We have observed that the bulk proton dipolar reservoir is cooled to a spin temperature of 15.50.3em0exμK in a dynamic nuclear polarization (DNP) experiment, following microwave irradiation for 8000.3em0exs. This is significantly cooler than the 350.3em0exmK spin temperature of the proton Zeeman reservoir following DNP. Equilibration of the two reservoirs results in a 50% increase in the NMR signal intensity, corresponding to a proton Zeeman spin temperature of 230.3em0exmK. In order to achieve this polarization directly, it was necessary to irradiate the sample with microwaves for 15000.3em0exs. The experiment was performed on a 400.3em0exmM solution of 4-amino-TEMPO in a 40:60 water/glycerol mixture. Cooling of the dipolar reservoir occurs during polarization transport through the magnetic field gradient around the paramagnetic impurity, and is rapidly communicated to the bulk by dipolar spin diffusion. As dipolar spin diffusion is significantly faster than Zeeman spin diffusion, the bulk dipolar reservoir cools faster than the Zeeman reservoir. This process can be exploited to rapidly polarize the nuclear spins, by repeatedly cooling the dipolar system and transferring the polarization to the Zeeman reservoir.
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Dementyev et al. (2008) studied this question.
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