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017 | _ | _ | |a This version is available at the following Publisher URL: http://dx.doi.org/10.1088/0741-3335/43/12A/325 |
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041 | _ | _ | |a eng |
082 | _ | _ | |a 530 |
084 | _ | _ | |2 WoS |a Physics, Fluids & Plasmas |
084 | _ | _ | |2 WoS |a Physics, Nuclear |
100 | 1 | _ | |a Ryter, F. |0 P:(DE-HGF)0 |b 0 |
245 | _ | _ | |a Experimental studies of electron transport |
260 | _ | _ | |a Bristol |b IOP Publ. |c 2001 |
300 | _ | _ | |a A323 - A338 |
336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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336 | 7 | _ | |a article |2 DRIVER |
440 | _ | 0 | |a Plasma Physics and Controlled Fusion |x 0741-3335 |0 4996 |v 43 |
500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
520 | _ | _ | |a Electron transport in tokamaks has many different features which are briefly reviewed. The paper is focused on electron heat transport in conventional tokamak plasmas. An inter-machine comparison indicates that the non-dimensional gradient length of the electron temperature profiles R/L-Te, is almost independent of the devices and varies little with plasma parameters. This strongly suggests that electron heat transport is governed by turbulence with a threshold in R/L-Te.. This is confirmed by modulation experiments using electron cyclotron heating. Simulations with empirical and physics-based transport models confirm this assumption. |
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700 | 1 | _ | |a Angioni, C. |0 P:(DE-HGF)0 |b 1 |
700 | 1 | _ | |a Beurskens, M. |0 P:(DE-Juel1)VDB3329 |b 2 |
700 | 1 | _ | |a Cirant, S. |0 P:(DE-HGF)0 |b 3 |
700 | 1 | _ | |a Hoang, G. T. |0 P:(DE-HGF)0 |b 4 |
700 | 1 | _ | |a Hogeweij, G. M. D. |0 P:(DE-Juel1)VDB3779 |b 5 |
700 | 1 | _ | |a Imbeaux, F. |0 P:(DE-HGF)0 |b 6 |
700 | 1 | _ | |a Jacchia, A. |0 P:(DE-HGF)0 |b 7 |
700 | 1 | _ | |a Mantica, P. |0 P:(DE-HGF)0 |b 8 |
700 | 1 | _ | |a Suttrop, W. |0 P:(DE-Juel1)VDB3233 |b 9 |
700 | 1 | _ | |a Tardini, G. |0 P:(DE-HGF)0 |b 10 |
773 | _ | _ | |g Vol. 43, p. A323 - A338 |p A323 - A338 |q 43 |t Plasma physics and controlled fusion |v 43 |y 2001 |x 0741-3335 |
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