Download PDF by Benjamin Bederson (ed.), Herbert Walther (ed.): Advances In Atomic, Molecular, and Optical Physics, Vol. 42

By Benjamin Bederson (ed.), Herbert Walther (ed.)

ISBN-10: 0120038420

ISBN-13: 9780120038428

This sequence, validated in 1965, is worried with contemporary advancements within the common quarter of atomic, molecular, and optical physics. the sphere is in a kingdom of swift progress, as new experimental and theoretical suggestions are used on many elderly and new difficulties. subject matters lined additionally contain comparable utilized components, akin to atmospheric technological know-how, astrophysics, floor physics, and laser physics.

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Extra resources for Advances In Atomic, Molecular, and Optical Physics, Vol. 42

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C 2a 4- 5 8 1- 0. 1 I I -1 0 1 d position / rnrn ............. 6. Spatial fringe pattern in the far field of the interferometer. The solid line is a fit to the experimental data (circles). The dashed line shows the independently measured envelope. 0 pm, respectively. 48 Stephan Diirr and Gerhard Rempe pumping. This is because the atomic momentum changes as a result of photon recoils. This has been taken into account in the value of t,,,,, in Table I. Note that in Eq. (34) we chose z = 0 at the source, whereas in the following, we will always choose z = 0 midway between the transmitted and reflected beams.

Here tsource does not appear, because the change of the atomic transverse velocity by 2vrec takes place in the interaction region. It is easy to see that for tsource= 0, Eq. (34) reduces to Eqs. (31) and (33). - C a w 2- C ;1 0-1 1 0 position / mrn ............ c 2a 4- 5 8 1- 0. 1 I I -1 0 1 d position / rnrn ............. 6. Spatial fringe pattern in the far field of the interferometer. The solid line is a fit to the experimental data (circles). The dashed line shows the independently measured envelope.

At P M 50 pW, atoms with a momentum sufficiently close to the Bragg condition are Bragg-reflected to p z M +hk. 4. Bragg reffection of atoms from a standing light wave. The atomic momentum distribution after the interaction is shown for different values of the laser power, P , in the standing light wave. The initial momentum distribution (at P = 0) is centered around -hk. Atoms with a momentum sufficiently close to the Bragg condition can be first-order Braggreflected to f f i k . The fraction of Bragg-reflected atoms exhibits Pendellosung oscillations as a function of the laser power.

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Advances In Atomic, Molecular, and Optical Physics, Vol. 42 by Benjamin Bederson (ed.), Herbert Walther (ed.)


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