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. 2016 Mar 9;113(12):3164–3168. doi: 10.1073/pnas.1600379113

Fig. 1.

Fig. 1.

(A) SEOP-generated 129Xe and 83Kr spin polarization in mixtures containing 5% noble gas and 95% buffer gas as a function of total SEOP gas pressure. Using H2 as buffer gas, the 129Xe spin polarization (obtained at 378 K) is shown in red filled circles and the 83Kr polarization (obtained at 440 K) is displayed as blue filled squares. For comparison, previous data from ref. 39 with N2 as buffer gas is shown for 129Xe SEOP at 378 K (green open circles) and for 83Kr SEOP at 433 K (green open squares). In contrast, CH4 is an inefficient buffer gas that led to low spin polarization (orange open triangles, taken from ref. 54). (B) The D2 fluorescence at 780 nm (in arbitrary units, a.u.) measured at the front of the cell during SEOP indicates that sufficient radiation quenching with H2 at 378 K (red circles) and at 433 K (blue squares) requires pressures above 50 kPa. Using N2 (green open circles), the D2 radiation is efficiently quenched at pressures above ∼5 kPa. Inset (i) shows the high D2 fluorescence measured for Xe SOEP at 378 K with methane that is a very ineffective quenching gas.