Eintrag weiter verarbeiten
Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma
Gespeichert in:
| Zeitschriftentitel: | High Power Laser Science and Engineering |
|---|---|
| Personen und Körperschaften: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
| In: | High Power Laser Science and Engineering, 7, 2019 |
| Format: | E-Article |
| Sprache: | Englisch |
| veröffentlicht: |
Cambridge University Press (CUP)
|
| Schlagwörter: |
| author_facet |
Cristoforetti, G. Antonelli, L. Mancelli, D. Atzeni, S. Baffigi, F. Barbato, F. Batani, D. Boutoux, G. D’Amato, F. Dostal, J. Dudzak, R. Filippov, E. Gu, Y. J. Juha, L. Klimo, O. Krus, M. Malko, S. Martynenko, A. S. Nicolai, Ph. Ospina, V. Pikuz, S. Renner, O. Santos, J. Tikhonchuk, V. T. Trela, J. Viciani, S. Volpe, L. Weber, S. Gizzi, L. A. Cristoforetti, G. Antonelli, L. Mancelli, D. Atzeni, S. Baffigi, F. Barbato, F. Batani, D. Boutoux, G. D’Amato, F. Dostal, J. Dudzak, R. Filippov, E. Gu, Y. J. Juha, L. Klimo, O. Krus, M. Malko, S. Martynenko, A. S. Nicolai, Ph. Ospina, V. Pikuz, S. Renner, O. Santos, J. Tikhonchuk, V. T. Trela, J. Viciani, S. Volpe, L. Weber, S. Gizzi, L. A. |
|---|---|
| author |
Cristoforetti, G. Antonelli, L. Mancelli, D. Atzeni, S. Baffigi, F. Barbato, F. Batani, D. Boutoux, G. D’Amato, F. Dostal, J. Dudzak, R. Filippov, E. Gu, Y. J. Juha, L. Klimo, O. Krus, M. Malko, S. Martynenko, A. S. Nicolai, Ph. Ospina, V. Pikuz, S. Renner, O. Santos, J. Tikhonchuk, V. T. Trela, J. Viciani, S. Volpe, L. Weber, S. Gizzi, L. A. |
| spellingShingle |
Cristoforetti, G. Antonelli, L. Mancelli, D. Atzeni, S. Baffigi, F. Barbato, F. Batani, D. Boutoux, G. D’Amato, F. Dostal, J. Dudzak, R. Filippov, E. Gu, Y. J. Juha, L. Klimo, O. Krus, M. Malko, S. Martynenko, A. S. Nicolai, Ph. Ospina, V. Pikuz, S. Renner, O. Santos, J. Tikhonchuk, V. T. Trela, J. Viciani, S. Volpe, L. Weber, S. Gizzi, L. A. High Power Laser Science and Engineering Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma Nuclear Energy and Engineering Nuclear and High Energy Physics Atomic and Molecular Physics, and Optics Electronic, Optical and Magnetic Materials |
| author_sort |
cristoforetti, g. |
| spelling |
Cristoforetti, G. Antonelli, L. Mancelli, D. Atzeni, S. Baffigi, F. Barbato, F. Batani, D. Boutoux, G. D’Amato, F. Dostal, J. Dudzak, R. Filippov, E. Gu, Y. J. Juha, L. Klimo, O. Krus, M. Malko, S. Martynenko, A. S. Nicolai, Ph. Ospina, V. Pikuz, S. Renner, O. Santos, J. Tikhonchuk, V. T. Trela, J. Viciani, S. Volpe, L. Weber, S. Gizzi, L. A. 2095-4719 2052-3289 Cambridge University Press (CUP) Nuclear Energy and Engineering Nuclear and High Energy Physics Atomic and Molecular Physics, and Optics Electronic, Optical and Magnetic Materials http://dx.doi.org/10.1017/hpl.2019.37 <jats:p>Laser–plasma interaction (LPI) at intensities <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline1" xlink:type="simple" /><jats:tex-math>$10^{15}{-}10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives> </jats:inline-formula> is dominated by parametric instabilities which can be responsible for a significant amount of non-collisional absorption and generate large fluxes of high-energy nonthermal electrons. Such a regime is of paramount importance for inertial confinement fusion (ICF) and in particular for the shock ignition scheme. In this paper we report on an experiment carried out at the Prague Asterix Laser System (PALS) facility to investigate the extent and time history of stimulated Raman scattering (SRS) and two-plasmon decay (TPD) instabilities, driven by the interaction of an infrared laser pulse at an intensity <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline2" xlink:type="simple" /><jats:tex-math>${\sim}1.2\times 10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives> </jats:inline-formula> with a <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline3" xlink:type="simple" /><jats:tex-math>${\sim}100~\unicode[STIX]{x03BC}\text{m}$</jats:tex-math></jats:alternatives> </jats:inline-formula> scalelength plasma produced from irradiation of a flat plastic target. The laser pulse duration (300 ps) and the high value of plasma temperature (<jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline4" xlink:type="simple" /><jats:tex-math>${\sim}4~\text{keV}$</jats:tex-math></jats:alternatives> </jats:inline-formula>) expected