A general transport equation for the center of mass motion is constructed to study transports of an electronic system under uniform magnetic field and microwave radiation. The equation is applied to study the twodimensional ͑2D͒ electron system in the limit of weak disorder where negative resistance instability is observed when the radiation field is strong enough. A solution of the transport equation with spontaneous ac is proposed to explain the experimentally observed radiation-induced zero-resistance state. DOI: 10.1103/PhysRevB.72.235333 PACS number͑s͒: 73.40.Ϫc, 73.50.Ϫh, 78.67.Ϫn The discovery of the zero-resistance states ͑ZRS͒ in two dimensional electron gas under uniform magnetic field 1,2 and microwave radiation has triggered a lot of theoretical [3][4][5][6][7][8][9]12 and experimental activities 10,11 to understand the origin of this nontrivial state. Most of the theoretical work suggests that the origin of the ZRS is closely related to a negativeresistance instability that occurs in the system due to the combined effect of quantized Landau levels and photonassisted scattering. [3][4][5][6][7]12 It was proposed that the ZRS can be explained if the current-dependent resistance of the system which becomes negative at small current ͑for strong enough microwave radiation͒ becomes positive again when the current j ជ becomes large enough. [3][4][5][6][7] The above physics was put together phenomenologically into an equationwhere R͓j͔ is a phenomenological current-dependent resistance which is negative at j = 0, increases as a function of j and passes through zero at ͉j ជ ͉ = j o , 7 E ជ d is the applied dc electric field and H is the ordinary Hall resistivity. It was suggested that Eq. ͑1͒ admits a time-independent, stripelike spatially inhomogeneous solution which leads to zero differential resistance for net dc current less than a threshold value.7 An obvious theoretical question is whether Eq. ͑1͒ with the required property of R͓j͔ can be derived microscopically. This is the subject of this paper.Starting from first principles we shall derive in the following a transport equation for the center of mass velocity v ជ = j ជ / ne that treats the effect of radiation to all order with the only expansion parameter in the problem being the strength of disorder. Our approach is very similar to the approach adopted by Lei et al. 4 although the final result is different because of the different approximations involved. We note that a transport equation can also be derived from a quantum Boltzmann equation approach. 12 However, it is difficult to obtain a clear analytical result in this approach because of the intrinsic complexity of the Boltzmann equation formulation itself and the equation of motion for the center of mass offers a much simpler alternative. 4 We find that the equation of motion we derive differs from Eq. ͑1͒ in one important aspect which leads to an alternative solution which can also explain the ZRS.
I. DERIVATION OF THE TRANSPORT EQUATIONOur approach to the transport equation begins from ...