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Research Needs for Magnetic Fusion Energy Sciences - US Burning ...

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as a final note, the overall importance of the boundary layer is underscored by the european tokamak<br />

program’s fundamental reorientation toward boundary research over the past decade. an<br />

outcome of this shift is the decision to dedicate europe’s two most important tokamaks to exploring<br />

materials other than carbon; Jet is committed to studying a beryllium-wall plus tungsten-divertor<br />

PFc system, while aUG is focusing on an all-tungsten PFc system. Thus they have decided<br />

that enhanced tokamak core physics priorities be subordinated to learning how to tame the plasma-materials<br />

interface. The europeans have also been steadily growing their boundary modeling<br />

and diagnostic ef<strong>for</strong>ts. The present Us situation stands in significant contrast: staffing levels in<br />

Us tokamak scrape-off layer diagnosis and physics research have decreased over the past decade<br />

from about 40 to about 20 people working at the major devices. The Us fusion program cannot<br />

af<strong>for</strong>d to fall behind in this critical area, recognized by the Greenwald Report as being at the top<br />

of the magnetic <strong>Fusion</strong> energy priority list. at a minimum the heavy investment in the existing<br />

major Us devices needs to be better exploited <strong>for</strong> addressing critical boundary issues. This will require<br />

restoring, at least, the earlier level of ef<strong>for</strong>t as well as major investment in edge diagnostics.<br />

Proposed actions:<br />

1. Develop and deploy new diagnostics<br />

Understanding complex systems requires extensive diagnostics. For example, exploiting aerodynamic<br />

lift and drag <strong>for</strong> aircraft design would have been impossible if the air velocity were measured<br />

at just one or two locations around airfoils; such measurements are typically made at dozens<br />

of locations. The pedestal/sol is much more complicated than air flow around an object and<br />

one can hardly expect to identify edge controlling physics with the spatially sparse diagnostic deployments<br />

available today. in addition to the diagnostics sets described below, other techniques<br />

should be assessed.<br />

extensive sets of pop-up (or similar drive) probes should be used to map out the 4-d (spatially<br />

and temporally) distributions of density, electron temperature, and electric potential (langmuir<br />

probes); parallel flow velocity (mach probes); cross-field transport (turbulence probes); and ion<br />

temperature and energy distributions of electrons and ions (gridded energy analyzers). magnetically<br />

activated probe drives of various types have been developed, including swing action and reciprocation,<br />

achieving viable penetration to the separatrix. deployments of such probes are needed<br />

in significant numbers (e.g., > 10 systems), around the periphery of tokamaks. While materials<br />

costs will be relatively modest, the additional staffing requirements will be significant.<br />

Thomson scattering is complicated in edge plasmas by high background light, but it has been successfully<br />

used on diii-d to reconstruct the 2-d profiles of electron density and temperature (n e and<br />

t e ) by sweeping of the magnetic X-point relative to the Thomson channels. With the addition of a<br />

high-dispersion instrument such as a Fabry-Perot interferometer, measurements could be made<br />

of electron/ion energy distributions and z eff . in addition, a multi-laser Thomson system (firing<br />

laser 1, 2, 3 in rapid succession) could make images that reveal the detailed time evolution of socalled<br />

“blobs” and elms. charge-exchange recombination (ceR) spectroscopy using new powerful<br />

pulsed ion diode neutral beams (10 6 a/m 2 , 1 μs, 100 kev/amu) may permit measurement of t i and<br />

v || (along b) in to the separatrix. advances in ultrasoft X-ray spectroscopy would allow reconstruction<br />

of the t e profiles with time resolution higher than possible from Thomson scattering alone.<br />

305

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