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Ding H, Döpp A, Gilljohann M, Götzfried J, Schindler S, Wildgruber L, Cheung G, Hooker SM, Karsch S. Nonlinear plasma wavelength scalings in a laser wakefield accelerator. Phys Rev E 2020; 101:023209. [PMID: 32168651 DOI: 10.1103/physreve.101.023209] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/26/2019] [Accepted: 01/24/2020] [Indexed: 11/07/2022]
Abstract
Laser wakefield acceleration relies on the excitation of a plasma wave due to the ponderomotive force of an intense laser pulse. However, plasma wave trains in the wake of the laser have scarcely been studied directly in experiments. Here we use few-cycle shadowgraphy in conjunction with interferometry to quantify plasma waves excited by the laser within the density range of GeV-scale accelerators, i.e., a few 10^{18}cm^{-3}. While analytical models suggest a clear dependency between the nonlinear plasma wavelength and the peak potential a_{0}, our study shows that the analytical models are only accurate for driver strength a_{0}≲1. Experimental data and systematic particle-in-cell simulations reveal that nonlinear lengthening of the plasma wave train depends not solely on the laser peak intensity but also on the waist of the focal spot.
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Affiliation(s)
- H Ding
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany.,Max Planck Institut für Quantenoptik, Hans-Kopfermann-Strasse 1, D-85748 Garching, Germany
| | - A Döpp
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany.,Max Planck Institut für Quantenoptik, Hans-Kopfermann-Strasse 1, D-85748 Garching, Germany
| | - M Gilljohann
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany.,Max Planck Institut für Quantenoptik, Hans-Kopfermann-Strasse 1, D-85748 Garching, Germany
| | - J Götzfried
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
| | - S Schindler
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
| | - L Wildgruber
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
| | - G Cheung
- John Adams Institute & Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - S M Hooker
- John Adams Institute & Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - S Karsch
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany.,Max Planck Institut für Quantenoptik, Hans-Kopfermann-Strasse 1, D-85748 Garching, Germany
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3
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Li S, Li G, Ain Q, Hur MS, Ting AC, Kulagin VV, Kamperidis C, Hafz NAM. A laser-plasma accelerator driven by two-color relativistic femtosecond laser pulses. SCIENCE ADVANCES 2019; 5:eaav7940. [PMID: 31803828 PMCID: PMC6874490 DOI: 10.1126/sciadv.aav7940] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 10/21/2018] [Accepted: 09/27/2019] [Indexed: 06/10/2023]
Abstract
A typical laser-plasma accelerator (LPA) is driven by a single, ultrarelativistic laser pulse from terawatt- or petawatt-class lasers. Recently, there has been some theoretical work on the use of copropagating two-color laser pulses (CTLP) for LPA research. Here, we demonstrate the first LPA driven by CTLP where we observed substantial electron energy enhancements. Those results have been further confirmed in a practical application, where the electrons are used in a bremsstrahlung-based positron generation configuration, which led to a considerable boost in the positron energy as well. Numerical simulations suggest that the trailing second harmonic relativistic laser pulse is capable of sustaining the acceleration structure for much longer distances after the preceding fundamental pulse is depleted in the plasma. Therefore, our work confirms the merits of driving LPAs by two-color pulses and paves the way toward a downsizing of LPAs, making their potential applications in science and technology extremely attractive and affordable.
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Affiliation(s)
- Song Li
- Key Laboratory for Laser Plasmas (Ministry of Education), Collaborative Innovation Center of IFSA (CICIFSA), School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
- ELI-ALPS, ELI-HU Nonprofit Ltd., Dugonics tér 13, Szeged 6720, Hungary
| | - Guangyu Li
- Key Laboratory for Laser Plasmas (Ministry of Education), Collaborative Innovation Center of IFSA (CICIFSA), School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
| | - Quratul Ain
- Key Laboratory for Laser Plasmas (Ministry of Education), Collaborative Innovation Center of IFSA (CICIFSA), School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
| | - Min Sup Hur
- Ulsan National Institute of Science and Technology (UNIST), Ulsan 44919, Republic of Korea
| | - Antonio C. Ting
- Institute for Research in Electronics and Applied Physics, University of Maryland, College Park, MD 20742, USA
| | - Victor V. Kulagin
- Sternberg Astronomical Institute of Moscow State University, Moscow 119992, Russia
- Kotelnikov Institute of Radioengineering and Electronics of Russian Academy of Sciences, Moscow, 125009, Russia
| | | | - Nasr A. M. Hafz
- ELI-ALPS, ELI-HU Nonprofit Ltd., Dugonics tér 13, Szeged 6720, Hungary
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4
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Hussein AE, Senabulya N, Ma Y, Streeter MJV, Kettle B, Dann SJD, Albert F, Bourgeois N, Cipiccia S, Cole JM, Finlay O, Gerstmayr E, González IG, Higginbotham A, Jaroszynski DA, Falk K, Krushelnick K, Lemos N, Lopes NC, Lumsdon C, Lundh O, Mangles SPD, Najmudin Z, Rajeev PP, Schlepütz CM, Shahzad M, Smid M, Spesyvtsev R, Symes DR, Vieux G, Willingale L, Wood JC, Shahani AJ, Thomas AGR. Laser-wakefield accelerators for high-resolution X-ray imaging of complex microstructures. Sci Rep 2019; 9:3249. [PMID: 30824838 PMCID: PMC6397215 DOI: 10.1038/s41598-019-39845-4] [Citation(s) in RCA: 27] [Impact Index Per Article: 5.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/03/2018] [Accepted: 01/29/2019] [Indexed: 12/19/2022] Open
