Dominant Role of a Pseudogap in the Physics of the Colossal Magnetoresistive Oxides

1998 ◽  
Vol 12 (29n31) ◽  
pp. 3389-3392 ◽  
Author(s):  
D. S. Dessau ◽  
T. Saitoh ◽  
C.-H. Park ◽  
Z.-X. Shen ◽  
Y. Moritomo ◽  
...  

We have performed direct electronic structure measurements of the colosssal magnetoresistive oxides using high energy resolution photoemission spectroscopy. A key result of these measurements is the discovery of a pseudogap which drastically supresses or completely removes the spectral weight (density of states) at the Fermi energy E F . It is shown that the pseudogap plays a dominant role in the "colossal" conductivity changes which occur across the magnetic ordering temperature. We briefly discuss possible origins for the pseudogap.

1968 ◽  
Vol 4 (7) ◽  
pp. 573-579 ◽  
Author(s):  
T. Hofmokl ◽  
L. Michejda ◽  
S. Otwinowski ◽  
R. Sosnowski ◽  
M. Szeptycka ◽  
...  

Symmetry ◽  
2020 ◽  
Vol 12 (11) ◽  
pp. 1784
Author(s):  
László Jenkovszky

The role of spin degrees of freedom in high-energy hadron-hadron and lepton-hadron scattering is reviewed with emphasis on the dominant role of soft, diffractive, non-perturbative effects. Explicit models based on analyticity and Regge-pole theory, including the pomeron trajectory (gluon exchange in the t channel) are discussed. We argue that there is a single, universal pomeron in Nature, manifest as relatively “soft” or “hard”, depending on the kinematics considered. Both the pomeron and the non-leading (secondary) Regge trajectories, made of quarks are non-linear, complex functions. They are populated by a finite number of resonances: known baryons and mesons in case of the reggeons and hypothetical glueballs in case of the pomeron (“oddballs” on the odderon trajectory). Explicit models and fits are presented that may be used in recovering generalized parton distributions from deeply virtual Compton scattering and electoproduction of vector mesons.


2005 ◽  
Vol 7 (13) ◽  
pp. 2629 ◽  
Author(s):  
C. J. Weststrate ◽  
J. W. Bakker ◽  
E. D. L. Rienks ◽  
C. P. Vinod ◽  
S. Lizzit ◽  
...  

2011 ◽  
Vol 82 (9) ◽  
pp. 093901 ◽  
Author(s):  
M. Maniraj ◽  
S. W. D’Souza ◽  
J. Nayak ◽  
Abhishek Rai ◽  
Sanjay Singh ◽  
...  

2021 ◽  
Author(s):  
Kristina Kvashnina ◽  
Sergei M Butorin

In recent years, scientists have progressively recognized the role of electronic structure in the characterization of chemical properties for actinide containing materials. High-energy resolution X-ray spectroscopy at the actinide M4,5...


2002 ◽  
Vol 09 (02) ◽  
pp. 1079-1083 ◽  
Author(s):  
H. SATO ◽  
Y. NISHIKAWA ◽  
F. NAGASAKI ◽  
H. FUJINO ◽  
Y. TAKEDA ◽  
...  

Valence-band and Yb 4d photoemission spectra of YbXCu 4 (X=In, Cd, Mg) have been measured with high energy resolution from 10 to 300 K. In the valence-band photoemission spectra of YbInCu 4 and YbCdCu 4, the structure due to the Yb 2+ 4f 7/2 states is clearly observed near the Fermi level (E F ) at 10 K. The intensity of the Yb 2+ 4f 7/2 structure decreases with increasing temperature and the structure almost disappears at 300 K. The amount of the enhancement from 50 to 107 K is much stronger for YbInCu 4 than for YbCdCu 4. On the other hand, the Yb 2+ 4f 7/2 structure of YbMgCu 4 is observed as a broad peak near E F and the spectra show little temperature dependence. In the Yb 4d photoemission spectra of YbInCu 4 and YbCdCu 4, the structures due to the Yb 2+ and Yb 3+ states are recognized. The intensity ratio Yb 2+/ Yb 3+ increases with decreasing temperature. In the Yb 4d spectra of YbMgCu 4, on the other hand, almost only structures due to Yb 2+ states are observed.


2006 ◽  
Vol 100 (5) ◽  
pp. 053710 ◽  
Author(s):  
Yasuto Hijikata ◽  
Hiroyuki Yaguchi ◽  
Sadafumi Yoshida ◽  
Yasutaka Takata ◽  
Keisuke Kobayashi ◽  
...  

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