CA2137013A1 - Nanoelectric devices - Google Patents
Nanoelectric devicesInfo
- Publication number
- CA2137013A1 CA2137013A1 CA002137013A CA2137013A CA2137013A1 CA 2137013 A1 CA2137013 A1 CA 2137013A1 CA 002137013 A CA002137013 A CA 002137013A CA 2137013 A CA2137013 A CA 2137013A CA 2137013 A1 CA2137013 A1 CA 2137013A1
- Authority
- CA
- Canada
- Prior art keywords
- metal
- nanowire
- pores
- substrate
- oxide
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
- 229910052751 metal Inorganic materials 0.000 claims abstract description 85
- 239000002184 metal Substances 0.000 claims abstract description 85
- 239000011148 porous material Substances 0.000 claims abstract description 71
- 239000000758 substrate Substances 0.000 claims abstract description 64
- 239000002070 nanowire Substances 0.000 claims abstract description 46
- 239000004020 conductor Substances 0.000 claims abstract description 33
- 239000002253 acid Substances 0.000 claims abstract description 18
- 238000007743 anodising Methods 0.000 claims abstract description 17
- 239000011888 foil Substances 0.000 claims abstract description 9
- 238000000034 method Methods 0.000 claims description 30
- 230000008569 process Effects 0.000 claims description 20
- 238000000151 deposition Methods 0.000 claims description 17
- 229910052782 aluminium Inorganic materials 0.000 claims description 9
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 9
- 239000000126 substance Substances 0.000 claims description 9
- 229910044991 metal oxide Inorganic materials 0.000 claims description 8
- 150000004706 metal oxides Chemical class 0.000 claims description 7
- 150000002739 metals Chemical class 0.000 claims description 6
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 claims description 4
- 229910052758 niobium Inorganic materials 0.000 claims description 4
- 239000010955 niobium Substances 0.000 claims description 4
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 claims description 4
- 229910052719 titanium Inorganic materials 0.000 claims description 4
- 239000010936 titanium Substances 0.000 claims description 4
- 229910052715 tantalum Inorganic materials 0.000 claims description 3
- GUVRBAGPIYLISA-UHFFFAOYSA-N tantalum atom Chemical compound [Ta] GUVRBAGPIYLISA-UHFFFAOYSA-N 0.000 claims description 3
- 229910045601 alloy Inorganic materials 0.000 claims description 2
- 239000000956 alloy Substances 0.000 claims description 2
- 238000006243 chemical reaction Methods 0.000 claims description 2
- 230000000694 effects Effects 0.000 abstract description 12
- 238000003491 array Methods 0.000 abstract description 3
- 239000010410 layer Substances 0.000 description 81
- 230000004888 barrier function Effects 0.000 description 40
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 20
- 230000008021 deposition Effects 0.000 description 11
- 230000003647 oxidation Effects 0.000 description 11
- 238000007254 oxidation reaction Methods 0.000 description 11
- MUBZPKHOEPUJKR-UHFFFAOYSA-N Oxalic acid Chemical compound OC(=O)C(O)=O MUBZPKHOEPUJKR-UHFFFAOYSA-N 0.000 description 9
- NBIIXXVUZAFLBC-UHFFFAOYSA-N Phosphoric acid Chemical compound OP(O)(O)=O NBIIXXVUZAFLBC-UHFFFAOYSA-N 0.000 description 8
- 230000015572 biosynthetic process Effects 0.000 description 7
- 239000003792 electrolyte Substances 0.000 description 7
- 239000000463 material Substances 0.000 description 7
- 229910052759 nickel Inorganic materials 0.000 description 7
- 229910000480 nickel oxide Inorganic materials 0.000 description 7
- GNRSAWUEBMWBQH-UHFFFAOYSA-N oxonickel Chemical compound [Ni]=O GNRSAWUEBMWBQH-UHFFFAOYSA-N 0.000 description 7
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 6
- QAOWNCQODCNURD-UHFFFAOYSA-N Sulfuric acid Chemical compound OS(O)(=O)=O QAOWNCQODCNURD-UHFFFAOYSA-N 0.000 description 6
- 238000005530 etching Methods 0.000 description 6
- 239000011810 insulating material Substances 0.000 description 6
- 229910052709 silver Inorganic materials 0.000 description 5
- 239000004332 silver Substances 0.000 description 5
- CDBYLPFSWZWCQE-UHFFFAOYSA-L Sodium Carbonate Chemical compound [Na+].[Na+].[O-]C([O-])=O CDBYLPFSWZWCQE-UHFFFAOYSA-L 0.000 description 4
- 150000007513 acids Chemical class 0.000 description 4
- 229910000147 aluminium phosphate Inorganic materials 0.000 description 4
- 238000003486 chemical etching Methods 0.000 description 4
- KRVSOGSZCMJSLX-UHFFFAOYSA-L chromic acid Substances O[Cr](O)(=O)=O KRVSOGSZCMJSLX-UHFFFAOYSA-L 0.000 description 4
- AWJWCTOOIBYHON-UHFFFAOYSA-N furo[3,4-b]pyrazine-5,7-dione Chemical compound C1=CN=C2C(=O)OC(=O)C2=N1 AWJWCTOOIBYHON-UHFFFAOYSA-N 0.000 description 4
- 238000002360 preparation method Methods 0.000 description 4
- 229910000838 Al alloy Inorganic materials 0.000 description 3
- PNEYBMLMFCGWSK-UHFFFAOYSA-N Alumina Chemical group [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 3
- YMWUJEATGCHHMB-UHFFFAOYSA-N Dichloromethane Chemical compound ClCCl YMWUJEATGCHHMB-UHFFFAOYSA-N 0.000 description 3
- 238000004140 cleaning Methods 0.000 description 3
- 238000004070 electrodeposition Methods 0.000 description 3
- 238000005868 electrolysis reaction Methods 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 235000006408 oxalic acid Nutrition 0.000 description 3
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 3
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 2
- LFQSCWFLJHTTHZ-UHFFFAOYSA-N Ethanol Chemical compound CCO LFQSCWFLJHTTHZ-UHFFFAOYSA-N 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- GRYLNZFGIOXLOG-UHFFFAOYSA-N Nitric acid Chemical compound O[N+]([O-])=O GRYLNZFGIOXLOG-UHFFFAOYSA-N 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 2
- 238000004364 calculation method Methods 0.000 description 2
- 239000003153 chemical reaction reagent Substances 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 239000010931 gold Substances 0.000 description 2
- 229910002804 graphite Inorganic materials 0.000 description 2
- 239000010439 graphite Substances 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 150000002500 ions Chemical class 0.000 description 2
- 238000006386 neutralization reaction Methods 0.000 description 2
- 229910017604 nitric acid Inorganic materials 0.000 description 2
- 230000001590 oxidative effect Effects 0.000 description 2
- 229910052760 oxygen Inorganic materials 0.000 description 2
- 239000001301 oxygen Substances 0.000 description 2
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 2
- 229910000029 sodium carbonate Inorganic materials 0.000 description 2
- 238000004544 sputter deposition Methods 0.000 description 2
- 239000001117 sulphuric acid Substances 0.000 description 2
- 235000011149 sulphuric acid Nutrition 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- XSTXAVWGXDQKEL-UHFFFAOYSA-N Trichloroethylene Chemical group ClC=C(Cl)Cl XSTXAVWGXDQKEL-UHFFFAOYSA-N 0.000 description 1
- 239000003513 alkali Substances 0.000 description 1
- -1 aluminum Chemical class 0.000 description 1
- 125000000129 anionic group Chemical group 0.000 description 1
- 239000012298 atmosphere Substances 0.000 description 1
- 239000002585 base Substances 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 229910052797 bismuth Inorganic materials 0.000 description 1
- JCXGWMGPZLAOME-UHFFFAOYSA-N bismuth atom Chemical compound [Bi] JCXGWMGPZLAOME-UHFFFAOYSA-N 0.000 description 1
- KGBXLFKZBHKPEV-UHFFFAOYSA-N boric acid Chemical compound OB(O)O KGBXLFKZBHKPEV-UHFFFAOYSA-N 0.000 description 1
- 239000004327 boric acid Substances 0.000 description 1
- 229910052793 cadmium Inorganic materials 0.000 description 1
- BDOSMKKIYDKNTQ-UHFFFAOYSA-N cadmium atom Chemical compound [Cd] BDOSMKKIYDKNTQ-UHFFFAOYSA-N 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 238000001311 chemical methods and process Methods 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 239000012153 distilled water Substances 0.000 description 1
- 238000001493 electron microscopy Methods 0.000 description 1
- 238000006056 electrooxidation reaction Methods 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 238000011049 filling Methods 0.000 description 1
- 239000012467 final product Substances 0.000 description 1
- 239000004519 grease Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 230000002401 inhibitory effect Effects 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000007769 metal material Substances 0.000 description 1
- 239000013528 metallic particle Substances 0.000 description 1
- 230000003472 neutralizing effect Effects 0.000 description 1
- LGQLOGILCSXPEA-UHFFFAOYSA-L nickel sulfate Chemical compound [Ni+2].[O-]S([O-])(=O)=O LGQLOGILCSXPEA-UHFFFAOYSA-L 0.000 description 1
- 229910000363 nickel(II) sulfate Inorganic materials 0.000 description 1
- 239000003960 organic solvent Substances 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000037361 pathway Effects 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 235000011007 phosphoric acid Nutrition 0.000 description 1
- 229910052697 platinum Inorganic materials 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 239000002344 surface layer Substances 0.000 description 1
- UBOXGVDOUJQMTN-UHFFFAOYSA-N trichloroethylene Natural products ClCC(Cl)Cl UBOXGVDOUJQMTN-UHFFFAOYSA-N 0.000 description 1
