Angle -Scanned X-ray Photoelectron Diffraction (XPD) - PowerPoint PPT Presentation

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Angle -Scanned X-ray Photoelectron Diffraction (XPD)

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Epitaxial growth - Vanadium and Vanadium Oxides on TiO2 (110) -0.2 ML V on TiO2 (110) ... Home Lab XPS ARXPS XPD LEED e-beam evaporator Gas line e-beam heater ... – PowerPoint PPT presentation

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Title: Angle -Scanned X-ray Photoelectron Diffraction (XPD)


1
Angle -Scanned X-ray Photoelectron Diffraction
(XPD)
2
Energy -Scanned X-ray Photoelectron
Diffraction Angle Resolved Photoemission Fine
Structure (ARPEFS)
3
The Physical Origin of Intensity Modulations
4
The Shape of the Primary Wave
dipole selection rules Dl1
s initial state Dl1
5
The Amplitude of Scattered Waves Scattering
Factors and their Energy Dependence
6
FS vs BS
FS dominates for KE500 eV - direct information
about interatomic directions with no
need of theoretical simulations
- if simulations are needed, Single
Scattering is often OK.
7
Simulations
-cluster based (from a few to several hundred
atoms)
  • real space (long range order not explicitly
    needed)
  • electron waves (plane or curved) scattered off
    muffin-tin atomic potentials

- calculations of I(k) repeated as a function of
(q, f) or k.
-SSC-SW
-MSC-SW (MSCD by Chen and van Hove TXPD by
Fadley and coworkers)
8
A Note on Short-Range Order
9
Experimental - Home Lab
XPD
LEED
XPS
e-beam evaporator
Gas line
ARXPS
e-beam heater
10
Experimental - ELETTRA SRS
11
Chemisorption Formate on Cu (100)
M. Sambi, G. Granozzi, M. Casarin, G. A. Rizzi,
A. Vittadini, L. S. Caputi and G. Chiarello
Surf. Sci., 315 (1994) 309.
  1. Cross Bridge (CB)
  2. Diagonal Atop (DA)
  3. Short Bridge (SB)

12
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13
Quantitative determination SSC-SW simulations
d(Cu-O) 1.950.05 Å lt(OCO) 1295
14
  • pseudomorphic growth
  • Kikuchi bands developed medium-to-long range
    order

15
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16
Polar PD
17
zV-O(expt.)0.720.07 Å zV-O(DFT)0.723 Å
18
Soft phonon mode involving in-plane
displacements of O scatterers with respect to V
emitters?
19
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20
w4025 cm-1
21
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22
O 1s and Zn 3s, KE300 eV
23
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24
Why does it work?
25
Near Node Photoelectron Holography
26
  • problems due to the strong anisotropy of
    electron-atom scattering
  • both in amplitude and in phase

27
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28
Near Node Photoelectron Holography - the
Experiment
J. Wider, F. Baumberger, M. Sambi, R. Gotter, A.
Verdini, F. Bruno, D. Cvetko, A. Morgante, T.
Greber and J. Osterwalder,Phys. Rev. Lett. 86
(2001) 2337.
J. Spence, Nature 410 (2001) 1037.
29
BESSY II
The role of the Si-suboxide structure at the
interface an angle scanned photoelectron
diffraction study
C. Westphal, S. Dreiner, M. Schürman, F. Senf, H.
Zacharias, Thin Solid Films 400 (2001) 101.
30
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31
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32
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33
ALS
Surface core level shift PD clean W (110), (1x1)
Fe/W(110) and (7x14) Gd/W(110)
C.S. Fadley M. Van Hove Group, Berkeley
Surf. Sci. 441 (1999) 301.
34
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35
PRL 79 (1997) 2085.
Z12 2.0760.05 Å Z23 2.2860.05 Å.
36
Epitaxial growth - Vanadium and Vanadium
Oxides on TiO2 (110)
37
Bridging oxygen relaxation
38
ASTRID
1 ML V on TiO2 (110) annealing at 473 K in O2
CHEMICAL SHIFT PD
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