Aqueous flat cells perpendicular to the electric field for use in electron paramagnetic resonance spectroscopy
R.R. Mett, and J.S. Hyde Aqueous flat cells perpendicular to the electric field for use in electron paramagnetic resonance spectroscopy J. Magn. Reson. 165 2003 137 152
Axially uniform resonant cavity modes for potential us in electron paramagnetic resonance spectroscopy
R.R. Mett, W. Froncisz, and J.S. Hyde Axially uniform resonant cavity modes for potential us in electron paramagnetic resonance spectroscopy Rev. Sci. Instrum. 72 2001 4188 4200
Cavities with axially uniform field for use in electron paramagnetic resonance. II. Free space generalization
J. Anderson, R.R. Mett, and J.S. Hyde Cavities with axially uniform field for use in electron paramagnetic resonance. II. Free space generalization Rev. Sci. Instrum. 73 2002 3027 3037
Cavities with axially uniform field for use in electron paramagnetic resonance. III. Re-entrant geometries
J. Hyde, R. Mett, and J. Anderson Cavities with axially uniform field for use in electron paramagnetic resonance. III. Re-entrant geometries Rev. Sci. Instrum. 73 2002 4003 4009
Aqueous sample considerations in uniform field resonators for electron paramagnetic resonance spectroscopy
J.S. Hyde, and R.R. Mett Aqueous sample considerations in uniform field resonators for electron paramagnetic resonance spectroscopy Curr. Top. Biophys. 26 2002 7 14
A coding error in Mett and Hyde [3] led to the conclusion that a closely-packed cell cluster would produce optimum tangential electric field node centering in the cells. This error is manifest in Fig. 3E of [3] and was caused by a sign error in programming. All equations and all other graphs in [3] are believed to be accurate
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Here, we hold the resonator dimensions fixed and assume that the dielectric of the sample holder does not have a significant effect on the resonant frequency. As indicated in Table 1, the largest frequency shift caused by the Teflon sample holder is less than 1%
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102 cavity, a standard flat-cell in nodal orientation has 4.1 times the signal of a standard capillary of 1.1 mm diameter, neglecting the effects of the sample holder dielectrics
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