Journal
NATURE NANOTECHNOLOGY
Volume 10, Issue 12, Pages 1033-1038Publisher
NATURE PUBLISHING GROUP
DOI: 10.1038/NNANO.2015.216
Keywords
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Funding
- Sandia's Laboratory Directed Research and Development program
- US Department of Defense
- US Department of Energy's National Nuclear Security Administration [DE-AC04-94AL85000]
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Direct rectification of electromagnetic radiation is a well-established method for wireless power conversion in the microwave region of the spectrum, for which conversion efficiencies in excess of 84% have been demonstrated(1-6). Scaling to the infrared or optical part of the spectrum requires ultrafast rectification(7-10) that can only be obtained by direct tunnelling(11,12). Many research groups have looked to plasmonics to overcome antenna-scaling limits and to increase the confinement(10,13-21). Recently, surface plasmons on heavily doped Si surfaces were investigated as a way of extending surface-mode confinement to the thermal infrared region(22). Here we combine a nanostructured metallic surface with a heavily doped Si infrared-reflective ground plane designed to confine infrared radiation in an active electronic direct-conversion device. The interplay of strong infrared photon-phonon coupling and electromagnetic confinement in nanoscale devices is demonstrated to have a large impact on ultrafast electronic tunnelling in metal-oxidesemiconductor (MOS) structures. Infrared dispersion of SiO2 near a longitudinal optical (LO) phonon mode gives large transverse-field confinement in a nanometre-scale oxide-tunnel gap as the wavelength-dependent permittivity changes from 1 to 0, which leads to enhanced electromagnetic fields at material interfaces and a rectified displacement current that provides a direct conversion of infrared radiation into electric current. The spectral and electrical signatures of the nanoantenna-coupled tunnel diodes are examined under broadband black-body and quantum-cascade laser (QCL) illumination. In the region near the LO phonon resonance, we obtained a measured photoresponsivity of 2.7 mAW(-1) cm(-2) at -0.1 V.
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