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We set up a general microscopic theory for the transfer of energy, momentum, and angular momentum mediated by photons among arbitrary objects in vacuum together with the environment at infinity. Using the nonequilibrium Greens function for the electromagnetic field and the self energies (polarizability) representing the properties of materials, we derive Meir-Wingreen type formulas for the energy emitted, force, and torque experienced by the objects in a unified formalism. The theory is applied to transport problems of graphene edges under nonequilibrium conditions. We find that the energy radiation of graphene obeys the $T^4$ law with an emissivity of 2.058$%$ that is consistent with both theoretical and experimental work. To generate momentum and angular momentum radiation, potential bias is needed. The observed effects go beyond the predictions of fluctuational electrodynamics.
In condensed matter systems it is necessary to distinguish between the momentum of the constituents of the system and the pseudomomentum of quasiparticles. The same distinction is also valid for angular momentum and pseudoangular momentum. Based on N
Phonon modes in crystals can have angular momenta in general. It nevertheless cancels in equilibrium when the time-reversal symmetry is preserved. In this paper we show that when a temperature gradient is applied and heat current flows in the crystal
Transport of angular momentum is a long-standing problem in stellar physics which recently became more acute thanks to the observations of the space-borne mission emph{Kepler}. Indeed, the need for an efficient mechanism able to explain the rotation
Pseudospin, an additional degree of freedom inherent in graphene, plays a key role in understanding many fundamental phenomena such as the anomalous quantum Hall effect, electron chirality and Klein paradox. Unlike the electron spin, the pseudospin w
So far experimental confirmation of entanglement has been restricted to qubits, i.e. two-state quantum systems including recent realization of three- and four-qubit entanglements. Yet, an ever increasing body of theoretical work calls for entanglemen