Design and preliminary operation of a laser absorption diagnostic for the SPIDER RF source

TL;DR

This paper presents the design and initial testing of a laser absorption diagnostic for measuring cesium density in the SPIDER RF negative ion source, aiding the development of ITER's neutral beam injectors.

Contribution

It introduces a novel laser absorption diagnostic setup for Cs density measurement in the SPIDER source, including design details and preliminary experimental results.

Findings

Diagnostic successfully measures Cs ground state density

Ground state depopulation affects measurements and is partially corrected

First experimental results demonstrate feasibility of the diagnostic

Abstract

The ITER Heating Neutral Beam (HNB) injector is required to deliver 16.7 MW power into the plasma from a neutralised beam of H-/D- negative ions, produced by an RF source and accelerated up to 1 MeV. To enhance the H-/D- production, the surface of the acceleration system grid facing the source (the plasma grid) will be coated with Cs because of its low work function. Cs will be routinely evaporated in the source by means of specific ovens. Monitoring the evaporation rate and the distribution of Cs inside the source is fundamental to get the desired performances on the ITER HNB. In order to proper design the source of the ITER HNB and to identify the best operation practices for it, the prototype RF negative ion source SPIDER has been developed and built in the Neutral Beam Test Facility at Consorzio RFX. A Laser Absorption Spectroscopy diagnostic will be installed in SPIDER for a quantitative estimation of Cs density. By using a wavelength tunable laser, the diagnostic will measure the absorption spectrum of the 852 nm line along 4 lines of sight, parallel to the plasma grid surface and close to it. From the absorption spectra the line-integrated density of Cs at ground state will be measured. The design of this diagnostic for SPIDER is presented, with details of the layout and of the key components. A preliminary installation of the diagnostic on the test stand for Cs ovens is also described, together with its first experimental results; the effect of ground state depopulation on collected measurements is discussed and partially corrected.