- 238000004506 ultrasonic cleaning Methods 0.000 description 1
- 238000009834 vaporization Methods 0.000 description 1
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y10/00—Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y30/00—Nanotechnology for materials or surface science, e.g. nanocomposites
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N99/00—Subject matter not provided for in other groups of this subclass
- H10N99/05—Devices based on quantum mechanical effects, e.g. quantum interference devices or metal single-electron transistors
Landscapes
- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Nanotechnology (AREA)
- Physics & Mathematics (AREA)
- Crystallography & Structural Chemistry (AREA)
- Composite Materials (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Materials Engineering (AREA)
- Mathematical Physics (AREA)
- Theoretical Computer Science (AREA)
- Semiconductor Memories (AREA)
Abstract
Single-electron devices useful as diodes, transistors or other electronic components are prepared by anodizing a metal substrate in sheet or foil form electrolytically in an acid bath, to deposit thereon an oxide film having axially disposed micropores of substantially uniform diameter in the range of from about 1 to about 500 nanometres and substantially uniform depth less than the thickness of the oxide film, leaving an ultra thin oxide layer between the bottom of each pore in the metal substrate. The conductive material is deposited in the pores to form nanowires contacting the oxide layer at the bottom of the pores. Macro metal is deposited over the ends of the nanowires for external electrical contact purposes. Devices can be made according to the present invention which are suitable to exhibit single-electron tunnelling effects and arrays of tunnel junction devices can be prepared having a density up to the order of 1010 per square cm.
Description
~370i3 , This invention relates to single-electronics.
More specifically, it relates to single-electron devices useful as diodes and transistors or as other electronic devices, and to chemical processes for their preparation.
A single-electron device, as the term is generally understood, is a device which controls the movement of individual electrons in solids. They commonly take the form of tunnel junctions, consisting of two conductors separated by an ultrathin (less than 100 nanometers) layer of insulating material. When a voltage is applied across the tunnel junction, inducing current (electron movement) to flow in the conductors, a surface charge accumulates on one surface of the conductor against the insulating layer, with an equal and opposite charge on the other insulator/conductor surface. When this surface charge exceeds a predetermined value, an electron tunnels through the insulating layer, thereby reducing the surface charge. When the surface charge is less than the predetermined value, tunnelling is suppressed (the Coulomb blockade). As a surface charge increases due to continued current flow in the conductor, i.e. continued application of the voltage across the insulator, the charge increases again, until the Coulomb blockade is overcome, whereupon another single electron tunnels through. The phenomenon can be observed experimentally, as a fl~n~mpntal relation between applied voltage and the frequency of oscillation in the current flowing through the junction. The height of the Coulomb blockade depends upon the conductance and capacitance of the insulating layer.
A general description of single electronics and single-electron devices and their method of operation appears in "Scientific American", June 1992, page 80, in an article by Likharev and Claeson.
`- 21~701~
These single-electron phenomena show promise for application to digital integrated circuits. Currently computer chips can have a density of about ten million devices per square centimetre, to handle the commonly used digital electrical pulses. Using single electronics, even further reductions in size are possible, since bits of information can be represented through the passage of individual electrons. For this to happen, however, techniques need to be developed to fabricate complex structures whose smallest dimension is, controllably and reproducibly, less than 100 nanometers. Such techniques also need to be capable of operation economically and efficiently, for the production of single-electronic devices incorporating one or more such tunnel junctions.
It is an object of the present invention to provide novel, single-electron devices.
It is a further object of the invention to provide novel processes for making single-electron devices.
In the present invention, single-electron devices are made by a technique of electro deposition. A layer of porous oxide is deposited on the surface of a conductive substrate of a metal selected from aluminum, titanium, niobium and tantalum, by electrolytic anodizing. The pores formed in the oxide layer are of extremely small but very uniform shape, diameter and depth, controllable within close limits by the conditions of anodizing and/or by subsequent chemical etching. These highly uniform, nanometer-sized, densely packed pores are used in the present invention as templates, for the formation therein of conducting or semiconducting materials, to form an active region ("nanowire") of a tunnel junction device.
The insulating layer or layers of the device can be formed by oxidation or other chemical conversion of the or each end portion of the, nanowire. Alternatively, the residual ` 21~7013 oxide layer at the bottom of each pore, separating the pore from the electrically conducting metal substrate, can form an insulating layer, with the metal substrate itself acting as the second conductor separated by this insulating oxide layer from the nanowire which is formed in the pore.
The invention thus takes advantage of the very small but highly uniform and controllable sizes of the pores formed in the oxide layer, by anodizing and if desired by subsequent chemical etching, to make single-electron devices. The pore sizes can be controlled to adiameter of about 90 Angstroms up to several thousand Angstroms, and to a height of several hundred Angstroms to several thousand Angstroms, to give devices with an array of conductor-barrier arrangements of dimensions suitable to exhibit single-electron tunnelling effects. Moreover, the pores and hence the nanowires formed in them can be extremely densely packed, allowing the preparation of arrays of tunnel junction devices, of a density up to the order of 101 per square centimetre.
FIGURE 1 is an idealized illustration of a pores template formed as a part of the process of the invention;
FIGURE 2 is a schematic view of a cross section of a nickel nanowire prepared and studied in the present inventlon;
FIGURE 3 is a diagrammatic cross section of an alternative and preferred embodiment of the present invention.
FIGURE 4 is a voltage-current curve derived from devices according to the present invention as described in Example 2 below.
Devices according the present invention can take ``- 2137013 a variety of different forms, and incorporate one or more insulating barrier layers and correspondingly two or more conductors, at least one of which is a nanowire. The conductive metal substrate may constitute a conductor of the finally produced single-electron device, in which case the metal substrate is chosen from among aluminum, titanium, niobium, tantalum and alloys thereof on the basis of desired electrical properties. In other embodimentsl the conductive metal substrate may be fully removed and replaced during the manufacturing process, and not constitute any part of the final device. In such cases, the initial choice of substrate is dictated by cost and by ease of manufacture, and is preferably all~m;nllm.
Similarly, the insulating metal oxide formed initially on the conductive metal substrate may or may not form one or more of the insulating barrier layers in the final device. This will influence the choice of metal substrate, for similar reasons.
The simplest device according to the present invention, and the device most easily prepared (although not the most preferred embodiment) is one which has a single insulating layer (barrier) comprised of the oxide of the metal substrate, disposed between the metal substrate constituting one conductor, and a nanowire conductor formed in a pore in the oxide layer. Such a device is prepared by cleaning and anodizing the metal substrate, under carefully controlled conditions to provide thereon oxide film with the dense array of uniformly sized pores, the depth of the pores being controlled to leave a suitably thin oxide layer between the pore and the substrate to act as an insulating layer of a single-electron device. Metal, semi-conductor or other conducting material is subsequently deposited in the pores of the oxide layer, to contact the insulating oxide layer. A thin metal film (also referred to macro-metal), for electrical connection purposes, is deposited ~ 5 _ over the nanowire in the pores, and in electrical contacttherewith.
