Molecular electronics is an emerging field associated with computing and data storage utilizing energy transfer at the molecular scale. At this scale, thermal energy is associated exclusively with the vibration of molecular chains. The primary resistance to energy transfer in these proposed devices is the contact resistance at metal-molecule interfaces. To measure the contact resistance, individual molecules are self-assembled in a regular pattern onto a very thin gold substrate. The substrate is suddenly heated by a short pulse of laser irradiation, simultaneously transferring thermal energy to the molecules. The molecules vibrate rapidly in their “hot” state, and their vibrational intensity can be measured by detecting the randomness of the electric field produced by the molecule tips, as indicated by the dashed, circular lines in the schematic.

Molecules that are of density p = 180 kg/m³ and specific heat c_p = 3000 J/kg · K have an initial, relaxed length of L = 2 nm. The intensity of the molecular vibration increases exponentially from an initial value of I_i to a steady-state value of I_ss  > I_i  with the time constant associated with the exponential response being τ_I = 5 ps. Assuming the intensity of the molecular vibration represents temperature on the molecular scale and that each molecule can be viewed as a cylinder of initial length L and cross-sectional area A_c, determine the thermal contact resistance, R"_t.c, at the metal–molecule interface.

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Gold substrate ------ 13:3=== 3:37 Slowly vibrating molecules dadadada dadadada dadadada oooooooo doogoooo | | Initial, cool state 11 Laser irradiation Rapidly vibrating molecules Jobord agogjall Dolby Hot state Metal-molecule interface Randomly vibrating electric field