Nonlinear Self-Similar Beams of Electromagnetic Waves in Vacuum
We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Vlasov, S. N. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media New York 2015 |
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| Übergeordnetes Werk: |
Enthalten in: Radiophysics and quantum electronics - Springer US, 1969, 58(2015), 7 vom: Dez., Seite 497-503 |
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| Übergeordnetes Werk: |
volume:58 ; year:2015 ; number:7 ; month:12 ; pages:497-503 |
| Links: |
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| DOI / URN: |
10.1007/s11141-015-9622-1 |
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OLC2063587515 |
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| 520 | |a We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. | ||
| 650 | 4 | |a Beam Width | |
| 650 | 4 | |a Beam Power | |
| 650 | 4 | |a Critical Power | |
| 650 | 4 | |a Resonance Curve | |
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10.1007/s11141-015-9622-1 doi (DE-627)OLC2063587515 (DE-He213)s11141-015-9622-1-p DE-627 ger DE-627 rakwb eng 530 620 VZ Vlasov, S. N. verfasserin aut Nonlinear Self-Similar Beams of Electromagnetic Waves in Vacuum 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. Beam Width Beam Power Critical Power Resonance Curve Wave Beam Enthalten in Radiophysics and quantum electronics Springer US, 1969 58(2015), 7 vom: Dez., Seite 497-503 (DE-627)130499560 (DE-600)760167-0 (DE-576)016080793 0033-8443 nnns volume:58 year:2015 number:7 month:12 pages:497-503 https://doi.org/10.1007/s11141-015-9622-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_70 AR 58 2015 7 12 497-503 |
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10.1007/s11141-015-9622-1 doi (DE-627)OLC2063587515 (DE-He213)s11141-015-9622-1-p DE-627 ger DE-627 rakwb eng 530 620 VZ Vlasov, S. N. verfasserin aut Nonlinear Self-Similar Beams of Electromagnetic Waves in Vacuum 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. Beam Width Beam Power Critical Power Resonance Curve Wave Beam Enthalten in Radiophysics and quantum electronics Springer US, 1969 58(2015), 7 vom: Dez., Seite 497-503 (DE-627)130499560 (DE-600)760167-0 (DE-576)016080793 0033-8443 nnns volume:58 year:2015 number:7 month:12 pages:497-503 https://doi.org/10.1007/s11141-015-9622-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_70 AR 58 2015 7 12 497-503 |
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10.1007/s11141-015-9622-1 doi (DE-627)OLC2063587515 (DE-He213)s11141-015-9622-1-p DE-627 ger DE-627 rakwb eng 530 620 VZ Vlasov, S. N. verfasserin aut Nonlinear Self-Similar Beams of Electromagnetic Waves in Vacuum 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. Beam Width Beam Power Critical Power Resonance Curve Wave Beam Enthalten in Radiophysics and quantum electronics Springer US, 1969 58(2015), 7 vom: Dez., Seite 497-503 (DE-627)130499560 (DE-600)760167-0 (DE-576)016080793 0033-8443 nnns volume:58 year:2015 number:7 month:12 pages:497-503 https://doi.org/10.1007/s11141-015-9622-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_70 AR 58 2015 7 12 497-503 |
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10.1007/s11141-015-9622-1 doi (DE-627)OLC2063587515 (DE-He213)s11141-015-9622-1-p DE-627 ger DE-627 rakwb eng 530 620 VZ Vlasov, S. N. verfasserin aut Nonlinear Self-Similar Beams of Electromagnetic Waves in Vacuum 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. Beam Width Beam Power Critical Power Resonance Curve Wave Beam Enthalten in Radiophysics and quantum electronics Springer US, 1969 58(2015), 7 vom: Dez., Seite 497-503 (DE-627)130499560 (DE-600)760167-0 (DE-576)016080793 0033-8443 nnns volume:58 year:2015 number:7 month:12 pages:497-503 https://doi.org/10.1007/s11141-015-9622-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_70 AR 58 2015 7 12 497-503 |
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10.1007/s11141-015-9622-1 doi (DE-627)OLC2063587515 (DE-He213)s11141-015-9622-1-p DE-627 ger DE-627 rakwb eng 530 620 VZ Vlasov, S. N. verfasserin aut Nonlinear Self-Similar Beams of Electromagnetic Waves in Vacuum 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. Beam Width Beam Power Critical Power Resonance Curve Wave Beam Enthalten in Radiophysics and quantum electronics Springer US, 1969 58(2015), 7 vom: Dez., Seite 497-503 (DE-627)130499560 (DE-600)760167-0 (DE-576)016080793 0033-8443 nnns volume:58 year:2015 number:7 month:12 pages:497-503 https://doi.org/10.1007/s11141-015-9622-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_70 AR 58 2015 7 12 497-503 |
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We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. © Springer Science+Business Media New York 2015 |
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We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. © Springer Science+Business Media New York 2015 |
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We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams. © Springer Science+Business Media New York 2015 |
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N.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Nonlinear Self-Similar Beams of Electromagnetic Waves in Vacuum</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2015</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Springer Science+Business Media New York 2015</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">We study nonlinear beams of electromagnetic waves in vacuum. Within the lowest approximation, their structure is determined by the cubic self-focusing nonlinearity, which manifests itself with the maximum intensity in the presence of counterpropagating waves. It is shown that the fields in the beams have no singularities if their power is less than the critical power of the self-focusing. The dependences of the eigenfrequencies of the modes of the quasioptical resonator on the beam power are found. The structure of the fields of these modes corresponds to self-similar wave beams.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Beam Width</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Beam Power</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Critical Power</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Resonance Curve</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Wave Beam</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Radiophysics and quantum electronics</subfield><subfield code="d">Springer US, 1969</subfield><subfield code="g">58(2015), 7 vom: Dez., Seite 497-503</subfield><subfield code="w">(DE-627)130499560</subfield><subfield code="w">(DE-600)760167-0</subfield><subfield code="w">(DE-576)016080793</subfield><subfield code="x">0033-8443</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:58</subfield><subfield code="g">year:2015</subfield><subfield code="g">number:7</subfield><subfield code="g">month:12</subfield><subfield code="g">pages:497-503</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s11141-015-9622-1</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OPC-AST</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">58</subfield><subfield code="j">2015</subfield><subfield code="e">7</subfield><subfield code="c">12</subfield><subfield code="h">497-503</subfield></datafield></record></collection>
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