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Additional resources for Advances in Electronics and Electron Physics, Vol. 15
I (76) Notice that the field intensity required is about half that required for the optimum condition for a Rabi flop in an cscillating field of length 1. The halfwidth of the central peak of the Ramsey pattern is a! 64 - L (77) under the conditions of Eq. The form of the Ramsey pattern is shown in Fig. 19. The pedestal upon which the interference pattern sits is usually much broader than the interference pattern. In some cases the pedestal width is over 700 times the width of the central peak.
The magnitude of the field intensity can be shown to be (ideally) H, H = -T. (47) R The transverse force on an atom within this magnet assembly is radial: 30 RICHARD C. 14. Cross section of a four pole magnetic deflection field. where 8, is a radial unit vector and aH - -. H, _ ar R (49) R is the distance from the axis of the assembly to the nearest point on each of the four-pole surfaces, and H,,, is the magnetic field at these points on the surfaces. In general, W is a function of the magnitude of the field H and is given by the Breit-Rabi formula.
ATOMIC BEAM FREQUENCY STANDARDS 47 VII. MEASUREMENT UNCERTAINTIES There are a number of uncertainties introduced into the absolute frequency measurements of a cesium standard. The ideal circumstance, of course, is to have the accuracy of these devices limited only by the random scatter in the data-all systematic frequency shifts having been measured or eliminated. Ideally then, the accuracy would be determined by the spectral line width and signal-to-noise ratio. 20. NBS-I atomic beam frequency standard.
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