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Cavity mode enhancement of terahertz emission from equilateral triangular microstrip antennas of the high-T c superconductor Bi2Sr2CaCu2O8 + δ

机译:高T c超导体Bi2Sr2CaCu2O8 +δ等边三角形微带天线的太赫兹发射的腔模增强

摘要

We study the transverse magnetic (TM) electromagnetic cavity mode wave functions for an ideal equilateral triangular microstrip antenna (MSA) exhibiting C 3v point group symmetry. When the C 3v operations are imposed upon the antenna, the TM(m,n) modes with wave vectors $propto sqrt{{{m}^{2}}+nm+{{n}^{2}}}$ are much less dense than commonly thought. The R 3 operations restrict the integral n and m to satisfy $|m-n|,=3p$ , where $pgeqslant 0$ and $pgeqslant 1$ for the modes even and odd under reflections about the three mirror planes, respectively. We calculate the forms of representative wave functions and the angular dependence of the output power when these modes are excited by the uniform and non-uniform ac Josephson current sources in thin, ideally equilateral triangular MSAs employing the intrinsic Josephson junctions in the high transition temperature T c superconductor Bi2Sr2CaCu2 ${{ext{O}}_{8+delta}}$ , and fit the emissions data from an earlier sample for which the C 3v symmetry was apparently broken.
机译:我们研究表现出C 3v点群对称性的理想等边三角形微带天线(MSA)的横向磁(TM)电磁腔模波函数。在天线上执行C 3v操作时,TM(m,n)模式的波矢为$ propto sqrt {{{m} ^ {2}} + nm + {{n} ^ {2}}} $密度比通常认为的要低得多。 R 3运算将积分n和m限制为满足$ | mn | ,= 3p $,其中$ p geqslant 0 $和$ p geqslant 1 $对于在关于三个镜面的反射情况下的偶数和奇数模式,分别。当在高转变温度T中采用本征约瑟夫森结的薄,理想等边三角形MSA中的均匀和非均匀交流约瑟夫森电流源激发这些模式时,我们计算出代表性波函数的形式和输出功率的角度依赖性。 c超导体Bi2Sr2CaCu2 $ {{ text {O}} _ {8+ delta}} $,并拟合显然破坏了C 3v对称性的早期样本的发射数据。

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