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Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury

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Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury. / Priebe, G.; Laundy, D.; MacDonald, M.A.; Diakun, G.P.; Jamison, S.P.; Jones, L.B.; Holder, D.J.; Smith, S.L.; Phillips, P.J.; Fell, B.D.; Sheehy, B.; Naumova, N.; Sokolov, I.V.; Ter-Avetisyan, S.; Spohr, K.; Krafft, G.A.; Rosenzweig, J.B.; Schramm, U.; Grüner, F.; Hirst, G.J.; Collier, J.; Chattopadhyay, S.; Seddon, E.A.

In: Laser and Particle Beams, Vol. 26, No. 4, 12.2008, p. 649-660.

Research output: Contribution to journalJournal articlepeer-review

Harvard

Priebe, G, Laundy, D, MacDonald, MA, Diakun, GP, Jamison, SP, Jones, LB, Holder, DJ, Smith, SL, Phillips, PJ, Fell, BD, Sheehy, B, Naumova, N, Sokolov, IV, Ter-Avetisyan, S, Spohr, K, Krafft, GA, Rosenzweig, JB, Schramm, U, Grüner, F, Hirst, GJ, Collier, J, Chattopadhyay, S & Seddon, EA 2008, 'Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury', Laser and Particle Beams, vol. 26, no. 4, pp. 649-660. https://doi.org/10.1017/S0263034608000700

APA

Priebe, G., Laundy, D., MacDonald, M. A., Diakun, G. P., Jamison, S. P., Jones, L. B., Holder, D. J., Smith, S. L., Phillips, P. J., Fell, B. D., Sheehy, B., Naumova, N., Sokolov, I. V., Ter-Avetisyan, S., Spohr, K., Krafft, G. A., Rosenzweig, J. B., Schramm, U., Grüner, F., ... Seddon, E. A. (2008). Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury. Laser and Particle Beams, 26(4), 649-660. https://doi.org/10.1017/S0263034608000700

Vancouver

Priebe G, Laundy D, MacDonald MA, Diakun GP, Jamison SP, Jones LB et al. Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury. Laser and Particle Beams. 2008 Dec;26(4):649-660. https://doi.org/10.1017/S0263034608000700

Author

Priebe, G. ; Laundy, D. ; MacDonald, M.A. ; Diakun, G.P. ; Jamison, S.P. ; Jones, L.B. ; Holder, D.J. ; Smith, S.L. ; Phillips, P.J. ; Fell, B.D. ; Sheehy, B. ; Naumova, N. ; Sokolov, I.V. ; Ter-Avetisyan, S. ; Spohr, K. ; Krafft, G.A. ; Rosenzweig, J.B. ; Schramm, U. ; Grüner, F. ; Hirst, G.J. ; Collier, J. ; Chattopadhyay, S. ; Seddon, E.A. / Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury. In: Laser and Particle Beams. 2008 ; Vol. 26, No. 4. pp. 649-660.

Bibtex

@article{077f0d3941e34dd99452e703a6721ea7,
title = "Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury",
abstract = "Inverse Compton scattering is a promising method to implement a high brightness, ultra-short, energy tunable X-ray source at accelerator facilities. We have developed an inverse Compton backscattering X-ray source driven by the multi-10 TW laser installed at Daresbury. Hard X-rays, with spectral peaks ranging from 15 to 30 keV, depending on the scattering geometry, will be generated through the interaction of laser pulses with electron bunches delivered by the energyrecovery linac machine, initially known as energy recovery linac prototype and subsequently renamed accelerators and lasers in combined experiments. X-ray pulses containing 9 107 photons per pulse will be created from head-on collisions, with a pulse duration comparable to the incoming electron bunch length. For transverse collisions 8 106 photons per pulse will be generated, where the laser pulse transit time defines the X-ray pulse duration. The peakspectral brightness is predicted to be 1021 photons/(s mm2 mrad2 0.1% Dl/l).",
author = "G. Priebe and D. Laundy and M.A. MacDonald and G.P. Diakun and S.P. Jamison and L.B. Jones and D.J. Holder and S.L. Smith and P.J. Phillips and B.D. Fell and B. Sheehy and N. Naumova and I.V. Sokolov and S. Ter-Avetisyan and K. Spohr and G.A. Krafft and J.B. Rosenzweig and U. Schramm and F. Gr{\"u}ner and G.J. Hirst and J. Collier and S. Chattopadhyay and E.A. Seddon",
year = "2008",
month = dec,
doi = "10.1017/S0263034608000700",
language = "English",
volume = "26",
pages = "649--660",
journal = "Laser and Particle Beams",
issn = "0263-0346",
publisher = "CAMBRIDGE UNIV PRESS",
number = "4",

}

RIS

TY - JOUR

T1 - Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury

AU - Priebe, G.

AU - Laundy, D.

AU - MacDonald, M.A.

AU - Diakun, G.P.

AU - Jamison, S.P.

AU - Jones, L.B.

AU - Holder, D.J.

AU - Smith, S.L.

AU - Phillips, P.J.

AU - Fell, B.D.

AU - Sheehy, B.

AU - Naumova, N.

AU - Sokolov, I.V.

AU - Ter-Avetisyan, S.

AU - Spohr, K.

AU - Krafft, G.A.

AU - Rosenzweig, J.B.

AU - Schramm, U.

AU - Grüner, F.

AU - Hirst, G.J.

AU - Collier, J.

AU - Chattopadhyay, S.

AU - Seddon, E.A.

PY - 2008/12

Y1 - 2008/12

N2 - Inverse Compton scattering is a promising method to implement a high brightness, ultra-short, energy tunable X-ray source at accelerator facilities. We have developed an inverse Compton backscattering X-ray source driven by the multi-10 TW laser installed at Daresbury. Hard X-rays, with spectral peaks ranging from 15 to 30 keV, depending on the scattering geometry, will be generated through the interaction of laser pulses with electron bunches delivered by the energyrecovery linac machine, initially known as energy recovery linac prototype and subsequently renamed accelerators and lasers in combined experiments. X-ray pulses containing 9 107 photons per pulse will be created from head-on collisions, with a pulse duration comparable to the incoming electron bunch length. For transverse collisions 8 106 photons per pulse will be generated, where the laser pulse transit time defines the X-ray pulse duration. The peakspectral brightness is predicted to be 1021 photons/(s mm2 mrad2 0.1% Dl/l).

AB - Inverse Compton scattering is a promising method to implement a high brightness, ultra-short, energy tunable X-ray source at accelerator facilities. We have developed an inverse Compton backscattering X-ray source driven by the multi-10 TW laser installed at Daresbury. Hard X-rays, with spectral peaks ranging from 15 to 30 keV, depending on the scattering geometry, will be generated through the interaction of laser pulses with electron bunches delivered by the energyrecovery linac machine, initially known as energy recovery linac prototype and subsequently renamed accelerators and lasers in combined experiments. X-ray pulses containing 9 107 photons per pulse will be created from head-on collisions, with a pulse duration comparable to the incoming electron bunch length. For transverse collisions 8 106 photons per pulse will be generated, where the laser pulse transit time defines the X-ray pulse duration. The peakspectral brightness is predicted to be 1021 photons/(s mm2 mrad2 0.1% Dl/l).

U2 - 10.1017/S0263034608000700

DO - 10.1017/S0263034608000700

M3 - Journal article

VL - 26

SP - 649

EP - 660

JO - Laser and Particle Beams

JF - Laser and Particle Beams

SN - 0263-0346

IS - 4

ER -