Home > Research > Publications & Outputs > Wakefield-induced ionization injection in beam-...

Links

Text available via DOI:

View graph of relations

Wakefield-induced ionization injection in beam-driven plasma accelerators

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Published

Standard

Wakefield-induced ionization injection in beam-driven plasma accelerators. / Martinez De La Ossa, A.; Mehrling, T. J.; Schaper, L. et al.
In: Physics of Plasmas, Vol. 22, No. 9, 093107, 09.2015.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Martinez De La Ossa, A, Mehrling, TJ, Schaper, L, Streeter, MJV & Osterhoff, J 2015, 'Wakefield-induced ionization injection in beam-driven plasma accelerators', Physics of Plasmas, vol. 22, no. 9, 093107. https://doi.org/10.1063/1.4929921

APA

Martinez De La Ossa, A., Mehrling, T. J., Schaper, L., Streeter, M. J. V., & Osterhoff, J. (2015). Wakefield-induced ionization injection in beam-driven plasma accelerators. Physics of Plasmas, 22(9), Article 093107. https://doi.org/10.1063/1.4929921

Vancouver

Martinez De La Ossa A, Mehrling TJ, Schaper L, Streeter MJV, Osterhoff J. Wakefield-induced ionization injection in beam-driven plasma accelerators. Physics of Plasmas. 2015 Sept;22(9):093107. Epub 2015 Sept 4. doi: 10.1063/1.4929921

Author

Martinez De La Ossa, A. ; Mehrling, T. J. ; Schaper, L. et al. / Wakefield-induced ionization injection in beam-driven plasma accelerators. In: Physics of Plasmas. 2015 ; Vol. 22, No. 9.

Bibtex

@article{6386dfc7828b401a8e1112bbe3a39dea,
title = "Wakefield-induced ionization injection in beam-driven plasma accelerators",
abstract = "We present a detailed analysis of the features and capabilities of Wakefield-Induced Ionization (WII) injection in the blowout regime of beam driven plasma accelerators. This mechanism exploits the electric wakefields to ionize electrons from a dopant gas and trap them in a well-defined region of the accelerating and focusing wake phase, leading to the formation of high-quality witness-bunches [Martinez de la Ossa et al., Phys. Rev. Lett. 111, 245003 (2013)]. The electron-beam drivers must feature high-peak currents (\r\nI\r\nb\r\n0\r\n≳\r\n8.5\r\n \r\nkA\r\n) and a duration comparable to the plasma wavelength to excite plasma waves in the blowout regime and enable WII injection. In this regime, the disparity of the magnitude of the electric field in the driver region and the electric field in the rear of the ion cavity allows for the selective ionization and subsequent trapping from a narrow phase interval. The witness bunches generated in this manner feature a short duration and small values of the normalized transverse emittance (\r\nk\r\np\r\nσ\r\nz\r\n∼\r\nk\r\np\r\nϵ\r\nn\r\n∼\r\n0.1\r\n). In addition, we show that the amount of injected charge can be adjusted by tuning the concentration of the dopant gas species, which allows for controlled beam loading and leads to a reduction of the total energy spread of the witness beams.\r\nElectron bunches, produced in this way, fulfil the requirements to drive blowout regime plasma wakes at a higher density and to trigger WII injection in a second stage. This suggests a promising new concept of self-similar staging of WII injection in steps with increasing plasma density, giving rise to the potential of producing electron beams with unprecedented energy and brilliance from plasma-wakefield accelerators.",
author = "{Martinez De La Ossa}, A. and Mehrling, {T. J.} and L. Schaper and Streeter, {M. J. V.} and J. Osterhoff",
year = "2015",
month = sep,
doi = "10.1063/1.4929921",
language = "English",
volume = "22",
journal = "Physics of Plasmas",
issn = "1070-664X",
publisher = "American Institute of Physics Inc.",
number = "9",

}

RIS

TY - JOUR

T1 - Wakefield-induced ionization injection in beam-driven plasma accelerators

AU - Martinez De La Ossa, A.

AU - Mehrling, T. J.

AU - Schaper, L.

AU - Streeter, M. J. V.

AU - Osterhoff, J.

PY - 2015/9

Y1 - 2015/9

N2 - We present a detailed analysis of the features and capabilities of Wakefield-Induced Ionization (WII) injection in the blowout regime of beam driven plasma accelerators. This mechanism exploits the electric wakefields to ionize electrons from a dopant gas and trap them in a well-defined region of the accelerating and focusing wake phase, leading to the formation of high-quality witness-bunches [Martinez de la Ossa et al., Phys. Rev. Lett. 111, 245003 (2013)]. The electron-beam drivers must feature high-peak currents (\r\nI\r\nb\r\n0\r\n≳\r\n8.5\r\n \r\nkA\r\n) and a duration comparable to the plasma wavelength to excite plasma waves in the blowout regime and enable WII injection. In this regime, the disparity of the magnitude of the electric field in the driver region and the electric field in the rear of the ion cavity allows for the selective ionization and subsequent trapping from a narrow phase interval. The witness bunches generated in this manner feature a short duration and small values of the normalized transverse emittance (\r\nk\r\np\r\nσ\r\nz\r\n∼\r\nk\r\np\r\nϵ\r\nn\r\n∼\r\n0.1\r\n). In addition, we show that the amount of injected charge can be adjusted by tuning the concentration of the dopant gas species, which allows for controlled beam loading and leads to a reduction of the total energy spread of the witness beams.\r\nElectron bunches, produced in this way, fulfil the requirements to drive blowout regime plasma wakes at a higher density and to trigger WII injection in a second stage. This suggests a promising new concept of self-similar staging of WII injection in steps with increasing plasma density, giving rise to the potential of producing electron beams with unprecedented energy and brilliance from plasma-wakefield accelerators.

AB - We present a detailed analysis of the features and capabilities of Wakefield-Induced Ionization (WII) injection in the blowout regime of beam driven plasma accelerators. This mechanism exploits the electric wakefields to ionize electrons from a dopant gas and trap them in a well-defined region of the accelerating and focusing wake phase, leading to the formation of high-quality witness-bunches [Martinez de la Ossa et al., Phys. Rev. Lett. 111, 245003 (2013)]. The electron-beam drivers must feature high-peak currents (\r\nI\r\nb\r\n0\r\n≳\r\n8.5\r\n \r\nkA\r\n) and a duration comparable to the plasma wavelength to excite plasma waves in the blowout regime and enable WII injection. In this regime, the disparity of the magnitude of the electric field in the driver region and the electric field in the rear of the ion cavity allows for the selective ionization and subsequent trapping from a narrow phase interval. The witness bunches generated in this manner feature a short duration and small values of the normalized transverse emittance (\r\nk\r\np\r\nσ\r\nz\r\n∼\r\nk\r\np\r\nϵ\r\nn\r\n∼\r\n0.1\r\n). In addition, we show that the amount of injected charge can be adjusted by tuning the concentration of the dopant gas species, which allows for controlled beam loading and leads to a reduction of the total energy spread of the witness beams.\r\nElectron bunches, produced in this way, fulfil the requirements to drive blowout regime plasma wakes at a higher density and to trigger WII injection in a second stage. This suggests a promising new concept of self-similar staging of WII injection in steps with increasing plasma density, giving rise to the potential of producing electron beams with unprecedented energy and brilliance from plasma-wakefield accelerators.

U2 - 10.1063/1.4929921

DO - 10.1063/1.4929921

M3 - Journal article

VL - 22

JO - Physics of Plasmas

JF - Physics of Plasmas

SN - 1070-664X

IS - 9

M1 - 093107

ER -