Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles
Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the mag...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Ustinov, V. V. [verfasserIn] Rinkevich, A. B. [verfasserIn] Perov, D. V. [verfasserIn] Burkhanov, A. M. [verfasserIn] Samoylovich, M. I. [verfasserIn] Kleshcheva, S. M. [verfasserIn] Kuznetsov, E. A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2013 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Technical physics - Berlin : Springer Science + Business Media, 1997, 58(2013), 4 vom: Apr., Seite 568-577 |
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| Übergeordnetes Werk: |
volume:58 ; year:2013 ; number:4 ; month:04 ; pages:568-577 |
| Links: |
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| DOI / URN: |
10.1134/S1063784213040257 |
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| Katalog-ID: |
SPR019775881 |
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| 520 | |a Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. | ||
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| 650 | 4 | |a Zinc Ferrite |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Ferrite Spinel |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Rinkevich, A. B. |e verfasserin |4 aut | |
| 700 | 1 | |a Perov, D. V. |e verfasserin |4 aut | |
| 700 | 1 | |a Burkhanov, A. M. |e verfasserin |4 aut | |
| 700 | 1 | |a Samoylovich, M. I. |e verfasserin |4 aut | |
| 700 | 1 | |a Kleshcheva, S. M. |e verfasserin |4 aut | |
| 700 | 1 | |a Kuznetsov, E. A. |e verfasserin |4 aut | |
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10.1134/S1063784213040257 doi (DE-627)SPR019775881 (SPR)S1063784213040257-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl 31.00 bkl 50.30 bkl Ustinov, V. V. verfasserin aut Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. Ferrite (dpeaa)DE-He213 Field Dependence (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Zinc Ferrite (dpeaa)DE-He213 Ferrite Spinel (dpeaa)DE-He213 Rinkevich, A. B. verfasserin aut Perov, D. V. verfasserin aut Burkhanov, A. M. verfasserin aut Samoylovich, M. I. verfasserin aut Kleshcheva, S. M. verfasserin aut Kuznetsov, E. A. verfasserin aut Enthalten in Technical physics Berlin : Springer Science + Business Media, 1997 58(2013), 4 vom: Apr., Seite 568-577 (DE-627)311278795 (DE-600)2008502-3 1090-6525 nnns volume:58 year:2013 number:4 month:04 pages:568-577 https://dx.doi.org/10.1134/S1063784213040257 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT 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_65 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_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 33.00 ASE 31.00 ASE 50.30 ASE AR 58 2013 4 04 568-577 |
| spelling |
10.1134/S1063784213040257 doi (DE-627)SPR019775881 (SPR)S1063784213040257-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl 31.00 bkl 50.30 bkl Ustinov, V. V. verfasserin aut Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. Ferrite (dpeaa)DE-He213 Field Dependence (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Zinc Ferrite (dpeaa)DE-He213 Ferrite Spinel (dpeaa)DE-He213 Rinkevich, A. B. verfasserin aut Perov, D. V. verfasserin aut Burkhanov, A. M. verfasserin aut Samoylovich, M. I. verfasserin aut Kleshcheva, S. M. verfasserin aut Kuznetsov, E. A. verfasserin aut Enthalten in Technical physics Berlin : Springer Science + Business Media, 1997 58(2013), 4 vom: Apr., Seite 568-577 (DE-627)311278795 (DE-600)2008502-3 1090-6525 nnns volume:58 year:2013 number:4 month:04 pages:568-577 https://dx.doi.org/10.1134/S1063784213040257 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT 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_65 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_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 33.00 ASE 31.00 ASE 50.30 ASE AR 58 2013 4 04 568-577 |
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10.1134/S1063784213040257 doi (DE-627)SPR019775881 (SPR)S1063784213040257-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl 31.00 bkl 50.30 bkl Ustinov, V. V. verfasserin aut Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. Ferrite (dpeaa)DE-He213 Field Dependence (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Zinc Ferrite (dpeaa)DE-He213 Ferrite Spinel (dpeaa)DE-He213 Rinkevich, A. B. verfasserin aut Perov, D. V. verfasserin aut Burkhanov, A. M. verfasserin aut Samoylovich, M. I. verfasserin aut Kleshcheva, S. M. verfasserin aut Kuznetsov, E. A. verfasserin aut Enthalten in Technical physics Berlin : Springer Science + Business Media, 1997 58(2013), 4 vom: Apr., Seite 568-577 (DE-627)311278795 (DE-600)2008502-3 1090-6525 nnns volume:58 year:2013 number:4 month:04 pages:568-577 https://dx.doi.org/10.1134/S1063784213040257 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT 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_65 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_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 33.00 ASE 31.00 ASE 50.30 ASE AR 58 2013 4 04 568-577 |
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10.1134/S1063784213040257 doi (DE-627)SPR019775881 (SPR)S1063784213040257-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl 31.00 bkl 50.30 bkl Ustinov, V. V. verfasserin aut Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. Ferrite (dpeaa)DE-He213 Field Dependence (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Zinc Ferrite (dpeaa)DE-He213 Ferrite Spinel (dpeaa)DE-He213 Rinkevich, A. B. verfasserin aut Perov, D. V. verfasserin aut Burkhanov, A. M. verfasserin aut Samoylovich, M. I. verfasserin aut Kleshcheva, S. M. verfasserin aut Kuznetsov, E. A. verfasserin aut Enthalten in Technical physics Berlin : Springer Science + Business Media, 1997 58(2013), 4 vom: Apr., Seite 568-577 (DE-627)311278795 (DE-600)2008502-3 1090-6525 nnns volume:58 year:2013 number:4 month:04 pages:568-577 https://dx.doi.org/10.1134/S1063784213040257 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT 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_65 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_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 33.00 ASE 31.00 ASE 50.30 ASE AR 58 2013 4 04 568-577 |
