Accurate valence band maximum determination for SrTiO3(001)

Abstract We reexamine a well-established method for determining valence band maxima (VBM) in semiconductors based on fitting photoemission valence band spectra to theoretical densities of states. In contrast to the situation for covalent semiconductors, application of this technique to SrTiO3 produces poor fits when the density of states is computed within the local density or generalized gradient approximation. The resulting VBM is too high by several tenths of an eV. However, an excellent fit, and a more physically reasonable VBM, is obtained when the density of states is computed within a recently-developed self-consistent GW approximation. Extrapolating the X-ray excited leading edge to the energy axis, and finding the energy at which the UV-excited leading edge intensity goes to zero, also yield physically reasonable VBM values that are in good mutual agreement, and in good agreement with the VBM obtained by fitting to GW theory. These numbers are useful for accurate band offset determination.

[1]  E. A. Kraut,et al.  Precise Determination of the Valence-Band Edge in X-Ray Photoemission Spectra: Application to Measurement of Semiconductor Interface Potentials , 1980 .

[2]  Maruyama,et al.  Angle-resolved photoemission study of SrTiO3 (100) and (110) surfaces. , 1996, Physical review. B, Condensed matter.

[3]  James R. Chelikowsky,et al.  Nonlocal pseudopotential calculations for the electronic structure of eleven diamond and zinc-blende semiconductors , 1976 .

[4]  Y. Aiura,et al.  Photoemission study of the metallic state of lightly electron-doped SrTiO3 , 2002 .

[5]  Jackson,et al.  Atoms, molecules, solids, and surfaces: Applications of the generalized gradient approximation for exchange and correlation. , 1992, Physical review. B, Condensed matter.

[6]  E. A. Kraut,et al.  Semiconductor core-level to valence-band maximum binding-energy differences: Precise determination by x-ray photoelectron spectroscopy , 1983 .

[7]  Alfonso Franciosi,et al.  Heterojunction band offset engineering , 1996 .

[8]  T. Higuchi,et al.  Electronic structure of p -type SrTiO 3 by photoemission spectroscopy , 1998 .

[9]  R. Droopad,et al.  Band offset and structure of SrTiO3 /Si(001) heterojunctions , 2001 .

[10]  C. Sa,et al.  Epitaxial growth and band bending of n- and p-type Ge on GaAs(001) , 1988 .

[11]  L. Hedin NEW METHOD FOR CALCULATING THE ONE-PARTICLE GREEN'S FUNCTION WITH APPLICATION TO THE ELECTRON-GAS PROBLEM , 1965 .

[12]  G. M. Stocks,et al.  The Interface Phase and the Schottky Barrier for a Crystalline Dielectric on Silicon , 2003, Science.

[13]  C. Fadley,et al.  Observation of d -band narrowing near copper and nickel surfaces by means of angle-resolved x-ray photoelectron spectroscopy , 1979 .

[14]  R. Droopad,et al.  Band discontinuities at epitaxial SrTiO3/Si(001) heterojunctions , 2000 .

[15]  J. Perdew,et al.  Accurate and simple density functional for the electronic exchange energy: Generalized gradient approximation. , 1986, Physical review. B, Condensed matter.

[16]  G. Dresselhaus,et al.  Surface defects and the electronic structure of SrTi O 3 surfaces , 1978 .

[17]  J. W. Rogers,et al.  Band offsets for the epitaxial TiO2/SrTiO3/Si(001) system , 2003 .

[18]  Horst Rogalla,et al.  Quasi-ideal strontium titanate crystal surfaces through formation of strontium hydroxide , 1998 .

[19]  N. Shanthi,et al.  Electronic structure of electron doped SrTiO 3 : SrTiO 3 − δ and Sr 1 − x La x TiO 3 , 1998 .

[20]  Roger H. French,et al.  Bulk electronic structure of SrTiO3: Experiment and theory , 2001 .

[21]  H. Koinuma,et al.  Atomic Control of the SrTiO3 Crystal Surface , 1994, Science.

[22]  L. Mattheiss Energy Bands for KNiF_{3}, SrTiO_{3}, KMoO_{3}, and KTaO_{3} , 1972 .

[23]  C. Fadley,et al.  Surface d-Band Narrowing in Copper from Angle-Resolved X-Ray Photoelectron Spectra , 1977 .