from hydrodynamic simulations make these results interesting for a deeper understanding of LPI in shock ignition conditions. Experimental results show that absolute TPD/SRS, driven at a quarter of the critical density, and convective SRS, driven at lower plasma densities, are well separated in time, with absolute instabilities driven at early times of interaction and convective backward SRS emerging at the laser peak and persisting all over the tail of the pulse. Side-scattering SRS, driven at low plasma densities, is also clearly observed. Experimental results are compared to fully kinetic large-scale, two-dimensional simulations. Particle-in-cell results, beyond reproducing the framework delineated by the experimental measurements, reveal the importance of filamentation instability in ruling the onset of SRS and stimulated Brillouin scattering instabilities and confirm the crucial role of collisionless absorption in the LPI energy balance.</jats:p> Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma High Power Laser Science and Engineering |
| doi_str_mv |
10.1017/hpl.2019.37 |
| facet_avail |
Online Free |
| finc_class_facet |
Physik Technik |
| format |
ElectronicArticle |
| fullrecord |
blob:ai-49-aHR0cDovL2R4LmRvaS5vcmcvMTAuMTAxNy9ocGwuMjAxOS4zNw |
| id |
ai-49-aHR0cDovL2R4LmRvaS5vcmcvMTAuMTAxNy9ocGwuMjAxOS4zNw |
| institution |
DE-Gla1 DE-Zi4 DE-15 DE-Pl11 DE-Rs1 DE-105 DE-14 DE-Ch1 DE-L229 DE-D275 DE-Bn3 DE-Brt1 DE-Zwi2 DE-D161 |
| imprint |
Cambridge University Press (CUP), 2019 |
| imprint_str_mv |
Cambridge University Press (CUP), 2019 |
| issn |
2095-4719 2052-3289 |
| issn_str_mv |
2095-4719 2052-3289 |
| language |
English |
| mega_collection |
Cambridge University Press (CUP) (CrossRef) |
| match_str |
cristoforetti2019timeevolutionofstimulatedramanscatteringandtwoplasmondecayatlaserintensitiesrelevantforshockignitioninahotplasma |
| publishDateSort |
2019 |
| publisher |
Cambridge University Press (CUP) |
| recordtype |
ai |
| record_format |
ai |
| series |
High Power Laser Science and Engineering |
| source_id |
49 |
| title |
Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_unstemmed |
Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_full |
Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_fullStr |
Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_full_unstemmed |
Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_short |
Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_sort |
time evolution of stimulated raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| topic |
Nuclear Energy and Engineering Nuclear and High Energy Physics Atomic and Molecular Physics, and Optics Electronic, Optical and Magnetic Materials |
| url |
http://dx.doi.org/10.1017/hpl.2019.37 |
| publishDate |
2019 |
| physical |
|
| description |
<jats:p>Laser–plasma interaction (LPI) at intensities <jats:inline-formula>
<jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline1" xlink:type="simple" /><jats:tex-math>$10^{15}{-}10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives>
</jats:inline-formula> is dominated by parametric instabilities which can be responsible for a significant amount of non-collisional absorption and generate large fluxes of high-energy nonthermal electrons. Such a regime is of paramount importance for inertial confinement fusion (ICF) and in particular for the shock ignition scheme. In this paper we report on an experiment carried out at the Prague Asterix Laser System (PALS) facility to investigate the extent and time history of stimulated Raman scattering (SRS) and two-plasmon decay (TPD) instabilities, driven by the interaction of an infrared laser pulse at an intensity <jats:inline-formula>
<jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline2" xlink:type="simple" /><jats:tex-math>${\sim}1.2\times 10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives>
</jats:inline-formula> with a <jats:inline-formula>
<jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline3" xlink:type="simple" /><jats:tex-math>${\sim}100~\unicode[STIX]{x03BC}\text{m}$</jats:tex-math></jats:alternatives>
</jats:inline-formula> scalelength plasma produced from irradiation of a flat plastic target. The laser pulse duration (300 ps) and the high value of plasma temperature (<jats:inline-formula>
<jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline4" xlink:type="simple" /><jats:tex-math>${\sim}4~\text{keV}$</jats:tex-math></jats:alternatives>
</jats:inline-formula>) expected from hydrodynamic simulations make these results interesting for a deeper understanding of LPI in shock ignition conditions. Experimental results show that absolute TPD/SRS, driven at a quarter of the critical density, and convective SRS, driven at lower plasma densities, are well separated in time, with absolute instabilities driven at early times of interaction and convective backward SRS emerging at the laser peak and persisting all over the tail of the pulse. Side-scattering SRS, driven at low plasma densities, is also clearly observed. Experimental results are compared to fully kinetic large-scale, two-dimensional simulations. Particle-in-cell results, beyond reproducing the framework delineated by the experimental measurements, reveal the importance of filamentation instability in ruling the onset of SRS and stimulated Brillouin scattering instabilities and confirm the crucial role of collisionless absorption in the LPI energy balance.</jats:p> |
| container_start_page |
0 |
| container_title |
High Power Laser Science and Engineering |
| container_volume |
7 |
| format_de105 |
Article, E-Article |
| format_de14 |
Article, E-Article |
| format_de15 |
Article, E-Article |
| format_de520 |
Article, E-Article |
| format_de540 |
Article, E-Article |
| format_dech1 |
Article, E-Article |
| format_ded117 |
Article, E-Article |
| format_degla1 |
E-Article |
| format_del152 |
Buch |
| format_del189 |
Article, E-Article |
| format_dezi4 |
Article |
| format_dezwi2 |
Article, E-Article |
| format_finc |
Article, E-Article |
| format_nrw |
Article, E-Article |
| _version_ |
1792340615575371792 |
| geogr_code |
not assigned |
| last_indexed |
2024-03-01T16:06:49.617Z |
| geogr_code_person |
not assigned |
| openURL |
url_ver=Z39.88-2004&ctx_ver=Z39.88-2004&ctx_enc=info%3Aofi%2Fenc%3AUTF-8&rfr_id=info%3Asid%2Fvufind.svn.sourceforge.net%3Agenerator&rft.title=Time+evolution+of+stimulated+Raman+scattering+and+two-plasmon+decay+at+laser+intensities+relevant+for+shock+ignition+in+a+hot+plasma&rft.date=2019-01-01&genre=article&issn=2052-3289&volume=7&jtitle=High+Power+Laser+Science+and+Engineering&atitle=Time+evolution+of+stimulated+Raman+scattering+and+two-plasmon+decay+at+laser+intensities+relevant+for+shock+ignition+in+a+hot+plasma&aulast=Gizzi&aufirst=L.+A.&rft_id=info%3Adoi%2F10.1017%2Fhpl.2019.37&rft.language%5B0%5D=eng |
| SOLR | |
| _version_ | 1792340615575371792 |
| author | Cristoforetti, G., Antonelli, L., Mancelli, D., Atzeni, S., Baffigi, F., Barbato, F., Batani, D., Boutoux, G., D’Amato, F., Dostal, J., Dudzak, R., Filippov, E., Gu, Y. J., Juha, L., Klimo, O., Krus, M., Malko, S., Martynenko, A. S., Nicolai, Ph., Ospina, V., Pikuz, S., Renner, O., Santos, J., Tikhonchuk, V. T., Trela, J., Viciani, S., Volpe, L., Weber, S., Gizzi, L. A. |
| author_facet | Cristoforetti, G., Antonelli, L., Mancelli, D., Atzeni, S., Baffigi, F., Barbato, F., Batani, D., Boutoux, G., D’Amato, F., Dostal, J., Dudzak, R., Filippov, E., Gu, Y. J., Juha, L., Klimo, O., Krus, M., Malko, S., Martynenko, A. S., Nicolai, Ph., Ospina, V., Pikuz, S., Renner, O., Santos, J., Tikhonchuk, V. T., Trela, J., Viciani, S., Volpe, L., Weber, S., Gizzi, L. A., Cristoforetti, G., Antonelli, L., Mancelli, D., Atzeni, S., Baffigi, F., Barbato, F., Batani, D., Boutoux, G., D’Amato, F., Dostal, J., Dudzak, R., Filippov, E., Gu, Y. J., Juha, L., Klimo, O., Krus, M., Malko, S., Martynenko, A. S., Nicolai, Ph., Ospina, V., Pikuz, S., Renner, O., Santos, J., Tikhonchuk, V. T., Trela, J., Viciani, S., Volpe, L., Weber, S., Gizzi, L. A. |
| author_sort | cristoforetti, g. |
| container_start_page | 0 |
| container_title | High Power Laser Science and Engineering |
| container_volume | 7 |
