Abstract

The Karlsruhe Tritium Neutrino Experiment (KATRIN) will measure the mass of the electron antineutrino with a sensitivity of 0.2 eV / c 2 , based on the precise measurement of the T 2 β spectrum in a region close to the endpoint. This requires a T 2 source, which can provide 10 11 β decay electrons per second. The KATRIN source cryostat consists in its centre of a 10 m long beam tube of 90 mm inner diameter, operated at 30 K. Molecular T 2 is injected in the beam tube through a central injection chamber and pumped at either tube end. The T 2 density profile must have a stability of 10 - 3 in order to limit the systematic errors, yielding stringent requirements on the beam tube temperature homogeneity and stability of ± 30 mK . This shall be achieved with a design, where the thermal radiation from the vacuum pumps is almost entirely absorbed by LN 2 and He heat exchangers on the pump ports. The beam tube itself is cooled with two-phase tubes that are part of a Ne thermosiphon. After describing the thermal environment of the beam tube, the design parameters and the operational limits of the thermosiphon will be discussed. This is followed by a detailed analysis of its dynamic behaviour, based on experimental data taken in the primary He cooling system. A “tailor-made” Ne condenser design is presented, enabling the suppression of the primary He temperature variations by two orders of magnitude, from c. ± 0.3 K to below ± 3 mK .

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