intensities I BCF and symmetrically detuned by ±|δ Γ sp | from atomic resonance.…”
Section: B Coherent Optical Forcesmentioning
confidence: 99%
“…The idea of the pulse trap based on the counterpropagating pulse trains [5] stems from Kazantsev's analysis [8] of the atomic motion in the field of the counterpropagating π -pulse trains, advanced in [6,9]. Let the train of the π -pulses propagate in a z direction with the repetition period T and the other train of the π -pulses propagate in the opposite direction (see figure 1).…”
Section: The Simple Model Of the Pulse Trap Based On The Counterpropa...mentioning
confidence: 99%
“…This simple physical consideration is valid for the quite large spontaneous emission rate γ = 1/τ sp , namely for γ 1/T . The detailed analysis [6,9] shows that the force exerted on an atom in the field of the counterpropagating πpulse trains with the high repetition rate of the pulses,…”
Section: The Simple Model Of the Pulse Trap Based On The Counterpropa...mentioning
confidence: 99%
“…1) and point C is the point where the counterpropagating pulses collide. We assume that an atom at point A is in the ground state before the recent interaction with pulse R (this is true in most cases because of the short time between the interaction of the atom with R and L pulses in comparison with the time between the interaction with R and R pulses [22]). As a result of the interaction with this pulse, the atom absorbs a photon and becomes excited.…”
Section: Introductionmentioning
confidence: 99%