Abstract
Laser-wakefield accelerators (LWFAs) are high acceleration-gradient plasma-based particle accelerators capable of producing ultra-relativistic electron beams. Within the strong focusing fields of the wakefield, accelerated electrons undergo betatron oscillations, emitting a bright pulse of X-rays with a micrometer-scale source size that may be used for imaging applications. Non-destructive X-ray phase contrast imaging and tomography of heterogeneous materials can provide insight into their processing, structure, and performance. To demonstrate the imaging capability of X-rays from an LWFA we have examined an irregular eutectic in the aluminum-silicon (Al-Si) system. The lamellar spacing of the Al-Si eutectic microstructure is on the order of a few micrometers, thus requiring high spatial resolution. We present comparisons between the sharpness and spatial resolution in phase contrast images of this eutectic alloy obtained via X-ray phase contrast imaging at the Swiss Light Source (SLS) synchrotron and X-ray projection microscopy via an LWFA source. An upper bound on the resolving power of 2.7 ± 0.3 μm of the LWFA source in this experiment was measured. These results indicate that betatron X-rays from laser wakefield acceleration can provide an alternative to conventional synchrotron sources for high resolution imaging of eutectics and, more broadly, complex microstructures.
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Affiliation(s)
- A E Hussein
- Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA.
| | - N Senabulya
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, 48109-2099, USA
| | - Y Ma
- Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA.,Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.,The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK
| | - M J V Streeter
- Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.,The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.,The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK
| | - B Kettle
- The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK
| | - S J D Dann
- Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.,The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK
| | - F Albert
- Lawrence Livermore National Laboratory, NIF and Photon Sciences, Livermore, CA, 94550, USA
| | - N Bourgeois
- Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, OX11 0QX, UK
| | - S Cipiccia
- Diamond Light Source, Harwell Science and Innovation Campus, Fermi Avenue, Didcot, OX11 0DE, UK
| | - J M Cole
- The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK
| | - O Finlay
- Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.,The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK
| | - E Gerstmayr
- The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK
| | | | - A Higginbotham
- York Plasma Institute, Department of Physics, University of York, York, YO10 5DD, UK
| | - D A Jaroszynski
- The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.,SUPA, Department of Physics, University of Strathclyde, Glasgow, G4 0NG, UK
| | - K Falk
- Helmholtz-Zentrum Dresden-Rossendorf, Bautzner Landstraße 400, 01328, Dresden, Germany.,Technische Universität Dresden, 01062, Dresden, Germany.,Institute of Physics of the ASCR, 182 21, Prague, Czech Republic
| | - K Krushelnick
- Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA
| | - N Lemos
- Lawrence Livermore National Laboratory, NIF and Photon Sciences, Livermore, CA, 94550, USA
| | - N C Lopes
- The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.,GoLP/Instituto de Plasmas e Fusão Nuclear, Instituto Superior Técnico, U.L., Lisboa, 1049-001, Portugal
| | - C Lumsdon
- York Plasma Institute, Department of Physics, University of York, York, YO10 5DD, UK
| | - O Lundh
- Department of Physics, Lund University, P.O. Box 118, S-22100, Lund, Sweden
| | - S P D Mangles
- The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK
| | - Z Najmudin
- The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK
| | - P P Rajeev
- Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, OX11 0QX, UK
| | - C M Schlepütz
- Swiss Light Source, Paul Scherrer Institute, CH-5232, Villigen, Switzerland
| | - M Shahzad
- The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.,SUPA, Department of Physics, University of Strathclyde, Glasgow, G4 0NG, UK
| | - M Smid
- Helmholtz-Zentrum Dresden-Rossendorf, Bautzner Landstraße 400, 01328, Dresden, Germany.,ELI Beamlines, Institute of Physics of the ASCR, 182 21, Prague, Czech Republic
| | - R Spesyvtsev
- The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.,SUPA, Department of Physics, University of Strathclyde, Glasgow, G4 0NG, UK
| | - D R Symes
- Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, OX11 0QX, UK
| | - G Vieux
- The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.,SUPA, Department of Physics, University of Strathclyde, Glasgow, G4 0NG, UK
| | - L Willingale
- Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA
| | - J C Wood
- The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK
| | - A J Shahani
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, 48109-2099, USA
| | - A G R Thomas
- Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA.,Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.,The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK
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