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Dielectric microwave resonators in TE011 cavities for electron paramagnetic resonance spectroscopy

机译:TE011型腔中的介电微波谐振器,用于电子顺磁共振光谱

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摘要

The coupled system of the microwave cylindrical TE011 cavity and the TE01δ dielectric modes has been analyzed in order to determine the maximum achievable resonator efficiency parameter of a dielectric inserted into a cavity, and whether this value can exceed that of a dedicated TE01δ mode dielectric resonator. The frequency, Q value, and resonator efficiency parameter Λ for each mode of the coupled system were calculated as the size of the dielectric was varied. Other output parameters include the relative field magnitudes and phases. Two modes are found: one with fields in the dielectric parallel to the fields in the cavity center and the other with antiparallel fields. Results closely match those from a computer program that solves Maxwell’s equations by finite element methods. Depending on the relative natural resonance frequencies of the cavity and dielectric, one mode has a higher Q value and correspondingly lower Λ than the other. The mode with the higher Q value is preferentially excited by a coupling iris or loop in or near the cavity wall. However, depending on the frequency separation between modes, either can be excited in this way. A relatively narrow optimum is found for the size of the insert that produces maximum signal for both modes simultaneously. It occurs when the self-resonance frequencies of the two resonators are nearly equal. The maximum signal is almost the same as that of the dedicated TE01δ mode dielectric resonator alone, Λ≅40 G∕W1∕2 at X-band for a KTaO3 crystal. The cavity is analogous to the second stage of a two-stage coupler. In general, there is no electron paramagnetic resonance (EPR) signal benefit by use of a second stage. However, there is a benefit of convenience. A properly designed sample-mounted resonator inserted into a cavity can give EPR signals as large as what one would expect from the dielectric resonator alone.
机译:为了确定插入空腔中的电介质的最大可达到的谐振器效率参数,以及该值是否可以超过专用TE01δ模式电介质谐振器的谐振器效率参数,已经对微波圆柱形TE011谐振腔和TE01δ介质模式的耦合系统进行了分析。随着电介质尺寸的变化,计算耦合系统每种模式的频率,Q值和谐振器效率参数Λ。其他输出参数包括相对场大小和相位。发现两种模式:一种具有电介质中的场与腔中心中的场平行的模式,另一种具有反平行的场。结果与计算机程序的结果非常接近,该计算机程序通过有限元方法求解麦克斯韦方程。取决于腔和电介质的相对自然共振频率,一种模式具有更高的Q值,并且相应地具有比另一种更低的Λ。具有较高Q值的模式优先由腔壁内或腔壁附近的耦合虹膜或环激发。但是,根据模式之间的频率间隔,可以通过这种方式激励任何一个。对于插入件的尺寸,找到了一个相对较窄的最佳值,该尺寸可以同时为两种模式产生最大信号。当两个谐振器的自谐振频率几乎相等时,就会发生这种情况。最大信号几乎与单独的专用TE01δ模式介质谐振器相同,对于KTaO3晶体,其X波段的Λ≅40G ∕ W1 ∕ 2。该腔类似于两级耦合器的第二级。通常,使用第二级没有电子顺磁共振(EPR)信号的好处。但是,有方便的好处。插入腔中的经过适当设计的样品安装谐振器可以提供与单独的介电谐振器一样大的EPR信号。

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