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Formation of atomic point contacts and molecular junctions with a ...

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can flow between the electrodes. The current was typicallywell below 0.2 nA in the electrolyte shown as the grey solidline in Fig. 5b, much smaller than the conduction currentthrough the <strong>molecular</strong> junction. The electrochemical gateeffect observed here is rather weak, which could be partiallydue to the screening <strong>of</strong> the gate field by the proximity <strong>of</strong> thetwo electrodes (serving as source <strong>and</strong> drain).3 Ni <strong>atomic</strong> <strong>point</strong> contactThe same setup can create <strong>atomic</strong> <strong>point</strong> <strong>contacts</strong> by eithermechanically controlling the elongation <strong>of</strong> the Au electrodesor by electrodeposition/etching process (Fig. 4a). Theuse <strong>of</strong> electrodeposition makes it easy to fabricate <strong>atomic</strong><strong>point</strong> <strong>contacts</strong> <strong>of</strong> different metals, <strong>and</strong> even a <strong>point</strong>contact between two different metals. To demonstrate thisapplication, we have fabricated Ni <strong>atomic</strong> <strong>point</strong> <strong>contacts</strong>using this combined approach. The first step is to electrochemicallydeposit Ni onto Au electrodes by holding thepotentials <strong>of</strong> the two electrodes at 21.1 V against Ag/AgCl <strong>with</strong> 0.1 M nickel sulphamate in 0.5 M boric acid(pH 3.5). We can also choose to deposit Ni onto only one<strong>of</strong> the two electrodes to fabricate an Au–Ni contact. Aftera <strong>point</strong> contact is formed, we can further control the size<strong>of</strong> the <strong>atomic</strong> <strong>point</strong> contact mechanically. Since Ni is aferromagnetic material <strong>with</strong> partial occupied d-orbital, ithas been argued that the strong exchange splitting <strong>of</strong> theelectron b<strong>and</strong>s may lift the spin degeneracy. The up- <strong>and</strong>down-spin electrons contribute independently to the electrictransport, which results in the conductance <strong>of</strong> <strong>atomic</strong> <strong>point</strong>contact located at integer multiples <strong>of</strong> e 2 /h. In the preliminaryexperiments, we have performed the measurement<strong>with</strong> a magnetic field (0.4 T). A typical conductancetrace is shown in Fig. 6a. Unlike the results <strong>with</strong>out a magneticfield (result not shown), steps near or at integer multiples<strong>of</strong> e 2 /h have rather frequently been observed in Ni<strong>point</strong> <strong>contacts</strong>. The conductance histogram (Fig. 6b) constructedfrom 18 individual curves from two differentdevices shows some evidence <strong>of</strong> conductance peakslocated at integer multiples <strong>of</strong> e 2 /h [30–32]. Furtherstudies are in progress to verify <strong>and</strong> underst<strong>and</strong> the preliminaryfindings.4 SummaryWe have described a combined mechanical <strong>and</strong> electrochemicaldeposition method to fabricate <strong>atomic</strong> <strong>point</strong> <strong>contacts</strong><strong>and</strong> <strong>molecular</strong> <strong>junctions</strong>. Using the method, we have created<strong>atomic</strong> <strong>point</strong> <strong>contacts</strong> <strong>and</strong> studied electron transport through4,4 0 -bipyridine. The setup is particularly suitable for studying<strong>atomic</strong> <strong>point</strong> <strong>contacts</strong> <strong>and</strong> <strong>molecular</strong> <strong>junctions</strong> inaqueous solutions, which is required for biologically relevantmolecules, <strong>molecular</strong> binding events <strong>and</strong> electrochemicalgate-control <strong>of</strong> single molecule conductance.5 AcknowledgmentsWe would like to thank Bingqian Xu <strong>and</strong> Joshua Hihath forthe help <strong>and</strong> acknowledge the financial support fromNSF-DMR-03-05242.6 ReferencesFig. 6 Conductance quantisation <strong>of</strong> Nia Conductance quantisation steps <strong>of</strong> a Ni <strong>atomic</strong> <strong>point</strong> contact. Thequantised conductance steps are located at integer multiples <strong>of</strong> e 2 /hb Conductance histogram constructed from 18 individual curves asshown in a1 Li, C.Z., Bogozi, A., Huang, W., <strong>and</strong> Tao, N.J.: ‘Fabrication <strong>of</strong> stablemetallic nanowires <strong>with</strong> quantized conductance’, Nanotechnology,1999, 10, pp. 221–2232 Morpurgo, A.F., Marcus, C.M., <strong>and</strong> Robinson, D.B.: ‘Controlledfabrication <strong>of</strong> metallic electrodes <strong>with</strong> <strong>atomic</strong> separation’, Appl.Phys. Lett., 1999, 14, p. 20823 Kervennic, Y.V., Thijssen, J.M., Vanmaekelbergh, D., Dabirian, R.,Jenneskens, L.W., van Walree, C.A., <strong>and</strong> van der Zant, H.S.J.:‘Charge transport in three-terminal <strong>molecular</strong> <strong>junctions</strong> incorporatingsulfur-end-functionalized tercyclohexylidene spacers’, Angew. Chem.Int. Ed. 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Rev. Lett., 2002, 92, pp. 186805/186801–186805/18680411 Ghosh, S., Halimun, H., Mahapatro, A.K., Choi, J., Lodha, S., <strong>and</strong>Janes, D.: ‘Device structure for electronic transport throughindividual molecules using nanoelectrodes’, Appl. Phys. Lett., 2005,87, p. 233509Micro & Nano Letters, Volume 1, Issue 2 87

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