4,427
edits
TJ-II:Heavy Ion Beam Probe: Difference between revisions
no edit summary
mNo edit summary |
No edit summary |
||
| Line 2: | Line 2: | ||
The advanced Heavy Ion Beam Probe can simulataneously measure the plasma electric potential ''φ'', the electron density ''n<sub>e</sub>'', the electron temperature ''T<sub>e</sub>'', and a poloidal magnetic field component ''B<sub>p</sub>'' at a point inside the plasma. | The advanced Heavy Ion Beam Probe can simulataneously measure the plasma electric potential ''φ'', the electron density ''n<sub>e</sub>'', the electron temperature ''T<sub>e</sub>'', and a poloidal magnetic field component ''B<sub>p</sub>'' at a point inside the plasma. | ||
<ref>[http://dx.doi.org/10.1016/S0920-3796(01)00428-8 L.I. Krupnik et al., Fusion Engineering and Design '''56-57''' (2001) 935]</ref> | <ref>[http://dx.doi.org/10.1016/S0920-3796(01)00428-8 L.I. Krupnik et al., ''The first operation of the advanced heavy ion beam probing diagnostic on the TJ-II flexible heliac'', Fusion Engineering and Design '''56-57''' (2001) 935]</ref> | ||
<ref>[http://link.aip.org/link/?RSINAK/72/583/1 I.S. Bondarenko et al., Rev. Sci. Instrum. '''72''', 583 (2001)]</ref> | <ref>[http://link.aip.org/link/?RSINAK/72/583/1 I.S. Bondarenko et al., ''Installation of an advanced heavy ion beam diagnostic on the TJ-II stellarator'', Rev. Sci. Instrum. '''72''', 583 (2001)]</ref> | ||
<ref>[http://dx.doi.org/10.1007/s10582-005-0044-8 L. Krupnik et al, ''Radial electric fields and confinement in the TJ-II stellarator'', Czechoslovak Journal of Physics '''55''', 3 (2005) 317-339(23)]</ref> | |||
This point can be scanned through the plasma cross-section by varying the deflection potentials (active beam control). | This point can be scanned through the plasma cross-section by varying the deflection potentials (active beam control). | ||
== References == | == References == | ||
<references /> | <references /> | ||