1966
DOI: 10.1007/bf02711418
|View full text |Cite
|
Sign up to set email alerts
|

Temperature effects in the relaxation of optically oriented alkali vapours

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
5
0
1

Year Published

1967
1967
2002
2002

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 44 publications
(7 citation statements)
references
References 9 publications
1
5
0
1
Order By: Relevance
“…Remarquons que nos hypotheses different de celles adopt6es par P. Minguzzi et al [14] en deux points. Ces auteurs adoptent pour d(5) Q>/dt 1'expression suivante :…”
Section: Equation D'évolution Globale D'une Obser-unclassified
“…Remarquons que nos hypotheses different de celles adopt6es par P. Minguzzi et al [14] en deux points. Ces auteurs adoptent pour d(5) Q>/dt 1'expression suivante :…”
Section: Equation D'évolution Globale D'une Obser-unclassified
“…It is well known that as a result of the strongly relaxing glass surface, the presence of a buffer gas results in spatial modes for the population imbalance between the two hyperfine manifolds. 17 Consequently, not all spatial regions within the field contribute to the observed line shape to the same degree. Hence, the experimentally observed line shape is a manifestation of two inhomogeneities: one due to the field, and the other due to the equilibrium population imbalance (i.e., the population imbalance between the two states in the absence of the microwave field).…”
Section: Methodsmentioning
confidence: 96%
“…(1). 2 2 However, since atoms in different regions of the cavity experience different microwave-field strengths, and since atomic diffusion through the molecular buffer gas yields spatial modes of hyperfine polarization, 17 the microscopic response to the field varies on the macroscopic scale of the field's and polarization's spatial distributions.…”
Section: Ih Numerical Simulationmentioning
confidence: 99%
“…As our beam diameter is relatively small compared to the cavity radius, we need only consider the axial spatial varia¬ tions, so that for the spatial variation of the Rabi frequency we have Q(z) = flpeakSin| (16) 023806-3 where L is the cavity length. Though the weighting function W(z) is determined by a complicated interplay between atomic diffusion to the resonance cell walls, where the hyperfine population imbalance is destroyed by wall collisions [17], and the exponential attenuation of the optical pumping rate due to Beer's law absorption in the alkali vapor, for the purposes of the present discussion we consider W(z) to be reasonably well approximated as the simple product of two terms. The first term describes the local "microscopic" in¬ fluence of various parameters on the signal, most notably the optical pumping rate, while the second term accounts for the macroscopic variation of the signal associated with spatial diffusion [18,19], which for simplicity we assume to be well described by the first-order diffusion mode [i.e., sin(7:z/L)]:…”
Section: Inhomogeneous Broadeningmentioning
confidence: 99%