TJ-II:Helium Beam: Difference between revisions

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(Hamamatsu, model R5900U-20-L16) with interference filters
(Hamamatsu, model R5900U-20-L16) with interference filters
(FWHM = 1 nm).
(FWHM = 1 nm).
<ref>[http://link.aip.org/link/?RSINAK/72/602/1 B. Brañas et al., ''Atomic beam diagnostics for characterization of edge plasma in TJ-II stellarator'', Rev. Sci. Instrum. '''72''', 602 (2001)]</ref>
<ref>B. Brañas et al., ''Atomic beam diagnostics for characterization of edge plasma in TJ-II stellarator'', [[doi:10.1063/1.1319868|Rev. Sci. Instrum. '''72''', 602 (2001)]]</ref>
A Collisional Radiative (CR) model for the line emission intensity ratios is used
A Collisional Radiative (CR) model for the line emission intensity ratios is used
to deduce electron densities and temperatures.
to deduce electron densities and temperatures.
<ref>[http://link.aip.org/link/?RSINAK/75/3478/1 A. Hidalgo et al., ''Multipulse supersonic helium beam diagnostic in the TJ-II stellarator'', Rev. Sci Instrum. '''75''', 3478 (2004)]</ref>
<ref name="Hidalgo">A. Hidalgo et al., ''Multipulse supersonic helium beam diagnostic in the TJ-II stellarator'', [[doi:10.1063/1.1779617|Rev. Sci Instrum. '''75''', 3478 (2004)]]</ref>
<ref name="Guzman">[http://dx.doi.org/10.1016/j.jnucmat.2009.01.290 F. Guzmán et al, ''On the determination of edge Ti profiles by a supersonic He beam in TJ-II'', Journal of Nuclear Materials '''390-391''' (2009) 1127-1130]</ref>
<ref name="Guzman">F. Guzmán et al, ''On the determination of edge Ti profiles by a supersonic He beam in TJ-II'', [[doi:10.1016/j.jnucmat.2009.01.290|Journal of Nuclear Materials '''390-391''' (2009) 1127-1130]]</ref>
It provides profiles of the electron temperature and density in the plasma edge at a repetition rate of up to 200 Hz.
It provides profiles of the electron temperature and density in the plasma edge at a repetition rate of up to 200 Hz.


It is located at &phi; = 355.3&deg; ([[TJ-II:Sectors|sector]] C8).
It is located at &phi; = 355.3&deg; ([[TJ-II:Sectors|sector]] C8).


[[File:TJ-II_Helium_beam.png|300px|thumb|right|The TJ-II Helium beam diagnostic. The laser can be crossed with the Helium beam for LiF measurements of the excited He population <ref name="Guzman" /> and validation of the CR model.]]
[[File:TJ-II_Helium_beam.png|300px|thumb|right|The TJ-II Helium beam diagnostic. The laser can be crossed with the Helium beam for LiF measurements of the excited He population <ref name="Hidalgo" /> and validation of the CR model.]]


== Data description ==
== Data description ==
The Helium beam pulse shape is stored in the [[TJ-II:Shot database|TJ-II database]] with the name 'HELIO_HAZ'.
The Helium beam pulse shape is stored in the [[TJ-II:Shot database|TJ-II database]] with the name 'HELIO_HAZ'.
The detected line emission signals are stored with the names 'He_xxx_yy', where 'xxx' is the wavelength in nm (667, 706, or 728), while 'yy' is the position (from 01 through 16).
The detected line emission signals are stored with the names 'He_xxx_yy', where 'xxx' is the wavelength in nm (667, 706, or 728), while 'yy' is the position (from 01 through 16).
[[File:TJ-II He beam.jpg|400px|thumb|left|Photo of He beam diagnostic (top port)]]  
[[File:TJ-II He beam.jpg|400px|thumb|left|Photo of Helium and [[TJ-II:Lithium Beam|Lithium]] beam diagnostics (top ports)]]  


== References ==
== References ==
<references />
<references />

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