Quasioptical transformer which transforms the waves in a waveguide having a circular cross section into a highly directional wave beam
Quasioptical transformer which transforms the waves in a waveguide having a circular cross section into a highly directional wave beam
复制标题
DOI:
10.1007/bf01037072
复制
发表时间:
1974
影响因子:
0.8
通讯作者:
S. Vlasov;I. M. Orlova
中科院分区:
文献类型:
--
作者:
S. Vlasov;I. M. Orlova
(2) b, n= a 1 k: a"'d,,= 1 k 2a 2sin20, while f! and f2 are functions of the coordinate z which describes the field distribution of the m-th harmonic on a cylinder of radius a in waves propagating toward the z axis and from the z axis, respectively, at an angle 0= arccos (h/k); h is the propagation constant of the wave in the waveguide. In (2) it is assumed that fi is nonvanishing only for-ll< z'+ aeotan0< ll, while fl and f2 vary slightly over dimensions of the order of a wavelength.If the dependence of the fields on q) can be described with a sufficient degree of accuracy by a superposition of harmonics having m<< ka sin0, so that for each of them the dependence of bm and dm on r may be neglected, then for propagation of the field from the waveguide surface onto the surface near the parabolic mirror no substantial distortions develop. For propagation of fields of the type (1) distortions may be neglected within~ 5-10% for~ mp~ 10, since in this ease the first five harmonics (m= 0,~: 1,• already contain more than 95% of the beam energy.