Author
Listed:
- C. K. Li
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- P. Tzeferacos
(University of Chicago)
- D. Lamb
(University of Chicago)
- G. Gregori
(University of Oxford)
- P. A. Norreys
(University of Oxford)
- M. J. Rosenberg
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- R. K. Follett
(Laboratory for Laser Energetics, University of Rochester
University of Rochester)
- D. H. Froula
(Laboratory for Laser Energetics, University of Rochester
University of Rochester)
- M. Koenig
(LULI-CNRS, Ecole Polytechnique, CEA: Université Paris-Saclay
UPMC Univ Paris 06: Sorbonne Universités
Institute of Laser Engineering, Osaka University)
- F. H. Seguin
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- J. A. Frenje
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- H. G. Rinderknecht
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- H. Sio
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- A. B. Zylstra
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- R. D. Petrasso
(Plasma Science and Fusion Center, Massachusetts Institute of Technology)
- P. A. Amendt
(Lawrence Livermore National Laboratory)
- H. S. Park
(Lawrence Livermore National Laboratory)
- B. A. Remington
(Lawrence Livermore National Laboratory)
- D. D. Ryutov
(Lawrence Livermore National Laboratory)
- S. C. Wilks
(Lawrence Livermore National Laboratory)
- R. Betti
(Laboratory for Laser Energetics, University of Rochester
University of Rochester)
- A. Frank
(Laboratory for Laser Energetics, University of Rochester
University of Rochester)
- S. X. Hu
(Laboratory for Laser Energetics, University of Rochester)
- T. C. Sangster
(Laboratory for Laser Energetics, University of Rochester)
- P. Hartigan
(Rice University 6100 S. Main)
- R. P. Drake
(Ocean and Space Science, University of Michigan)
- C. C. Kuranz
(Ocean and Space Science, University of Michigan)
- S. V. Lebedev
(The Blackett Laboratory, Imperial College London)
- N. C. Woolsey
(University of York)
Abstract
The remarkable discovery by the Chandra X-ray observatory that the Crab nebula’s jet periodically changes direction provides a challenge to our understanding of astrophysical jet dynamics. It has been suggested that this phenomenon may be the consequence of magnetic fields and magnetohydrodynamic instabilities, but experimental demonstration in a controlled laboratory environment has remained elusive. Here we report experiments that use high-power lasers to create a plasma jet that can be directly compared with the Crab jet through well-defined physical scaling laws. The jet generates its own embedded toroidal magnetic fields; as it moves, plasma instabilities result in multiple deflections of the propagation direction, mimicking the kink behaviour of the Crab jet. The experiment is modelled with three-dimensional numerical simulations that show exactly how the instability develops and results in changes of direction of the jet.
Suggested Citation
C. K. Li & P. Tzeferacos & D. Lamb & G. Gregori & P. A. Norreys & M. J. Rosenberg & R. K. Follett & D. H. Froula & M. Koenig & F. H. Seguin & J. A. Frenje & H. G. Rinderknecht & H. Sio & A. B. Zylstra, 2016.
"Scaled laboratory experiments explain the kink behaviour of the Crab Nebula jet,"
Nature Communications, Nature, vol. 7(1), pages 1-8, December.
Handle:
RePEc:nat:natcom:v:7:y:2016:i:1:d:10.1038_ncomms13081
DOI: 10.1038/ncomms13081
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