Keegan Behm
University of Michigan
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Featured researches published by Keegan Behm.
Physical Review X | 2018
J. M. Cole; Keegan Behm; E. Gerstmayr; Tom Blackburn; Jonathan Wood; C. D. Baird; Matthew J. Duff; Christopher Harvey; Antony Ilderton; A. S. Joglekar; K. Krushelnick; S. Kuschel; Mattias Marklund; P. McKenna; C. D. Murphy; K. Poder; C. P. Ridgers; G. M. Samarin; Gianluca Sarri; D. R. Symes; A. G. R. Thomas; J. Warwick; M. Zepf; Z. Najmudin; S. P. D. Mangles
The dynamics of energetic particles in strong electromagnetic fields can be heavily influenced by the energy loss arising from the emission of radiation during acceleration, known as radiation reaction. When interacting with a high-energy electron beam, todays lasers are sufficiently intense to explore the transition between the classical and quantum radiation reaction regimes. We present evidence of radiation reaction in the collision of an ultrarelativistic electron beam generated by laser-wakefield acceleration (epsilon > 500 MeV) with an intense laser pulse (a(0) > 10). We measure an energy loss in the postcollision electron spectrum that is correlated with the detected signal of hard photons (gamma rays), consistent with a quantum description of radiation reaction. The generated gamma rays have the highest energies yet reported from an all-optical inverse Compton scattering scheme, with critical energy epsilon(crit) > 30 MeV.
Physical Review X | 2018
K. Poder; Matteo Tamburini; Gianluca Sarri; A. Di Piazza; S. Kuschel; C. D. Baird; Keegan Behm; S. Bohlen; J. M. Cole; D. J. Corvan; Matthew J. Duff; E. Gerstmayr; Christoph H. Keitel; K. Krushelnick; S. P. D. Mangles; P. McKenna; C. D. Murphy; Z. Najmudin; C. P. Ridgers; G. M. Samarin; D. R. Symes; A. G. R. Thomas; J. Warwick; M. Zepf
The description of the dynamics of an electron in an external electromagnetic field of arbitrary intensity is one of the most fundamental outstanding problems in electrodynamics. Remarkably, to date, there is no unanimously accepted theoretical solution for ultrahigh intensities and little or no experimental data. The basic challenge is the inclusion of the self-interaction of the electron with the field emitted by the electron itself - the so-called radiation reaction force. We report here on the experimental evidence of strong radiation reaction, in an all-optical experiment, during the propagation of highly relativistic electrons (maximum energy exceeding 2 GeV) through the field of an ultraintense laser (peak intensity of 4×1020 W/cm2). In their own rest frame, the highest-energy electrons experience an electric field as high as one quarter of the critical field of quantum electrodynamics and are seen to lose up to 30% of their kinetic energy during the propagation through the laser field. The experimental data show signatures of quantum effects in the electron dynamics in the external laser field, potentially showing departures from the constant cross field approximation.
Plasma Physics and Controlled Fusion | 2016
T. Z. Zhao; Keegan Behm; Zihuai He; Anatoly Maksimchuk; John A. Nees; V. Yanovsky; A. G. R. Thomas; K. Krushelnick
The electron injection process into a plasma-based laser wakefield accelerator can be influenced by modifying the parameters of the driver pulse. We present an experimental study on the combined effect of the laser pulse duration, pulse shape, and frequency chirp on the electron injection and acceleration process and the associated radiation emission for two different gas types-a 97.5% He and 2.5% N-2 mixture and pure He. In general, the shortest pulse duration with minimal frequency chirp produced the highest energy electrons and the most charge. Pulses on the positive chirp side sustained electron injection and produced higher charge, but lower peak energy electrons, compared with negatively chirped pulses. A similar trend was observed for the radiant energy. The relationship between the radiant energy and the electron charge remained linear over a threefold change in the electron density and was independent of the drive pulse characteristics. X-ray spectra showed that ionization injection of electrons into the wakefield generally produced more photons than self-injection for all pulse durations/frequency chirp and had less of a spread in the number of photons around the peak x-ray energy.
Scientific Reports | 2018
Jonathan Wood; David J. Chapman; K. Poder; Nelson Lopes; M. E. Rutherford; T. G. White; Felicie Albert; Keegan Behm; N. Booth; Jonathan Bryant; P. S. Foster; S. H. Glenzer; E. Hill; K. Krushelnick; Z. Najmudin; B. B. Pollock; S.J. Rose; W. Schumaker; R. H. H. Scott; M. Sherlock; A. G. R. Thomas; Z. Zhao; Daniel E. Eakins; S. P. D. Mangles
Betatron radiation from laser wakefield accelerators is an ultrashort pulsed source of hard, synchrotron-like x-ray radiation. It emanates from a centimetre scale plasma accelerator producing GeV level electron beams. In recent years betatron radiation has been developed as a unique source capable of producing high resolution x-ray images in compact geometries. However, until now, the short pulse nature of this radiation has not been exploited. This report details the first experiment to utilize betatron radiation to image a rapidly evolving phenomenon by using it to radiograph a laser driven shock wave in a silicon target. The spatial resolution of the image is comparable to what has been achieved in similar experiments at conventional synchrotron light sources. The intrinsic temporal resolution of betatron radiation is below 100 fs, indicating that significantly faster processes could be probed in future without compromising spatial resolution. Quantitative measurements of the shock velocity and material density were made from the radiographs recorded during shock compression and were consistent with the established shock response of silicon, as determined with traditional velocimetry approaches. This suggests that future compact betatron imaging beamlines could be useful in the imaging and diagnosis of high-energy-density physics experiments.
Archive | 2017
K. Poder; Matteo Tamburini; Gianluca Sarri; A. Di Piazza; S. Kuschel; C. D. Baird; Keegan Behm; S. Bohlen; J. M. Cole; Matthew J. Duff; E. Gerstmayr; Christoph H. Keitel; K. Krushelnick; S. P. D. Mangles; P. McKenna; C. D. Murphy; Z. Najmudin; C. P. Ridgers; G. M. Samarin; D. R. Symes; A. G. R. Thomas; J. Warwick; M. Zepf
Physical Review Letters | 2016
T. Z. Zhao; Keegan Behm; Chuanfei Dong; Xavier Davoine; Serge Y. Kalmykov; V. Petrov; V. Chvykov; Paul Cummings; B. Hou; Anatoly Maksimchuk; John A. Nees; V. Yanovsky; A. G. R. Thomas; K. Krushelnick
New Journal of Physics | 2018
A E Hussein; J Ludwig; Keegan Behm; Y Horovitz; P-E Masson-Laborde; V. Chvykov; Anatoly Maksimchuk; T. Matsuoka; Christopher McGuffey; V. Yanovsky; W Rozmus; K. Krushelnick
New Journal of Physics | 2018
J Elle; T. Z. Zhao; Y Ma; Keegan Behm; A Lucero; Anatoly Maksimchuk; John A. Nees; A. G. R. Thomas; Andreas Schmitt-Sody; K. Krushelnick
Bulletin of the American Physical Society | 2017
Anatoly Maksimchuk; Keegan Behm; Tony Zhao; A. S. Joglekar; Amina Hussein; John A. Nees; A. G. R. Thomas; K. Krushelnick; J. Elle; A. Lucero; G. M. Samarin; G. Sarry; J. Warwick
Bulletin of the American Physical Society | 2016
Keegan Behm; Amina Hussein; Tony Zhao; E. Hill; Anatoly Maksimchuk; John A. Nees; Victor Yanovsky; S. P. D. Mangles; K. Krushelnick; A. G. R. Thomas