No abstract

Some experiments are performed in several kinds of discharged plasma to investigate the influence of a magnetic field upon the saturation electron current of an electrostatic probe. The apparent electron density N e ' and the positive ion density N + are calculated from the saturation electron current and the positive ion saturation current respectively and the ratio N e '/N + is plotted against ωτ (ω: the angular cyclotron frequency of electrons, τ: the mean collision time between electrons and molecules). The curve is found to show a clear dependence on the gas pressure, and when the ratio is log -log plotted against the magnetic field, it gives a nearly straight line, showing N e '/N + to be 0.1 at about 1,000 gauss. Since the positive ion saturation current is hardly influenced by the magnetic field of the order of several kilogauss, it is apparent that these properties are based upon the behavior of the electrons around the probe. A theory developed by Bohm and others is applied here to explain the experimental results.

Bloch and Gentile, " the explanation is probably that the arrangement of atoms in the hexagonal gratings does not deviate too greatly from cubic form. VA'th strict cubic symmetry, the expression (53) would vanish, and with hexagonal the various members of (53) may nearly cancel, so that Q~is considerably smaller than XC in magnitude. There is no corresponding cancellation in the fourthorder coefticient, which one should thus expect to be of about the same order 10' ergs/cm' as the cubic anisotropy coeKcient E2 in (1).This is indeed what is found experimentally in cobalt, '~a s at room temperatures X" is 2.2&(10' ergs/cm', or about one-half as large as X'=5.1&&10'. The two terms of (51) are thus comparable even though they involve the spin-orbit parameter A to diferent powers (sos. the second and fourth).