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Effect of defocusing on picosecond laser-coupling into gold cones

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Effect of defocusing on picosecond laser-coupling into gold cones. / Bush, I. A.; Thomas, Alexander George Roy; Gartside, L. et al.
In: Physics of Plasmas, Vol. 21, No. 1, 012702, 01.2014.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Bush, IA, Thomas, AGR, Gartside, L, Sarfraz, S, Wagenaars, E, Green, JS, Notley, M, Lowe, H, Spindloe, C, Winstone, T, Robinson, APL, Clarke, R, Ma, T, Yabuuchi, T, Wei, M, Beg, FN, Stephens, RB, MacPhee, A, Mackinnon, AJ, Key, MH, Nazarov, W, Sherlock, M & Pasley, J 2014, 'Effect of defocusing on picosecond laser-coupling into gold cones', Physics of Plasmas, vol. 21, no. 1, 012702. https://doi.org/10.1063.1.4861375

APA

Bush, I. A., Thomas, A. G. R., Gartside, L., Sarfraz, S., Wagenaars, E., Green, J. S., Notley, M., Lowe, H., Spindloe, C., Winstone, T., Robinson, A. P. L., Clarke, R., Ma, T., Yabuuchi, T., Wei, M., Beg, F. N., Stephens, R. B., MacPhee, A., Mackinnon, A. J., ... Pasley, J. (2014). Effect of defocusing on picosecond laser-coupling into gold cones. Physics of Plasmas, 21(1), Article 012702. https://doi.org/10.1063.1.4861375

Vancouver

Bush IA, Thomas AGR, Gartside L, Sarfraz S, Wagenaars E, Green JS et al. Effect of defocusing on picosecond laser-coupling into gold cones. Physics of Plasmas. 2014 Jan;21(1):012702. doi: 10.1063.1.4861375

Author

Bush, I. A. ; Thomas, Alexander George Roy ; Gartside, L. et al. / Effect of defocusing on picosecond laser-coupling into gold cones. In: Physics of Plasmas. 2014 ; Vol. 21, No. 1.

Bibtex

@article{3aefb7e3c1db4c0ea5891e74ef376e33,
title = "Effect of defocusing on picosecond laser-coupling into gold cones",
abstract = "Here, we show that defocusing of the laser in the interaction of a picosecond duration, 1.053 μm wavelength, high energy pulse with a cone-wire target does not significantly affect the laser energy coupling efficiency, but does result in a drop in the fast electron effective temperature. This may be beneficial for fast ignition, since not only were more electrons with lower energies seen in the experiment but also the lower prepulse intensity will reduce the amount of preplasma present on arrival of the main pulse, reducing the distance the hot electrons have to travel. We used the Vulcan Petawatt Laser at the Rutherford Appleton Laboratory and gold cone targets with approximately 1 mm long, 40 μm diameter copper wires attached to their tip. Diagnostics included a quartz crystal imager, a pair of highly oriented pyrolytic graphite crystal spectrometers and a calibrated CCD operating in the single photon counting regime, all of which looked at the copper Kα emission from the wire. A short pulse optical probe, delayed 400 ps relative to the main pulse was employed to diagnose the extent of plasma expansion around the wire. A ray-tracing code modeled the change in intensity on the interior surface of the cone with laser defocusing. Using a model for the wire copper Kα emission coupled to a hybrid Vlasov-Fokker-Planck code, we ran a series of simulations, holding the total energy in electrons constant whilst varying the electron temperature, which support the experimental conclusions.",
author = "Bush, {I. A.} and Thomas, {Alexander George Roy} and L. Gartside and S. Sarfraz and E. Wagenaars and Green, {J. S.} and M. Notley and H. Lowe and C. Spindloe and T. Winstone and Robinson, {A. P. L.} and R. Clarke and T. Ma and T. Yabuuchi and M. Wei and Beg, {F. N.} and Stephens, {R. B.} and A. MacPhee and Mackinnon, {A. J.} and Key, {M. H.} and W. Nazarov and M. Sherlock and J. Pasley",
year = "2014",
month = jan,
doi = "10.1063.1.4861375",
language = "English",
volume = "21",
journal = "Physics of Plasmas",
issn = "1070-664X",
publisher = "American Institute of Physics Inc.",
number = "1",

}

RIS

TY - JOUR

T1 - Effect of defocusing on picosecond laser-coupling into gold cones

AU - Bush, I. A.