Other single-barrier devices according to the invention can be prepared by the process outlined above, followed by a removal and replacement of one or both of the metal substrate and the residual oxide separating the metal substrate from the pore. This can be effected chemically, by known metal and metal oxide removing techniques, e.g.
chemical etching. After removal of only the metal substrate, another metal can be deposited over the metal oxide insulating barrier layer. After removal of both the metal substrate and the metal oxide insulating barrier layer, another insulating barrier layer can be deposited on one end of the nanowire, e.g. by controlled oxidation or other chemical treatment thereof. Then another conductor, e.g. metal, can be deposited over the newly formed barrier layer, to complete the single barrier device according to the invention.
Double barrier devices according to the invention can be prepared by depositing or oxidizing an insulating barrier layer on the end of the nanowire remote from the metal substrate, followed by deposition of another conductor over this insulating barrier layer, in the case where the original substrate and intervening oxide layer below the pores are left intact to constitute one barrier layer and conductor. In the case where the original substrate and the intervening oxide layer below the pores are both removed, double barrier devices according to the invention can be prepared after their r~ ovdl, by deposition onto, or oxidation of, both ends of the residual nanowire of the insulating barrier layer, e.g. an oxide layer, followed by deposition thereover of conductive layers, e.g. of metal.
In order to constitute single electron devices, 21~7013 the em~bodiments of this invention only need to include one nanowire, and in all embodiments the pores formed in the oxide layers formed on the metal substrates provide the templates for these nanowires. Then one or two barrier layers can be deposited, of a size suitable for exhibiting single electron tunnelling effects, on account of the extremely small sizes of these nanowires, particularly their end surface areas. The uniformity and density of the pores allows the preparation of useful devices with practical applications.
A further, preferred embodiment of the invention is a multiple barrier device having a thin conductive intermediate layer, to which electrical connections can readily be made. This is prepared by initially providing an electrically conductive metal substrate of one of the aforementioned metals, e.g. all~m;n~m~ and providing a microporous oxide coating as previously described, on both sides. If desired, the substrate in this em.bodiment can comprise a conductive core, chosen on the basis of its electrical characteristics for a suitable application, carrying a deposit on both sides of one of the aforementioned metals, e.g. aluminum, this metal layer having a micro porous oxide coating as previously described. Metal can then be deposited in the pores to form nanowires, separated from the metal substrate by residual oxide forming the insulating barrier, on each side, thereby providing a double barrier device. A thin metal film can then be applied over the nanowires at their ends remote from the substrate, for electrical contact purposes, thereby providing a double barrier, three contact device comprising a very large array of nanowire-barrier "pathways", operable in the manner of a transistor.
This embodiment of the invention, utilizing a two sided porous substrate, can be further expanded from a two-barrier device to a three-barrier device or a four-barrier `- 2137~13 device, if desired, by creation of another barrier layer, e.g. by controlled oxidation, on the distal end of one or both of the sets of nanowires protruding from each side of the substrate. In such cases, the metal film is applied over the or each of the barrier layer, to provide electrical contact means.
The metallic substrate used in the process of the present invention, and in one embodiment serving as the conductor contacting the insulating layer, is normally all]m;nl~m or an aluminum alloy in which aluminum is the predominant metal, in foil or sheet form, or as a deposited alllm;nllm film on an inert substrate. A surface layer of alnm;n-lm oxide is deposited thereon, to constitute the insulating layer, by anodizing the metal sheet or foil.
Firstly, the sheet or foil should be cleaned, ultra-sonically and/or with organic solvent to remove grease residues from its surface. Then it is preferably washed with an alkaline chemical liquid so as to achieve a degree of surface etching, followed by neutralization to remove alkali excess. A wide variety of different chemical reagents may be used for these purposes. Sodium carbonate solution is an example of a suitable base with which to effect the etching. Nitric acid is a suitable neutralizing agent for subsequent use. Thus, the preferred cleaning process is ultrasonic cleaning in dichloromethane, followed by treatment with dilute sodium carbonate and then with dilute nitric acid. However, the cleaning process can be conducted with a very wide variety of different reagents.
Electrolytic anodizing of the cleaned sheet or foil, for the purposes of depositing thereon a porous surface of oxide, is suitably accomplished by making the metal the anode of an electrolytic cell, using suitable (e.g. lead) counter-electrodes in an acid bath. Suitably, the bath is a relatively dilute solution of strong acids such as sulfuric acid, phosphoric acid, oxalic acid, or chromic acid. Direct current is passed through the cell between the electrodes, at a current or voltage suitably adjusted to provide the correct film deposition. This can be accomplished at room temperatures.
After suitable anodizing as described, the substrate is removed from the bath and rinsed. It is desirable to rid the surface of the treated substrate of residual acid, and neutralize it at this point. It is, however, undesirable to neutralize the acid chemically, since this might have the effect of damaging the deposited film. Accordingly, it is preferred to rinse the anodized film with suitable quantities of water to remove acid and effect appropriate neutralization.
A substrate so prepared has micro-pores in the oxide surface film, of substantially uniform size in the nanometer size range, and extending substantially perpendicularly from the substrate surface and therefore substantially parallel to one another. At the bottom of each such micropore is a very thin layer of alllm;nllm oxide, an electrical insulating material, separating the body of the pore from the conducting metal alllm;nllm or aluminum alloy substrate. By appropriate means according to the present invention, this pore structure is utilized to provide another conductor, separated from the conducting all~m;mlm or aluminum alloy substrate, by a nanometer-size range thickness of insulating layer to form the principle of the single-electron devices according to the present invention.
In a next step, therefore, an appropriate conductor is applied to the interior of the pores. A
typical example of such a conductor is nickel. Before or after deposition of the metal such as nickel into the pores, the height and size of the pores can be chemically adjusted, by chemical etching. The length of this "column"
21~7013 ' g of deposited metal defined by the size of pore, is not critical, but is typically in the size range from 1-10 microns .
The diameter, the density and the height of the pores is determined to some extent by the choice of acid in the anodizing bath. Suitable acids from which to choose are phosphoric acid, oxalic acid, sulphuric acid and chromic acid. The use of phosphoric acid leads the formation of relatively large pores. The use of oxalic acid or chromic acid leads towards the formation of smaller pores, while the use of sulphuric acid leads the formation of pores of the smallest diameters. The relative concentration of the acid used also has a minor effect on the pore sizes produced, but this effect is of little significance in comparison with that derived from the choice of acid.
Pore density, i.e. the distance between individual pores in the substrate, can be further varied by choosing the DC anodizing voltage appropriately. High anodizing voltages lead to low pore densities, whilst low anodizing voltages tend towards the film with high poor densities. The anodizing voltage has a lesser effect on the individual pore sizes.
After the anodizing process has been completed, the diameters and the depths of the pores can be further adjusted by etching the oxide film with an appropriate acid medium. As noted above, this can be done before or after deposition of metal into the pores. This acid etching thus makes the final adjustment in the thickness of the oxide layer which eventually separates the metal substrate from the deposited conductor metal in the pore.
The acid chosen for etching purposes, to remove controlled amounts of the oxide film, can be selected from -`- 2137013 the same group of acids as chosen in respect of the anodizing bath.
Deposition of metal or other conductor into the uniform pores to form the nanowires is suitably accomplished by immersing the previously anodized alllm;nllm surface into an appropriate electrolyte containing the desired metal in anionic form, then applying alternating current between the all]m;nllm and a suitable counter electrode such as graphite. The metallic particles eventually formed are faithful replicas of the interiors of the pores in the metallic oxide layer. There do not appear to be any surface effects, inhibiting a true filling of the pores to the lower and side extremities thereof with the deposited metal. Individual metallic deposits are initially formed within the pores, and grow from the bottom of the pores upwardly and outwardly. The deposits eventually coalesce into compact metal rods, posts or cylinders, i.e. nanowires. The length of the nanowires depends on the duration of the AC electrolysis process, among other parameters.
