By M. B Schaffer

An software of Lanchester thought to the review of small-unit floor activities general of insurgency in Vietnam.

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Surface ¢2 s1 = Thus in Fig. 2, the flux ¢1 through is"" 0 and that through s2 is ¢1 - 4ng. Hence with the presence of a magnetic monopole, the flux through a loop L has two values, one value for all surfaces (Sz) behind the monopole which we shall call ~back' and one value for all surfaces (Sl) in front of the monopole, which we shall call ¢f roa t . (b) . Now replace the loop L in Figure 2 by a superconducting wire of finite thickness. Since H = -VxE at any space-time point not on the world line of the monopole, the flux in front of the monopole has the time rate of change (inside wire), q,front which is zero inside a superconductor.

It For the Sturm-Liouville problem the fundamental trick which allows for an elegant analysis of the eigenvalues is the definition of a phase angle (related to the logarithmic derivative of the wave function) which is monotonic with respect to the energy. It turns out that the eigenvalue problem (10) allows for a similar analysis through the definition of two phase angles. Multiplying (10) on the left by ia 1 b 2 we obtain a b [(ia 1 b 2 )ap- *a 2b 2 + ~/ + A0 b 3 - B0 ] h(o) = 0. (13) Choosing a representation where a 1 ,a 3 , b 1 , b 3 are real symmetrical and a 2 , b 2 are equal to i times real antisymmetrical matrices, we find (13) to be of the form [w Cl + V )h(o) 0 p 0 = B h(o) 0 (l4) where and V 0 is real symmetrical.

Dl6:1815 (1977). 4. clearis 2:225 (1978). 5. Y. Kazama and Chen Ning Yang, Phys. Rev. Dl5:2300 (1977). 6. 237, Edited by N. S. Craigie, P. Goddard and W. Nahm, (World Scientific, 1982). 7. Tai Tsun Wu and Chen Ning Yang, Phys. Rev. Dl4:437 (1976). 8. M. Dirac, Phys. Rev. 74:817 (1948). Schwinger, Particles, Sources and Fields (Addison-Wesley), vols. 1 and 2. 9. a Sinica 21:317 (1978). N. YANG C. Devchand, V. Dobrev and S. Mukhi HOFSAsS: The classical action for the monopole-electron system contains a term which couples the electric charge to the gauge field, Then for this expression to be independent of Q one needs that the two gauge fields A~ and have to be gauge copies of each other in the overlap region.