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| 001 | 205163 | ||
| 005 | 20250730145034.0 | ||
| 024 | 7 | _ | |2 doi |a 10.1088/0741-3335/56/8/084013 |
| 024 | 7 | _ | |2 ISSN |a 0032-1028 |
| 024 | 7 | _ | |2 ISSN |a 0368-3281 |
| 024 | 7 | _ | |2 ISSN |a 0741-3335 |
| 024 | 7 | _ | |2 ISSN |a 1361-6587 |
| 024 | 7 | _ | |2 ISSN |a 1879-2979 |
| 024 | 7 | _ | |2 arXiv |a arXiv:1401.4823 |
| 024 | 7 | _ | |2 WOS |a WOS:000340055300014 |
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| 037 | _ | _ | |a PUBDB-2014-04590 |
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| 088 | 1 | _ | |a arXiv:1401.4823 |
| 088 | _ | _ | |a arXiv:1401.4823 |2 arXiv |
| 100 | 1 | _ | |0 P:(DE-H253)PIP1017739 |a Assmann, R. |b 0 |e Corresponding Author |
| 245 | _ | _ | |a Proton-driven plasma wakefield acceleration: a path to the future of high-energy particle physics |
| 260 | _ | _ | |a Bristol |b IOP Publ. |c 2014 |
| 336 | 7 | _ | |2 DRIVER |a article |
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| 336 | 7 | _ | |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |a Journal Article |b journal |m journal |s 1481031849_12009 |
| 336 | 7 | _ | |2 BibTeX |a ARTICLE |
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| 500 | _ | _ | |a OA |
| 520 | _ | _ | |a New acceleration technology is mandatory for the future elucidation of fundamental particles and theirinteractions. A promising approach is to exploit the properties of plasmas. Past research has focused oncreating large-amplitude plasma waves by injecting an intense laser pulse or an electron bunch into theplasma. However, the maximum energy gain of electrons accelerated in a single plasma stage is limitedby the energy of the driver. Proton bunches are the most promising drivers of wakefields to accelerateelectrons to the TeV energy scale in a single stage. An experimental program at CERN—the AWAKEexperiment—has been launched to study in detail the important physical processes and to demonstrate the power of proton-driven plasma wakefield acceleration. Here we review the physical principles andsome experimental considerations for a future proton-driven plasma wakefield accelerator. |
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| 700 | 1 | _ | |a Bingham, R. |b 1 |
| 700 | 1 | _ | |a Bohl, T. |b 2 |
| 700 | 1 | _ | |a Bracco, C. |b 3 |
| 700 | 1 | _ | |a Buttenschön, B. |b 4 |
| 700 | 1 | _ | |a Butterworth, A. |b 5 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1003358 |a Caldwell, A. |b 6 |
| 700 | 1 | _ | |a Chattopadhyay, S. |b 7 |
| 700 | 1 | _ | |a Cipiccia, S. |b 8 |
| 700 | 1 | _ | |a Feldbaumer, E. |b 9 |
| 700 | 1 | _ | |a Fonseca, R. A. |b 10 |
| 700 | 1 | _ | |a Goddard, B. |b 11 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1013620 |a Gross, M. |b 12 |
| 700 | 1 | _ | |a Grulke, O. |b 13 |
| 700 | 1 | _ | |a Gschwendtner, E. |b 14 |
| 700 | 1 | _ | |a Holloway, J. |b 15 |
| 700 | 1 | _ | |a Huang, C. |b 16 |
| 700 | 1 | _ | |a Jaroszynski, D. |b 17 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1023403 |a Jolly, S. |b 18 |
| 700 | 1 | _ | |a Kempkes, P. |b 19 |
| 700 | 1 | _ | |a Lopes, N. |b 20 |
| 700 | 1 | _ | |a Lotov, K. |b 21 |
| 700 | 1 | _ | |a Machacek, J. |b 22 |
| 700 | 1 | _ | |a Mandry, S. R. |b 23 |
| 700 | 1 | _ | |a McKenzie, J. W. |b 24 |
| 700 | 1 | _ | |a Meddahi, M. |b 25 |
| 700 | 1 | _ | |a Militsyn, B. L. |b 26 |
| 700 | 1 | _ | |a Moschuering, N. |b 27 |
| 700 | 1 | _ | |a Muggli, P. |b 28 |
| 700 | 1 | _ | |a Najmudin, Z. |b 29 |
| 700 | 1 | _ | |a Noakes, T. C. Q. |b 30 |
| 700 | 1 | _ | |a Norreys, P. A. |b 31 |
| 700 | 1 | _ | |a Öz, E. |b 32 |
| 700 | 1 | _ | |a Pardons, A. |b 33 |
| 700 | 1 | _ | |a Petrenko, A. |b 34 |
| 700 | 1 | _ | |a Pukhov, A. |b 35 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1020456 |a Rieger, K. |b 36 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1020455 |a Reimann, O. |b 37 |
| 700 | 1 | _ | |a Ruhl, H. |b 38 |
| 700 | 1 | _ | |a Shaposhnikova, E. |b 39 |
| 700 | 1 | _ | |a Silva, L. O. |b 40 |
| 700 | 1 | _ | |a Sosedkin, A. |b 41 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1006715 |a Tarkeshian, R. |b 42 |
| 700 | 1 | _ | |a Trines, R. M. G. N. |b 43 |
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| 700 | 1 | _ | |0 P:(DE-H253)PIP1002533 |a Wing, M. |b 47 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1005760 |a Xia, G. |b 48 |
| 773 | _ | _ | |0 PERI:(DE-600)1473144-7 |a 10.1088/0741-3335/56/8/084013 |g Vol. 56, no. 8, p. 084013 - |n 8 |p 084013 |t Plasma physics and controlled fusion |v 56 |x 1361-6587 |y 2014 |
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