1982
DOI: 10.1051/jphys:01982004305072900
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Possible M1 - E1 interference effects in m1 forbidden transitions with crossed magnetic and electric fields

Abstract: Résumé. 2014 Abstract. 2014 In this paper we predict new possible M1 -E1 Stark interference effects which should appear in nS -n' S M1 forbidden transitions when a static magnetic field crossed with the static electric field is applied. In particular it becomes possible to measure the ratio M1/E1 Stark directly on the fluorescence intensity. These effects are also of importance for the problem of systematic errors in Parity Violation experiments and give new ways of calibrating the PV signal.

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Cited by 13 publications
(5 citation statements)
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“…These signals have proved useful for calibrating the PV signal and as atomic probes of experimental imperfections (part II). References [37,38] give a detailed analysis of the new effects arising from M'-Stark or Stark-Stark interference in a magnetic field of arbitrary direction. In the PV experiment two classes of effects are involved : hyperfine mixing, and Hanle effect.…”
Section: Atomic Signals In Non-zero Magnetic Field -mentioning
confidence: 99%
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“…These signals have proved useful for calibrating the PV signal and as atomic probes of experimental imperfections (part II). References [37,38] give a detailed analysis of the new effects arising from M'-Stark or Stark-Stark interference in a magnetic field of arbitrary direction. In the PV experiment two classes of effects are involved : hyperfine mixing, and Hanle effect.…”
Section: Atomic Signals In Non-zero Magnetic Field -mentioning
confidence: 99%
“…In this appendix, we study new terms which appear in the expression of the fluorescence signal when a magnetic field H is present in addition to the Stark field E. The details of the calculation can be found in references [37,38]. Here we only outline the assumptions and the results relevant to our PV experiments.…”
Section: Appendix Bmentioning
confidence: 99%
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“…Highly-forbidden optical transitions have been measured with great precision using the interference between the forbidden transition and a much stronger transition between the same two states. Key examples of these techniques are found in measurements of magnetic dipole transitions [1][2][3][4][5][6][7][8], electric quadrupole transitions [9,10], and parity nonconserving (PNC) electroweak interactions [11][12][13][14][15][16][17][18][19]. Still, pushing the precision of these measurements to greater limits, as well as extending them to a variety of other atomic systems, is an active pursuit, in that it will allow further tests of the Standard model and of nucleon-nucleon interactions within the nucleus [20,21].…”
Section: Introductionmentioning
confidence: 99%
“…This is a crucial advantage in the case of our parity violation experiment, since many possible systematics can be shown to belong to the category of suppressed signals (in contrast with the parity violation signal under search) : e.g. systematics associated with a stray magnetic field along the laser beam [4].…”
mentioning
confidence: 99%