Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas
Drake, R. P. ; Bauer, B. S. ; Baker, K. L. ; Mizuno, K. ; Sleaford, B. ; Rubenchik, A. M. ; Estabrook, Kent ; Labaune, C. ; Baton, S. ; Jalinaud, T. ; Schifano, E. ; Goldman, M. V. ; Newman, D. L.
[S.l.] : American Institute of Physics (AIP)
Published 1995
[S.l.] : American Institute of Physics (AIP)
Published 1995
| ISSN: |
1089-7674
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|---|---|
| Source: |
AIP Digital Archive
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| Topics: |
Physics
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| Notes: |
We have measured and analyzed the second harmonic emission, both in the plane of the laser electric field and perpendicular to it, at several angles near 135° from the laser wave vector. The experiments used from 1 to 80 J of 1.053 μm light to irradiate carbon–hydrogen (CH) targets with a 550 ps pulse. A random phase plate was used, producing characteristic intensities in the range of 1013–1014 W/cm2. This was sufficient to drive the Ion Acoustic Decay Instability, producing Stokes emission well-separated from the emission spike at the second harmonic of the laser frequency. The spectral structure of the Stokes emission was qualitatively similar for all intensities and angles of observation. The duration of the signals showed trends anticipated from linear theory. To explain the scaling of the signal strength and spectral width requires nonlinear theory. © 1995 American Institute of Physics.
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| Type of Medium: |
Electronic Resource
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| URL: |
| _version_ | 1798289734756204545 |
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| autor | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. |
| autorsonst | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. |
| book_url | http://dx.doi.org/10.1063/1.871449 |
| datenlieferant | nat_lic_papers |
| hauptsatz | hsatz_simple |
| identnr | NLZ219382425 |
| issn | 1089-7674 |
| journal_name | Physics of Plasmas |
| materialart | 1 |
| notes | We have measured and analyzed the second harmonic emission, both in the plane of the laser electric field and perpendicular to it, at several angles near 135° from the laser wave vector. The experiments used from 1 to 80 J of 1.053 μm light to irradiate carbon–hydrogen (CH) targets with a 550 ps pulse. A random phase plate was used, producing characteristic intensities in the range of 1013–1014 W/cm2. This was sufficient to drive the Ion Acoustic Decay Instability, producing Stokes emission well-separated from the emission spike at the second harmonic of the laser frequency. The spectral structure of the Stokes emission was qualitatively similar for all intensities and angles of observation. The duration of the signals showed trends anticipated from linear theory. To explain the scaling of the signal strength and spectral width requires nonlinear theory. © 1995 American Institute of Physics. |
| package_name | American Institute of Physics (AIP) |
| publikationsjahr_anzeige | 1995 |
| publikationsjahr_facette | 1995 |
| publikationsjahr_intervall | 8004:1995-1999 |
| publikationsjahr_sort | 1995 |
| publikationsort | [S.l.] |
| publisher | American Institute of Physics (AIP) |
| reference | 2 (1995), S. 3473-3483 |
| search_space | articles |
| shingle_author_1 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. |
| shingle_author_2 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. |
| shingle_author_3 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. |
| shingle_author_4 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. |
| shingle_catch_all_1 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas We have measured and analyzed the second harmonic emission, both in the plane of the laser electric field and perpendicular to it, at several angles near 135° from the laser wave vector. The experiments used from 1 to 80 J of 1.053 μm light to irradiate carbon–hydrogen (CH) targets with a 550 ps pulse. A random phase plate was used, producing characteristic intensities in the range of 1013–1014 W/cm2. This was sufficient to drive the Ion Acoustic Decay Instability, producing Stokes emission well-separated from the emission spike at the second harmonic of the laser frequency. The spectral structure of the Stokes emission was qualitatively similar for all intensities and angles of observation. The duration of the signals showed trends anticipated from linear theory. To explain the scaling of the signal strength and spectral width requires nonlinear theory. © 1995 American Institute of Physics. 1089-7674 10897674 American Institute of Physics (AIP) |
| shingle_catch_all_2 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas We have measured and analyzed the second harmonic emission, both in the plane of the laser electric field and perpendicular to it, at several angles near 135° from the laser wave vector. The experiments used from 1 to 80 J of 1.053 μm light to irradiate carbon–hydrogen (CH) targets with a 550 ps pulse. A random phase plate was used, producing characteristic intensities in the range of 1013–1014 W/cm2. This was sufficient to drive the Ion Acoustic Decay Instability, producing Stokes emission well-separated from the emission spike at the second harmonic of the laser frequency. The spectral structure of the Stokes emission was qualitatively similar for all intensities and angles of observation. The duration of the signals showed trends anticipated from linear theory. To explain the scaling of the signal strength and spectral width requires nonlinear theory. © 1995 American Institute of Physics. 1089-7674 10897674 American Institute of Physics (AIP) |
| shingle_catch_all_3 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas We have measured and analyzed the second harmonic emission, both in the plane of the laser electric field and perpendicular to it, at several angles near 135° from the laser wave vector. The experiments used from 1 to 80 J of 1.053 μm light to irradiate carbon–hydrogen (CH) targets with a 550 ps pulse. A random phase plate was used, producing characteristic intensities in the range of 1013–1014 W/cm2. This was sufficient to drive the Ion Acoustic Decay Instability, producing Stokes emission well-separated from the emission spike at the second harmonic of the laser frequency. The spectral structure of the Stokes emission was qualitatively similar for all intensities and angles of observation. The duration of the signals showed trends anticipated from linear theory. To explain the scaling of the signal strength and spectral width requires nonlinear theory. © 1995 American Institute of Physics. 1089-7674 10897674 American Institute of Physics (AIP) |
| shingle_catch_all_4 | Drake, R. P. Bauer, B. S. Baker, K. L. Mizuno, K. Sleaford, B. Rubenchik, A. M. Estabrook, Kent Labaune, C. Baton, S. Jalinaud, T. Schifano, E. Goldman, M. V. Newman, D. L. Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas We have measured and analyzed the second harmonic emission, both in the plane of the laser electric field and perpendicular to it, at several angles near 135° from the laser wave vector. The experiments used from 1 to 80 J of 1.053 μm light to irradiate carbon–hydrogen (CH) targets with a 550 ps pulse. A random phase plate was used, producing characteristic intensities in the range of 1013–1014 W/cm2. This was sufficient to drive the Ion Acoustic Decay Instability, producing Stokes emission well-separated from the emission spike at the second harmonic of the laser frequency. The spectral structure of the Stokes emission was qualitatively similar for all intensities and angles of observation. The duration of the signals showed trends anticipated from linear theory. To explain the scaling of the signal strength and spectral width requires nonlinear theory. © 1995 American Institute of Physics. 1089-7674 10897674 American Institute of Physics (AIP) |
| shingle_title_1 | Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas |
| shingle_title_2 | Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas |
| shingle_title_3 | Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas |
| shingle_title_4 | Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas |
| sigel_instance_filter | dkfz geomar wilbert ipn albert |
| source_archive | AIP Digital Archive |
| timestamp | 2024-05-06T08:05:33.111Z |
| titel | Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas |
| titel_suche | Measurements of the angular and temporal structure of second-harmonic emission from laser-produced plasmas |
| topic | U |
| uid | nat_lic_papers_NLZ219382425 |