903 research outputs found

    Improvements in diagnosis have changed the incidence of histological types in advanced gastric cancer.

    Get PDF
    The data on 912 patients with early cancer and 1245 with advanced cancer who were seen between 1971 and 1990 were compared. The incidence of undifferentiated-type cancer increased significantly in patients with advanced gastric cancer, but not in patients with early gastric cancer. When the histological types were compared with regard to sex, age and location in patients with early gastric cancer the undifferentiated type was found to increase only in males, while in patients with advanced gastric cancer the undifferentiated type increased in both sexes as well as in younger patients and in both the upper and middle third of the stomach. These differences in the trends between early and advanced cancers are probably due to the different degrees of diagnostic accuracy for the early detection of histological types

    Importance of the V 3d-O 2p hybridization in the Mott-Hubbard material V2O3

    Full text link
    We studied the changes in the electronic structure of V2O3 using a cluster model. The calculations included fluctuations from the coherent band in the metallic phase, and non-local Mott-Hubbard fluctuations in the insulating phase. The incoherent structure is mostly related to the usual ligand screening channel (3d2L). The coherent peak in the metallic phase corresponds to coherent band fluctuations (3d2C). The non-local screened state in the insulating phase (3d2D) appears at higher energies, opening the band gap. The photon energy dependence of the spectra is mostly due to the relative V 3d and O 2p cross sections. The present model reproduces also the observed changes in the V 1s core-level spectra. The above results suggest that the Mott-Hubbard transition in V2O3 requires a multi-band model.Comment: 4 pages, 4 figure

    Layer dependent band dispersion and correlations using tunable Soft X-ray ARPES

    Full text link
    Soft X-ray Angle-Resolved Photoemission Spectroscopy is applied to study in-plane band dispersions of Nickel as a function of probing depth. Photon energies between 190 and 780 eV were used to effectively probe up to 3-7 layers. The results show layer dependent band dispersion of the Delta_2 minority-spin band which crosses the Fermi level in 3 or more layers, in contrast to known top 1-2 layers dispersion obtained using ultra-violet rays. The layer dependence corresponds to an increased value of exchange splitting and suggests reduced correlation effects in the bulk compared to the surface.Comment: 7 pages, 3 figures Revised text and figur

    Temperature dependent Eu 3d-4f X-ray Absorption and Resonant Photoemission Study of the Valence Transition in EuNi2(Si0.2Ge0.8)2EuNi_2(Si_{0.2}Ge_{0.8})_2

    Full text link
    We study the mixed valence transition (TTv_{v} ∼\sim80 K) in EuNi2_{2}(Si0.2_{0.2}Ge0.8_{0.8})2_{2} using Eu 3d−4fd-4f X-ray absorption spectroscopy (XAS) and resonant photoemission spectroscopy (RESPES). The Eu2+^{2+} and Eu3+^{3+} main peaks show a giant resonance and the spectral features match very well with atomic multiplet calculations. The spectra show dramatic temperature (TT)-dependent changes over large energies (∼\sim10 eV) in RESPES and XAS. The observed non-integral mean valencies of ∼\sim2.35 ±\pm 0.03 (TT = 120 K) and ∼\sim2.70 ±\pm 0.03 (TT = 40 K) indicate homogeneous mixed valence above and below TTv_{v}. The redistribution between Eu2+^{2+}4f74f^7+[spd]0[spd]^0 and Eu3+^{3+}4f64f^6+[spd]1[spd]^1 states is attributed to a hybridization change coupled to a Kondo-like volume collapse.Comment: 4 pages, 3 figure

    Bulk screening in core level photoemission from Mott-Hubbard and Charge-Transfer systems

    Full text link
    We report bulk-sensitive hard X-ray (hνh\nu = 5.95 KeV) core level photoemission spectroscopy (PES) of single crystal V1.98_{1.98}Cr0.02_{0.02}O3_{3} and the high-TcT_c cuprate Bi2_2Sr2_{2}CaCu2_{2}O8+δ_{8+\delta} (Bi2212). V1.98_{1.98}Cr0.02_{0.02}O3_{3} exhibits low binding energy "satellites" to the V 2p2p "main lines" in the metallic phase, which are suppressed in the antiferromagnetic insulator phase. In contrast, the Cu 2p2p spectra of Bi2212 do not show temperature dependent features, but a comparison with soft X-ray PES indicates a large increase in the 2p53d92p^5 3d^9 "satellites" or 3d93d^9 weight in the bulk. Cluster model calculations, including full multiplet structure and a screening channel derived from the coherent band at the Fermi energy, give very satisfactory agreement with experiments

    Spin-polarized surface state of MnSb(0001)

    Get PDF
    Knowledge of the spin-dependent electronic structure at surfaces and interfaces plays an increasingly important role when assessing possible use of novel magnetic materials for spintronic applications. It is shown that spin- and angle-resolved photoelectron spectroscopy together with ab initio electronic structure methods provides a full characterization of the surface electronic structure of ferromagnetic MnSb(0 0 0 1). Two different surface reconstructions have been compared in spin- and angle-resolved valence-band photoemission. For annealing at elevated temperatures, the ( 1 x 1)-structure transforms into 2 x 2 and a majority-spin peak appears at - 1.7 eV inside a majority-spin bulk band gap at the surface Brillouin zone centre. Its sensitivity to oxygen supports an interpretation as magnetic compound surface state. Local spin density calculations predict at the same energy (- 1.75 eV) a prominent d(z)2 surface state of majority spin for ( 1 x 1)- Mn terminated MnSb(0 0 0 1) but no such feature for ( 1 x 1)-Sb termination. The calculation shows that neither the bulk nor the surface is half-metallic, in agreement with the expectation for the hexagonal NiAs structure

    Impact Ionization in ZnS

    Full text link
    The impact ionization rate and its orientation dependence in k space is calculated for ZnS. The numerical results indicate a strong correlation to the band structure. The use of a q-dependent screening function for the Coulomb interaction between conduction and valence electrons is found to be essential. A simple fit formula is presented for easy calculation of the energy dependent transition rate.Comment: 9 pages LaTeX file, 3 EPS-figures (use psfig.sty), accepted for publication in PRB as brief Report (LaTeX source replaces raw-postscript file

    Bulk Electronic structure of Na0.35_{0.35}CoO2_{2}.1.3H2_{2}O

    Full text link
    High-energy (hν\nu = 5.95 keV) synchrotron Photoemission spectroscopy (PES) is used to study bulk electronic structure of Na0.35_{0.35}CoO2_{2}.1.3H2_{2}O, the layered superconductor. In contrast to 3-dimensional doped Co oxides, Co 2p\it{2p} core level spectra show well-separated Co3+^{3+} and Co4+^{4+} ions. Cluster calculations suggest low spin Co3+^{3+} and Co4+^{4+} character, and a moderate on-site Coulomb correlation energy Udd∼_{dd}\sim3-5.5 eV. Photon dependent valence band PES identifies Co 3d\it{3d} and O 2p\it{2p} derived states, in near agreement with band structure calculations.Comment: 4 pages 4 figures Revised text added referenc
    • …
    corecore