By means of tight-binding molecular dynamics simulations we find that the g
round-state atomic structure of a typical high-energy grain boundary in dia
mond is highly disordered with a large fraction of sp(2) bonded atoms. This
structure gives rise to localised bands within the band gap. We describe h
ow multiphonon assisted hopping conduction can arise from such electronic s
tates in high-energy grain boundaries, giving in turn a basis for the exper
imentally observed conductivity and electron field emission in nanocrystall
ine diamond. Simulated electron-energy-loss spectra indicate correlations b
etween the disordered atomic structure and features of the electronic struc
ture.