1986
DOI: 10.6028/jres.091.027
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Room Temperature Gold-Vacuum-Gold Tunneling Experiments

Abstract: Preface Number 4An experiment has been completed which demonstrated quantum mechanical tunneling of electrons between two gold electrodes separated in vacuum. The tunneling current between the gold electrodes has been measured, for fixed voltages of 0.1 and 0.01 volts, as the electrode spacing was varied from a distance of approximately 2.0 nm down to a point where the electrodes touched. Current changes of over five orders of magnitude were found for electrode spacing changes of approximately 1.2 nm. For the … Show more

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Cited by 68 publications
(19 citation statements)
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“…It is important to note that the Fowler-Nordheim slope does not measure the height of the tunneling barrier, usually described as the work function (), but is strongly dependent on it-going as 3/2 for a simple Sommerfeld metal 9 as opposed to 1/2 for the tunneling barrier probed by the STM. 11 Since the tunneling current depends both on the local tunneling probability and on the supply of tunneling electrons ͑i.e., the LDOS͒, 12 the patterns observed in tunneling electron microscope images arise from an interplay of these two factors. However, the Fowler-Nordheim slope is a derivative of the current-voltage characteristic and essentially independent of the magnitude of the tunneling current.…”
Section: Methodsmentioning
confidence: 99%
“…It is important to note that the Fowler-Nordheim slope does not measure the height of the tunneling barrier, usually described as the work function (), but is strongly dependent on it-going as 3/2 for a simple Sommerfeld metal 9 as opposed to 1/2 for the tunneling barrier probed by the STM. 11 Since the tunneling current depends both on the local tunneling probability and on the supply of tunneling electrons ͑i.e., the LDOS͒, 12 the patterns observed in tunneling electron microscope images arise from an interplay of these two factors. However, the Fowler-Nordheim slope is a derivative of the current-voltage characteristic and essentially independent of the magnitude of the tunneling current.…”
Section: Methodsmentioning
confidence: 99%
“…We studied the graphite -tungsten system because it has been the subject of many high resolution STM investigations [17,18], including some which have obtained atomic resolution in air [18]. There is good evidence that 1arge forces between the tip and sample [19] may play a role in forming the STM image for the tungsten-graphite [20] and tungsten-si1ver [4] systems.…”
Section: Resultsmentioning
confidence: 99%
“…The height and the width of a potential barrier between the electrodes which an electron must overcome are controlled by the physical parameters, particularly interelectrode separation (d) and the work function of the electrodes (φ e and φ c for the emitting and collecting electrodes) [2][3][4][5][6], with both the engineering of low work-functions and uniform nano-meter separations over relatively large areas being simultaneous challenges to overcome. Recent advances in work function reduction of semiconductor surfaces, particularly of diamond [11,12], and in parallel, the fabrication of nano-scale vacuum gap [8][9][10]13] show that fabrication of such free-standing structures will be possible in near future. By applying a thermal gradient across the ultra-thin (a few nm) vacuum gap of a tunnel device, a large unidirectional flux of thermionic and thermo-tunnel currents between an emitter and collector, and a thermal potential difference can be achieved.…”
Section: Introductionmentioning
confidence: 98%
“…Thermionic energy-conversion is of particular interest because of the potential of providing relatively efficient thermalenergy conversion in comparison to commonly used techniques, such as thermoelectric and thermophotovoltaic conversion [1]. Recently, combined thermionic emission and tunneling of hot electrons (thermo-tunneling) has come to the fore, capable of providing very high output power-densities via a nano-scale, vacuum-spaced thermo-tunnel device [2][3][4][5][6][7][8][9][10]. The height and the width of a potential barrier between the electrodes which an electron must overcome are controlled by the physical parameters, particularly interelectrode separation (d) and the work function of the electrodes (φ e and φ c for the emitting and collecting electrodes) [2][3][4][5][6], with both the engineering of low work-functions and uniform nano-meter separations over relatively large areas being simultaneous challenges to overcome.…”
Section: Introductionmentioning
confidence: 99%