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1.
J Am Chem Soc ; 131(1): 22-3, 2009 Jan 14.
Article in English | MEDLINE | ID: mdl-19072281

ABSTRACT

A multi-readout orthogonal detection of alloy nanowire barcodes is shown to maximize the identification power of such encoded nanostructures. The built-in redundancy associated with the simultaneous use of several independent and powerful readout modes, based on different distinct processes and phenomena, offers great promise for decoding barcoded nanomaterials and for meeting the major challenges of product protection and multiplexed biodetection.


Subject(s)
Alloys/chemistry , Electronic Data Processing/methods , Nanotechnology/methods , Nanowires/chemistry , Indium/chemistry , Nickel/chemistry , Zinc/chemistry
3.
J Phys Chem B ; 110(3): 1137-40, 2006 Jan 26.
Article in English | MEDLINE | ID: mdl-16471655

ABSTRACT

We investigated silicon nanoclusters Si(nc) in a SiO2 matrix prepared by the plasma-enhanced chemical vapor deposition technique, using X-ray photoelectron spectroscopy (XPS) with external voltage stimuli in both static and pulsed modes. This method enables us to induce an additional charging shift of 0.8 eV between the Si2p peaks of the oxide and the underlying silicon, both in static and time-resolved modes, for a silicon sample containing a 6 nm oxide layer. In the case of the sample containing silicon nanoclusters, both Si2p peaks of Si(nc) and host SiO2 undergo a charging shift that is 1 order of magnitude larger (>15 eV), with no measurable difference between them (i.e., no differential charging between the silicon nanoclusters and the oxide matrix could be detected). By use of a measured Auger parameter, we estimate the relaxation energy of the Si(nc) in the SiO2 matrix as -0.4 eV, which yields a -0.6 eV shift in the binding energy of the Si(nc) with respect to that of bulk Si in the opposite direction of the expected quantum size effect. This must be related to the residual differential charging between the silicon nanoclusters and the oxide host. Therefore, differential charging is still the biggest obstacle for extracting size-dependent binding energy shifts with XPS when one uses the oxide peak as the reference.


Subject(s)
Nanostructures/chemistry , Silicon Dioxide/chemistry , Silicon/chemistry , Photons , Sensitivity and Specificity , Spectrum Analysis , Surface Properties , X-Rays
4.
J Phys Chem B ; 109(50): 24182-4, 2005 Dec 22.
Article in English | MEDLINE | ID: mdl-16375410

ABSTRACT

By recording XPS spectra while applying external voltage stress to the sample rod, we can control the extent of charging developed on core-shell-type gold nanoparticles deposited on a copper substrate, in both steady-state and time-resolved fashions. The charging manifests itself as a shift in the measured binding energy of the corresponding XPS peak. Whereas the bare gold nanoparticles exhibit no measurable binding energy shift in the Au 4f peaks, both the Au 4f and the Si 2p peaks exhibit significant and highly correlated (in time and magnitude) shifts in the case of gold (core)/silica (shell) nanoparticles. Using the shift in the Au 4f peaks, the capacitance of the 15-nm gold (core)/6-nm silica (shell) nanoparticle/nanocapacitor is estimated as 60 aF. It is further estimated that, in the fully charged situation, only 1 in 1000 silicon dioxide units in the shell carries a positive charge during our XPS analysis. Our simple method of controlling the charging, by application of an external voltage stress during XPS analysis, enables us to detect, locate, and quantify the charges developed on surface structures in a completely noncontact fashion.


Subject(s)
Gold/chemistry , Nanostructures/chemistry , Silicon Dioxide/chemistry , Sensitivity and Specificity , Spectrometry, X-Ray Emission/methods
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