We demonstrate room-temperature C hyperpolarization by dynamic nuclear polarization(DNP) using optically polarized triplet electron spins in two polycrystalline systems: pentacene-doped [carboxyl-C] benzoic acid and microdiamonds containing nitrogen-vacancy (NV) centers. For both samples, the integrated solid effect (ISE) is used to polarize the C spin system in magnetic fields of 350-400 mT. In the benzoic acid sample, the C spin polarization is enhanced by up to 0.12 % through direct electron-to-C polarization transfer without performing dynamic H polarization followed by cross-polarization. In addition, the ISE has been successfully applied to polarize naturally abundant C spins in a microdiamond sample to 0.01 %. To characterize the buildup of the C polarization, we discuss the efficiencies of direct polarization transfer between the electron and C spins as well as that of spin diffusion, examining various parameters which are beneficial or detrimental for successful bulk dynamic C polarization.
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