Abstract: Systems and methods for generating hyperpolarized target materials are disclosed. The disclosed systems and methods can include hyperpolarizing a compound then transferring polarization to a target material. The compound can be selected to have nuclear spins. The compound can be further selected to have electron spins that, when exposed to certain electromagnetic radiation, exceed a predetermined level of polarization. The compound can be exposed to such electromagnetic radiation, optically hyperpolarizing the electron spins of the compound. Polarization can then be transferred from the electron spins of the compound to nuclear spins of the compound, at least in part by exposing the compound to a magnetic field. The compound can be exposed to the target material before or after pulverizing the compound to increase the surface area of the compound, thereby facilitating transfer of polarization from the compound to the target material.

Abstract: A method for the preparation of a sample comprising highly polarized nuclear spins is proposed, comprising at least the following steps: a) provision of molecules with 1,2-dione structural units and/or molecules with 2,5-diene-1,4-dione structural units in the solid state; b) generation of radicals from these molecules by photo induced electron transfer by a first electromagnetic irradiation in the visible or ultraviolet frequency range in the solid state; c) dynamic nuclear polarization in the presence of a magnetic field in the solid state by applying a second electromagnetic irradiation with a frequency adapted to transfer spin polarization from the electrons to the nuclear spins leading to a highly polarized state thereof. Furthermore uses of correspondingly prepared samples for NMR, MRS and MRI experiments are proposed.

Abstract: A method for the preparation of a sample comprising highly polarized nuclear spins is proposed, comprising at least the following steps: a) provision of molecules with 1,2-dione structural units and/or molecules with 2,5-diene-1,4-dione structural units in the solid state; b) generation of radicals from these molecules by photo induced electron transfer by a first electromagnetic irradiation in the visible or ultraviolet frequency range in the solid state; c) dynamic nuclear polarization in the presence of a magnetic field in the solid state by applying a second electromagnetic irradiation with a frequency adapted to transfer spin polarization from the electrons to the nuclear spins leading to a highly polarized state thereof. Furthermore uses of correspondingly prepared samples for NMR, MRS and MRI experiments are proposed.