Abstract

We demonstrate that the dynamic nuclear polarization (DNP) of phosphorus donors in silicon can be very effective in a magnetic field of 4.6 T and at temperatures below 1 K. The DNP occurs due to the Overhauser effect following a cross relaxation via the forbidden flip-flop or flip-flip transitions. Nuclear polarization values P>0.98P>0.98 were reached after 20 min of pumping with 0.4 μμW of microwave power. We evaluated that the ratio of hyperfine state populations increased by three orders of magnitude after 2 hours of pumping, and an extremely pure nuclear spin system containing <10−11<10^{-11} of the other spin state can be created. An inverted DNP has been obtained by pumping the low field ESR line of P followed by the flip-flip cross relaxation. This transition has much smaller relaxation rate and required substantially longer pumping times. We found that the nuclear polarization dynamics deviates substantially from a simple exponential function. The evolution of the polarization is characterized by two time constants Tac′≈T^{'}_{ac}\approx15 s in the beginning, and Tac"≈T^{"}_{ac}\approx1100 s for long pumping time. Temperature dependence of the nuclear relaxation rate of 31^{31}P was studied down to 0.75 K, below which the relaxation time became too long to be measured. The nuclear polarization followed a bi-exponential time dependence during relaxation. We suggest that the non-exponential behavior of DNP dynamics and the subsequent relaxation is mediated by the nuclei of 29^{29}Si surrounding 31^{31}P donors, which affect the transition probabilities of the forbidden cross-relaxation processes.

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