The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap
Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic fi...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Gospodchikov, E. D. [verfasserIn] Smolyakova, O. B. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Radiophysics and quantum electronics - New York, NY [u.a.] : Consultants Bureau, 1965, 57(2015), 12 vom: Mai, Seite 857-867 |
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| Übergeordnetes Werk: |
volume:57 ; year:2015 ; number:12 ; month:05 ; pages:857-867 |
| Links: |
|---|
| DOI / URN: |
10.1007/s11141-015-9570-9 |
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| Katalog-ID: |
SPR017046831 |
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| 100 | 1 | |a Gospodchikov, E. D. |e verfasserin |4 aut | |
| 245 | 1 | 4 | |a The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap |
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| 520 | |a Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. | ||
| 650 | 4 | |a Plasma Density |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Electron Cyclotron Resonance |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Magnetic Trap |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Electromagnetic Wave Propagation |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Trap Axis |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Smolyakova, O. B. |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Radiophysics and quantum electronics |d New York, NY [u.a.] : Consultants Bureau, 1965 |g 57(2015), 12 vom: Mai, Seite 857-867 |w (DE-627)325573395 |w (DE-600)2037675-3 |x 1573-9120 |7 nnns |
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| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s11141-015-9570-9 |z lizenzpflichtig |3 Volltext |
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10.1007/s11141-015-9570-9 doi (DE-627)SPR017046831 (SPR)s11141-015-9570-9-e DE-627 ger DE-627 rakwb eng 530 620 ASE 33.16 bkl 53.74 bkl 33.80 bkl 39.22 bkl Gospodchikov, E. D. verfasserin aut The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. Plasma Density (dpeaa)DE-He213 Electron Cyclotron Resonance (dpeaa)DE-He213 Magnetic Trap (dpeaa)DE-He213 Electromagnetic Wave Propagation (dpeaa)DE-He213 Trap Axis (dpeaa)DE-He213 Smolyakova, O. B. verfasserin aut Enthalten in Radiophysics and quantum electronics New York, NY [u.a.] : Consultants Bureau, 1965 57(2015), 12 vom: Mai, Seite 857-867 (DE-627)325573395 (DE-600)2037675-3 1573-9120 nnns volume:57 year:2015 number:12 month:05 pages:857-867 https://dx.doi.org/10.1007/s11141-015-9570-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.16 ASE 53.74 ASE 33.80 ASE 39.22 ASE AR 57 2015 12 05 857-867 |
| spelling |
10.1007/s11141-015-9570-9 doi (DE-627)SPR017046831 (SPR)s11141-015-9570-9-e DE-627 ger DE-627 rakwb eng 530 620 ASE 33.16 bkl 53.74 bkl 33.80 bkl 39.22 bkl Gospodchikov, E. D. verfasserin aut The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. Plasma Density (dpeaa)DE-He213 Electron Cyclotron Resonance (dpeaa)DE-He213 Magnetic Trap (dpeaa)DE-He213 Electromagnetic Wave Propagation (dpeaa)DE-He213 Trap Axis (dpeaa)DE-He213 Smolyakova, O. B. verfasserin aut Enthalten in Radiophysics and quantum electronics New York, NY [u.a.] : Consultants Bureau, 1965 57(2015), 12 vom: Mai, Seite 857-867 (DE-627)325573395 (DE-600)2037675-3 1573-9120 nnns volume:57 year:2015 number:12 month:05 pages:857-867 https://dx.doi.org/10.1007/s11141-015-9570-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.16 ASE 53.74 ASE 33.80 ASE 39.22 ASE AR 57 2015 12 05 857-867 |
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10.1007/s11141-015-9570-9 doi (DE-627)SPR017046831 (SPR)s11141-015-9570-9-e DE-627 ger DE-627 rakwb eng 530 620 ASE 33.16 bkl 53.74 bkl 33.80 bkl 39.22 bkl Gospodchikov, E. D. verfasserin aut The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. Plasma Density (dpeaa)DE-He213 Electron Cyclotron Resonance (dpeaa)DE-He213 Magnetic Trap (dpeaa)DE-He213 Electromagnetic Wave Propagation (dpeaa)DE-He213 Trap Axis (dpeaa)DE-He213 Smolyakova, O. B. verfasserin aut Enthalten in Radiophysics and quantum electronics New York, NY [u.a.] : Consultants Bureau, 1965 57(2015), 12 vom: Mai, Seite 857-867 (DE-627)325573395 (DE-600)2037675-3 1573-9120 nnns volume:57 year:2015 number:12 month:05 pages:857-867 https://dx.doi.org/10.1007/s11141-015-9570-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.16 ASE 53.74 ASE 33.80 ASE 39.22 ASE AR 57 2015 12 05 857-867 |
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10.1007/s11141-015-9570-9 doi (DE-627)SPR017046831 (SPR)s11141-015-9570-9-e DE-627 ger DE-627 rakwb eng 530 620 ASE 33.16 bkl 53.74 bkl 33.80 bkl 39.22 bkl Gospodchikov, E. D. verfasserin aut The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. Plasma Density (dpeaa)DE-He213 Electron Cyclotron Resonance (dpeaa)DE-He213 Magnetic Trap (dpeaa)DE-He213 Electromagnetic Wave Propagation (dpeaa)DE-He213 Trap Axis (dpeaa)DE-He213 Smolyakova, O. B. verfasserin aut Enthalten in Radiophysics and quantum electronics New York, NY [u.a.] : Consultants Bureau, 1965 57(2015), 12 vom: Mai, Seite 857-867 (DE-627)325573395 (DE-600)2037675-3 1573-9120 nnns volume:57 year:2015 number:12 month:05 pages:857-867 https://dx.doi.org/10.1007/s11141-015-9570-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.16 ASE 53.74 ASE 33.80 ASE 39.22 ASE AR 57 2015 12 05 857-867 |
