Dangling-bond surface states on the Si and Ge(111) surfaces

1978 ◽  
Vol 11 (6) ◽  
pp. 1217-1222 ◽  
Author(s):  
M Nishida
Keyword(s):  
1976 ◽  
Vol 9 (16) ◽  
pp. L429-L432 ◽  
Author(s):  
F Flores ◽  
F Garcia-Moliner ◽  
E Louis ◽  
C Tejedor

1984 ◽  
Vol 30 (12) ◽  
pp. 7355-7357 ◽  
Author(s):  
J. M. Layet ◽  
J. Y. Hoarau ◽  
H. Lüth ◽  
J. Derrien
Keyword(s):  

2000 ◽  
Vol 638 ◽  
Author(s):  
Sergey K. Gordeev ◽  
Peter I. Belobrov ◽  
Nikolay I. Kiselev ◽  
Eleonora A. Petrakovskaya ◽  
Thommy C. Ekstrom

AbstractPorous solids made of nano diamonds cemented by pyrocarbon show a semiconductor behavior where the properties are controlled by the factor γ = mass ratio of sp2/sp3 phases. The volume electrical conductivity μ (T) was measured in the temperature range 77 - 290 K as a function of γ. By controlling the ratio γ from 0 to 50 %, the electrical conductivity will change by 12 orders of magnitude. The semiconductor activation energy depends on γ-ratio and has values between 0.03 - 0.3 eV. The variable-range hopping conduction was checked by measuring μ against T and to look for a T1/4 dependence. A positive thermoelectric power showed that NDC was p-semiconductor with a narrow band gap. The paramagnetic nanodiamonds, g = 2.0027(1) and δH = 0.86(2) mT, will still have this property in the NDC material and both the g-value and line width are not dependent on γ-ratio and temperature. The concentration of unpaired electrons is 41019 spin/g that equals to one dangling bond per nanodiamond particle. Absences of magnetoresistance and Hall potential were observed for all NDC materials. This was interpreted as resulting from a Tamm - Lifshitz - Pekar electronic conduction mechanism within onedimensional band of surface states.


2011 ◽  
Vol 222 ◽  
pp. 56-61
Author(s):  
K.Z. Liu ◽  
Masaru Shimomura ◽  
Y. Fukuda

Surface electronic structures of n-GaP(001) and p-InP(001) with and without sulfur treatment have been studied by X-ray photoelectron spectroscopy (XPS), synchrotron radiation photoemission spectroscopy (SRPES), and inverse photoemission spectroscopy (IPES). The Fermi level (EF) of a clean n-GaP(001)-(2x4) surface is found to be pinned at 0.2 eV above the valence band maximum (VBM), suggesting that the surface electronic bands are bent upward. XPS spectra reveal that the EF is moved to 2.3 eV above the VBM by the sulfur treatment, implying that the sulfur-treated surface has flat bands. The IPES result shows that empty dangling bond states on Ga atoms at the surface are located at the conduction band minimum (CBM) and they disappeared with the treatment. SRPES spectra of a clean p-InP(001)-(2x4) surface indicate that the EF is located at 0.3 eV above the VBM and surface states due to phosphorus atoms are at –0.9 eV below the EF. The result implies that the surface has almost flat bands. Empty dangling bond states on In atoms at the clean surface are found to be located at the conduction band edge. Surface states due to the In-S bonds are found at –3.5 eV below the EF for the sulfur-treated surface. The sulfur treatment of the clean surface leads to a little shift (0.1 –0.2 eV) of the EF and to considerable reduction of the empty states in the band gap. A type conversion of p- to n- is not observed in the present work. This is discussed in terms of the thickness of a sulfide layer.


1982 ◽  
Vol 44 (12) ◽  
pp. 1633-1636 ◽  
Author(s):  
E. Louis ◽  
F. Flores ◽  
F. Guinea ◽  
C. Tejedor

1996 ◽  
Vol 357-358 ◽  
pp. 427-431 ◽  
Author(s):  
Y.Q. Cai ◽  
P. Storer ◽  
A.S. Kheifets ◽  
I.E. McCarthy ◽  
E. Weigold

1992 ◽  
Vol 259 ◽  
Author(s):  
Jaewon Cho ◽  
T.P. Schneider ◽  
R.J. Nemanich

ABSTRACTThe surfaces of Si(100) and Ge(100), cleaned at low temperatures by H-plasma, were studied by Angle Resolved UV-Photoemission Spectroscopy(ARUPS). In the case of Si(100), H-plasma exposure produced ordered H-terminated crystallographic structures with either a 2×1 or 1×1 LEED pattern while for Ge(100) a weak H-terminated 2x1 pattern was obtained. The hydride phases, found on the surfaces of the cleaned Si(100), were shown to depend on the temperature of the surface during H-plasma cleaning. The electronic states for the monohydride and dihydride phases were identified by ARUPS. When the plasma cleaned surface was annealed, the phase transition from the dihydride to monohydride was observed. For the Ge(100) surface, an ordered 2x1 monohydride phase was obtained from the surface cleaned at 180°C. After plasma exposure at ≤170°C a 1×1 surface was observed, but the ARUPS indicated that the surface was predominantly composed of disordered monohydride structures. After annealing above the H-dissociation temperatures, the dangling bond surface states were identified for both Si and Ge. The Si(100) and Ge(100) ARUPS spectra shifted after annealing, indicating that the H-terminated surfaces were unpinned.


Author(s):  
J.C.H. Spence ◽  
J. Mayer

The Zeiss 912 is a new fully digital, side-entry, 120 Kv TEM/STEM instrument for materials science, fitted with an omega magnetic imaging energy filter. Pumping is by turbopump and ion pump. The magnetic imaging filter allows energy-filtered images or diffraction patterns to be recorded without scanning using efficient parallel (area) detection. The energy loss intensity distribution may also be displayed on the screen, and recorded by scanning it over the PMT supplied. If a CCD camera is fitted and suitable new software developed, “parallel ELS” recording results. For large fields of view, filtered images can be recorded much more efficiently than by Scanning Reflection Electron Microscopy, and the large background of inelastic scattering removed. We have therefore evaluated the 912 for REM and RHEED applications. Causes of streaking and resonance in RHEED patterns are being studied, and a more quantitative analysis of CBRED patterns may be possible. Dark field band-gap REM imaging of surface states may also be possible.


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