Surface state like bulk band emission in the photoelectron energy spectra of Cu(111)

1986 ◽  
Vol 59 (4) ◽  
pp. 205-208 ◽  
Author(s):  
L. Walldén
2021 ◽  
Author(s):  
Juan Miguel Urco Cordero ◽  
Farzad Kamalabadi ◽  
Ulas Kamaci ◽  
Brian J Harding ◽  
Harald U. Frey ◽  
...  

1976 ◽  
Vol 3 (3) ◽  
pp. 129-131 ◽  
Author(s):  
J. P. Doering ◽  
W. K. Peterson ◽  
C. O. Bostrom ◽  
T. A. Potemra

1998 ◽  
Vol 81 (6) ◽  
pp. 1199-1202 ◽  
Author(s):  
N. L. S. Martin ◽  
D. B. Thompson ◽  
R. P. Bauman ◽  
C. D. Caldwell ◽  
M. O. Krause ◽  
...  

1971 ◽  
Vol 0 (3) ◽  
pp. 142-143 ◽  
Author(s):  
S. Pignataro ◽  
V. Mancini ◽  
J. N. A. Ridyard ◽  
H. J. Lempka

The electronic structure of the {110} surface of tungsten has been investigated by using angle-resolved photoemission. A surface state has been identified and characterized throughout the surface Brillouin zone (s. B. z.). Its dispersion is found to correlate with the projected band gap between the third and fourth bands of the tungsten bulk band structure. It is identified by comparison with Inglesfield’s calculation as having predominantly m = 1 d-orbital character. With photon energies of 21.2 and 40.8 eV, intense photoemission from the surface state is only observed after surface Umklapp, whereas, with 16.8 eV, photon emission is observed in both the first and second s. B. zs. The applicability of the tight-binding approximation to the elucidation of the electronic structure of a metal surface is examined with particular reference to this surface state. A qualitative analysis of the observed photoemission intensities is consistent with emission from a tungsten e g orbital that is hybridized with e g orbitals on neighbouring atoms.


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