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10.1007/s11141-015-9570-9 doi (DE-627)SPR017046831 (SPR)s11141-015-9570-9-e DE-627 ger DE-627 rakwb eng 530 620 ASE 33.16 bkl 53.74 bkl 33.80 bkl 39.22 bkl Gospodchikov, E. D. verfasserin aut The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. Plasma Density (dpeaa)DE-He213 Electron Cyclotron Resonance (dpeaa)DE-He213 Magnetic Trap (dpeaa)DE-He213 Electromagnetic Wave Propagation (dpeaa)DE-He213 Trap Axis (dpeaa)DE-He213 Smolyakova, O. B. verfasserin aut Enthalten in Radiophysics and quantum electronics New York, NY [u.a.] : Consultants Bureau, 1965 57(2015), 12 vom: Mai, Seite 857-867 (DE-627)325573395 (DE-600)2037675-3 1573-9120 nnns volume:57 year:2015 number:12 month:05 pages:857-867 https://dx.doi.org/10.1007/s11141-015-9570-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-AST SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.16 ASE 53.74 ASE 33.80 ASE 39.22 ASE AR 57 2015 12 05 857-867 |
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Enthalten in Radiophysics and quantum electronics 57(2015), 12 vom: Mai, Seite 857-867 volume:57 year:2015 number:12 month:05 pages:857-867 |
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Enthalten in Radiophysics and quantum electronics 57(2015), 12 vom: Mai, Seite 857-867 volume:57 year:2015 number:12 month:05 pages:857-867 |
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Plasma Density Electron Cyclotron Resonance Magnetic Trap Electromagnetic Wave Propagation Trap Axis |
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Gospodchikov, E. D. @@aut@@ Smolyakova, O. B. @@aut@@ |
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| author |
Gospodchikov, E. D. |
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Gospodchikov, E. D. ddc 530 bkl 33.16 bkl 53.74 bkl 33.80 bkl 39.22 misc Plasma Density misc Electron Cyclotron Resonance misc Magnetic Trap misc Electromagnetic Wave Propagation misc Trap Axis The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap |
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530 620 ASE 33.16 bkl 53.74 bkl 33.80 bkl 39.22 bkl The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap Plasma Density (dpeaa)DE-He213 Electron Cyclotron Resonance (dpeaa)DE-He213 Magnetic Trap (dpeaa)DE-He213 Electromagnetic Wave Propagation (dpeaa)DE-He213 Trap Axis (dpeaa)DE-He213 |
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ddc 530 bkl 33.16 bkl 53.74 bkl 33.80 bkl 39.22 misc Plasma Density misc Electron Cyclotron Resonance misc Magnetic Trap misc Electromagnetic Wave Propagation misc Trap Axis |
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ddc 530 bkl 33.16 bkl 53.74 bkl 33.80 bkl 39.22 misc Plasma Density misc Electron Cyclotron Resonance misc Magnetic Trap misc Electromagnetic Wave Propagation misc Trap Axis |
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ddc 530 bkl 33.16 bkl 53.74 bkl 33.80 bkl 39.22 misc Plasma Density misc Electron Cyclotron Resonance misc Magnetic Trap misc Electromagnetic Wave Propagation misc Trap Axis |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap |
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The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap |
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Gospodchikov, E. D. |
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Radiophysics and quantum electronics |
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Radiophysics and quantum electronics |
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2015 |
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Gospodchikov, E. D. Smolyakova, O. B. |
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530 620 ASE 33.16 bkl 53.74 bkl 33.80 bkl 39.22 bkl |
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Elektronische Aufsätze |
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Gospodchikov, E. D. |
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10.1007/s11141-015-9570-9 |
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530 620 |
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verfasserin |
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features of refraction of electromagnetic waves near the electron cyclotron resonance surface in an open magnetic trap |
| title_auth |
The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap |
| abstract |
Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. |
| abstractGer |
Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. |
| abstract_unstemmed |
Some features of the electromagnetic wave propagation near the electron cyclotron resonance region in axisymmetric magnetic traps are studied both analytically and numerically. The ray paths are obtained with allowance for the plasma density inhomogeneities, magnetic field direction, and magnetic field strength. Criteria for the limiting cases of constructive refraction (the ray paths are attracted to the trap axis, where effective absorption takes place) and destructive refraction (the ray paths are expelled from the trap axis, and efficient heating of the central part of the plasma column is not possible) are found. It is shown that the inhomogeneities of the magnetic field direction and plasma density, which are typical of axisymmetric magnetic traps, as well as the spatial dispersion effects, can strongly affect the electromagnetic wave propagation near the electron cyclotron resonance surface. |
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The Features of Refraction of Electromagnetic Waves Near the Electron Cyclotron Resonance Surface in an Open Magnetic Trap |
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https://dx.doi.org/10.1007/s11141-015-9570-9 |
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Smolyakova, O. B. |
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|
| score |
7.4019375 |