TJ-II:Interferometry: Difference between revisions
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The probing wavelength is 10.6 μm. | The probing wavelength is 10.6 μm. | ||
<ref>[http://link.aip.org/link/?RSINAK/72/96/1 H. Lamela et al, Rev. Sci. Instrum. '''72''', 96 (2001)]</ref> | <ref>[http://link.aip.org/link/?RSINAK/72/96/1 H. Lamela et al, Rev. Sci. Instrum. '''72''', 96 (2001)]</ref> | ||
<ref>[http://link.aip.org/link/?RSINAK/75/3414/1 M. Sánchez at al, Rev. Sci. Instrum. '''75''', 3414 (2004)]</ref> | |||
The system is located in [[TJ-II:Sectors|sector]] B1. | The system is located in [[TJ-II:Sectors|sector]] B1. | ||
==References== | ==References== | ||
<references /> | <references /> | ||
Revision as of 18:00, 5 August 2009
TJ-II has two interferometry systems for the measurement of the line-integrated density.
The Microwave interferometer
The diagnostic is located in sector B8. The probing beam has an inclination of 18.7º with respect to the vertical and a frequency of 140 GHz, corresponding to a wavelength of λ = 2.14 mm. The diagnostic provides a time trace of the-line integrated electron density (65536 points, sampling rate 100 kHz). The time trace is called 'Densidad2_' in the TJ-II database. The signal is less reliable for high densities (above 2-3 1019 m-3). This time trace is fundamental for machine operation.
The CO2 interferometer
The probing wavelength is 10.6 μm. [1] [2] The system is located in sector B1.