| Article ID | Journal | Published Year | Pages | File Type |
|---|---|---|---|---|
| 1593298 | Solid State Communications | 2011 | 7 Pages |
The origin of the singular diamagnetic susceptibility at the Dirac point is probed through the study of effects of band-gap opening and spatially varying magnetic field. In the presence of a band gap, the susceptibility is nonzero only inside the band gap and exhibits a discrete jump at the band edges down to zero in the conduction and valence bands. The jump height is understood in terms of the pseudo-spin paramagnetism arising from valley degree of freedom. In spatially varying magnetic field with wave vector qq, the susceptibility becomes nonzero only in a finite energy region containing the Dirac point, determined by qq. This behavior is understood in terms of electronic states numerically calculated in periodic magnetic field.
► We study the origin of singular diamagnetism of graphene. ► The susceptibility is calculated for graphene with band gap. ► The singular diamagnetism is understood in terms of valley pseudo-spin paramagnetism. ► The susceptibility is calculated for graphene with space-dependent magnetic field.
