1. Stark‐effect measurement of high free‐electron laser electric fields in MTX by laser‐aided particle‐probe spectroscopy
- Author
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M. Shiho, K. Ohasa, D. G. Nilson, K. Mizuno, Toshiatsu Oda, K. Odajima, Ken Takiyama, and J. H. Foote
- Subjects
Physics ,Dye laser ,Free-electron laser ,Plasma ,Laser ,law.invention ,symbols.namesake ,Stark effect ,law ,Electric field ,symbols ,Physics::Accelerator Physics ,Plasma diagnostics ,Physics::Atomic Physics ,Atomic physics ,Instrumentation ,Beam (structure) - Abstract
We are constructing a diagnostic system to measure the electric field (≳100 kV/cm) of a free‐electron laser (FEL) beam when injected into the plasma of the Microwave Tokamak Experiment (MTX). The apparatus allows a crossed‐beam measurement, with 2 cm spatial resolution in the plasma, involving the FEL beam (with 140 GHz, ≊1 GW ECH pulses), a neutral helium beam, and a dye laser beam. After the laser beam pumps metastable helium atoms to higher excited states, their decay light is detected by an efficient optical system. Because of the Stark effect arising from the FEL electric field (E), a forbidden transition can be strongly induced. The intensity of emitted light resulting from the forbidden transition is proportional to E2. Because photon counting rates are estimated to be low, extra effort is made to minimize background and noise levels. It is possible that the lower E of an MTX gyrotron‐produced ECH beam with its longer duration pulses can also be measured using this method. Other applications of the...
- Published
- 1990
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