2015
DOI: 10.1088/1748-0221/10/12/c12021
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Thomson scattering at 250 kHz

Abstract: A: Several upgrades have been applied to the high-repetition-rate Thomson scattering diagnostic on the MST experiment, having increased the rate and number of electron temperature measurements. The detector portion of the Thomson scattering system requires 1.5-2.0 J, 10-20 ns laser pulses at 1064 nm. A high-repetition-rate laser produces suitable pulses for short 3-4 pulse bursts with only 3 µs pulse spacing. Alternatively, the laser timing can be optimized to maximize the number of pulses in a single burst, p… Show more

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Cited by 2 publications
(2 citation statements)
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“…A two-dimensional view of the T e structure is captured in a single discharge for the first time in an RFP by the new high-repetition-rate Thomson scattering (TS) laser. [25][26][27] We demonstrate that peaked island-shaped T e structures do not necessarily imply remnant islands in which closed flux surfaces fill the majority of the island volume.…”
Section: Introductionmentioning
confidence: 80%
“…A two-dimensional view of the T e structure is captured in a single discharge for the first time in an RFP by the new high-repetition-rate Thomson scattering (TS) laser. [25][26][27] We demonstrate that peaked island-shaped T e structures do not necessarily imply remnant islands in which closed flux surfaces fill the majority of the island volume.…”
Section: Introductionmentioning
confidence: 80%
“…About a decade ago we built a pulse-burst laser system that produced acceptable 100 kHz bursts, and could be operated up to 333 kHz with substantial pulse energy variation during the burst [10]. This laser system was overly complex and had compromises that made it impractical to further improve and to continue operation long term.…”
Section: Jinst 18 C10023mentioning
confidence: 99%