scholarly journals Hole dynamics in a quantum-well state at Na/Cu(111)

2003 ◽  
Vol 68 (19) ◽  
Author(s):  
E. V. Chulkov ◽  
J. Kliewer ◽  
R. Berndt ◽  
V. M. Silkin ◽  
B. Hellsing ◽  
...  
2013 ◽  
Vol 87 (23) ◽  
Author(s):  
S. Jakobs ◽  
A. Ruffing ◽  
M. Cinchetti ◽  
S. Mathias ◽  
M. Aeschlimann

2015 ◽  
Vol 107 (16) ◽  
pp. 161602 ◽  
Author(s):  
S. R. Song ◽  
S. Meng ◽  
S. X. Du ◽  
F. Liu ◽  
H. J. Gao

AIP Advances ◽  
2020 ◽  
Vol 10 (12) ◽  
pp. 125211
Author(s):  
Woojoo Lee ◽  
Chi-Ruei Pan ◽  
Hyoungdo Nam ◽  
Mei-Yin Chou ◽  
Chih-Kang Shih

2009 ◽  
Vol 80 (19) ◽  
Author(s):  
S. Achilli ◽  
G. Butti ◽  
M. I. Trioni ◽  
E. V. Chulkov

1997 ◽  
Vol 04 (06) ◽  
pp. 1233-1237 ◽  
Author(s):  
A. CARLSSON ◽  
D. CLAESSON ◽  
G. KATRICH ◽  
S.-Å LINDGREN ◽  
L. WALLDÉN

Via photoemission in the near UV from discrete quantum well states, four different types of atom rearrangements are observed for Cu (111)/ Li . In the monolayer range a gradual energy shift reflects a gradual compression of the Li layer as more atoms are adsorbed. The onset of Li substitution and formation of a (2×2) structure when, at RT, monolayer Li coverage is exceeded is monitored via the appearance of a quantum well state characteristic of the new phase. A small energy shift indicates that, if it is cooled (170 K), the new structure is unstable with respect to Li adsorption. Finally, an energy downshift with increasing coverage observed for a state characteristic of 2 ML Li is ascribed to an increasing area for one-atomic-layer-high islands formed by Li atoms on top of the first full layer.


2002 ◽  
Vol 09 (02) ◽  
pp. 1375-1378 ◽  
Author(s):  
A. M. SHIKIN ◽  
O. RADER ◽  
W. GUDAT ◽  
G. V. PRUDNIKOVA ◽  
V. K. ADAMCHUK

Using angle-resolved photoemission, we observe quantum-well-state formation as pronounced peaks up to large thicknesses in epitaxial Ag and Au films on W(110). These systems serve as a test case for the assignment of sp and d orbital character to quantum-well states since overlap of sp with d states is strong for both systems but differs in detail. Starting out from peak assignments on the basis of the extended phase accumulation model, the angle dispersion of several features is discussed in detail and related to the orbital character.


2007 ◽  
Vol 601 (22) ◽  
pp. 5254-5257 ◽  
Author(s):  
M. Nagira ◽  
M. Sawada ◽  
M. Higashiguchi ◽  
K. Yaji ◽  
T. Moko ◽  
...  

2002 ◽  
Vol 66 (16) ◽  
Author(s):  
Chang-Cheng Chuo ◽  
Guan-Ting Chen ◽  
Ming-I Lin ◽  
Chia-Ming Lee ◽  
Jen-Inn Chyi

Sign in / Sign up

Export Citation Format

Share Document