Zonal flow generation in the improved confinement mode plasma and its role in confinement bifurcations
| dc.contributor.author | Shats, Michael | |
| dc.contributor.author | Solomon, W | |
| dc.date.accessioned | 2009-05-06T05:15:58Z | en_US |
| dc.date.accessioned | 2010-12-20T06:03:53Z | |
| dc.date.available | 2009-05-06T05:15:58Z | en_US |
| dc.date.available | 2010-12-20T06:03:53Z | |
| dc.date.issued | 2002-05-29 | en_US |
| dc.date.updated | 2015-12-11T07:40:20Z | |
| dc.description.abstract | Unstable fluctuations develop in the initially quiescent plasma in the improved confinement mode of the H-1 heliac when the radial electric field (Er) shear exceeds some critical value. These unstable Er shear-driven modes are shown to generate zonal-flow-like poloidally symmetric potential structures, similar to those generated in the low confinement mode (Shats M G and Solomon W M 2002 Phys. Rev. Lett. 88 045001). The structures modulate their parent waves, the background Er shear and the fluctuation-driven radial transport. The onset of zonal flows is observed as a precursor to the plasma confinement bifurcation to an even higher confinement regime. | |
| dc.description.abstract | We discuss the interband light tunneling in a two-dimensional periodic photonic structure, as studied recently in experiments for optically induced photonic lattices [Trompeter et al., Phys. Rev. Lett. 96, 053903 (2006)]. We identify the Zener tunneling regime at the crossing of two Bloch bands, which occurs in the generic case of a Bragg reflection when the Bloch index crosses the edge of the irreducible Brillouin zone. Similarly, higher-order Zener tunneling involves four Bloch bands when the Bloch index passes through a high-symmetry point on the edge of the Brillouin zone. We derive simple analytical models that describe the tunneling effect, and calculate the corresponding tunneling probabilities. | |
| dc.format | 19 pages | |
| dc.identifier.citation | New Journal of Physics 4 (2002): 30.1-30.14 | |
| dc.identifier.issn | 1367-2630 | en_US |
| dc.identifier.uri | http://hdl.handle.net/10440/229 | en_US |
| dc.identifier.uri | http://digitalcollections.anu.edu.au/handle/10440/229 | |
| dc.publisher | Institute of Physics Publishing | |
| dc.source | New Journal of Physics | |
| dc.source.uri | http://www.iop.org/EJ/article/1367-2630/4/1/330/nj2130.pdf?request-id=4ccaaed2-10ea-43ca-ae08-d00802894a36 | en_US |
| dc.source.uri | http://www.iop.org/EJ/article/1367-2630/4/1/330/nj2130.html | en_US |
| dc.title | Zonal flow generation in the improved confinement mode plasma and its role in confinement bifurcations | |
| dc.type | Journal article | |
| local.bibliographicCitation.lastpage | 30.14 | |
| local.bibliographicCitation.startpage | 30.1 | |
| local.contributor.affiliation | Shats, Michael, Research School of Physical Sciences and Engineering, Plasma Research Laboratory | en_US |
| local.contributor.affiliation | Solomon, W, Research School of Physical Sciences and Engineering, Plasma Research Laboratory | en_US |
| local.contributor.authoruid | u9113958 | en_US |
| local.contributor.authoruid | u9617162 | en_US |
| local.description.refereed | Yes | |
| local.identifier.absfor | 020204 | en_US |
| local.identifier.ariespublication | MigratedxPub2709 | en_US |
| local.identifier.citationvolume | 4 | |
| local.identifier.doi | 10.1088/1367-2630/4/1/330 | |
| local.identifier.scopusID | 2-s2.0-3042558478 | |
| local.type.status | Published Version | en_US |
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