Titlebook: Laser Spectroscopy VIII; Proceedings of the E Willy Persson,Sune Svanberg Conference proceedings 1987 Springer-Verlag Berlin Heidelberg 198

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Parity Violation in Atomsron to the nucleus. The PNC neutral weak coupling is decribed by an effective zero-range pseudoscalar potential H. = H. + H. that must be added to the usual atomic Hamiltonian. The dominant portion H. involves the axial and vector parts of the electronic and nucleonic neutral weak currents, respecti

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Intracavity Polarimetry with a Sodium Dimer Ring Lasererence in frequency between two such modes is determined by the optical anisotropy of the cavity and has been measured using a beat technique and electronic counter. Such a device forms the basis of an intracavity Polarimeter. We discuss the salient features of the laser and report on preliminary re

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Laser Cooling and Trapping of Atomsne in recent years. Instead, this paper will summarize the work done on atom cooling and trapping at AT&T Bell Laboratories during the last three years, emphasizing the status of our most recent experimental results.

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New Measurements with Optical Molasseswas it appreciated that the very strong damping of atomic velocity provided by three dimensional laser cooling would lead to diffusive atomic motion and relatively long confinement times, even in the absence of restoring forces. Because of the similarity of the diffusive atomic motion to the Brownia

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Absolute Wavelength Measurements and Fundamental Atomic PhysicsThe Rydberg constant ties together several areas of fundamental physics: fundamental constants; atomic and molecular theory; and spectroscopy of basic systems. As determined at Yale, (Zhao ..[1]) R is the most precisely measured, fundamental constant[2]: R = 109 737.315 73(3) [cm.].

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https://doi.org/10.1007/978-3-540-47973-4UV; laser; laser spectroscopy; optics; spectroscopy