Current Methods for the Study of the Stark Effect in Atoms

Bonch-Bruevich, A. M.; Khodovoi, V. A.

doi:10.1070/pu1968v010n05abeh005850

Cited by 119 publications

(20 citation statements)

References 2 publications

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“…(4) 5v=[p /(4h coca'~Dw )](P/Av) . (6) Since p =eohA, /(16' r), ultimately, the frequency shift of the Ramsey resonance is 5v =a. (P/bv) = -[A, /(64hcmDwr.…”

Section: Principlementioning

confidence: 99%

“…The measurement of a phase shift due to the ac Stark effect [6] is an example of the state-selective use of atomic interferometry, because one partial wave of the interferometer, which is labeled according to the internal state, is decelerated or accelerated by dipole forces in the inhomogeneous intensity profile. The dipole force has been explained well by a dressed-atom approach to atomic motion in laser light [7].…”

Section: Introductionmentioning

confidence: 99%

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Sensitive measurement of phase shifts due to the ac Stark effect in a Ca optical Ramsey interferometer

Morinaga

Tako

Ito³

1993

Phys. Rev. A

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We constructed an optical Ramsey atomic interferometer, which has a resolution of 8 frn for the difference between arms of the interferometer, and used it to examine the phase shift due to the ac Stark effect of the excited state of the intercombination line ('So-'P&) of Ca. It was clearly observed that the phase shift is in proportion to the field power and in inverse proportion to the detuning frequency of the laser. The proportionality coefficient obtained was in good agreement with the theoretical one.PACS number(s): 32.60.+i, 32.80.t, 42.62.Fi, 07.60.Ly

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“…(4) 5v=[p /(4h coca'~Dw )](P/Av) . (6) Since p =eohA, /(16' r), ultimately, the frequency shift of the Ramsey resonance is 5v =a. (P/bv) = -[A, /(64hcmDwr.…”

Section: Principlementioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Sensitive measurement of phase shifts due to the ac Stark effect in a Ca optical Ramsey interferometer

Morinaga

Tako

Ito³

1993

Phys. Rev. A

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“…The optical Stark shift of atoms has been observed and discussed in great detail in the radio-frequency, microwave and optical domains [1][2][3] . In principle, a similar situation should also be encountered in solids, as for intrinsic transitions, such as excitons in semiconductors .…”

Section: Introductionmentioning

confidence: 99%

Dynamics of the Optical Stark Effect in Semiconductors

Hulín

Antonetti

1988

Journal of Modern Optics

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“…The transformed radiation can also be tuned via the dye spectrum, which may [5,9] be controlled by inserting an inclined F a b r y -Perot interferometer in the cavity. This does not reduce the output power substantially.…”

Section: Hhmentioning

confidence: 99%

Solutions of organic compounds as mixers for the radiation from a ruby laser and the emission excited by the latter from a liquid laser

Bokut¹,

Savkin²,

Lugina³

1968

J Appl Spectrosc

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Dye solution oscillation occurs [1][2][3][4][5] in excitation by giant laser pulses. Such l a s e r s produce wavelengths g r e a t e r than those of the exciting source.Here we report frequency shift by dye solutions and mixing of the dye radiation with that from a ruby l a s e r by KDP single c r y s t a l s , as well as tuning of the transformed frequency in the short-wave range.A dye solution can oscillate in a cavity longitudinal or t r a n s v e r s e with respect to the pumping. Figure 1 shows an optical system for producing sum and doubled frequencies on longitudinal excitation of a dye. The oscillation occurs in the same direction as the ruby laser emission. M i r r o r s 1 and 2 are plane-paral[el plates of T F -5 glass 4 m m thick, which are used simultaneously in the ruby and dye cavities. The glass plate 3 is the second m i r r o r in the liquid l a s e r and provides optimum oscillation conditions. The longitudinal excitation system is very convenient in examining transformation, as beams coincident in time are readily produced in the crystal. The dye solution was placed in a cylindrical cell 20 mm long with planeparallel quartz walls and a window diameter of 20 mm. In mixing experiments one needs appropriate power from the dye and ruby l a s e r s , the ruby radiation being residual after passage through the dye solution. The mixing conditions are best if the two radiations have the same power level. The energy of each beam was about 0.3 J, corresponding to powers of about 7 MW.In the t r a n s v e r s e system, the dye flux is perpendicular to the exciting flux. In that case, a rectangular cell 10 • 24 x 30 mm was used, with the oscillation layer 24 m m thick. The dye cavity (base 40 cm) ! 2 3 I HH Fig. 1 t0 -p

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Current Methods for the Study of the Stark Effect in Atoms

Cited by 119 publications

References 2 publications

Sensitive measurement of phase shifts due to the ac Stark effect in a Ca optical Ramsey interferometer

Sensitive measurement of phase shifts due to the ac Stark effect in a Ca optical Ramsey interferometer

Dynamics of the Optical Stark Effect in Semiconductors

Solutions of organic compounds as mixers for the radiation from a ruby laser and the emission excited by the latter from a liquid laser

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