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Zeeman slower

The divergence of this atom laser beam is very small and the brightness of such a very cold atomic beam source is larger by several orders of magnitude than that achievable with Zeeman slower (see Sect. 14.1.4). The brightness of the atom laser beam, defined as the integrated flux of atoms per source area divided by the velocity spread AvxAvyAvz is about 2 x 10 " atoms (s m"" ) [14.126]. [Pg.823]

Fig. 9.66. Arrangement for cooling atoms in a beam using a Zeeman slower. In the middle of the figure a magnetic trap is shown [9.411]... Fig. 9.66. Arrangement for cooling atoms in a beam using a Zeeman slower. In the middle of the figure a magnetic trap is shown [9.411]...
OIDEP usually results from Tq-S mixing in radical pairs, although T i-S mixing has also been considered (Atkins et al., 1971, 1973). The time development of electron-spin state populations is a function of the electron Zeeman interaction, the electron-nuclear hyperfine interaction, the electron-electron exchange interaction, together with spin-rotational and orientation dependent terms (Pedersen and Freed, 1972). Electron spin lattice relaxation Ti = 10 to 10 sec) is normally slower than the polarizing process. [Pg.121]

Let us discuss first the case in which only the first term is present. In the Solomon and Bloembeigen equations for / , (i = 1, 2) there is the cos parameter at the denominator of a Lorentzian function. Up to now cos has been taken equal to that of the free electron. However, in the presence of orbital contributions, the Zeeman splitting of the Ms levels changes its value and cos equals xs / o or (g/h)pBBo- When g is anisotropic (see Fig. 1.16), the value of cos is different from that of the free electron and is orientation dependent. The principal consequence is that another parameter (at least) is needed, i.e. the 0 angle between the metal-nucleus vector and the z direction of the g tensor (see Section 1.4). A second consequence is that the cos fluctuations in solution must be taken into account when integrating over all the orientations. Appropriate equations for nuclear relaxation have been derived for both the cases in which rotation is faster [40,41] or slower [42,43] than the electronic relaxation time. In practical cases, the deviations from the Solomon profile are within 10-20% (see for example Fig. 3.14). [Pg.101]


See other pages where Zeeman slower is mentioned: [Pg.426]    [Pg.381]    [Pg.426]    [Pg.381]    [Pg.102]    [Pg.161]    [Pg.430]    [Pg.178]    [Pg.5]    [Pg.6]   
See also in sourсe #XX -- [ Pg.375 ]




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