AU - Thomas, Alexander George Roy

AU - Gartside, L.

AU - Sarfraz, S.

AU - Wagenaars, E.

AU - Green, J. S.

AU - Notley, M.

AU - Lowe, H.

AU - Spindloe, C.

AU - Winstone, T.

AU - Robinson, A. P. L.

AU - Clarke, R.

AU - Ma, T.

AU - Yabuuchi, T.

AU - Wei, M.

AU - Beg, F. N.

AU - Stephens, R. B.

AU - MacPhee, A.

AU - Mackinnon, A. J.

AU - Key, M. H.

AU - Nazarov, W.

AU - Sherlock, M.

AU - Pasley, J.

PY - 2014/1

Y1 - 2014/1

N2 - Here, we show that defocusing of the laser in the interaction of a picosecond duration, 1.053 μm wavelength, high energy pulse with a cone-wire target does not significantly affect the laser energy coupling efficiency, but does result in a drop in the fast electron effective temperature. This may be beneficial for fast ignition, since not only were more electrons with lower energies seen in the experiment but also the lower prepulse intensity will reduce the amount of preplasma present on arrival of the main pulse, reducing the distance the hot electrons have to travel. We used the Vulcan Petawatt Laser at the Rutherford Appleton Laboratory and gold cone targets with approximately 1 mm long, 40 μm diameter copper wires attached to their tip. Diagnostics included a quartz crystal imager, a pair of highly oriented pyrolytic graphite crystal spectrometers and a calibrated CCD operating in the single photon counting regime, all of which looked at the copper Kα emission from the wire. A short pulse optical probe, delayed 400 ps relative to the main pulse was employed to diagnose the extent of plasma expansion around the wire. A ray-tracing code modeled the change in intensity on the interior surface of the cone with laser defocusing. Using a model for the wire copper Kα emission coupled to a hybrid Vlasov-Fokker-Planck code, we ran a series of simulations, holding the total energy in electrons constant whilst varying the electron temperature, which support the experimental conclusions.

AB - Here, we show that defocusing of the laser in the interaction of a picosecond duration, 1.053 μm wavelength, high energy pulse with a cone-wire target does not significantly affect the laser energy coupling efficiency, but does result in a drop in the fast electron effective temperature. This may be beneficial for fast ignition, since not only were more electrons with lower energies seen in the experiment but also the lower prepulse intensity will reduce the amount of preplasma present on arrival of the main pulse, reducing the distance the hot electrons have to travel. We used the Vulcan Petawatt Laser at the Rutherford Appleton Laboratory and gold cone targets with approximately 1 mm long, 40 μm diameter copper wires attached to their tip. Diagnostics included a quartz crystal imager, a pair of highly oriented pyrolytic graphite crystal spectrometers and a calibrated CCD operating in the single photon counting regime, all of which looked at the copper Kα emission from the wire. A short pulse optical probe, delayed 400 ps relative to the main pulse was employed to diagnose the extent of plasma expansion around the wire. A ray-tracing code modeled the change in intensity on the interior surface of the cone with laser defocusing. Using a model for the wire copper Kα emission coupled to a hybrid Vlasov-Fokker-Planck code, we ran a series of simulations, holding the total energy in electrons constant whilst varying the electron temperature, which support the experimental conclusions.

U2 - 10.1063.1.4861375

DO - 10.1063.1.4861375

M3 - Journal article

VL - 21

JO - Physics of Plasmas

JF - Physics of Plasmas

SN - 1070-664X

IS - 1

M1 - 012702

ER -