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Title: Axisymmetric global Alfvén eigenmodes within the ellipticity-induced frequency gap in the Joint European Torus

Authors:
 [1] ;  [2] ;  [3] ; ORCiD logo [3] ;
  1. Institute for Fusion Studies, The University of Texas, Austin, Texas 78712, USA, CCFE, Culham Science Centre, Abingdon, Oxfordshire OX14 3DB, United Kingdom
  2. CCFE, Culham Science Centre, Abingdon, Oxfordshire OX14 3DB, United Kingdom
  3. Institute for Fusion Studies, The University of Texas, Austin, Texas 78712, USA
Publication Date:
Grant/Contract Number:
AC02-05CH11231; FG02-04ER54742
Type:
Publisher's Accepted Manuscript
Journal Name:
Physics of Plasmas
Additional Journal Information:
Journal Name: Physics of Plasmas Journal Volume: 24 Journal Issue: 12; Journal ID: ISSN 1070-664X
Publisher:
American Institute of Physics
Sponsoring Org:
USDOE
Country of Publication:
United States
Language:
English
OSTI Identifier:
1412628

Oliver, H. J. C., Sharapov, S. E., Breizman, B. N., Zheng, L. -J., and JET Contributors. Axisymmetric global Alfvén eigenmodes within the ellipticity-induced frequency gap in the Joint European Torus. United States: N. p., Web. doi:10.1063/1.5005939.
Oliver, H. J. C., Sharapov, S. E., Breizman, B. N., Zheng, L. -J., & JET Contributors. Axisymmetric global Alfvén eigenmodes within the ellipticity-induced frequency gap in the Joint European Torus. United States. doi:10.1063/1.5005939.
Oliver, H. J. C., Sharapov, S. E., Breizman, B. N., Zheng, L. -J., and JET Contributors. 2017. "Axisymmetric global Alfvén eigenmodes within the ellipticity-induced frequency gap in the Joint European Torus". United States. doi:10.1063/1.5005939.
@article{osti_1412628,
title = {Axisymmetric global Alfvén eigenmodes within the ellipticity-induced frequency gap in the Joint European Torus},
author = {Oliver, H. J. C. and Sharapov, S. E. and Breizman, B. N. and Zheng, L. -J. and JET Contributors},
abstractNote = {},
doi = {10.1063/1.5005939},
journal = {Physics of Plasmas},
number = 12,
volume = 24,
place = {United States},
year = {2017},
month = {12}
}