TJ-II:Diagnostic neutral beam: Difference between revisions
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[[File:TJ-II DNBI.jpg|500px|thumb|right|Diagram of the TJ-II Diagnostic Neutral Beam Injector]] | [[File:TJ-II DNBI.jpg|500px|thumb|right|Diagram of the TJ-II Diagnostic Neutral Beam Injector]] | ||
[[TJ-II]] | [[TJ-II]] is equipped with a compact diagnostic neutral beam injector, designed for performing spatially resolved Charge-exchange Recombination Spectroscopy (CXRS) and Motional Stark Effect (MSE) analysis measurements. It is located in [[TJ-II:Sectors|sector]] A7 and it is employed to obtain either measure radial profiles of impurity ion (carbon) temperature and velocity (CXRS) or to measure the wavelength separation of the Stark splitting of beam hydrogen atom emissions at 656.3 nm . | ||
<ref>K.J. McCarthy et al, ''Diagnostic neutral beam injector and associated diagnostic systems for the TJ-II stellarator device'', [[doi:10.1063/1.1784512|Rev. Sci. Instrum. '''75''', 3499 (2004)]]</ref> | <ref>K.J. McCarthy et al, ''Diagnostic neutral beam injector and associated diagnostic systems for the TJ-II stellarator device'', [[doi:10.1063/1.1784512|Rev. Sci. Instrum. '''75''', 3499 (2004)]]</ref> | ||
The injector, an upgraded DINA-5 model, is supported on a mobile cradle that permits its path through the plasma to be varied by ±3° poloidally. In parallel, a dedicated bidirectional (two vertical opposing views) multichannel spectroscopic diagnostic, incorporating fiber arrays, an f/1.8 spectrograph, and a back-illuminated charge-coupled device, | The injector, an upgraded DINA-5 model, is supported on a mobile cradle that permits its path through the plasma to be varied by ±3° poloidally. In parallel, a dedicated bidirectional (two vertical opposing views plus a single toroidal view) multichannel spectroscopic diagnostic, incorporating fiber arrays, an f/1.8 spectrograph, and a back-illuminated charge-coupled device, is installed to obtain Doppler line shifts and widths (around 529.2 nm) with ~1 cm spatial resolution for CXRS. | ||
<ref>J.M. Carmona et al, ''Charge-exchange spectroscopic diagnostic for the TJ-II stellarator'', [[doi:10.1063/1.2229200|Rev. Sci. Instrum. '''77''', 10F107 (2006)]]</ref> | <ref>J.M. Carmona et al, ''Charge-exchange spectroscopic diagnostic for the TJ-II stellarator'', [[doi:10.1063/1.2229200|Rev. Sci. Instrum. '''77''', 10F107 (2006)]]</ref> | ||
<ref>J.M. Carmona et al, ''Density Dependence of Ion Temperature Measured by Active Charge-Exchange Spectroscopy in ECRH Plasmas of the TJ-II Stellarator'', [http://www.new.ans.org/store/j_1911 Fusion Science and Technology '''54''', 4 (2008) 962-969]</ref> | <ref>J.M. Carmona et al, ''Density Dependence of Ion Temperature Measured by Active Charge-Exchange Spectroscopy in ECRH Plasmas of the TJ-II Stellarator'', [http://www.new.ans.org/store/j_1911 Fusion Science and Technology '''54''', 4 (2008) 962-969]</ref> | ||
The Diagnostic Neutral Beam Injector | The Diagnostic Neutral Beam Injector is also used for Motional Stark Effect measurements to quantify the magnitude and pitch of components of the magnetic field<ref>K. J. McCarthy, N. Panadero, A. López-Fraguas, J. Hernández, and B. van Milligen, ''A Spectrally Resolved Motional Stark Effect Diagnostic for the TJ-II Stellarator'', [[doi:10.1002/ctpp.201400067|Contrib. Plasma Phys. 55, No. 6 (2015) 459]]</ref>. | ||
== See also == | == See also == | ||
Revision as of 12:15, 13 May 2024
TJ-II is equipped with a compact diagnostic neutral beam injector, designed for performing spatially resolved Charge-exchange Recombination Spectroscopy (CXRS) and Motional Stark Effect (MSE) analysis measurements. It is located in sector A7 and it is employed to obtain either measure radial profiles of impurity ion (carbon) temperature and velocity (CXRS) or to measure the wavelength separation of the Stark splitting of beam hydrogen atom emissions at 656.3 nm . [1] The injector, an upgraded DINA-5 model, is supported on a mobile cradle that permits its path through the plasma to be varied by ±3° poloidally. In parallel, a dedicated bidirectional (two vertical opposing views plus a single toroidal view) multichannel spectroscopic diagnostic, incorporating fiber arrays, an f/1.8 spectrograph, and a back-illuminated charge-coupled device, is installed to obtain Doppler line shifts and widths (around 529.2 nm) with ~1 cm spatial resolution for CXRS. [2] [3]
The Diagnostic Neutral Beam Injector is also used for Motional Stark Effect measurements to quantify the magnitude and pitch of components of the magnetic field[4].
See also
References
- ↑ K.J. McCarthy et al, Diagnostic neutral beam injector and associated diagnostic systems for the TJ-II stellarator device, Rev. Sci. Instrum. 75, 3499 (2004)
- ↑ J.M. Carmona et al, Charge-exchange spectroscopic diagnostic for the TJ-II stellarator, Rev. Sci. Instrum. 77, 10F107 (2006)
- ↑ J.M. Carmona et al, Density Dependence of Ion Temperature Measured by Active Charge-Exchange Spectroscopy in ECRH Plasmas of the TJ-II Stellarator, Fusion Science and Technology 54, 4 (2008) 962-969
- ↑ K. J. McCarthy, N. Panadero, A. López-Fraguas, J. Hernández, and B. van Milligen, A Spectrally Resolved Motional Stark Effect Diagnostic for the TJ-II Stellarator, Contrib. Plasma Phys. 55, No. 6 (2015) 459