A tuneable doubly stacked dielectric resonator housed in an intact TE102 cavity for electron paramagnetic resonance spectroscopy
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[1] A. Emwas,et al. Accurate computations of the methyl isotropic hyperfine coupling constants in 2-methyl-1,4-benzosemiquinone radical intermediate , 2002 .
[2] Eliah Aronoff-Spencer,et al. Molecular features of the copper binding sites in the octarepeat domain of the prion protein. , 2002, Biochemistry.
[3] A. Emwas,et al. Generation and spectroscopic characterization of the 2,3,5,6-tetramethoxy-1,4-benzosemiquinone reactive intermediate , 2002 .
[4] S. Mattar,et al. Solvent dependence of the di-tert-butyl nitroxide (DTBN) hyperfine tensors: an experimental and computational study , 2001 .
[5] S. Mattar,et al. Magnetic Inequivalency, Electron Paramagnetic Resonance, Electronic Structure, Optimal Geometry, and Electronic Spectra of the 4,5-Bis(trifluoromethyl)-1,3,2-dithiazol-2-yl Radical † , 2000 .
[6] P. Fajer,et al. Dielectric resonator-based side-access probe for muscle fiber EPR study. , 2000, Journal of magnetic resonance.
[7] A. Sienkiewicz,et al. Dielectric resonator-based flow and stopped-flow EPR with rapid field scanning: A methodology for increasing kinetic information. , 1999, Journal of magnetic resonance.
[8] S. Misra. Estimation of Mn2+ zero-field splitting parameters from a polycrystalline EPR spectrum: case of orthorhombic distortion , 1997 .
[9] J. Freed,et al. Multifrequency two-dimensional Fourier transform ESR: an X/Ku-band spectrometer. , 1997, Journal of magnetic resonance.
[10] J. Fetrow,et al. Kinetics and motional dynamics of spin-labeled yeast iso-1-cytochrome c: 1. Stopped-flow electron paramagnetic resonance as a probe for protein folding/unfolding of the C-terminal helix spin-labeled at cysteine 102. , 1997, Biochemistry.
[11] A. Sienkiewicz,et al. Double-stacked dielectric resonator for sensitive EPR measurements. , 1997, Journal of magnetic resonance.
[12] J. Hyde,et al. Bimodal loop‐gap resonator , 1996 .
[13] A. Sotgiu,et al. Dielectric resonators in a TE102 X‐band rectangular cavity , 1995 .
[14] J. Hyde,et al. Probehead with interchangeable loop‐gap resonators and rf coils for multifrequency EPR/ENDOR , 1994 .
[15] A. Sienkiewicz,et al. Dielectric resonator‐based stopped‐flow electron paramagnetic resonance , 1994 .
[16] I. Chan,et al. Enhanced sensitivity for high-pressure EPR using dielectric resonators , 1992 .
[17] T. Weiland,et al. Bridged loop–gap resonator: A resonant structure for pulsed ESR transparent to high‐frequency radiation , 1988 .
[18] S. Mattar. Elucidation of the geometry of the dipotassium bis(biuretato)cuprate(II) dimer by simulation of its EPR spectra , 1988 .
[19] J. Hyde,et al. Continuous and stopped flow EPR spectrometer based on a loop gap resonator , 1987 .
[20] G. D. Markham,et al. A dielectric sample resonator design for enhanced sensitivity of EPR spectroscopy , 1986 .
[21] J. Hyde,et al. Q‐band loop‐gap resonator , 1986 .
[22] J. Freed,et al. Electron spin echoes with a loop-gap resonator☆ , 1985 .
[23] J. Hyde,et al. The loop-gap resonator: a new microwave lumped circuit ESR sample structure , 1982 .
[24] N. Dalal,et al. Electron paramagnetic resonance (EPR) and electron‐nuclear double resonance (ENDOR) of hyperfine interactions in solutions of α, α′‐diphenyl‐β‐picryl hydrazyl (DPPH) , 1973 .