Comment on ‘‘Adsorbate structures from photoelectron diffraction: Holographic reconstruction or real-space triangulation?’’

1993 ◽  
Vol 71 (2) ◽  
pp. 299-299 ◽  
Author(s):  
A. P. Kaduwela ◽  
M. A. Van Hove ◽  
C. S. Fadley
1992 ◽  
Vol 68 (10) ◽  
pp. 1543-1546 ◽  
Author(s):  
R. Dippel ◽  
D. P. Woodruff ◽  
X.-M. Hu ◽  
M. C. Asensio ◽  
A. W. Robinson ◽  
...  

1994 ◽  
Vol 312 (1-2) ◽  
pp. 82-96 ◽  
Author(s):  
M. Zharnikov ◽  
D. Mehl ◽  
M. Weinelt ◽  
P. Zebisch ◽  
H.-P. Steinrück

2017 ◽  
Vol 24 (1) ◽  
pp. 354-366 ◽  
Author(s):  
Matthias Muntwiler ◽  
Jun Zhang ◽  
Roland Stania ◽  
Fumihiko Matsui ◽  
Peter Oberta ◽  
...  

The Photo-Emission and Atomic Resolution Laboratory (PEARL) is a new soft X-ray beamline and surface science laboratory at the Swiss Light Source. PEARL is dedicated to the structural characterization of local bonding geometry at surfaces and interfaces of novel materials, in particular of molecular adsorbates, nanostructured surfaces, and surfaces of complex materials. The main experimental techniques are soft X-ray photoelectron spectroscopy, photoelectron diffraction, and scanning tunneling microscopy (STM). Photoelectron diffraction in angle-scanned mode measures bonding angles of atoms near the emitter atom, and thus allows the orientation of small molecules on a substrate to be determined. In energy scanned mode it measures the distance between the emitter and neighboring atoms; for example, between adsorbate and substrate. STM provides complementary, real-space information, and is particularly useful for comparing the sample quality with reference measurements. In this article, the key features and measured performance data of the beamline and the experimental station are presented. As scientific examples, the adsorbate–substrate distance in hexagonal boron nitride on Ni(111), surface quantum well states in a metal-organic network of dicyano-anthracene on Cu(111), and circular dichroism in the photoelectron diffraction of Cu(111) are discussed.


2014 ◽  
Vol 599-601 ◽  
pp. 1985-1988
Author(s):  
Bo Tang ◽  
Zong Bo Zhang ◽  
Shuang Xi Tang ◽  
Guo Ping Liu ◽  
Jie Gao

During the near-field acoustic holographic reconstruction with sampling GREEN’s function in k space, there will be aliasing which results in the wrapping error for the infinite extension of GREEN’s function in real space. The magnitude of wrapping error lies on the decrement of GREEN’s function in real space. The paper applies a 2-D low-pass filter to remove the hyper space element in order to reduce the wrapping error. The simulation indicates that the method can reduce the wrapping error in the holographic reconstruction efficiently.


2012 ◽  
Vol 81 (11) ◽  
pp. 114604 ◽  
Author(s):  
Fumihiko Matsui ◽  
Tomohiro Matsushita ◽  
Hiroshi Daimon

1996 ◽  
Vol 437 ◽  
Author(s):  
J. D. Denlinger ◽  
Eli Rotenberg ◽  
S. D. Kevan ◽  
B. P. Tonner

AbstractA highly detailed x-ray photoelectron diffraction data set has been acquired for crystalline Cu(001). The data set for bulk Cu 3p emission encompasses a large k-space volume (k=3–10 Å-1) with sufficient energy and angular sampling to monitor the continuous variation of diffraction intensities. The evolution of back-scattered intensity oscillations is visualized by energy and angular slices of this ‘volume’ data set. Large diffractyyion data sets such as this will provide rigorous experimental tests of real-space reconstruction algorithms and multiple-scattering simulations.


2011 ◽  
Vol 393-395 ◽  
pp. 424-427
Author(s):  
Tang Bo ◽  
Xu Yu

During the near-field acoustic holographic reconstruction, there will be error which make the reconstruction uncertain in sampling GREEN’s function in real space. The magnitude of discrete error lies on the size of sampling interval and the change rate of GREEN’s function. The longer interval, the greater error. The faster change rate, the greater error. Because the GREEN’s function is sensitive to the reconstruction distance and the reconstruction frequency and change with direct ratio and inverse ratio, the discrete error is with direct ratio to the reconstruction frequency and with inverse ratio the reconstruction distance.


1992 ◽  
Vol 295 ◽  
Author(s):  
R. Denecke ◽  
R. Eckstein ◽  
L. Ley ◽  
A. Bocquet ◽  
J. Riley ◽  
...  

AbstractFor GaAs (001) and (III) we have measured the photoelectron diffraction patterns at a kinetic energy of 86 eV. We applied an extended Fourier-transform algorithm to the (001) data to obtain real space images. The origin of structures in these images not representing atomic positions is investigated with the help of single scattering calculations


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