Interaction of forward and backward waves in a Kerr medium
Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequen...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Maimistov, A. I. [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: |
© Pleiades Publishing, Ltd. 2015 |
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| Übergeordnetes Werk: |
Enthalten in: Optics and spectroscopy - Pleiades Publishing, 1959, 118(2015), 5 vom: Mai, Seite 803-808 |
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| Übergeordnetes Werk: |
volume:118 ; year:2015 ; number:5 ; month:05 ; pages:803-808 |
| Links: |
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| DOI / URN: |
10.1134/S0030400X15050094 |
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OLC2047091381 |
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| 520 | |a Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequency has the same direction as the group velocity, while the phase and the group velocities at the other frequency have opposite directions. Coupling between the waves in a Kerr medium is caused by cross modulation. It is demonstrated that a steady-state biharmonic wave propagating as a single whole can be formed in this situation. | ||
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10.1134/S0030400X15050094 doi (DE-627)OLC2047091381 (DE-He213)S0030400X15050094-p DE-627 ger DE-627 rakwb eng 530 VZ 11 ssgn Maimistov, A. I. verfasserin aut Interaction of forward and backward waves in a Kerr medium 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2015 Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequency has the same direction as the group velocity, while the phase and the group velocities at the other frequency have opposite directions. Coupling between the waves in a Kerr medium is caused by cross modulation. It is demonstrated that a steady-state biharmonic wave propagating as a single whole can be formed in this situation. Soliton Solitary Wave Group Velocity Group Velocity Dispersion Dark Soliton Lyashko, E. I. aut Enthalten in Optics and spectroscopy Pleiades Publishing, 1959 118(2015), 5 vom: Mai, Seite 803-808 (DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 0030-400X nnns volume:118 year:2015 number:5 month:05 pages:803-808 https://doi.org/10.1134/S0030400X15050094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_60 GBV_ILN_70 AR 118 2015 5 05 803-808 |
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10.1134/S0030400X15050094 doi (DE-627)OLC2047091381 (DE-He213)S0030400X15050094-p DE-627 ger DE-627 rakwb eng 530 VZ 11 ssgn Maimistov, A. I. verfasserin aut Interaction of forward and backward waves in a Kerr medium 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2015 Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequency has the same direction as the group velocity, while the phase and the group velocities at the other frequency have opposite directions. Coupling between the waves in a Kerr medium is caused by cross modulation. It is demonstrated that a steady-state biharmonic wave propagating as a single whole can be formed in this situation. Soliton Solitary Wave Group Velocity Group Velocity Dispersion Dark Soliton Lyashko, E. I. aut Enthalten in Optics and spectroscopy Pleiades Publishing, 1959 118(2015), 5 vom: Mai, Seite 803-808 (DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 0030-400X nnns volume:118 year:2015 number:5 month:05 pages:803-808 https://doi.org/10.1134/S0030400X15050094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_60 GBV_ILN_70 AR 118 2015 5 05 803-808 |
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Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequency has the same direction as the group velocity, while the phase and the group velocities at the other frequency have opposite directions. Coupling between the waves in a Kerr medium is caused by cross modulation. It is demonstrated that a steady-state biharmonic wave propagating as a single whole can be formed in this situation. © Pleiades Publishing, Ltd. 2015 |
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Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequency has the same direction as the group velocity, while the phase and the group velocities at the other frequency have opposite directions. Coupling between the waves in a Kerr medium is caused by cross modulation. It is demonstrated that a steady-state biharmonic wave propagating as a single whole can be formed in this situation. © Pleiades Publishing, Ltd. 2015 |
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Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequency has the same direction as the group velocity, while the phase and the group velocities at the other frequency have opposite directions. Coupling between the waves in a Kerr medium is caused by cross modulation. It is demonstrated that a steady-state biharmonic wave propagating as a single whole can be formed in this situation. © Pleiades Publishing, Ltd. 2015 |
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I.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Interaction of forward and backward waves in a Kerr medium</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">© Pleiades Publishing, Ltd. 2015</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Interaction of forward and backward waves in a nonlinear medium exhibiting a third-order nonlinearity (the Kerr medium) is investigated theoretically. We have analyzed the propagation of two quasi-harmonic waves with different carrier frequencies, such that the phase velocity at one frequency has the same direction as the group velocity, while the phase and the group velocities at the other frequency have opposite directions. Coupling between the waves in a Kerr medium is caused by cross modulation. It is demonstrated that a steady-state biharmonic wave propagating as a single whole can be formed in this situation.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Soliton</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Solitary Wave</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Group Velocity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Group Velocity Dispersion</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Dark Soliton</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lyashko, E. I.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optics and spectroscopy</subfield><subfield code="d">Pleiades Publishing, 1959</subfield><subfield code="g">118(2015), 5 vom: Mai, Seite 803-808</subfield><subfield code="w">(DE-627)129496499</subfield><subfield code="w">(DE-600)207391-2</subfield><subfield code="w">(DE-576)014895048</subfield><subfield code="x">0030-400X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:118</subfield><subfield code="g">year:2015</subfield><subfield code="g">number:5</subfield><subfield code="g">month:05</subfield><subfield code="g">pages:803-808</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/S0030400X15050094</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-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</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">118</subfield><subfield code="j">2015</subfield><subfield code="e">5</subfield><subfield code="c">05</subfield><subfield code="h">803-808</subfield></datafield></record></collection>
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