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A one-dimensional system of Si(111)-(5 x 2)-Au is explored using scanning tunneling microscopy and spectroscopy. The chain of Si adatoms called bright protrusions (BP's) is found to be semiconducting with an evanescent state in the gap, which originates from adjoining metallic BP-free segments. A quantitative analysis shows that the evanescent state decays in inverse-Gaussian form, leading to an appearance of a parabolic BP chain, and scales to its chain length. Spatial decay of the state suggests a quadratic band bending and the existence of a Schottky-like potential barrier at the interface driven by charge transfer.  相似文献   
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Paramagnetic and diamagnetic contributions to the magnetic susceptibility are calculated for a layered superlattice as a function of the temperature in both degenerate and nondegenerate regimes. The susceptibility shows distinctly different temperature dependences as the inter-layer bandwidth as well as the Fermi energy is varied from a two-dimensional to a three-dimensional regime, thus giving valuable information about the electron density and the inter-layer tunneling.  相似文献   
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The initial oxidation process of the ultraclean Si(001)-c(4x2) surface is studied using scanning tunneling microscopy at low temperature. At the early stage of oxygen adsorption, reactions with Si atoms at SB steps are dominant over those at terraces by more than 2 orders of magnitude, and they proceed in two distinct stages to high oxidation states. Guided by the ab initio calculations, the oxidation structures at each stage are proposed. The extreme reactivity of the step edge is due to the presence of rebonded adatoms with dangling bonds and weak rebonds, and their proximity allows the formation of -Si-O- chain structures along the step edge, unlike those on the Si(111) surface.  相似文献   
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In this study, the grain boundary diffusion of Cu through a TiN layer with columnar structure was investigated by X-ray photoelectron spectroscopy (XPS). It was observed that Cu atoms diffuse from the Cu layer to the surface along the grain boundaries in the TiN layer at elevated temperature. In order to estimate the grain boundary diffusion constants, we used the surface accumulation method. The diffusivity of Cu through TiN layer with columnar structure from 400 °C to 650 °C is Db≈6×10−11exp(−0.29/(kBT )) cm2/s. Received: 18 May 1999 / Accepted: 8 September 1999 / Published online: 23 February 2000  相似文献   
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The electrical resistivity arising from electron-electron Umklapp scattering is calculated at low temperatures for the anisotropic but two-dimensional charge-transfer complex (TMTSF)2PF6. Also, we consider a specular scattering correction to a recent one-phonon scattering mechanism and find a significant change in the temperature dependent behavior of the resistivity. Finally an exact solution is obtained for the resistivity arising from two-libron scattering and is found to give a small contribution at low temperatures. Comparing these results with recent data, we find that the electron-electron mechanism yields the most satisfactory agreement at low temperatures, while contributions from the other two mechanisms may not be negligible at high temperatures.  相似文献   
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Scanning tunneling microscopy of a quasi-one-dimensional (1D) metal-insulator transition in an In nanowire array on the Si(111) surface reveals unprecedented details in the transition dynamics. The transition proceeds in microscopic first order, namely, through the domain-by-domain conversion at the nanoscale, from the metallic to the insulating phase or vice versa. The definition of domains and their effective transition temperatures (Tc) are strongly correlated with the distribution of defects. Below Tc, the condensation and the fluctuation of 1D charge density waves are observed within the isolated metallic domains, as well as at the domain boundaries. The appearance of such isolated condensates suggests a strong intrawire coupling: a manifestation of the 1D nature of the critical fluctuation, as well as the origin of the first-order transition.  相似文献   
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S.K. Lyo 《Journal of luminescence》2012,132(11):3035-3041
Photon-mediated energy transfer is shown to play an important role for transfer of an electron–hole plasma between two quasi-two-dimensional quantum wells separated by a wide barrier. The magnitude and the dependence of the transfer rate of an electron–hole plasma on the temperature, the well-to-well distance, and the plasma density are compared with those of the standard Förster (i.e., dipolar) rate and also with the exciton transfer rate. The plasma transfer rate through the photon-exchange mechanism decays very slowly as a function of the well-to-well distance and is larger than the dipolar rate except for short distances. The transfer rate of plasmas saturates at high densities and decays rapidly with the temperature.  相似文献   
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