965 research outputs found
The influence of a single defect in composite gate insulators on the performance of nanotube transistors
The current through a carbon nanotube field-effect transistor (CNFET) with
cylindrical gate electrode is calculated using the nonequilibrium Greens
function method in a tight-binding approximation. The obtained result is in
good agreement with the experimental data. The space radiation and nuclear
radiation are known to cause defects in solids. The theoretical approach is
used to calculate the amplitude of the random-telegraph-signal (RTS) noise due
to a single defect in the gate oxide of a long channel p-type CNFET. We
investigate how the amplitude of the RTS noise is affected by the composite
structure of gate insulators, which contains an inner insulator with a
dielectric constant larger than 3.9 and an outer insulator with a dielectric
constant of 3.9 (as for SiO2). It is found that the RTS amplitude increases
apparently with the decreasing thickness of the inner gate insulator. If the
inner insulator is too thin, even though its dielectric constant is as large as
80, the amplitude of the RTS noise caused by the charge of Q = +1e may amount
to around 80% in the turn-on region. Due to strong effects of defects in
CNFETs, CNFETs have a potential to be used for detecting the space radiation or
nuclear radiation.Comment: 8 Figure
Intrinsic Regularization Method in QCD
There exist certain intrinsic relations between the ultraviolet divergent
graphs and the convergent ones at the same loop order in renormalizable quantum
field theories. Whereupon we may establish a new method, the intrinsic
regularization method, to regularize those divergent graphs. In this paper, we
apply this method to QCD at the one loop order. It turns out to be
satisfactory:The gauge invariance is preserved manifestly and the results are
the same as those derived by means of other regularization methods.Comment: 18 pages, LaTeX , 7 figures in a separate compressed postscript fil
Organometallic chemical vapor deposition of copper oxide thin films
Copper oxide thin films were prepared by organometallic chemical vapor deposition (OMCVD or MOCVD) technique. This MOCVD process uses copper acetylacetonate (Cu(acac)[subscript]2) as the copper precursor. Spectroscopic (X-ray photoelectron spectroscopy (XPS), Auger electron spectroscopy (AES), and infrared spectroscopy (IR)) and diffraction (X-ray diffraction (XRD)) methods were employed to analyze the chemical composition and oxidation state of copper in these films. According to spectroscopic results, the composition of these MOCVD film primarily depends on the deposition temperature and partial pressures of the reactants. As indicated by XPS and XRD results, Cu[subscript]2O films were prepared at 360°C, with an oxygen partial pressure of 150 torr and copper precursor partial pressure of 0.20 torr. CuO films were grown at temperatures above 420°C, with an oxygen pressure of 190 torr and precursor pressure of 0.20 torr. By using water vapor instead of oxygen as the co-reactant, Cu films were deposited at temperatures above 380°C, with a water vapor pressure of 15 torr and precursor pressure of 0.20 torr. To examine the specific mechanism of precursor decomposition, a molecular vibrational spectroscopic technique, Fourier Transform Infrared spectroscopy (FTIR), was employed to investigate the vapor phase product distribution in the MOCVD effluent stream. Based on FTIR results, a kinetic model was proposed. This model suggests that steric effect from chelating ligands and bond strength sequence in the precursor molecule are the principle factors determining the decomposition products of Cu(acac)[subscript]2 in the MOCVD reactor. Differential scanning calorimetry (DSC) was used to study the pyrolysis pattern of Cu(acac)[subscript]2. Particularly, the impacts of oxygen concentration, carrier gas molecular weight, and heating rate on the pyrolysis of this precursor were studied. From DSC results, it seems that Cu(acac)[subscript]2 undergoes a single-step, exothermic reaction in the ambient with oxygen gas present. In DSC pattern, the exothermic peak height also increased as oxygen concentration increased. The activation energy for the exothermic step was derived by Kissinger equation as 20 kcal/mol. Based on experimental results of deposition, FTIR, and DSC, it seems that a deposition temperature above a critical value is necessary to initiate the decomposition of Cu(acac)[subscript]2 and oxygen can assist this reaction by accelerating the reaction rate
A Robust Quantum Random Access Memory
A "bucket brigade" architecture for a quantum random memory of memory
cells needs times of quantum manipulation on control circuit nodes
per memory call. Here we propose a scheme, in which only average times
manipulation is required to accomplish a memory call. This scheme may
significantly decrease the time spent on a memory call and the average overall
error rate per memory call. A physical implementation scheme for storing an
arbitrary state in a selected memory cell followed by reading it out is
discussed.Comment: 5 pages, 3 figure
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