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February 1, 2018 | Science General | By admin | 0 Comments

By E. Arimondo, P.R. Berman and C.C. Lin (Eds.)

ISBN-10: 0123810213

ISBN-13: 9780123810212

This quantity maintains the culture of the Advances sequence. It includes contributions from specialists within the box of atomic, molecular, and optical (AMO) physics. The articles comprise a few evaluation fabric, yet are meant to supply a entire photo of modern very important advancements in AMO physics. either theoretical and experimental articles are incorporated within the quantity. . overseas specialists . entire articles . New advancements

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The fact that the light shift can in principle be eliminated is Advances in CPT for Atomic Clocks 39 of high interest to the application of CPT to atomic clocks, as this major source of long-term instability can potentially be eliminated. However, as we will see below, the complications associated with the multiplicity of levels, Doppler broadening, and other effects present in real atomic systems limit the extent to which the cancellation of the light shift can be accomplished in practice. Measurements of the light shift in CPT systems were described by Nagel et al.

In addition, unwanted energy levels introduce asymmetries in the CPT resonance lineshape (Post, 2003) and produce AC Stark shifts, both of which adversely affect the atomic clock performance by producing timedependent frequency shifts of the clock output. Some of these effects are further amplified if a light field with more than two modes is used for CPT excitation. Over the last several years, a number of advanced interrogation techniques have been developed with the goal of mitigat­ ing some of these effects and thereby improving various aspects of the atomic clock performance.

1993). The advantages of semiconductor lasers over dye lasers in this type of experiment are clear: smaller size and simpler operation. In addition, it is possible to modulate the optical field output of the laser by directly modulating the injection current. 6 GHz. 2-GHz frequency difference needed to excite the Raman—Ramsey fringes. , 1993). The details of the experiment are shown in Figure 8. 835 GHz), creating sidebands on the optical carrier, several of which are separated by approxi­ mately the atomic resonance frequency.

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Advances in Atomic, Molecular, and Optical Physics by E. Arimondo, P.R. Berman and C.C. Lin (Eds.)

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