In one em-bodiment of the present invention, after the template has been etched back to expose the tips of the nanowires, the tips of the nanowires are oxidized at their ends remote from the all~m;nllm substrate, to form insulating electrical barrier layers thereon. The oxidation is conducted carefully, in a controlled manner, so that an insulating, oxide layer of extremely thin but constant thickness is formed. On top of this oxide layer there is deposited a further conductor such as a metal (e.g. gold) so that a double-barrier device is created, having 2 insulating layers through which single-electron tunnelling can occur upon application of suitable voltage, in large number arrays. The uniformity of the pores initially formed in the all]m;nllm oxide on the substrate allows for the high degree of uniformity of metal deposited in such pores, which in turns allows for the high degree of uniformity of the oxide deposited on top of the metal, as the second very thin insulating layer.
For preparing an insulating barrier layer on the end of a nanowire, formed in the pores of the oxide as described above, a process of oxidation can be conducted in order to form an oxide insulating barrier layer. This can be done in the presence or absence of the initial metal substrate. Oxidation of metals is a simple, well controlled process, which can be conducted by heating the metal in the presence of oxygen, e.g. in an oven or under a heat lamp. The temperature to which the metal is heated, the time of exposure to oxygen and the nature of the atmosphere determine the depth of formation of the insulating oxide layer on the end of the nanowire, and is readily and easily controllable, since the oxidation is generally a slow process. Normally, barrier layers of a thickness of from about 10 to 1,000 Angstroms, most preferably from 10 to 100 Angstroms are formed. The best thickness depends to some extent upon the nature of the oxide material, e.g. on its dielectric constant and bandgap. The higher the dielectric constant, the thinner the oxide layer needs to be.
Instead of oxide formation to provide these barrier layers, other methods can be adopted, provided that they are controllable to give appropriate thicknesses of layers. Thus, insulating or semiconducting materials can be applied by solution deposition, for example when a polymeric insulating material is chosen. Deposition can also be conducted by vapour deposition by chemical means, sputtering or direct vapourization, all of which processes are capable of exact thickness control. When the initial all]m;mlm substrate and residual oxide has been removed, so that it is required to provide a new barrier layer on both ends of the nanowire, these can be provided simultaneously, especially in cases where the same insulating material to substantially the same thickness is being applied to both ends, or sequentially in the case where different insulating materials are being applied to each end.
Any such insulating barrier layer provided on a device according to the invention is overlayed by a conducting layer, preferably a metal layer, to which external electrical contact is made. In the case where the alllm;nllm substrate remains in place as one of the external connecting conductors, only the distal end of the nanowire carrying the insulating barrier layer needs to be provided with a metal deposit. Suitable methods for applying metal over the insulating barrier layers are known in the art, and include electrical chemical methods, sputtering and other metal vapour deposition techniques. In the case where the initial aluminum substrate and its associated oxide layer have been removed, it is usual but not necessary to apply the same metal to both ends of the nanowire, by one or other of these techniques, depending upon the electrical characteristics desired in the final product.
Reference has been made above to embodiments in which the initial substrate material, normally alllm;nllm is removed from the device, and replaced by another metal for electrical connection purposes. This can be performed by chemical methods, e.g. by etching with appropriate acids under carefully controlled conditions. By suitable choice of chemicals, within the skill of the art, the metal substrate can be etched away, and subsequently if desired, the residual metal oxide on the end of the nanowires can be etched away also, for replacement with another chosen barrier material. In this way, the metal material for use as the conductor, and the barrier material, can be chosen from a wide range of different materials selected on the basis of their electrical characteristics for use in the chosen application.
A wide range of metals is available to form the nanowires in the pores of the oxide insulating layer, according to the present invention. The basic criteria for its selection are that it must be a good electrical conductor, and that it must be depositable in the pores of the oxide layer by practical, acceptable means. It is also preferred that any chosen metal should be one which can readily and controllably be converted to an electrically insulating, or at least less electrically conducting, compound thereof, by relatively simple chemical means such as controlled oxidation. Examples of suitable such preferred metals are nickel, cadmium, bismuth, iron, titanium, niobium, silver, gold, and platinum.
Figure 1 of the accompanying drawings illustrates diagrammatically the nature of the pores template formed in anodic aluminum oxide, electrically chemically oxidized in an acid electrolyte. Residual al-lm;nl~m substrate 10 has a layer of oxide 12 thereon, with uniform, parallel pores 14 extending therethrough, substantially perpendicularly to the plane of the residual aluminum layer. A portion 16 of the al-lm;n-]m oxide layer separates each pore from the alllm;n-]m substrate layer 10. Each of the pores 14 is open at its distal end 18, remote from the alllm;nl]m substrate layer 10. By tuning the key parameters of the electrochemical oxidation process - voltage, temperature, acid electrolyte and time, one can obtain pores of any length up to several microns and any diameter between about 10 and 200 nanometers (100 and 2000 Angstroms).
In the next stage of the process according to the invention, metal is electrochemically deposited into the pores by transferring the pre-anodized alllm;nl~m to an appropriate electrolyte followed by AC electrolysis. As electro deposition continues, metal fills the pore from the bottom upward. This forms nanowires in the pores.
Figure 2 is a schematic view of the cross section of such a nanowire made by depositing nickel into the pores 14 of the alllm;nllm oxide layer 12 generally illustrated in Figure 1. The wires 22 are separated from the bottom most aluminum substrate 10, which provides an electrical contact, by an aluminum oxide thickness of insulating barrier 16 of about 250 Angstroms. By a process of controlled oxidation, a nickel oxide insulating layer 24 has been provided on the topmost portion of the nickel nanowire 22, and by electro deposition, a layer of silver metal 26 has been applied over the nickel oxide layer 24, so that the silver layer and the alllm;nllm substrate provide electrical contacts, separated by a double barrier device formed of the nickel nanowire 22, the alllm;nllm oxide barrier portion 16 and the nickel oxide barrier portion 24.
The thickness of the nickel oxide layer 24 is about 80 Angstroms. The nickel wire 22 is about 120 Angstroms in diameter, and about 9,000 Angstroms in length. The electrical performance of this device, and further detail of its preparation, are described below in Example 1.
Figure 3 of the accompanying drawings illustrates diagrammatically in cross section a different, preferred embodiment of the present invention, comprising an alllm;mlm substrate 30 having porous oxide layers 32,34 on each side thereof. The pores 36,38 therein extend close to the alllm;mlm substrate 30 but there is provided a barrier 40 of insulating aluminum oxide residue, between the pores and the alllm;nllm substrate. Metal e.g. nickel has been deposited into the pores, to form nanowires 42,44 extending away from the all~m;nllm substrate. A metal, e.g. silver has been electro deposited over the distal ends of the respective sets of nanowires to provide macromolecular `~ - 15 - 2137013 metal contacts 46,48.
With the device illustrated in Figure 3, electrical contact can be made to the aluminum substrate sheet 30, and to each of the peripheral metal layers 46,48.
Thus, different signals and settings can be provided to the central substrate 30. Conductivity through this substrate between metal layers 46 and 48 depends upon single electron tunnelling through the insulating barriers of oxide at each side of the substrate sheet. Accordingly, the device shown in Figure 3 can be operated in the manner of a transistor and as such incorporated into electronic circuits, e.g. for digital purposes.
The invention is further described, for illustrative purposes, in the following specific examples.
Example 1 To prepare single-electron devices by the process of the present invention, a super purity (99.99~) Alllm;nllm sheet, after being degreased in trichloroethylene, was used as the substrate, and anodized at 20V using a 0.5M sulfuric acid electrolyte and a high purity lead foil cathodes.
The sample was then rinsed in distilled water and then immersed in an aqueous electrolyte consisting of 120g/1 nickel sulfate and 45g/1 boric acid. The nickel metal was deposited into the pores by A.C electrolysis at 23C , at 200Hz and 16 V rms using graphite counter-electrodes to form the nanowires.
The alumina film was then etched to expose the tips of the nickel wires, in a solution consisting of 0.5M
phosphoric acid and 0.2M chromic acid at 80C for a period of time varying from 30 - 120 seconds. For some samples, to create a parallel array of equal length wires, the exposed tips were then polished off with gamma micropolish alumina (0.05). The samples were then left at room temperature for 48 hours in order to allow the formation of a nickel oxide tunnel barrier on the end of the nickel wire. After allowing the oxidation to take place, the samples were sonicated for two minutes in ethanol, air dried, then transferred to a vacuum chamber where silver pellets were evaporated and then deposited on the surface to form a contact.
