Download Atomic, Molecular, and Optical Physics: Charged Particles, by F. B. Dunning PDF

By F. B. Dunning

With this quantity, tools of Experimental Physics turns into Experimental tools within the actual Sciences, a reputation switch which displays the evolution of todays technology. This quantity is the 1st of 3 in order to supply a entire remedy of the most important experimental equipment of atomic, molecular, and optical physics; the 3 volumes as a collection will shape a very good experimental guide for the sector. The huge availability of tunable lasers within the pastseveral years has revolutionized the sphere and bring about the advent of many new experimental tools which are coated in those volumes. conventional equipment also are incorporated to make sure that the volumes could be a whole reference resource for the sector.

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Additional resources for Atomic, Molecular, and Optical Physics: Charged Particles, Volume 29A

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K. Sinclair, Proc. Int. Symp. High Energy Spin Phys. 8th, Minneapolis, 1988; AIP Conf. Proc. 187, 1412 (1989). 24. E. Reichert, Proc. Int. Symp. High Energy Spin Phys. 9th, Bonn, 1990, Vol. I, p. 303 (1991). 25. T. Nakanishi, Proc. Int. Symp. High Energy Spin Phys. loth, Nagoya, 1992. p. 279-290. , Tokyo). 36 SPIN-POLARIZED ELECTRON SOURCES 26. W. E. Spicer, Phys. Rev. 112, 114 (1958). 27. W. E. Spicer, Appl. Phys. 12, 115 (1977). 28. R. L. ” Oxford Univ. Press (Clarendon), Oxford, 1973. 29. L.

The quantum efficiency for a bulk crystal or thick epilayer can range from typical values in the neighborhood of 3% obtained in most research laboratories to around 30% which is not unusual for cathodes prepared commercially by proprietary processes. We present two approaches to preparing photocathodes for polarized electron sources: (1) a known, reliable method which gives cathodes with the lower quantum efficiency, but which are still quite adequate for most applications (we label these “adequate” cathodes), and (2) some considerations for obtaining the higher quantum efficiency cathodes (we label these “optimum” cathodes).

The quantum efficiency for a bulk crystal or thick epilayer can range from typical values in the neighborhood of 3% obtained in most research laboratories to around 30% which is not unusual for cathodes prepared commercially by proprietary processes. We present two approaches to preparing photocathodes for polarized electron sources: (1) a known, reliable method which gives cathodes with the lower quantum efficiency, but which are still quite adequate for most applications (we label these “adequate” cathodes), and (2) some considerations for obtaining the higher quantum efficiency cathodes (we label these “optimum” cathodes).

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