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. 2011 Jan;208(1-19):58–69. doi: 10.1016/j.jmr.2010.10.004

Fig. 3.

Fig. 3

Thermal equilibrium polarization P of spin active noble gas isotopes and a fictitious Kr isotope with spin I = 3/2 obtained from Eq. (A2). (A) Thermal equilibrium polarization curves as a function of temperature displayed at temperatures up to 0.05 K. (B) Semi-logarithmic plot of thermal equilibrium polarization curves as a function of temperature extended out to 3 K. To reach 1% polarization for hyperpolarized samples at 300 K and 9.4 T, the following enhancements are needed when compared to thermally polarized samples for each nuclei: 410 for 3He; 1121 for 129Xe; 2373 for 21Ne; 2206 for 83Kr; 2270 for 131Xe; and 4855 for the fictitious isotope with spin I = 3/2 and the same gyromagnetic ratio as 83Kr. For the three quadrupolar isotopes (21Ne, 83Kr, 131Xe) nearly identical polarization curves arise.