Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis
Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Mansfel’d, G. D. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2010 |
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| Schlagwörter: |
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| Anmerkung: |
© Pleiades Publishing, Ltd. 2010 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of communications technology and electronics - Moscow : MAIK Nauka/Interperiodica Publ., 1996, 55(2010), 11 vom: Nov., Seite 1295-1303 |
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| Übergeordnetes Werk: |
volume:55 ; year:2010 ; number:11 ; month:11 ; pages:1295-1303 |
| Links: |
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| DOI / URN: |
10.1134/S1064226910110124 |
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| Katalog-ID: |
SPR020076215 |
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| 100 | 1 | |a Mansfel’d, G. D. |e verfasserin |4 aut | |
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| 520 | |a Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. | ||
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| 700 | 1 | |a Popova, D. V. |4 aut | |
| 700 | 1 | |a Alekseev, S. G. |4 aut | |
| 700 | 1 | |a Polzikova, N. I. |4 aut | |
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10.1134/S1064226910110124 doi (DE-627)SPR020076215 (SPR)S1064226910110124-e DE-627 ger DE-627 rakwb eng Mansfel’d, G. D. verfasserin aut Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. Input Impedance (dpeaa)DE-He213 Acoustic Impedance (dpeaa)DE-He213 Piezoelectric Layer (dpeaa)DE-He213 Quarter Wave (dpeaa)DE-He213 Imped Ance (dpeaa)DE-He213 Popova, D. V. aut Alekseev, S. G. aut Polzikova, N. I. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 55(2010), 11 vom: Nov., Seite 1295-1303 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:55 year:2010 number:11 month:11 pages:1295-1303 https://dx.doi.org/10.1134/S1064226910110124 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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_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_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_4126 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 AR 55 2010 11 11 1295-1303 |
| spelling |
10.1134/S1064226910110124 doi (DE-627)SPR020076215 (SPR)S1064226910110124-e DE-627 ger DE-627 rakwb eng Mansfel’d, G. D. verfasserin aut Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. Input Impedance (dpeaa)DE-He213 Acoustic Impedance (dpeaa)DE-He213 Piezoelectric Layer (dpeaa)DE-He213 Quarter Wave (dpeaa)DE-He213 Imped Ance (dpeaa)DE-He213 Popova, D. V. aut Alekseev, S. G. aut Polzikova, N. I. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 55(2010), 11 vom: Nov., Seite 1295-1303 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:55 year:2010 number:11 month:11 pages:1295-1303 https://dx.doi.org/10.1134/S1064226910110124 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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_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_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_4126 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 AR 55 2010 11 11 1295-1303 |
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10.1134/S1064226910110124 doi (DE-627)SPR020076215 (SPR)S1064226910110124-e DE-627 ger DE-627 rakwb eng Mansfel’d, G. D. verfasserin aut Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. Input Impedance (dpeaa)DE-He213 Acoustic Impedance (dpeaa)DE-He213 Piezoelectric Layer (dpeaa)DE-He213 Quarter Wave (dpeaa)DE-He213 Imped Ance (dpeaa)DE-He213 Popova, D. V. aut Alekseev, S. G. aut Polzikova, N. I. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 55(2010), 11 vom: Nov., Seite 1295-1303 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:55 year:2010 number:11 month:11 pages:1295-1303 https://dx.doi.org/10.1134/S1064226910110124 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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_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_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_4126 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 AR 55 2010 11 11 1295-1303 |
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10.1134/S1064226910110124 doi (DE-627)SPR020076215 (SPR)S1064226910110124-e DE-627 ger DE-627 rakwb eng Mansfel’d, G. D. verfasserin aut Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. Input Impedance (dpeaa)DE-He213 Acoustic Impedance (dpeaa)DE-He213 Piezoelectric Layer (dpeaa)DE-He213 Quarter Wave (dpeaa)DE-He213 Imped Ance (dpeaa)DE-He213 Popova, D. V. aut Alekseev, S. G. aut Polzikova, N. I. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 55(2010), 11 vom: Nov., Seite 1295-1303 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:55 year:2010 number:11 month:11 pages:1295-1303 https://dx.doi.org/10.1134/S1064226910110124 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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_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_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_4126 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 AR 55 2010 11 11 1295-1303 |
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10.1134/S1064226910110124 doi (DE-627)SPR020076215 (SPR)S1064226910110124-e DE-627 ger DE-627 rakwb eng Mansfel’d, G. D. verfasserin aut Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. Input Impedance (dpeaa)DE-He213 Acoustic Impedance (dpeaa)DE-He213 Piezoelectric Layer (dpeaa)DE-He213 Quarter Wave (dpeaa)DE-He213 Imped Ance (dpeaa)DE-He213 Popova, D. V. aut Alekseev, S. G. aut Polzikova, N. I. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 55(2010), 11 vom: Nov., Seite 1295-1303 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:55 year:2010 number:11 month:11 pages:1295-1303 https://dx.doi.org/10.1134/S1064226910110124 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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_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_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_4126 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 AR 55 2010 11 11 1295-1303 |
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Mansfel’d, G. D. @@aut@@ Popova, D. V. @@aut@@ Alekseev, S. G. @@aut@@ Polzikova, N. I. @@aut@@ |
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Mansfel’d, G. D. |
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Mansfel’d, G. D. misc Input Impedance misc Acoustic Impedance misc Piezoelectric Layer misc Quarter Wave misc Imped Ance Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis |
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Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis Input Impedance (dpeaa)DE-He213 Acoustic Impedance (dpeaa)DE-He213 Piezoelectric Layer (dpeaa)DE-He213 Quarter Wave (dpeaa)DE-He213 Imped Ance (dpeaa)DE-He213 |
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analysis of thin-film bragg structures and piezoelectric microwave resonators on their basis |
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Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis |
| abstract |
Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. © Pleiades Publishing, Ltd. 2010 |
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Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. © Pleiades Publishing, Ltd. 2010 |
| abstract_unstemmed |
Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown. © Pleiades Publishing, Ltd. 2010 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR020076215</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230330161228.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2010 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1134/S1064226910110124</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR020076215</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)S1064226910110124-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Mansfel’d, G. D.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Analysis of thin-film Bragg structures and piezoelectric microwave resonators on their basis</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2010</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="500" ind1=" " ind2=" "><subfield code="a">© Pleiades Publishing, Ltd. 2010</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A number of regularities inherent in acoustic Bragg structures and microwave resonators manufactured on their basis are revealed. It is found out that, even in the case of a relatively small number of structure layers, the width of the forbidden gap is the same as for an infinite number of layers. The resonator eigenfrequencies are found to be dependent on not only the resonance frequency of the intrinsic resonator, which is determined by only the resonator thickness and the sound velocity, but also on the position of this resonance frequency in the forbidden gap. The existence of additional quasi-harmonic modes whose frequencies are close to harmonics of the calculated frequency and are nonlinearly dependent on this frequency is shown.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Input Impedance</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Acoustic Impedance</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Piezoelectric Layer</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Quarter Wave</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Imped Ance</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Popova, D. 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