| description | <jats:p>Laser–plasma interaction (LPI) at intensities <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline1" xlink:type="simple" /><jats:tex-math>$10^{15}{-}10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives> </jats:inline-formula> is dominated by parametric instabilities which can be responsible for a significant amount of non-collisional absorption and generate large fluxes of high-energy nonthermal electrons. Such a regime is of paramount importance for inertial confinement fusion (ICF) and in particular for the shock ignition scheme. In this paper we report on an experiment carried out at the Prague Asterix Laser System (PALS) facility to investigate the extent and time history of stimulated Raman scattering (SRS) and two-plasmon decay (TPD) instabilities, driven by the interaction of an infrared laser pulse at an intensity <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline2" xlink:type="simple" /><jats:tex-math>${\sim}1.2\times 10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives> </jats:inline-formula> with a <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline3" xlink:type="simple" /><jats:tex-math>${\sim}100~\unicode[STIX]{x03BC}\text{m}$</jats:tex-math></jats:alternatives> </jats:inline-formula> scalelength plasma produced from irradiation of a flat plastic target. The laser pulse duration (300 ps) and the high value of plasma temperature (<jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline4" xlink:type="simple" /><jats:tex-math>${\sim}4~\text{keV}$</jats:tex-math></jats:alternatives> </jats:inline-formula>) expected from hydrodynamic simulations make these results interesting for a deeper understanding of LPI in shock ignition conditions. Experimental results show that absolute TPD/SRS, driven at a quarter of the critical density, and convective SRS, driven at lower plasma densities, are well separated in time, with absolute instabilities driven at early times of interaction and convective backward SRS emerging at the laser peak and persisting all over the tail of the pulse. Side-scattering SRS, driven at low plasma densities, is also clearly observed. Experimental results are compared to fully kinetic large-scale, two-dimensional simulations. Particle-in-cell results, beyond reproducing the framework delineated by the experimental measurements, reveal the importance of filamentation instability in ruling the onset of SRS and stimulated Brillouin scattering instabilities and confirm the crucial role of collisionless absorption in the LPI energy balance.</jats:p> |
| doi_str_mv | 10.1017/hpl.2019.37 |
| facet_avail | Online, Free |
| finc_class_facet | Physik, Technik |
| format | ElectronicArticle |
| format_de105 | Article, E-Article |
| format_de14 | Article, E-Article |
| format_de15 | Article, E-Article |
| format_de520 | Article, E-Article |
| format_de540 | Article, E-Article |
| format_dech1 | Article, E-Article |
| format_ded117 | Article, E-Article |
| format_degla1 | E-Article |
| format_del152 | Buch |
| format_del189 | Article, E-Article |
| format_dezi4 | Article |
| format_dezwi2 | Article, E-Article |
| format_finc | Article, E-Article |
| format_nrw | Article, E-Article |
| geogr_code | not assigned |
| geogr_code_person | not assigned |
| id | ai-49-aHR0cDovL2R4LmRvaS5vcmcvMTAuMTAxNy9ocGwuMjAxOS4zNw |
| imprint | Cambridge University Press (CUP), 2019 |
| imprint_str_mv | Cambridge University Press (CUP), 2019 |
| institution | DE-Gla1, DE-Zi4, DE-15, DE-Pl11, DE-Rs1, DE-105, DE-14, DE-Ch1, DE-L229, DE-D275, DE-Bn3, DE-Brt1, DE-Zwi2, DE-D161 |
| issn | 2095-4719, 2052-3289 |
| issn_str_mv | 2095-4719, 2052-3289 |
| language | English |
| last_indexed | 2024-03-01T16:06:49.617Z |
| match_str | cristoforetti2019timeevolutionofstimulatedramanscatteringandtwoplasmondecayatlaserintensitiesrelevantforshockignitioninahotplasma |
| mega_collection | Cambridge University Press (CUP) (CrossRef) |
| physical | |
| publishDate | 2019 |
| publishDateSort | 2019 |
| publisher | Cambridge University Press (CUP) |
| record_format | ai |
| recordtype | ai |
| series | High Power Laser Science and Engineering |
| source_id | 49 |
