coaxial-cavity Improved Mode Selection in Coaxial Cavities for Sub-Terahertz Second-Harmonic IEEE
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[1] K. Avramidis,et al. Coaxial Cavity With Stepped Inner Conductor for a Sub-Terahertz Second-Harmonic Gyrotron With Broadband Continuous Frequency Tuning , 2019, IEEE Transactions on Electron Devices.
[2] M. Fukunari,et al. Oscillation Characteristics of a High Power 300 GHz Band Pulsed Gyrotron for Use in Collective Thomson Scattering Diagnostics , 2019, Plasma and Fusion Research.
[3] V. Shcherbinin,et al. Cutoff Frequencies of a Dielectric-Loaded Rectangular Waveguide With Arbitrary Anisotropic Surface Impedance , 2019, IEEE Transactions on Microwave Theory and Techniques.
[4] K. Avramidis,et al. Starting Currents for Eigenmodes of a Gyrotron Cavity With Mode Conversion , 2019, IEEE Transactions on Electron Devices.
[5] V. Shcherbinin,et al. Improved Cavity for Broadband Frequency-Tunable Gyrotron , 2018, IEEE Transactions on Electron Devices.
[6] V. Shcherbinin,et al. Effect of Cavity Ohmic Losses on Efficiency of Low-Power Terahertz Gyrotron , 2017, IEEE Transactions on Electron Devices.
[7] Vitalii I. Shcherbinin,et al. Cylindrical Cavity with Distributed Longitudinal Corrugations for Second-Harmonic Gyrotrons , 2017 .
[8] Vitalii I. Shcherbinin,et al. ANALOGY BETWEEN CIRCULAR CORE-CLADDING AND IMPEDANCE WAVEGUIDES AND THEIR MEMBRANE FUNCTIONS , 2017 .
[9] J. Rosenzweig,et al. Observation of acceleration and deceleration in gigaelectron-volt-per-metre gradient dielectric wakefield accelerators , 2016, Nature Communications.
[10] J. Stober,et al. Collective Thomson scattering measurements of fast-ion transport due to sawtooth crashes in ASDEX Upgrade , 2016 .
[11] G. Zaginaylov,et al. CAVITY WITH DISTRIBUTED DIELECTRIC COATING FOR SUBTERAHERTZ SECOND-HARMONIC GYROTRON , 2016 .
[12] K. Avramidis. Investigations and advanced concepts on gyrotron interaction modeling and simulations , 2015 .
[13] Emilio A. Nanni,et al. Terahertz-driven linear electron acceleration , 2014, Nature Communications.
[14] K. Kawahata,et al. Spectrum response and analysis of 77 GHz band collective Thomson scattering diagnostic for bulk and fast ions in LHD plasmas , 2014 .
[15] Y. Tatematsu,et al. High-power pulsed gyrotron for 300 GHz-band collective Thomson scattering diagnostics in the Large Helical Device , 2014 .
[16] C. T. Iatrou,et al. EURIDICE: A code-package for gyrotron interaction simulations and cavity design , 2012 .
[17] K. Kawahata,et al. Generation of high power sub-terahertz radiation from a gyrotron with second harmonic oscillation , 2012 .
[18] J. Butler,et al. Experimental demonstration of wakefield effects in a THz planar diamond accelerating structure , 2012, 1201.5420.
[19] La Agusu,et al. Development of a novel high power sub-THz second harmonic gyrotron. , 2009, Physical review letters.
[20] Y. Tatematsu,et al. Subterahertz gyrotron developments for collective Thomson scattering in LHD. , 2008, The Review of scientific instruments.
[21] P. Woskov,et al. Fast-ion dynamics in the TEXTOR tokamak measured by collective Thomson scattering , 2006, Physical review letters.
[22] J. L. Vomvoridis,et al. Coaxial Gyrotron Cavities with Resistive Corrugated Insert for Powerful Second‐Harmonic Operation , 2006 .
[23] C. Iatrou,et al. Design considerations for powerful continuous-wave second-Cyclotron-harmonic coaxial-cavity gyrotrons , 2004, IEEE Transactions on Plasma Science.
[24] O. Dumbrajs,et al. Coaxial gyrotrons: past, present, and future (review) , 2004, IEEE Transactions on Plasma Science.
[25] C. T. Iatrou,et al. Mode selective properties of coaxial gyrotron resonators , 1996 .
[26] R. A. Correa,et al. Design of a TE42,7 coaxial cavity for a 1 MW, 280 GHz gyrotron , 1992 .
[27] E. Borie,et al. A complex cavity with mode conversion for gyrotrons , 1988 .
[28] S. A. Malygin,et al. Coupled-resonator gyrotrons with mode conversion , 1984 .
[29] V. A. Flyagin,et al. The Gyrotron , 1977 .
[30] V. L. Bratman,et al. Theory of gyrotrons with a nonfixed structure of the high-frequency field , 1973 .