Samples as prepared above provided nanowires separated from the bottom Al contact by an alllm;mlm oxide layer of about 250 Angstroms thickness, and from the top silver contact by a nickel oxide layer of about 80 Angstroms thickness. The wires were about 120 Angstroms in diameter, about 9000 A in length, and about 1olO per sq. cm in area density. By controlling key parameters such as the oxidizing medium, post-anodizing etch time, the time for A.C. > deposition, temperature, and concentrations of electrolytes one can obtain pores filled with various materials with lengths up to several microns and any diameter between ~10 and ~200nm. The standard deviations in the wire diameter can be controlled to below ~15~ of the mean diameter.
The samples were measured at room temperature, using both Keithley 237 and HP4145. Most samples were ~0.5cm2 with a nickel wire density of ~3 x 10 10 cm~2.
Figure 4 of the accompanying drawings shows the current-voltage, typical of this family of samples.
The clearly observable stair-case like I-V
characteristics on Figure 4, the rather sharp rise edges of the stairs, the plateaus, and the very small current before the onset of the first step are reminiscent of single -- 21~701~
electron tunnelling in double-junction systems predicted by Coulomb blockade theory and observed in experiments at low temperatures.
The very small ~;m~n~ions of the junctions are consistent with the possibility of observing room-temperature Coulomb blockade effects. The unusually large onset voltage of the first current step (~0.9V) and the large voltage intervals between steps are consistent with the predictions of the conventional theory if the geometrical and material parameters characteristic of these structures are used. The sharpness of the steps on Figure 4 is also consistent with theory provided that there is a large difference in the resistances and capacitances of the two junctions.
Coulomb blockade theory predicts that the onset voltage of the first stair occurs at V1~ e/(2C1), i.e. V1 ~
lV when C1 is of the order of 10-19F. Assuming that in the samples according to the invention the top (nickel oxide) barrier is a hemispherical cap with a tip diameter of ~lOnm, a thickness of ~8nm and has a relative dielectric constant of ~4 its capacitance (C1) would be approximately 5xlO-19F. A similar calculation for the bottom (aluminum oxide) junction assuming a thickness of ~25nm and a dielectric constant of ~4.5 leads to a capacitance (C2) of approximately 2xlO-19F. The ~;men~ions used in the calculations are consistent with electron microscopy measurements. The estimated capacitance values are small enough to satisfy the inequality kT ~ e2, c = C1C2 2C c1+C2 the prerequisite for observing single electron tunnelling at room temperature. With these values of capacitance the calculated onset voltage would be approximately 0.2V, which is of the same order of magnitude as the experimentally measured 0.85V.
- 21~701~
It should be noted that for Coulomb blockade to be observed, the wires should be well isolated from the environment, i.e. the tunnelling resistance should be well above the quantum resistance RQ = e2/h = 23.6 kQ. This condition is satisfied for our samples.
It is to be noted that these results were obtained at room temperatures. At those temperatures, single electron events are rarely observable unless the energy change of the system associated with one electron crossing is much greater than kT. Structure parameters of the devices described herein give capacitances for the two junctions sufficiently low for this to occur. The capacitance values found are consistent with those required for the observed voltage differences between subsequent lS current jumps in a double-junction model. The system demonstrates Coulomb blockade effects.
More specifically, it relates to single-electron devices useful as diodes and transistors or as other electronic devices, and to chemical processes for their preparation.
A single-electron device, as the term is generally understood, is a device which controls the movement of individual electrons in solids. They commonly take the form of tunnel junctions, consisting of two conductors separated by an ultrathin (less than 100 nanometers) layer of insulating material. When a voltage is applied across the tunnel junction, inducing current (electron movement) to flow in the conductors, a surface charge accumulates on one surface of the conductor against the insulating layer, with an equal and opposite charge on the other insulator/conductor surface. When this surface charge exceeds a predetermined value, an electron tunnels through the insulating layer, thereby reducing the surface charge. When the surface charge is less than the predetermined value, tunnelling is suppressed (the Coulomb blockade). As a surface charge increases due to continued current flow in the conductor, i.e. continued application of the voltage across the insulator, the charge increases again, until the Coulomb blockade is overcome, whereupon another single electron tunnels through. The phenomenon can be observed experimentally, as a fl~n~mpntal relation between applied voltage and the frequency of oscillation in the current flowing through the junction. The height of the Coulomb blockade depends upon the conductance and capacitance of the insulating layer.
A general description of single electronics and single-electron devices and their method of operation appears in "Scientific American", June 1992, page 80, in an article by Likharev and Claeson.
`- 21~701~
These single-electron phenomena show promise for application to digital integrated circuits. Currently computer chips can have a density of about ten million devices per square centimetre, to handle the commonly used digital electrical pulses. Using single electronics, even further reductions in size are possible, since bits of information can be represented through the passage of individual electrons. For this to happen, however, techniques need to be developed to fabricate complex structures whose smallest dimension is, controllably and reproducibly, less than 100 nanometers. Such techniques also need to be capable of operation economically and efficiently, for the production of single-electronic devices incorporating one or more such tunnel junctions.
It is an object of the present invention to provide novel, single-electron devices.
It is a further object of the invention to provide novel processes for making single-electron devices.
In the present invention, single-electron devices are made by a technique of electro deposition. A layer of porous oxide is deposited on the surface of a conductive substrate of a metal selected from aluminum, titanium, niobium and tantalum, by electrolytic anodizing. The pores formed in the oxide layer are of extremely small but very uniform shape, diameter and depth, controllable within close limits by the conditions of anodizing and/or by subsequent chemical etching. These highly uniform, nanometer-sized, densely packed pores are used in the present invention as templates, for the formation therein of conducting or semiconducting materials, to form an active region ("nanowire") of a tunnel junction device.
The insulating layer or layers of the device can be formed by oxidation or other chemical conversion of the or each end portion of the, nanowire. Alternatively, the residual ` 21~7013 oxide layer at the bottom of each pore, separating the pore from the electrically conducting metal substrate, can form an insulating layer, with the metal substrate itself acting as the second conductor separated by this insulating oxide layer from the nanowire which is formed in the pore.
The invention thus takes advantage of the very small but highly uniform and controllable sizes of the pores formed in the oxide layer, by anodizing and if desired by subsequent chemical etching, to make single-electron devices. The pore sizes can be controlled to adiameter of about 90 Angstroms up to several thousand Angstroms, and to a height of several hundred Angstroms to several thousand Angstroms, to give devices with an array of conductor-barrier arrangements of dimensions suitable to exhibit single-electron tunnelling effects. Moreover, the pores and hence the nanowires formed in them can be extremely densely packed, allowing the preparation of arrays of tunnel junction devices, of a density up to the order of 101 per square centimetre.
FIGURE 1 is an idealized illustration of a pores template formed as a part of the process of the invention;
FIGURE 2 is a schematic view of a cross section of a nickel nanowire prepared and studied in the present inventlon;
FIGURE 3 is a diagrammatic cross section of an alternative and preferred embodiment of the present invention.
FIGURE 4 is a voltage-current curve derived from devices according to the present invention as described in Example 2 below.
Devices according the present invention can take ``- 2137013 a variety of different forms, and incorporate one or more insulating barrier layers and correspondingly two or more conductors, at least one of which is a nanowire. The conductive metal substrate may constitute a conductor of the finally produced single-electron device, in which case the metal substrate is chosen from among aluminum, titanium, niobium, tantalum and alloys thereof on the basis of desired electrical properties. In other embodimentsl the conductive metal substrate may be fully removed and replaced during the manufacturing process, and not constitute any part of the final device. In such cases, the initial choice of substrate is dictated by cost and by ease of manufacture, and is preferably all~m;nllm.
Similarly, the insulating metal oxide formed initially on the conductive metal substrate may or may not form one or more of the insulating barrier layers in the final device. This will influence the choice of metal substrate, for similar reasons.
The simplest device according to the present invention, and the device most easily prepared (although not the most preferred embodiment) is one which has a single insulating layer (barrier) comprised of the oxide of the metal substrate, disposed between the metal substrate constituting one conductor, and a nanowire conductor formed in a pore in the oxide layer. Such a device is prepared by cleaning and anodizing the metal substrate, under carefully controlled conditions to provide thereon oxide film with the dense array of uniformly sized pores, the depth of the pores being controlled to leave a suitably thin oxide layer between the pore and the substrate to act as an insulating layer of a single-electron device. Metal, semi-conductor or other conducting material is subsequently deposited in the pores of the oxide layer, to contact the insulating oxide layer. A thin metal film (also referred to macro-metal), for electrical connection purposes, is deposited ~ 5 _ over the nanowire in the pores, and in electrical contacttherewith.
