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Eermi surface

Loucks, T.L. (1966) Relativistic Electronic Structure in Crystals. II. Eermi Surface of Tungsten. Physical Review, 143, 506-512. [Pg.242]

Oshima K, Mori T, hiokuchi H, Urayama H, Yamochi H, Saito G (1988) Shubnikov-de Haas effect and the Eermi surface in an ambient-pressure organic superconductor (bis (ethylenedithiolo)tetrathiafulvalene)2Cu(NCS)2. Phys Rev B 38 938-941... [Pg.119]

The continuum model with the Hamiltonian equal to the sum of Eq. (3.10) and Eq. (3.12), describing the interaction of electrons close to the Eermi surface with the optical phonons, is called the Takayama-Lin-Liu-Maki (TLM) model [5, 6]. The Hamiltonian of the continuum model retains the important symmetries of the discrete Hamiltonian Eq. (3.2). In particular, the spectrum of the single-particle states of the TLM model is a symmetric function of energy. [Pg.69]

Anisotropic thermopower effects are observed in the CufNCSlj, Cu(CN)[N(CN)2], and Cu[N(CN)2]Br salts. The thermopower is negative in the direction of the electron-like Eermi surfaces, while it is positive in the direction of the hole pockets. The anisotropic temperature dependence is more quantitatively explained based on the Boltzmann equation by using the calculated band structure with some modification of the bandwidth. The optical spectra in the infrared region of the Cu(NCS)2 and Cu[N(CN)2]Br salts are ascribed to a mixture of intra- and interband transitions (centered around 2200 cm- c, and around 3500 cm b for the Cu(NCS)2 salt). [Pg.334]

Vickerman and Ertl (1983) have studied H2 and CO chemisorption on model Cu-on-Ru systems, where the Cu is deposited on single-crystal (0001) Ru, monitoring the process using LEED/Auger methods. However, the applicability of these studies carried out on idealized systems to real catalyst systems has not been established. Significant variations in the electronic structure near the Eermi level of Cu are thought to occur when the Cu monolayer is deposited on Ru. This implies electron transfer from Ru to Cu. Chemical thermodynamics can be used to predict the nature of surface segregation in real bimetallic catalyst systems. [Pg.197]

The term Ed, stands for charging contributions. This term is absent in spectra of samples exhibiting a finite density of states at the Eermi level. For all practical purposes this is correct for aU true metals and for many semiconductors with intrinsic states near zero binding energy. Many systems relevant in catalysis do, however, not fulfill this condition (all non-black samples, glasses, porous materials, supports) or even worse, are composites of metallic and non-metaUic systems, giving rise to mixed metalhc-insulating behavior of their surface under PES. Such... [Pg.252]

Exploring various phenomena at metal/solution interfaces relates directly to heterogeneous catalysis and its applications to fuel cell catalysis. By the late 1980s, electrochemical nuclear magnetic resonance spectroscopy (EC-NMR) was introduced as a new technique for electrochemical smface science. (See also recent reviews and some representative references covering NMR efforts in gas phase surface science. ) It has been demonstrated that electrochemical nuclear magnetic resonance (EC-NMR) is a local surface and bulk nanoparticle probe that combines solid-state, or frequently metal NMR with electrochemistry. Experiments can be performed either under direct in situ potentiostatic control, or with samples prepared in a separate electrochemical cell, where the potential is both known and constant. Among several virtues, EC-NMR provides an electron-density level description of electrochemical interfaces based on the Eermi level local densities of states (Ef-LDOS). Work to date has been predominantly conducted with C and PtNMR, since these nuclei... [Pg.1]

Enhancing the catalysis at the surface of PEC electrodes results in a lower kinetic overpotential and an increase in photocurrent. The effectiveness of the catalysts after surface treatment can be determined by utilizing three-electrode j-V measurements (see Section Three-Electrode j-V and Photocurrent Onset ) as well as IPCE measurements (see Chapter Incident Photon-to-Current Efficiency and Photocurrent Spectroscopy ). It may also useful to perform Mott-Schottky (see Section Mott-Schottky ) to determine any impacts these catalysts may have on the band structure (e.g., due to Eermi level pinning). [Pg.37]

E. Yablonovitchet al., Band-Bending, Eermi Level Pinning and Surface fixed Charge on Chemically Prepared GaAs Surfaces, Appl. Phys. Lett. 1989,54, 555-557. [Pg.148]


See other pages where Eermi surface is mentioned: [Pg.151]    [Pg.310]    [Pg.151]    [Pg.310]    [Pg.83]    [Pg.88]    [Pg.3]    [Pg.288]    [Pg.4229]    [Pg.3364]    [Pg.1156]    [Pg.816]    [Pg.528]   


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