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Energetic proton acceleration and bunch generation by ultraintense laser pulses on the surface of thin plasma targets. / Okada, T.; Andreev, A. A.; Mikado, Y.; Okubo, K.

In: Physical Review E - Statistical, Nonlinear, and Soft Matter Physics, Vol. 74, No. 2, 026401, 2006.

Research output: Contribution to journalArticlepeer-review

Harvard

Okada, T, Andreev, AA, Mikado, Y & Okubo, K 2006, 'Energetic proton acceleration and bunch generation by ultraintense laser pulses on the surface of thin plasma targets', Physical Review E - Statistical, Nonlinear, and Soft Matter Physics, vol. 74, no. 2, 026401. https://doi.org/10.1103/PhysRevE.74.026401

APA

Okada, T., Andreev, A. A., Mikado, Y., & Okubo, K. (2006). Energetic proton acceleration and bunch generation by ultraintense laser pulses on the surface of thin plasma targets. Physical Review E - Statistical, Nonlinear, and Soft Matter Physics, 74(2), [026401]. https://doi.org/10.1103/PhysRevE.74.026401

Vancouver

Okada T, Andreev AA, Mikado Y, Okubo K. Energetic proton acceleration and bunch generation by ultraintense laser pulses on the surface of thin plasma targets. Physical Review E - Statistical, Nonlinear, and Soft Matter Physics. 2006;74(2). 026401. https://doi.org/10.1103/PhysRevE.74.026401

Author

Okada, T. ; Andreev, A. A. ; Mikado, Y. ; Okubo, K. / Energetic proton acceleration and bunch generation by ultraintense laser pulses on the surface of thin plasma targets. In: Physical Review E - Statistical, Nonlinear, and Soft Matter Physics. 2006 ; Vol. 74, No. 2.

BibTeX

@article{f88f6761a73c45edae28db63d4b62b3b,
title = "Energetic proton acceleration and bunch generation by ultraintense laser pulses on the surface of thin plasma targets",
abstract = "Energetic proton acceleration from concave targets, the front of which were irradiated with 40 fs laser pulses with an intensity of 1020 W cm2, has been studied as a function of the depth of the concave shape. Three kinds of targets, a triangular concave target, a circular concave target and a parabolic concave target are considered. When the depth of the concave shape was varied, the peak proton energy showed a maximum. The underlying mechanism for the existence of a maximum peak proton energy is presented by tracing the proton trajectory. It is concluded that a parabolic concave target is the best, among the targets considered, for accelerating a proton beam, since a proton beam from a parabolic concave target goes through the strongest electric field.",
author = "T. Okada and Andreev, {A. A.} and Y. Mikado and K. Okubo",
year = "2006",
doi = "10.1103/PhysRevE.74.026401",
language = "English",
volume = "74",
journal = "Physical Review E",
issn = "1539-3755",
publisher = "American Physical Society",
number = "2",

}

RIS

TY - JOUR

T1 - Energetic proton acceleration and bunch generation by ultraintense laser pulses on the surface of thin plasma targets

AU - Okada, T.

AU - Andreev, A. A.

AU - Mikado, Y.

AU - Okubo, K.

PY - 2006

Y1 - 2006

N2 - Energetic proton acceleration from concave targets, the front of which were irradiated with 40 fs laser pulses with an intensity of 1020 W cm2, has been studied as a function of the depth of the concave shape. Three kinds of targets, a triangular concave target, a circular concave target and a parabolic concave target are considered. When the depth of the concave shape was varied, the peak proton energy showed a maximum. The underlying mechanism for the existence of a maximum peak proton energy is presented by tracing the proton trajectory. It is concluded that a parabolic concave target is the best, among the targets considered, for accelerating a proton beam, since a proton beam from a parabolic concave target goes through the strongest electric field.

AB - Energetic proton acceleration from concave targets, the front of which were irradiated with 40 fs laser pulses with an intensity of 1020 W cm2, has been studied as a function of the depth of the concave shape. Three kinds of targets, a triangular concave target, a circular concave target and a parabolic concave target are considered. When the depth of the concave shape was varied, the peak proton energy showed a maximum. The underlying mechanism for the existence of a maximum peak proton energy is presented by tracing the proton trajectory. It is concluded that a parabolic concave target is the best, among the targets considered, for accelerating a proton beam, since a proton beam from a parabolic concave target goes through the strongest electric field.

UR - http://www.scopus.com/inward/record.url?scp=33746924504&partnerID=8YFLogxK

U2 - 10.1103/PhysRevE.74.026401

DO - 10.1103/PhysRevE.74.026401

M3 - Article

AN - SCOPUS:33746924504

VL - 74

JO - Physical Review E

JF - Physical Review E

SN - 1539-3755

IS - 2

M1 - 026401

ER -

ID: 85668623