| spelling | Cristoforetti, G. Antonelli, L. Mancelli, D. Atzeni, S. Baffigi, F. Barbato, F. Batani, D. Boutoux, G. D’Amato, F. Dostal, J. Dudzak, R. Filippov, E. Gu, Y. J. Juha, L. Klimo, O. Krus, M. Malko, S. Martynenko, A. S. Nicolai, Ph. Ospina, V. Pikuz, S. Renner, O. Santos, J. Tikhonchuk, V. T. Trela, J. Viciani, S. Volpe, L. Weber, S. Gizzi, L. A. 2095-4719 2052-3289 Cambridge University Press (CUP) Nuclear Energy and Engineering Nuclear and High Energy Physics Atomic and Molecular Physics, and Optics Electronic, Optical and Magnetic Materials http://dx.doi.org/10.1017/hpl.2019.37 <jats:p>Laser–plasma interaction (LPI) at intensities <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline1" xlink:type="simple" /><jats:tex-math>$10^{15}{-}10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives> </jats:inline-formula> is dominated by parametric instabilities which can be responsible for a significant amount of non-collisional absorption and generate large fluxes of high-energy nonthermal electrons. Such a regime is of paramount importance for inertial confinement fusion (ICF) and in particular for the shock ignition scheme. In this paper we report on an experiment carried out at the Prague Asterix Laser System (PALS) facility to investigate the extent and time history of stimulated Raman scattering (SRS) and two-plasmon decay (TPD) instabilities, driven by the interaction of an infrared laser pulse at an intensity <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline2" xlink:type="simple" /><jats:tex-math>${\sim}1.2\times 10^{16}~\text{W}\cdot \text{cm}^{-2}$</jats:tex-math></jats:alternatives> </jats:inline-formula> with a <jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline3" xlink:type="simple" /><jats:tex-math>${\sim}100~\unicode[STIX]{x03BC}\text{m}$</jats:tex-math></jats:alternatives> </jats:inline-formula> scalelength plasma produced from irradiation of a flat plastic target. The laser pulse duration (300 ps) and the high value of plasma temperature (<jats:inline-formula> <jats:alternatives><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="gif" xlink:href="S2095471919000379_inline4" xlink:type="simple" /><jats:tex-math>${\sim}4~\text{keV}$</jats:tex-math></jats:alternatives> </jats:inline-formula>) expected from hydrodynamic simulations make these results interesting for a deeper understanding of LPI in shock ignition conditions. Experimental results show that absolute TPD/SRS, driven at a quarter of the critical density, and convective SRS, driven at lower plasma densities, are well separated in time, with absolute instabilities driven at early times of interaction and convective backward SRS emerging at the laser peak and persisting all over the tail of the pulse. Side-scattering SRS, driven at low plasma densities, is also clearly observed. Experimental results are compared to fully kinetic large-scale, two-dimensional simulations. Particle-in-cell results, beyond reproducing the framework delineated by the experimental measurements, reveal the importance of filamentation instability in ruling the onset of SRS and stimulated Brillouin scattering instabilities and confirm the crucial role of collisionless absorption in the LPI energy balance.</jats:p> Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma High Power Laser Science and Engineering |
| spellingShingle | Cristoforetti, G., Antonelli, L., Mancelli, D., Atzeni, S., Baffigi, F., Barbato, F., Batani, D., Boutoux, G., D’Amato, F., Dostal, J., Dudzak, R., Filippov, E., Gu, Y. J., Juha, L., Klimo, O., Krus, M., Malko, S., Martynenko, A. S., Nicolai, Ph., Ospina, V., Pikuz, S., Renner, O., Santos, J., Tikhonchuk, V. T., Trela, J., Viciani, S., Volpe, L., Weber, S., Gizzi, L. A., High Power Laser Science and Engineering, Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma, Nuclear Energy and Engineering, Nuclear and High Energy Physics, Atomic and Molecular Physics, and Optics, Electronic, Optical and Magnetic Materials |
| title | Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_full | Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_fullStr | Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_full_unstemmed | Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_short | Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_sort | time evolution of stimulated raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| title_unstemmed | Time evolution of stimulated Raman scattering and two-plasmon decay at laser intensities relevant for shock ignition in a hot plasma |
| topic | Nuclear Energy and Engineering, Nuclear and High Energy Physics, Atomic and Molecular Physics, and Optics, Electronic, Optical and Magnetic Materials |
| url | http://dx.doi.org/10.1017/hpl.2019.37 |