109 resultados para B ... n C ... f.


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We investigate the quantum dynamics of the quantum-dot cellular automata qubit in the presence of a quantum point contact detector by modified rate equations. It is demonstrated that the qubit information can be resolved by measuring the detector current variation. Furthermore, we show that this oscillating current and the electron occupation probabilities in states \b> and \c> decay drastically as the dephasing rate increases, clearly revealing the influence of the dephasing induced by the detector. Moreover, it is shown that the operation speed of the quantum-dot cellular automata qubit may be adjusted by varying the interdot coupling strength. (C) 2003 American Institute of Physics.

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A systematic investigation of crystallographic and intrinsic magnetic properties of the hydrides R3Fe29 - xVxHy (R = Y, Ce, Nd, Sm, Gd, Tb, and Dy) has been performed in this work. The lattice constants a, b, and c and the unit cell volume of R3Fe29 - xVxHy decrease with increasing rare-earth atomic number from Nd to Dy, except for Ce, reflecting the lanthanide contraction. Hydrogenation results in regular anisotropic expansions along the a-, b-, and c-axes in this series of hydrides. Abnormal crystallographic and magnetic properties of Ce3Fe27.5V1.5H6.5, like Ce3Fe27.5V1.5, suggest that the Ce ion is non-triply ionized. Hydrogenation leads to the increase in both Curie temperature for all the compounds and in the saturation magnetization at 4.2 K and RT for R3Fe29 - xVx with R = Y, Ce, Nd, Sm, Gd, and Dy, except for Tb. Hydrogenation also leads to a decrease in the anisotropy field at 4.2 K and RT for R3Fe29 - xVx with R = Y, Ce, Nd, Gd, Tb, and Dy, except for Sm. The Ce3Fe27.5V1.5 and Gd3Fe28.4V0.6 show the larger storage of hydrogen with y = 6.5 and 6.9 in these hydrides. (C) 1998 Elsevier Science B.V. All rights reserved.

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Fourier transform photoluminescence measurements were carried out to investigate the optical transitions in InxGa1-xAs/InyAl1-yAs one-side-modulation-doped asymmetric step quantum wells. Samples with electron density n(s) between 0.8 and 5.3 x 10(12) cm(-2) rue studied. Strong recombination involving one to three populated electron subbands with the first heavy-hole subband is observed. Fermi edge singularity (FES) clearly can be observed for some samples. The electron subband energies in the InGaAs/InAlAs step quantum wells were calculated by a self-consistent method, taking into account strain and nonparabolicity effects and the comparison with the experimental data shows a good agreement. Our results can help improve understanding for the application of InGaAs/InAlAs step quantum wells in microelectronic and optoelectronic devices. (C) 1998 Elsevier Science Ltd. All rights reserved.

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High-quality InGaAs/InAlAs/InP high-electron-mobility transistor (HEMT) structures with lattice-matched or pseudomorphic channels have been grown by molecular-beam epitaxy (MBE). The purpose of this work is to enhance the channel conductivity by changing the epitaxial structure and growth process. With the use of pseudomorphic step quantum-well channel, the highest channel conductivity is achieved at x = 0.7, the corresponding electron mobilities are as high as 12300 (300 K) and 61000 cm(2)/V.s (77 K) with two-dimensional electron gas (2DEG) density of 3.3 x 10(12) cm(-2). These structures are comprehensively characterized by Hall measurements, photoluminescence, double crystal X-ray diffraction and transmission electron microscopy. Strong room-temperature luminescence is observed, demonstrating the high optical quality of the samples. We also show that decreasing the In composition in the InyAl1-yAs spacer is very effective to increase the 2DEG density of PHEMT structures. (C) 1998 Published by Elsevier Science B.V. All rights reserved.

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:(1).PHC/N.(2)BACC/NBC/N...

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The near-threshold highly bound states of all three stable isotopic variants of molecular hydrogen have been studied. Numerous perturbations and unexpected transitions are observed as far as 1cm(-1) just below the second dissociation threshold. This complex structure may arise from a combination of nonadiabatic coupling between B, B', C electronic states, perturbations due to. ne and hyperfine interactions, and strong shape resonances. The perturbed near-threshold states and vibrational continuum exhibit finegrained structure, differing greatly between isotopes because of varying nonadiabatic coupling.

