Abstract. We consider electrical transport properties of a molecular wire under the influence of time-dependent electromagnetic fields. A formalism based on Floquet theory is derived which allows one to calculate both the dc current through the molecular wire and the associated noise power. Approximations for the case of a weak wire-lead coupling are studied in detail.
IntroductionOwing to the recent experimental progress in the fabrication and characterisation of nanostructures involving single or a few molecules, the research field of molecular electronics currently enjoys a vivid activity, as exemplified by the present volume. Thereby, the main focus has been put on contacting single molecules by nanoelectrodes. This allows one to apply a transport voltage and to measure the resulting electrical current [1][2][3][4][5][6][7][8]. For the corresponding theoretical investigations, two lines of research are presently followed. The one is the ab-initio computation of the orbitals relevant for the motion of excess charges through the molecular wire [9-12], as described in Chaps. 3-6. The other line employs rather universal models to gain a qualitative understanding of the transport mechanisms involved [13][14][15][16][17][18][19]. Two particular problems addressed within model calculations are the conduction mechanism in the presence of electron-phonon coupling [14] and the length dependence of the current-voltage characteristics [13,17]. The present work also employs rather general models: We describe the molecules by a linear arrangement of tight-binding levels with the terminating sites attached to leads.Typical energy scales of molecules lie in the infrared regime where most of today's lasers work. Hence, lasers represent a natural possibility to excite the electrons of the molecular wire and, thus, to study the corresponding changes of the conduction properties [20]. One particular question in this context is the influence of excitations by electromagnetic fields and oscillatory gate voltages on the electron transport. Such excitations bear intriguing phenomena like photon-assisted electron tunnelling [21][22][23] and quantum ratchet effects [24,25]. From a fundamental point of view, these effects are of interest because the external fields enable selective electron excitations and allow one to study their interplay with the underlying transport mechanism. In prac-