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1 - Nuclear Sciences and Applications - IAEA

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INSIDE LAUNCH ELECTRON CYCLOTRON<br />

HEATING AND CURRENT DRIVE ON DITE<br />

<strong>IAEA</strong>-CN-50/E-I-3<br />

M. ASHRAF, R. BARNSLEY 1 , N. DELIYANAKIS 2 , T. EDLINGTON,<br />

S.J. FIELDING, J. HUGILL, P.C. JOHNSON, B. LLOYD, S. MANHOOD,<br />

P. MANTICA 3 , G.F. MATTHEWS, W. MILLAR, M. O'BRIEN,<br />

R.A. PITTS 4 , A.C. RIVIERE, D.C. ROBINSON, A. SIMONETTO 5 ,<br />

G. VAYAKIS 2<br />

Culham Laboratory,<br />

Euratom-UKAEA Fusion Association,<br />

Abingdon, Oxfordshire,<br />

United Kingdom<br />

Abstract<br />

INSIDE LAUNCH ELECTRON CYCLOTRON HEATING AND CURRENT DRIVE ON DITE.<br />

Electron cyclotron resonance heating at 60 GHz has been carried out on DITE (R = 1.2 m,<br />

a = 0.24 m) to investigate heating <strong>and</strong> current drive using the extraordinary mode launched with finite<br />

k| from the high field side. The first clear evidence of Doppler shifted resonance absorption in a nearthermal<br />

plasma is obtained. The heating efficiency is observed to fall sharply at densities above cut-off<br />

for the wave. At lower densities the increment in power to the limiter is measured during ECRH <strong>and</strong><br />

is compared with that expected from the global power balance. The degradation in particle confinement<br />

often associated with ECRH is observed as an increased particle flux at the boundary driven by local<br />

electrostatic fluctuations. Initial experiments on the electron cyclotron wave driven current at the second<br />

harmonic show effects that are consistent with the low efficiency expected from theory including trapped<br />

particle effects.<br />

1 INTRODUCTION<br />

At the fundamental EC resonance the right h<strong>and</strong> cut-off prevents X-mode<br />

access to the plasma when the wave is launched from the low field side.<br />

When launched from the HFS this limit is avoided <strong>and</strong> the cut-off density<br />

is then given by<br />

for a semi-infinite slab plasma. Here u> is the applied wave frequency, wp<br />

is the electron plasma frequency, n\\ — ck\\/u> <strong>and</strong> u>c = eB/m0. Earlier<br />

' Leicester University, Leicester, United Kingdom.<br />

2 Oxford University, Oxford, United Kingdom.<br />

3 Istituto di Fisica del Plasma, Consiglio Nazionale delle Ricerche, Milan, Italy.<br />

Royal Holloway <strong>and</strong> Bedford New College, University of London, London, United<br />

Kingdom.<br />

Attached under a Euratom Fellowship.<br />

541

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