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,,,(0.00.51.05.010.0ga.i.·kg-1),(),;;U=A/(1+B×C);0.322.8811.43ga.i.·kg-1;,18.61%8.36%,;

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沿""""Monte Carlo广Monte CarloBCBCBA/BCB80BBBO80%BA/BCBBA/BCABBBABCABCABMonte Car toBBABABAABABACBCABCABCBCACABAA/CCABAC'

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NiZrTi-VCrCrTiTi017Zr008V035Cr010Ni030BFeCoAlXRDICPSEMEDXXPSEIS线TiVCrTiVCrNiCrTi0.25-xZr_xV0.35Cr0.1Ni0.3x005-015bccc14LavesZr005008x008015xx00801550Tio17zr"sVscrol0Ni03303K313K9070275mAgTi17Zr008VSCr0Ni03050kJmolNlnBFeCAITio17zroosvo35Crol0Nio3Tio17Zr008Vo35Cro10Ni020Mnol390n1Ag253343KTiol7Zr08V035Cr0JONioz5Mnoos167298mAgZrVTiVCr

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Armco~-PH~-PH(a) 线Tafep(b)RpCI_cI_(2c)I_(3c)I_(4c)ΔE2E3ΔEEa = I_(2c)/I_c, b = I_(3c)/I_c, c = I_(4c)/I_(2c), (4b-3a~2)~(1/2)(3c-2b)~(1/2)(2c-a~2)~(1/2)S_jI_(corr) = I_c/S_j b_c = ΔE/lg((a+s_j)/2) b_a = -E/lg((a-s_j)/2)ΔEI_λSI_(corr) = from i=1 to n I/ from i=1 ton S_ b_c = form to n ΔE_/ form i=1 to n lg ((a_λ+S_)/2) b_a = form i=1 ton ΔE_/ form i=1 to n lg ((a_λ-S_)/2)LaplaceE_1(t) = λ_o(R_s+R_p) - 2_oR_p (e~(-)/RpC))/(1+e~(/RpC)) (o<<) E_2(t) = _o(R_s+R_p) + 2λ_oR_p (e~(-(-)/RpC))/(1+e~(λ/RpC)) <2)Eλ:ΔE = _oR_p (e~/RpC)-1)/(e~/RpC)+1) = 2λ_oR_p t_(anh)/(2RpC)) Δh = _o RsEhRp =E)/(2_o) >>RpC (_o)/(ΔE) = C/λ + 1/(2Rp) λ<pCR_pCR_s使R_p线λ_a = k_a [OH~-][ψ~-]~(0.5)e~(3/2Fψ/RT) λ_c = k_c [H~+] e~(/2RT) [((partial deriv) ψ_(corr))/((partial deriv) PH)]_([~-]) = -55 [((partial deriv) ψ_(corr))/((partial deriv) lg[~-])]_(PH) = -15 [((partial deriv) lg I_(corr))/((partial deriv) PH)]_([~-]) = -0.4 [((partial deriv) lg I_(corr))/((partial deriv) lg~-])]_(PH) = 0.13 α_(corr)/α lg[] = -44 α lg I_(corr)/α lg[] = 0.45 b_a = 40 b_c = 120 TafelTafelPHψ~-PHψ~-

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ab721cIII

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(SVMPs) , (Ophiophagus hannah)55,000Da N SQKKDFLEEKKYLELYIVADYVMFRN Ohagin Ohagin α-EDTA PMSF Ohagin TMVA cDNA Ohagin Ohagin cDNA 611 Ohagin P-III Ohagin P-22 Ohagin P-a P-b P-c P-III

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线bNiviventerMus musculus 932b93DNAA6B2CDNA1.2-0.131.64AB1.461.29-0.67 12184Genbank184660.950.01266Genbank62DNADNA84.03%DNADNA16 60022 00011 00020 00040 0006 70060 00016 000

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1176rCO3Lztciocyprinus2Sinocyclocheilus26small-scaledbarbidsSRparvusP.c.chunglienensisGp.potaniniL.langsoniP.pingiregani线saBbaoshanensisC.auratusC(C)chilia122463PAUPl1退198413419812000'33198419814506015线ae7

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BWWBSAA2318750AR spermBalb/CNT spermELISA23U937RajiJurkatNTARSASI1.NTARELISA12ARA6NTB5C2.2321IgMIgC_1IgG_(2a)3.23ABC4.NT sperm, AR spermARNT5.996.916146kDa1410WHOWHO