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10.1134/S1063784213040257 doi (DE-627)SPR019775881 (SPR)S1063784213040257-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl 31.00 bkl 50.30 bkl Ustinov, V. V. verfasserin aut Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. Ferrite (dpeaa)DE-He213 Field Dependence (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Zinc Ferrite (dpeaa)DE-He213 Ferrite Spinel (dpeaa)DE-He213 Rinkevich, A. B. verfasserin aut Perov, D. V. verfasserin aut Burkhanov, A. M. verfasserin aut Samoylovich, M. I. verfasserin aut Kleshcheva, S. M. verfasserin aut Kuznetsov, E. A. verfasserin aut Enthalten in Technical physics Berlin : Springer Science + Business Media, 1997 58(2013), 4 vom: Apr., Seite 568-577 (DE-627)311278795 (DE-600)2008502-3 1090-6525 nnns volume:58 year:2013 number:4 month:04 pages:568-577 https://dx.doi.org/10.1134/S1063784213040257 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT 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_65 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_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 33.00 ASE 31.00 ASE 50.30 ASE AR 58 2013 4 04 568-577 |
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Enthalten in Technical physics 58(2013), 4 vom: Apr., Seite 568-577 volume:58 year:2013 number:4 month:04 pages:568-577 |
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Ustinov, V. V. @@aut@@ Rinkevich, A. B. @@aut@@ Perov, D. V. @@aut@@ Burkhanov, A. M. @@aut@@ Samoylovich, M. I. @@aut@@ Kleshcheva, S. M. @@aut@@ Kuznetsov, E. A. @@aut@@ |
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V.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2013</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Ferrite</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Field Dependence</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Opal Matrice</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Zinc Ferrite</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Ferrite Spinel</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Rinkevich, A. 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Ustinov, V. V. |
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Ustinov, V. V. ddc 530 bkl 33.00 bkl 31.00 bkl 50.30 misc Ferrite misc Field Dependence misc Opal Matrice misc Zinc Ferrite misc Ferrite Spinel Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles |
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530 ASE 33.00 bkl 31.00 bkl 50.30 bkl Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles Ferrite (dpeaa)DE-He213 Field Dependence (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Zinc Ferrite (dpeaa)DE-He213 Ferrite Spinel (dpeaa)DE-He213 |
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ddc 530 bkl 33.00 bkl 31.00 bkl 50.30 misc Ferrite misc Field Dependence misc Opal Matrice misc Zinc Ferrite misc Ferrite Spinel |
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ddc 530 bkl 33.00 bkl 31.00 bkl 50.30 misc Ferrite misc Field Dependence misc Opal Matrice misc Zinc Ferrite misc Ferrite Spinel |
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ddc 530 bkl 33.00 bkl 31.00 bkl 50.30 misc Ferrite misc Field Dependence misc Opal Matrice misc Zinc Ferrite misc Ferrite Spinel |
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Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles |
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Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles |
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Ustinov, V. V. Rinkevich, A. B. Perov, D. V. Burkhanov, A. M. Samoylovich, M. I. Kleshcheva, S. M. Kuznetsov, E. A. |
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verfasserin |
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giant antiresonance in electromagnetic wave reflection from a 3d structure with ferrite spinel nanoparticles |
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Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles |
| abstract |
Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. |
| abstractGer |
Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. |
| abstract_unstemmed |
Abstract We analyze the microwave properties of nanocomposite materials obtained by embedding opal matrices (regular packing of $ SiO_{2} $ spheres about 250 nm in diameter) of ferrite spinel nanoparticles in the interspherical space. It is found that the main reason for microwave changes is the magnetic resonance in a nanocomposite. In addition to the resonance, antiresonance also takes place, which is manifested as a minimum of absorbed power at frequencies higher than a certain frequency characteristic of the given type of ferrite particles. Antiresonance appears in the fields smaller than the resonance field. The amplitude of the reflected signal in antiresonance increases fourfold. The measurements are taken in the frequency range from 26 to 38 GHz. The change in the moduli of transmission and reflection coefficients in the external magnetic field in a rectangular waveguide containing a nanocomposite is analyzed. The modulus of the wave transmittance through a rectangular resonator with a nanocomposite specimen is measured. The structural analysis of nanocomposites is carried out. In addition, the magnetization curves and hysteresis loops are measured. |
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4 |
| title_short |
Giant antiresonance in electromagnetic wave reflection from a 3D structure with ferrite spinel nanoparticles |
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https://dx.doi.org/10.1134/S1063784213040257 |
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| author2 |
Rinkevich, A. B. Perov, D. V. Burkhanov, A. M. Samoylovich, M. I. Kleshcheva, S. M. Kuznetsov, E. A. |
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Rinkevich, A. B. Perov, D. V. Burkhanov, A. M. Samoylovich, M. I. Kleshcheva, S. M. Kuznetsov, E. A. |
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2024-07-04T02:53:06.012Z |
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| score |
7.402915 |