Abstract

A hyperpolarized helium-3 (<sup>3</sup>He) has been researched extensively for application in fields such as polarization analysis, <sup>3</sup>He spin filtration for n (p, d) &gamma;, and medical imaging. In the medical field, nuclear magnetic resonant imaging (MRI) using hyperpolarized gas is attracted recently because air space in human lungs can be monitored in detail by aspirating polarized gas. There are two methods of producing hyperpolarized <sup>3</sup>He gas: spin-exchange optical pumping (SEOP) and metastability exchange optical pumping (MEOP). It is well known that the way of making polarization by the MEOP method is more shortly and more directly. In this study, however, the metastable <sup>3</sup>He atoms provided by hollow cathode discharge are polarized by circularly polarized light. When <sup>3</sup>He atoms pumped optically, the 2<sup>3</sup>S-2<sup>3</sup>P transition at the wavelength of 1083nm is leveraged typically. The <sup>3</sup>He atom actually has the optical transition 2<sup>3</sup>S&rarr; 2<sup>3</sup>P at 389nm, but the transition has never been used. Therefore, we developed the 389-nm coherent light source to polarize <sup>3</sup>He gas by MEOP method. This light source utilized the second harmonic generation (SHG) of continuous-wave Ti:sapphire laser operating at a wavelength of 778nm based on BiB<sub>3</sub>O<sub>6</sub> (BiBO) in an external cavity.

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