Other single-barrier devices according to the invention can be prepared by the process outlined above, followed by a removal and replacement of one or both of the metal substrate and the residual oxide separating the metal substrate from the pore. This can be effected chemically, by known metal and metal oxide removing techniques, e.g.
chemical etching. After removal of only the metal substrate, another metal can be deposited over the metal oxide insulating barrier layer. After removal of both the metal substrate and the metal oxide insulating barrier layer, another insulating barrier layer can be deposited on one end of the nanowire, e.g. by controlled oxidation or other chemical treatment thereof. Then another conductor, e.g. metal, can be deposited over the newly formed barrier layer, to complete the single barrier device according to the invention.
Double barrier devices according to the invention can be prepared by depositing or oxidizing an insulating barrier layer on the end of the nanowire remote from the metal substrate, followed by deposition of another conductor over this insulating barrier layer, in the case where the original substrate and intervening oxide layer below the pores are left intact to constitute one barrier layer and conductor. In the case where the original substrate and the intervening oxide layer below the pores are both removed, double barrier devices according to the invention can be prepared after their r~ ovdl, by deposition onto, or oxidation of, both ends of the residual nanowire of the insulating barrier layer, e.g. an oxide layer, followed by deposition thereover of conductive layers, e.g. of metal.
In order to constitute single electron devices, 21~7013 the em~bodiments of this invention only need to include one nanowire, and in all embodiments the pores formed in the oxide layers formed on the metal substrates provide the templates for these nanowires. Then one or two barrier layers can be deposited, of a size suitable for exhibiting single electron tunnelling effects, on account of the extremely small sizes of these nanowires, particularly their end surface areas. The uniformity and density of the pores allows the preparation of useful devices with practical applications.
A further, preferred embodiment of the invention is a multiple barrier device having a thin conductive intermediate layer, to which electrical connections can readily be made. This is prepared by initially providing an electrically conductive metal substrate of one of the aforementioned metals, e.g. all~m;n~m~ and providing a microporous oxide coating as previously described, on both sides. If desired, the substrate in this em.bodiment can comprise a conductive core, chosen on the basis of its electrical characteristics for a suitable application, carrying a deposit on both sides of one of the aforementioned metals, e.g. aluminum, this metal layer having a micro porous oxide coating as previously described. Metal can then be deposited in the pores to form nanowires, separated from the metal substrate by residual oxide forming the insulating barrier, on each side, thereby providing a double barrier device. A thin metal film can then be applied over the nanowires at their ends remote from the substrate, for electrical contact purposes, thereby providing a double barrier, three contact device comprising a very large array of nanowire-barrier "pathways", operable in the manner of a transistor.
This embodiment of the invention, utilizing a two sided porous substrate, can be further expanded from a two-barrier device to a three-barrier device or a four-barrier `- 2137~13 device, if desired, by creation of another barrier layer, e.g. by controlled oxidation, on the distal end of one or both of the sets of nanowires protruding from each side of the substrate. In such cases, the metal film is applied over the or each of the barrier layer, to provide electrical contact means.
The metallic substrate used in the process of the present invention, and in one embodiment serving as the conductor contacting the insulating layer, is normally all]m;nl~m or an aluminum alloy in which aluminum is the predominant metal, in foil or sheet form, or as a deposited alllm;nllm film on an inert substrate. A surface layer of alnm;n-lm oxide is deposited thereon, to constitute the insulating layer, by anodizing the metal sheet or foil.
Firstly, the sheet or foil should be cleaned, ultra-sonically and/or with organic solvent to remove grease residues from its surface. Then it is preferably washed with an alkaline chemical liquid so as to achieve a degree of surface etching, followed by neutralization to remove alkali excess. A wide variety of different chemical reagents may be used for these purposes. Sodium carbonate solution is an example of a suitable base with which to effect the etching. Nitric acid is a suitable neutralizing agent for subsequent use. Thus, the preferred cleaning process is ultrasonic cleaning in dichloromethane, followed by treatment with dilute sodium carbonate and then with dilute nitric acid. However, the cleaning process can be conducted with a very wide variety of different reagents.
Electrolytic anodizing of the cleaned sheet or foil, for the purposes of depositing thereon a porous surface of oxide, is suitably accomplished by making the metal the anode of an electrolytic cell, using suitable (e.g. lead) counter-electrodes in an acid bath. Suitably, the bath is a relatively dilute solution of strong acids such as sulfuric acid, phosphoric acid, oxalic acid, or chromic acid. Direct current is passed through the cell between the electrodes, at a current or voltage suitably adjusted to provide the correct film deposition. This can be accomplished at room temperatures.
After suitable anodizing as described, the substrate is removed from the bath and rinsed. It is desirable to rid the surface of the treated substrate of residual acid, and neutralize it at this point. It is, however, undesirable to neutralize the acid chemically, since this might have the effect of damaging the deposited film. Accordingly, it is preferred to rinse the anodized film with suitable quantities of water to remove acid and effect appropriate neutralization.
A substrate so prepared has micro-pores in the oxide surface film, of substantially uniform size in the nanometer size range, and extending substantially perpendicularly from the substrate surface and therefore substantially parallel to one another. At the bottom of each such micropore is a very thin layer of alllm;nllm oxide, an electrical insulating material, separating the body of the pore from the conducting metal alllm;nllm or aluminum alloy substrate. By appropriate means according to the present invention, this pore structure is utilized to provide another conductor, separated from the conducting all~m;mlm or aluminum alloy substrate, by a nanometer-size range thickness of insulating layer to form the principle of the single-electron devices according to the present invention.
In a next step, therefore, an appropriate conductor is applied to the interior of the pores. A
typical example of such a conductor is nickel. Before or after deposition of the metal such as nickel into the pores, the height and size of the pores can be chemically adjusted, by chemical etching. The length of this "column"
21~7013 ' g of deposited metal defined by the size of pore, is not critical, but is typically in the size range from 1-10 microns .
The diameter, the density and the height of the pores is determined to some extent by the choice of acid in the anodizing bath. Suitable acids from which to choose are phosphoric acid, oxalic acid, sulphuric acid and chromic acid. The use of phosphoric acid leads the formation of relatively large pores. The use of oxalic acid or chromic acid leads towards the formation of smaller pores, while the use of sulphuric acid leads the formation of pores of the smallest diameters. The relative concentration of the acid used also has a minor effect on the pore sizes produced, but this effect is of little significance in comparison with that derived from the choice of acid.
Pore density, i.e. the distance between individual pores in the substrate, can be further varied by choosing the DC anodizing voltage appropriately. High anodizing voltages lead to low pore densities, whilst low anodizing voltages tend towards the film with high poor densities. The anodizing voltage has a lesser effect on the individual pore sizes.
After the anodizing process has been completed, the diameters and the depths of the pores can be further adjusted by etching the oxide film with an appropriate acid medium. As noted above, this can be done before or after deposition of metal into the pores. This acid etching thus makes the final adjustment in the thickness of the oxide layer which eventually separates the metal substrate from the deposited conductor metal in the pore.
The acid chosen for etching purposes, to remove controlled amounts of the oxide film, can be selected from -`- 2137013 the same group of acids as chosen in respect of the anodizing bath.
Deposition of metal or other conductor into the uniform pores to form the nanowires is suitably accomplished by immersing the previously anodized alllm;nllm surface into an appropriate electrolyte containing the desired metal in anionic form, then applying alternating current between the all]m;nllm and a suitable counter electrode such as graphite. The metallic particles eventually formed are faithful replicas of the interiors of the pores in the metallic oxide layer. There do not appear to be any surface effects, inhibiting a true filling of the pores to the lower and side extremities thereof with the deposited metal. Individual metallic deposits are initially formed within the pores, and grow from the bottom of the pores upwardly and outwardly. The deposits eventually coalesce into compact metal rods, posts or cylinders, i.e. nanowires. The length of the nanowires depends on the duration of the AC electrolysis process, among other parameters.
