Laser-plasma electron acceleration in dielectric capillary tubes

Electron beams and betatron X-ray radiation generated by laser wakefield acceleration in long plasma targets are studied. The targets consist of hydrogen filled dielectric capillary tubes of diameter 150 to 200 microns and length 6 to 20 mm. Electron beams are observed for peak laser intensities as low as 5×1017 W/cm2. It is found that the capillary collects energy outside the main peak of the focal spot and contributes to keep the beam self-focused over a distance longer than in a gas jet of similar density. This enables the pulse to evolve enough to reach the threshold for wavebreaking, and thus trap and accelerate electrons. No electrons were observed for capillaries of large diameter (250 μm), confirming that the capillary influences the interaction and does not have the same behaviour as a gas cell. Finally, X-rays are used as a diagnostic of the interaction and, in particular, to estimate the position of the electrons trapping point inside the capillary.

[1]  A. E. Dangor,et al.  Monoenergetic beams of relativistic electrons from intense laser–plasma interactions , 2004, Nature.

[2]  D. A. Dunnett Classical Electrodynamics , 2020, Nature.

[3]  P. Audebert,et al.  Monomode Guiding of 10 16 W/cm 2 Laser Pulses over 100 Rayleigh Lengths in Hollow Capillary Dielectric Tubes , 1999 .

[4]  A. Rousse,et al.  Imaging Electron Trajectories in Laser Wakefield Cavity using betatron X-Ray Radiation , 2006, 2007 Conference on Lasers and Electro-Optics (CLEO).

[5]  J. Cary,et al.  High-quality electron beams from a laser wakefield accelerator using plasma-channel guiding , 2004, Nature.

[6]  K. Ta Phuoc,et al.  Coherence-based transverse measurement of synchrotron x-ray radiation from relativistic laser-plasma interaction and of laser-accelerated electrons , 2006, 2007 Quantum Electronics and Laser Science Conference.

[7]  Zulfikar Najmudin,et al.  Bright spatially coherent synchrotron X-rays from a table-top source , 2010 .

[8]  G. Matthieussent,et al.  Eigenmodes for capillary tubes with dielectric walls and ultraintense laser pulse guiding. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[9]  E. Esarey,et al.  Synchrotron radiation from electron beams in plasma-focusing channels. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[10]  Y. Glinec,et al.  A laser–plasma accelerator producing monoenergetic electron beams , 2004, Nature.

[11]  C. Wahlström,et al.  Active control of the pointing of a multi-terawatt laser. , 2011, The Review of scientific instruments.

[12]  Erik Lefebvre,et al.  Particle-in-Cell modelling of laser-plasma interaction using Fourier decomposition , 2009, J. Comput. Phys..

[13]  U Schramm,et al.  Generation of stable, low-divergence electron beams by laser-wakefield acceleration in a steady-state-flow gas cell. , 2008, Physical review letters.

[14]  Modelling of laser-plasma electron acceleration in capillary tubes , 2011 .

[15]  Antoine Rousse,et al.  Production of a keV x-ray beam from synchrotron radiation in relativistic laser-plasma interaction. , 2004, Physical review letters.

[16]  F. Albert,et al.  Analysis of wakefield electron orbits in plasma wiggler , 2008 .

[17]  C. Wahlström,et al.  Laser-wakefield acceleration of monoenergetic electron beams in the first plasma-wave period. , 2006, Physical review letters.

[18]  S. Kneip,et al.  Controlling the spectrum of x-rays generated in a laser-plasma accelerator by tailoring the laser wavefront , 2009, 0909.3440.

[19]  S R Nagel,et al.  Observation of synchrotron radiation from electrons accelerated in a petawatt-laser-generated plasma cavity. , 2008, Physical review letters.

[20]  D. Jaroszynski,et al.  Laser-driven plasma waves in capillary tubes. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.

[21]  K. Nakamura,et al.  GeV electron beams from a centimetre-scale accelerator , 2006 .