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## 5. For other orthogonal coordinates (u, L', z) (such as elliptic, parabolic coordinates, and so forth) problems will arise both in the solution of field components E, and H, from Eq. ( 9) and in fulfillment of the boundary conditions by calculating transverse field components with the use of Eq. (61, because the dependences of the field components on coordinates u and u are mixed and cannot be separated. Therefore, solutions of general bianisotropic waveguides in these coordinates appear quite complicated and are worthy of detailed investigation. ## APPENDIX For the case that all four matrices Et, pt, zt, and yt are antisymmetrical and the coupling zt and tz terms vanish, the derivation will be drastically simplified. The two second-order differential equations of E, and H, take the following form: - ~C L , / ( E C L -5 7 7 ) 1 -[ j P ( d 3 , -5D,) + d q a S -EEL,)D, + ~( € 5 ~ -E ~~) B , I -[(wC", + j P ) / ( ~p -571)I. [ j P ( pD, -vB,) + m ( E a p -7C"a)Bz + m ( q p aq a ~) D z I + w 2 ( 5 B , -@,I, where B, = P Z H Z 4-C " A 0, = eZ Ez + 7 , H, , pa, ta, qa-are the\_ diagonal and antidiago-E , p, 6, 17 and

Who reads Implementation of a Simple Optical Threshold Operation with the Use of the Prom Device and Its Application?

Author

Binquan Wang; Liren Liu; Haifeng Peng

Publisher

John Wiley and Sons; Wiley (John Wiley & Sons); John Wiley & Sons Inc.; Wiley (ISSN 0895-2477)

Published

1996

Language

EN

Field

Engineering (Physical Sciences)