In one em-bodiment of the present invention, after the template has been etched back to expose the tips of the nanowires, the tips of the nanowires are oxidized at their ends remote from the all~m;nllm substrate, to form insulating electrical barrier layers thereon. The oxidation is conducted carefully, in a controlled manner, so that an insulating, oxide layer of extremely thin but constant thickness is formed. On top of this oxide layer there is deposited a further conductor such as a metal (e.g. gold) so that a double-barrier device is created, having 2 insulating layers through which single-electron tunnelling can occur upon application of suitable voltage, in large number arrays. The uniformity of the pores initially formed in the all]m;nllm oxide on the substrate allows for the high degree of uniformity of metal deposited in such pores, which in turns allows for the high degree of uniformity of the oxide deposited on top of the metal, as the second very thin insulating layer.
For preparing an insulating barrier layer on the end of a nanowire, formed in the pores of the oxide as described above, a process of oxidation can be conducted in order to form an oxide insulating barrier layer. This can be done in the presence or absence of the initial metal substrate. Oxidation of metals is a simple, well controlled process, which can be conducted by heating the metal in the presence of oxygen, e.g. in an oven or under a heat lamp. The temperature to which the metal is heated, the time of exposure to oxygen and the nature of the atmosphere determine the depth of formation of the insulating oxide layer on the end of the nanowire, and is readily and easily controllable, since the oxidation is generally a slow process. Normally, barrier layers of a thickness of from about 10 to 1,000 Angstroms, most preferably from 10 to 100 Angstroms are formed. The best thickness depends to some extent upon the nature of the oxide material, e.g. on its dielectric constant and bandgap. The higher the dielectric constant, the thinner the oxide layer needs to be.
Instead of oxide formation to provide these barrier layers, other methods can be adopted, provided that they are controllable to give appropriate thicknesses of layers. Thus, insulating or semiconducting materials can be applied by solution deposition, for example when a polymeric insulating material is chosen. Deposition can also be conducted by vapour deposition by chemical means, sputtering or direct vapourization, all of which processes are capable of exact thickness control. When the initial all]m;mlm substrate and residual oxide has been removed, so that it is required to provide a new barrier layer on both ends of the nanowire, these can be provided simultaneously, especially in cases where the same insulating material to substantially the same thickness is being applied to both ends, or sequentially in the case where different insulating materials are being applied to each end.
Any such insulating barrier layer provided on a device according to the invention is overlayed by a conducting layer, preferably a metal layer, to which external electrical contact is made. In the case where the alllm;nllm substrate remains in place as one of the external connecting conductors, only the distal end of the nanowire carrying the insulating barrier layer needs to be provided with a metal deposit. Suitable methods for applying metal over the insulating barrier layers are known in the art, and include electrical chemical methods, sputtering and other metal vapour deposition techniques. In the case where the initial aluminum substrate and its associated oxide layer have been removed, it is usual but not necessary to apply the same metal to both ends of the nanowire, by one or other of these techniques, depending upon the electrical characteristics desired in the final product.
Reference has been made above to embodiments in which the initial substrate material, normally alllm;nllm is removed from the device, and replaced by another metal for electrical connection purposes. This can be performed by chemical methods, e.g. by etching with appropriate acids under carefully controlled conditions. By suitable choice of chemicals, within the skill of the art, the metal substrate can be etched away, and subsequently if desired, the residual metal oxide on the end of the nanowires can be etched away also, for replacement with another chosen barrier material. In this way, the metal material for use as the conductor, and the barrier material, can be chosen from a wide range of different materials selected on the basis of their electrical characteristics for use in the chosen application.
A wide range of metals is available to form the nanowires in the pores of the oxide insulating layer, according to the present invention. The basic criteria for its selection are that it must be a good electrical conductor, and that it must be depositable in the pores of the oxide layer by practical, acceptable means. It is also preferred that any chosen metal should be one which can readily and controllably be converted to an electrically insulating, or at least less electrically conducting, compound thereof, by relatively simple chemical means such as controlled oxidation. Examples of suitable such preferred metals are nickel, cadmium, bismuth, iron, titanium, niobium, silver, gold, and platinum.
Figure 1 of the accompanying drawings illustrates diagrammatically the nature of the pores template formed in anodic aluminum oxide, electrically chemically oxidized in an acid electrolyte. Residual al-lm;nl~m substrate 10 has a layer of oxide 12 thereon, with uniform, parallel pores 14 extending therethrough, substantially perpendicularly to the plane of the residual aluminum layer. A portion 16 of the al-lm;n-]m oxide layer separates each pore from the alllm;n-]m substrate layer 10. Each of the pores 14 is open at its distal end 18, remote from the alllm;nl]m substrate layer 10. By tuning the key parameters of the electrochemical oxidation process - voltage, temperature, acid electrolyte and time, one can obtain pores of any length up to several microns and any diameter between about 10 and 200 nanometers (100 and 2000 Angstroms).
In the next stage of the process according to the invention, metal is electrochemically deposited into the pores by transferring the pre-anodized alllm;nl~m to an appropriate electrolyte followed by AC electrolysis. As electro deposition continues, metal fills the pore from the bottom upward. This forms nanowires in the pores.
Figure 2 is a schematic view of the cross section of such a nanowire made by depositing nickel into the pores 14 of the alllm;nllm oxide layer 12 generally illustrated in Figure 1. The wires 22 are separated from the bottom most aluminum substrate 10, which provides an electrical contact, by an aluminum oxide thickness of insulating barrier 16 of about 250 Angstroms. By a process of controlled oxidation, a nickel oxide insulating layer 24 has been provided on the topmost portion of the nickel nanowire 22, and by electro deposition, a layer of silver metal 26 has been applied over the nickel oxide layer 24, so that the silver layer and the alllm;nllm substrate provide electrical contacts, separated by a double barrier device formed of the nickel nanowire 22, the alllm;nllm oxide barrier portion 16 and the nickel oxide barrier portion 24.
The thickness of the nickel oxide layer 24 is about 80 Angstroms. The nickel wire 22 is about 120 Angstroms in diameter, and about 9,000 Angstroms in length. The electrical performance of this device, and further detail of its preparation, are described below in Example 1.
Figure 3 of the accompanying drawings illustrates diagrammatically in cross section a different, preferred embodiment of the present invention, comprising an alllm;mlm substrate 30 having porous oxide layers 32,34 on each side thereof. The pores 36,38 therein extend close to the alllm;mlm substrate 30 but there is provided a barrier 40 of insulating aluminum oxide residue, between the pores and the alllm;nllm substrate. Metal e.g. nickel has been deposited into the pores, to form nanowires 42,44 extending away from the all~m;nllm substrate. A metal, e.g. silver has been electro deposited over the distal ends of the respective sets of nanowires to provide macromolecular `~ - 15 - 2137013 metal contacts 46,48.
With the device illustrated in Figure 3, electrical contact can be made to the aluminum substrate sheet 30, and to each of the peripheral metal layers 46,48.
Thus, different signals and settings can be provided to the central substrate 30. Conductivity through this substrate between metal layers 46 and 48 depends upon single electron tunnelling through the insulating barriers of oxide at each side of the substrate sheet. Accordingly, the device shown in Figure 3 can be operated in the manner of a transistor and as such incorporated into electronic circuits, e.g. for digital purposes.
The invention is further described, for illustrative purposes, in the following specific examples.
Example 1 To prepare single-electron devices by the process of the present invention, a super purity (99.99~) Alllm;nllm sheet, after being degreased in trichloroethylene, was used as the substrate, and anodized at 20V using a 0.5M sulfuric acid electrolyte and a high purity lead foil cathodes.
The sample was then rinsed in distilled water and then immersed in an aqueous electrolyte consisting of 120g/1 nickel sulfate and 45g/1 boric acid. The nickel metal was deposited into the pores by A.C electrolysis at 23C , at 200Hz and 16 V rms using graphite counter-electrodes to form the nanowires.
The alumina film was then etched to expose the tips of the nickel wires, in a solution consisting of 0.5M
phosphoric acid and 0.2M chromic acid at 80C for a period of time varying from 30 - 120 seconds. For some samples, to create a parallel array of equal length wires, the exposed tips were then polished off with gamma micropolish alumina (0.05). The samples were then left at room temperature for 48 hours in order to allow the formation of a nickel oxide tunnel barrier on the end of the nickel wire. After allowing the oxidation to take place, the samples were sonicated for two minutes in ethanol, air dried, then transferred to a vacuum chamber where silver pellets were evaporated and then deposited on the surface to form a contact.
