Optical-Cavity-Induced Current

The formation of a submicron optical cavity on one side of a metal–insulator–metal (MIM) tunneling device induces a measurable electrical current between the two metal layers with no applied voltage. Reducing the cavity thickness increases the measured current. Eight types of tests were carried out to determine whether the output could be due to experimental artifacts. All gave negative results, supporting the conclusion that the observed electrical output is genuinely produced by the device. We interpret the results as being due to the suppression of vacuum optical modes by the optical cavity on one side of the MIM device, which upsets a balance in the injection of electrons excited by zero-point fluctuations. This interpretation is in accord with observed changes in the electrical output as other device parameters are varied. A feature of the MIM devices is their femtosecond-fast transport and scattering times for hot charge carriers. The fast capture in these devices is consistent with a model in which an energy ∆E may be accessed from zero-point fluctuations for a time ∆t, following a ∆E∆t uncertainty-principle-like relation governing the process.

[1]  M. Soljačić,et al.  Light emission based on nanophotonic vacuum forces , 2019, Nature Physics.

[2]  Artur R. Davoyan,et al.  Quantifying the role of surface plasmon excitation and hot carrier transport in plasmonic devices , 2017, Nature Communications.

[3]  D. Gall Electron mean free path in elemental metals , 2016 .

[4]  D. Lynch,et al.  Handbook of Optical Constants of Solids , 1985 .

[5]  H. Rothuizen,et al.  Nanometer thin-film Ni-NiO-Ni diodes for detection and mixing of 30 THz radiation , 1998 .

[6]  P. H. Cutler,et al.  Mechanisms of current rectification in an STM tunnel junction and the measurement of an operational tunneling time , 1989 .

[7]  John G. Simmons,et al.  Potential Barriers and Emission‐Limited Current Flow Between Closely Spaced Parallel Metal Electrodes , 1964 .

[8]  J. Simmons Generalized Formula for the Electric Tunnel Effect between Similar Electrodes Separated by a Thin Insulating Film , 1963 .

[9]  G. Moddel,et al.  Casimir-cavity-induced conductance changes , 2021 .

[10]  G. Moddel,et al.  Responsivity–Resistance Relationship in MIIM Diodes , 2018, IEEE Journal of Photovoltaics.

[11]  Sachit Grover,et al.  Engineering the current-voltage characteristics of metal-insulator-metal diodes using double-insulator tunnel barriers , 2012 .

[12]  D. Roberts,et al.  On the attraction between two perfectly conducting plates , 2011 .

[13]  S. Lamoreaux DEMONSTRATION OF THE CASIMIR FORCE IN THE 0.6 TO 6 MU M RANGE , 1997 .

[14]  L. M. Woods,et al.  Perspective on Some Recent and Future Developments in Casimir Interactions , 2020, Applied Sciences.

[15]  Y. Kusaka,et al.  Palladium , 2022, Handbook on the Toxicology of Metals.

[16]  M. Fischetti,et al.  Ballistic hot-electron transistors , 1990 .

[17]  Ford Constraints on negative-energy fluxes. , 1991, Physical review. D, Particles and fields.

[18]  G. Moddel,et al.  Nonstoichiometric Nanolayered Ni/NiO/Al2O3/CrAu Metal–Insulator–Metal Infrared Rectenna , 2021 .

[19]  Ali Javan,et al.  The MOM tunneling diode - Theoretical estimate of its performance at microwave and infrared frequencies , 1978 .

[20]  J. Kadlec,et al.  Results and problems of internal photoemission in sandwich structures , 1976 .

[21]  A. Tkatchenko,et al.  Materials perspective on Casimir and van der Waals interactions , 2015, 1509.03338.

[22]  Frank R Libsch,et al.  Ni-NiO-Ni tunnel junctions for terahertz and infrared detection. , 2005, Applied optics.

[23]  Willis E. Lamb,et al.  Fine Structure of the Hydrogen Atom by a Microwave Method , 1947 .

[24]  E. Knoesel,et al.  Ultrafast dynamics of hot electrons and holes in copper: Excitation, energy relaxation, and transport effects , 1998 .

[25]  E. Cartier,et al.  Hot electron transport through metal–oxide–semiconductor structures studied by ballistic electron emission spectroscopy , 1995 .

[26]  Detection of negative energy: 4-dimensional examples , 2002, gr-qc/0203003.

[27]  A. Lambrecht,et al.  Role of surface plasmons in the Casimir effect , 2007, 0706.1184.

[28]  Cole,et al.  Extracting energy and heat from the vacuum. , 1993, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[29]  G. Moddel,et al.  Demonstration of distributed capacitance compensation in a metal-insulator-metal infrared rectenna incorporating a traveling-wave diode , 2019, Journal of Applied Physics.

[30]  The Casimir force for passive mirrors , 1997, quant-ph/9801055.

[31]  D. Diesing,et al.  Photo and particle induced transport of excited carriers in thin film tunnel junctions , 2007 .

[32]  Testing a Quantum Inequality with a Meta-analysis of Data for Squeezed Light , 2018, Foundations of Physics.

[33]  Mark L Brongersma,et al.  Hot-electron photodetection with a plasmonic nanostripe antenna. , 2014, Nano letters.

[34]  Peter W. Milonni,et al.  The Quantum Vacuum: An Introduction to Quantum Electrodynamics , 1993 .

[35]  D. E. Anderson,et al.  Hot‐Electron Transfer through Thin‐Film Al–Al2O3 Triodes , 1966 .