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Hyperbolic-cosine waveguide tapers and oversize rectangular waveguide for reduced broadband insertion loss in W-band electron paramagnetic resonance spectroscopy

机译:双曲余弦波导锥度和超大矩形波导,可减少W波段电子顺磁共振波谱中的宽带插入损耗

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摘要

The two-way insertion loss of a 1 m length of waveguide was reduced by nearly 5 dB over a 4% bandwidth at W-band (94 GHz) for an electron paramagnetic resonance (EPR) spectrometer relative to WR10 waveguide. The waveguide has an oversize section of commercially available rectangular WR28 and a novel pair of tapers that vary in cross section with axial position according to a hyperbolic-cosine (HC) function. The tapers connect conventional rectangular WR10 waveguide to the WR28. For minimum loss, the main mode electric field is parallel to the long side of the WR28. Using mode coupling theory, the position of maximum flare (inflection point) in the taper was optimized with respect to the coupling to higher order modes and the reflection of the main mode. The optimum inflection point position is about one-tenth of the taper length from the small end of the taper. Reflection and coupling were reduced by about 20 dB relative to a pyramidal (linear) taper of the same length. Comb-like dips in the transmission coefficient produced by resonances of the higher order modes in the oversize section were about 0.03 dB. Specially designed high-precision, adjustable WR28 flanges with alignment to about 5 μm were required to keep higher order mode amplitudes arising from the flanges comparable to those from the HC tapers. Minimum return loss was about 30 dB. This paper provides a foundation for further optimization, if needed. Methods are not specific to EPR or the microwave frequency band.
机译:对于电子顺磁共振(EPR)光谱仪,相对于WR10波导,在W波段(94 GHz)的4%带宽上,波导长度为1 m的双向插入损耗降低了近5 dB。该波导具有可购得的矩形WR28的超大截面和一对新颖的锥度,其锥角根据双曲线余弦(HC)函数随轴向位置而变化。锥度将常规的矩形WR10波导连接到WR28。为了使损耗最小,主模式电场平行于WR28的长边。使用模式耦合理论,相对于与高阶模式的耦合和主模式的反射,优化了锥度中最大光斑(拐点)的位置。最佳拐点位置约为锥度小端的锥度长度的十分之一。相对于相同长度的锥体(线性)锥度,反射和耦合减少了约20 dB。由超尺寸部分中的高阶模的共振产生的透射系数的梳状下降约为0.03 dB。需要特殊设计的高精度可调节WR28法兰,对准至约5μm,以保持与HC锥度相比更高的模态振幅。最小回波损耗约为30 dB。如果需要,本文可为进一步优化提供基础。方法不特定于EPR或微波频段。

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