Title of article
Performance of the COMPASS polarized target dilution refrigerator
Author/Authors
Doshita، نويسنده , , N. and Ball، نويسنده , , J. and Baum، نويسنده , , G. and Berglund، نويسنده , , P. and Gautheron، نويسنده , , F. and Goertz، نويسنده , , St. and Gustafsson، نويسنده , , K. and Hasegawa، نويسنده , , Van T. and Horikawa، نويسنده , , N. and Ishimoto، نويسنده , , S. and Iwata، نويسنده , , T. and Kisselev، نويسنده , , Y. and Koivuniemi، نويسنده , , Helen J. and Kondo، نويسنده , , K. and Matsuda، نويسنده , , T. and Meyer، نويسنده , , W. an، نويسنده ,
Pages
6
From page
138
To page
143
Abstract
The dynamic nuclear polarization (DNP) of 6LiD requires 1 mW/g or more microwave power in the beginning of the process. With the material of 350 g, this gives more than 350 mW in total for the COMPASS polarized target. A temperature around 300 mK or below is needed for an efficient polarization. These low temperatures can only be achieved with a dilution refrigerator designed to operate with a 3He flow of 100 mmol/s. In order to keep the polarization in the frozen mode, temperatures of about 65 mK are used with typical magnetic relaxation times of more than 1400 h at 0.42 T and of more than 15 000 h at 2.5 T. Low lattice temperature is important in achieving high nuclear polarization. The base temperature is limited by the heat brought to the mixing chamber by the inlet 3He and by radiation and conduction of heat.
Keywords
Polarized target , Dilution refrigerator , COMPASS , Cooling power
Journal title
Astroparticle Physics
Record number
2023682
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