Nanodiamonds containing nitrogen vacancy (NV -) centers show promise for a number of emerging applications including targeted in vivo imaging and generating nuclear spin hyperpolarization for enhanced NMR spectroscopy and imaging. Here, we develop a detailed understanding of the magnetic resonance behavior of NVcenters in an ensemble of nanodiamonds with random crystal orientations. Two-dimensional optically detected magnetic resonance spectroscopy reveals the distribution of energy levels, spin populations, and transition probabilities that give rise to a complex spectrum. We identify overtone transitions that are inherently insensitive to crystal orientation and give well-defined transition frequencies that access the entire nanodiamond ensemble. These transitions may be harnessed for high-resolution imaging and generation of nuclear spin hyperpolarization. The data are well described by numerical simulations from the zero-to high-field regimes, including the intermediate regime of maximum complexity. We evaluate the prospects of nanodiamond ensembles specifically for nuclear spin hyperpolarization and show that frequency-swept dynamic nuclear polarization may transfer a large amount of the NVcenter's hyperpolarization to nuclear spins by sweeping over a small region of its spin spectrum.The nitrogen vacancy (NV -) center in diamond, with its stable fluorescence, spin-1 ground state and optical spin polarization and readout, enables many emerging applications such as high spatial resolution sensing and magnetic resonance 1-9 , solid-state qubits 10-12 , and nuclear spin hyperpolarization [13][14][15][16][17][18][19][20][21][22][23] . In particular, biocompatible nanodiamonds are of interest for in vivo applications such as fluorescence-detected biomedical imaging 24,25 and as magnetic resonance contrast agents 26,27 . Owing to their high surface area, nanodiamonds have also been proposed as a general source for nuclear spin hyperpolarization transfer to target molecules for magnetic resonance signal enhancement 18,20 . All of these applications rely on the ability to access magnetic resonance transitions of the NVcenters. However, since the NVspin properties depend strongly on their orientation with respect to an external magnetic field 28,29 , the use of nanodiamond ensembles poses significant challenges.Neglecting the weak hyperfine interaction with nearby 14 N and the rare 13 C nuclei, the electron spin Hamiltonian of NVcenter is: = % & − ( ) & + , . / sin + % cos ,Where D = 2,870 MHz is zero field splitting, , = 2.8 MHz/G is the electron gyromagnetic ratio, and θ is the angle between the magnetic field and the NVaxis (Figure 1a).