Samples as prepared above provided nanowires separated from the bottom Al contact by an alllm;mlm oxide layer of about 250 Angstroms thickness, and from the top silver contact by a nickel oxide layer of about 80 Angstroms thickness. The wires were about 120 Angstroms in diameter, about 9000 A in length, and about 1olO per sq. cm in area density. By controlling key parameters such as the oxidizing medium, post-anodizing etch time, the time for A.C. > deposition, temperature, and concentrations of electrolytes one can obtain pores filled with various materials with lengths up to several microns and any diameter between ~10 and ~200nm. The standard deviations in the wire diameter can be controlled to below ~15~ of the mean diameter.
The samples were measured at room temperature, using both Keithley 237 and HP4145. Most samples were ~0.5cm2 with a nickel wire density of ~3 x 10 10 cm~2.
Figure 4 of the accompanying drawings shows the current-voltage, typical of this family of samples.
The clearly observable stair-case like I-V
characteristics on Figure 4, the rather sharp rise edges of the stairs, the plateaus, and the very small current before the onset of the first step are reminiscent of single -- 21~701~
electron tunnelling in double-junction systems predicted by Coulomb blockade theory and observed in experiments at low temperatures.
The very small ~;m~n~ions of the junctions are consistent with the possibility of observing room-temperature Coulomb blockade effects. The unusually large onset voltage of the first current step (~0.9V) and the large voltage intervals between steps are consistent with the predictions of the conventional theory if the geometrical and material parameters characteristic of these structures are used. The sharpness of the steps on Figure 4 is also consistent with theory provided that there is a large difference in the resistances and capacitances of the two junctions.
Coulomb blockade theory predicts that the onset voltage of the first stair occurs at V1~ e/(2C1), i.e. V1 ~
lV when C1 is of the order of 10-19F. Assuming that in the samples according to the invention the top (nickel oxide) barrier is a hemispherical cap with a tip diameter of ~lOnm, a thickness of ~8nm and has a relative dielectric constant of ~4 its capacitance (C1) would be approximately 5xlO-19F. A similar calculation for the bottom (aluminum oxide) junction assuming a thickness of ~25nm and a dielectric constant of ~4.5 leads to a capacitance (C2) of approximately 2xlO-19F. The ~;men~ions used in the calculations are consistent with electron microscopy measurements. The estimated capacitance values are small enough to satisfy the inequality kT ~ e2, c = C1C2 2C c1+C2 the prerequisite for observing single electron tunnelling at room temperature. With these values of capacitance the calculated onset voltage would be approximately 0.2V, which is of the same order of magnitude as the experimentally measured 0.85V.
- 21~701~
It should be noted that for Coulomb blockade to be observed, the wires should be well isolated from the environment, i.e. the tunnelling resistance should be well above the quantum resistance RQ = e2/h = 23.6 kQ. This condition is satisfied for our samples.
It is to be noted that these results were obtained at room temperatures. At those temperatures, single electron events are rarely observable unless the energy change of the system associated with one electron crossing is much greater than kT. Structure parameters of the devices described herein give capacitances for the two junctions sufficiently low for this to occur. The capacitance values found are consistent with those required for the observed voltage differences between subsequent lS current jumps in a double-junction model. The system demonstrates Coulomb blockade effects.
Claims (6)
1. A process of preparing single-electron devices comprising an array of elements each comprising at least two conductors contacting and separated by an ultrathin insulating or semiconducting layer, at least one of the conductors of each element being a nanowire, said process comprising:
providing a metal substrate in sheet or foil form, the metal thereof being selected from aluminum, titanium, niobium, tantalum and alloys containing a predominant amount of one of said metals;
anodizing said substrate electrolytically in an acid bath, to deposit thereon an oxide film having micropores of substantially mutually parallel axial disposition and substantially uniform diameter in the range from about 1 to about 500 nanometers and substantially uniform depth which is less than the thickness of the oxide film, so as to leave an ultrathin oxide layer between the bottom of each pore and the metal substrate;
depositing in said pores a conductive material, to form a nanowire in contact with the oxide layer at the bottom of said pore;
and depositing macro metal over the ends of the nanowires so formed, for external electrical contact purposes.
providing a metal substrate in sheet or foil form, the metal thereof being selected from aluminum, titanium, niobium, tantalum and alloys containing a predominant amount of one of said metals;
anodizing said substrate electrolytically in an acid bath, to deposit thereon an oxide film having micropores of substantially mutually parallel axial disposition and substantially uniform diameter in the range from about 1 to about 500 nanometers and substantially uniform depth which is less than the thickness of the oxide film, so as to leave an ultrathin oxide layer between the bottom of each pore and the metal substrate;
depositing in said pores a conductive material, to form a nanowire in contact with the oxide layer at the bottom of said pore;
and depositing macro metal over the ends of the nanowires so formed, for external electrical contact purposes.
2. The process of claim 1, including the additional step of forming an insulating layer over the end of each nanowire, interposed between the end of the nanowire and the macrometal.
3. The process of claim 2 wherein said additional step is accomplished by chemical conversion of the distal end portion of the nanowires
4. Single-electron devices comprising an array of single-electron elements, each said element comprising:
- at least one nanowire conductor having a first end and a second end;
- first and second ultrathin semi-conductive or insulating layers overlying and electrically contacting the first and second ends respectively of the nanowire conductor;
- first and second macro metal layers respectively overlying and electrically contacting the said ultrathin layers, for external electrical connection purposes.
- at least one nanowire conductor having a first end and a second end;
- first and second ultrathin semi-conductive or insulating layers overlying and electrically contacting the first and second ends respectively of the nanowire conductor;
- first and second macro metal layers respectively overlying and electrically contacting the said ultrathin layers, for external electrical connection purposes.
5. Single-electron devices according to claim 5 wherein one of said macro metal layers is a metal sheet or foil provided with a microporous metal oxide film on at least one side thereof, the nanowire conductors being metal deposited in the micropores thereof, and the residual metal film constituting one of said ultrathin layers.
6. Single-electron devices according to claim 6, wherein said metal sheet or foil is provided with a microporous metal oxide film on both sides thereof, with nanowire conductors formed of metal deposited in pores of both such films.
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CA002137013A CA2137013A1 (en) | 1994-11-30 | 1994-11-30 | Nanoelectric devices |
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CA002137013A CA2137013A1 (en) | 1994-11-30 | 1994-11-30 | Nanoelectric devices |
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Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9359195B2 (en) | 2010-10-21 | 2016-06-07 | Hewlett-Packard Development Company, L.P. | Method of forming a nano-structure |
US9410260B2 (en) | 2010-10-21 | 2016-08-09 | Hewlett-Packard Development Company, L.P. | Method of forming a nano-structure |
US9611559B2 (en) | 2010-10-21 | 2017-04-04 | Hewlett-Packard Development Company, L.P. | Nano-structure and method of making the same |
US9751755B2 (en) | 2010-10-21 | 2017-09-05 | Hewlett-Packard Development Company, L.P. | Method of forming a micro-structure |
US10927472B2 (en) | 2010-10-21 | 2021-02-23 | Hewlett-Packard Development Company, L.P. | Method of forming a micro-structure |
-
1994
- 1994-11-30 CA CA002137013A patent/CA2137013A1/en not_active Abandoned
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9359195B2 (en) | 2010-10-21 | 2016-06-07 | Hewlett-Packard Development Company, L.P. | Method of forming a nano-structure |
US9410260B2 (en) | 2010-10-21 | 2016-08-09 | Hewlett-Packard Development Company, L.P. | Method of forming a nano-structure |
US9611559B2 (en) | 2010-10-21 | 2017-04-04 | Hewlett-Packard Development Company, L.P. | Nano-structure and method of making the same |
US9751755B2 (en) | 2010-10-21 | 2017-09-05 | Hewlett-Packard Development Company, L.P. | Method of forming a micro-structure |
US10287697B2 (en) | 2010-10-21 | 2019-05-14 | Hewlett-Packard Development Company, L.P. | Nano-structure and method of making the same |
US10927472B2 (en) | 2010-10-21 | 2021-02-23 | Hewlett-Packard Development Company, L.P. | Method of forming a micro-structure |
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