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MOSS Spectroscopy Applications in Plasma
Physics
John Howard
Plasma Research LaboratoryAustralian National University
Outline
• MOSS spectrometer– Principle
– Doppler measurements on H-1
•Polarization Spectroscopy– Zeeman effect and MSE
•Spread spectrum FTS
•Imaging systems
Fourier Transform Spectroscopy
MOSS SpectrometerConcept
Instrument
Advantages of MOSS
•High light throughput•High time resolution •Compact, robust
MOSS is optimum in the sense that all photons contribute to three independent pieces of information - intensity, shift and contrast.
DC Light intensity
atan(odd,even) Flow velocity (shift)
sqrt(odd2+even2) Temperature (contrast)
MOSS Hardware
MOSS spectroscopy on H-1
Lines of sight
Plasma cross section
Central ring
conductor
Fringe contrast versus time delayArII 488nm, Ti=10, (10), 100 eV
Nominal delay for LiNbO3 ( 25mm)
L-H Confinement Transitions
Heat Modulation Experiments
Fluctuation Measurements
Polarization Spectroscopy
Polarization Spectroscopy
Spherical quadrature polarimeter
Polarization Spectroscopy
Spread Spectrum FTS
Spread Spectrum FTS
Imaging systems
Multiple spatial channels can be multiplexed through an imaging MOSS spectrometer while maintaining high light throughput and low instrument temperature.
Multiple-crystal modulators can be employed for truly 2-D spectral imaging: the spectrum at each spatial position is encoded in the temporal frequency domain.
Spread spectrum data at 587nm HeI
Plasma light Calibrationlaser pulse
Laser interferogram
Power spectrum of interferogram
time (ms)
Conclusion
• MOSS spectroscopy is a high throughput alternative to traditional grating spectrometers
• Well suited to plasma Doppler and polarization spectroscopy
• Fully 2-D spectral imaging is possible.
• Facilitates tomography of scalar (intensity) and vector (velocity) fields in H-1NF for force balance, fluctuation and particle/heat modulation studies