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Stopping power of a heterogeneous warm dense matter. / Casas, D.; Andreev, A. A.; Schnürer, M.; Barriga-Carrasco, M. D.; Morales, R.; González-Gallego, L.

в: Laser and Particle Beams, Том 34, № 2, 01.06.2016, стр. 306-314.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Casas, D, Andreev, AA, Schnürer, M, Barriga-Carrasco, MD, Morales, R & González-Gallego, L 2016, 'Stopping power of a heterogeneous warm dense matter', Laser and Particle Beams, Том. 34, № 2, стр. 306-314. https://doi.org/10.1017/S0263034616000161

APA

Casas, D., Andreev, A. A., Schnürer, M., Barriga-Carrasco, M. D., Morales, R., & González-Gallego, L. (2016). Stopping power of a heterogeneous warm dense matter. Laser and Particle Beams, 34(2), 306-314. https://doi.org/10.1017/S0263034616000161

Vancouver

Casas D, Andreev AA, Schnürer M, Barriga-Carrasco MD, Morales R, González-Gallego L. Stopping power of a heterogeneous warm dense matter. Laser and Particle Beams. 2016 Июнь 1;34(2):306-314. https://doi.org/10.1017/S0263034616000161

Author

Casas, D. ; Andreev, A. A. ; Schnürer, M. ; Barriga-Carrasco, M. D. ; Morales, R. ; González-Gallego, L. / Stopping power of a heterogeneous warm dense matter. в: Laser and Particle Beams. 2016 ; Том 34, № 2. стр. 306-314.

BibTeX

@article{59d9296122584d8e9ee71ee5c0a3ac94,
title = "Stopping power of a heterogeneous warm dense matter",
abstract = "The stopping power of warm dense matter (WDM) is estimated by means of the individual contributions of free electrons and bound electrons existing in this special kind of matter, located between classical and degenerate plasmas. For free electrons, the dielectric formalism, well described in our studies, is used to estimate the free electron stopping power. For bound electrons, the mean excitation energy of ions is used. Excitation energies are obtained through atomic calculations of the whole atom or, shell by shell in order to estimate their stopping power. Influence of temperature and density is analyzed in case of an impinging projectile. This influence becomes important for low projectile velocities and is negligible for high ones. Using free and bound electron analysis, the stopping power of an extended WDM is inferred from a dynamical calculation of energy transferred from the projectile to the plasma, where the stopping range is calculated. Finally, this theoretical framework is used to study a typical plasma density profile of a WDM heated by lasers.",
keywords = "Partially ionized plasmas, Stopping power, Warm dense matter",
author = "D. Casas and Andreev, {A. A.} and M. Schn{\"u}rer and Barriga-Carrasco, {M. D.} and R. Morales and L. Gonz{\'a}lez-Gallego",
year = "2016",
month = jun,
day = "1",
doi = "10.1017/S0263034616000161",
language = "English",
volume = "34",
pages = "306--314",
journal = "Laser and Particle Beams",
issn = "0263-0346",
publisher = "Cambridge University Press",
number = "2",

}

RIS

TY - JOUR

T1 - Stopping power of a heterogeneous warm dense matter

AU - Casas, D.

AU - Andreev, A. A.

AU - Schnürer, M.

AU - Barriga-Carrasco, M. D.

AU - Morales, R.

AU - González-Gallego, L.

PY - 2016/6/1

Y1 - 2016/6/1

N2 - The stopping power of warm dense matter (WDM) is estimated by means of the individual contributions of free electrons and bound electrons existing in this special kind of matter, located between classical and degenerate plasmas. For free electrons, the dielectric formalism, well described in our studies, is used to estimate the free electron stopping power. For bound electrons, the mean excitation energy of ions is used. Excitation energies are obtained through atomic calculations of the whole atom or, shell by shell in order to estimate their stopping power. Influence of temperature and density is analyzed in case of an impinging projectile. This influence becomes important for low projectile velocities and is negligible for high ones. Using free and bound electron analysis, the stopping power of an extended WDM is inferred from a dynamical calculation of energy transferred from the projectile to the plasma, where the stopping range is calculated. Finally, this theoretical framework is used to study a typical plasma density profile of a WDM heated by lasers.

AB - The stopping power of warm dense matter (WDM) is estimated by means of the individual contributions of free electrons and bound electrons existing in this special kind of matter, located between classical and degenerate plasmas. For free electrons, the dielectric formalism, well described in our studies, is used to estimate the free electron stopping power. For bound electrons, the mean excitation energy of ions is used. Excitation energies are obtained through atomic calculations of the whole atom or, shell by shell in order to estimate their stopping power. Influence of temperature and density is analyzed in case of an impinging projectile. This influence becomes important for low projectile velocities and is negligible for high ones. Using free and bound electron analysis, the stopping power of an extended WDM is inferred from a dynamical calculation of energy transferred from the projectile to the plasma, where the stopping range is calculated. Finally, this theoretical framework is used to study a typical plasma density profile of a WDM heated by lasers.

KW - Partially ionized plasmas

KW - Stopping power

KW - Warm dense matter

UR - http://www.scopus.com/inward/record.url?scp=84964054014&partnerID=8YFLogxK

U2 - 10.1017/S0263034616000161

DO - 10.1017/S0263034616000161

M3 - Article

AN - SCOPUS:84964054014

VL - 34

SP - 306

EP - 314

JO - Laser and Particle Beams

JF - Laser and Particle Beams

SN - 0263-0346

IS - 2

ER -

ID: 9329202