Elementary energy bands concept, band structure, and peculiarities of bonding in β-InSe crystal

2010 ◽  
Vol 247 (2) ◽  
pp. 318-324 ◽  
Author(s):  
K. E. Glukhov ◽  
N. K. Tovstyuk
1972 ◽  
Vol 14 (4) ◽  
pp. 485-488 ◽  
Author(s):  
J.-M. André ◽  
J. Delhalle ◽  
G. Kapsomenos ◽  
G. Leroy

1979 ◽  
Vol 92 (2) ◽  
pp. 379-387 ◽  
Author(s):  
P. Plenkiewicz ◽  
B. Dowgiałło-Plenkiewicz

2004 ◽  
Vol 70 (23) ◽  
Author(s):  
D. M. Bercha ◽  
I. V. Slipukhina ◽  
M. Sznajder ◽  
K. Z. Rushchanskii

2001 ◽  
Vol 79 (4) ◽  
pp. 749-756
Author(s):  
H F Hu ◽  
Y B Li ◽  
K L Yao

We have studied the energy band structure of polydiacetylenes (PDAs) using the extensional Hückel Hamiltonian that includes the nonnearest-neighbor hopping interactions. The results show that with increase in the nonnearest-neighbor hopping interaction parameters ρ1 and ρ2, (i) the energy band symmetry is broken and the energy gap 2Δ has changed, (ii) the locations and the widths of energy bands have changed and their shifts depend mainly on ρ1 (next-neighbor hopping interactions), and (iii) the energy gap 2Δ depends mainly on ρ2 (third-neighbor hopping interactions), the effects of the nonnearest-neighbor hopping interaction on the band structure are discussed. PACS No.: 31.15Ct


1987 ◽  
Vol 91 ◽  
Author(s):  
T. P. Pearsall ◽  
J. Bevk ◽  
J. C. Bean ◽  
J. M. Bonar ◽  
J. P. Mannaerts

ABSTRACTA systematic study of the band-to-band optical transitions in commensurate strainedlayer superlattices of Ge and Si grown on (001) Si substrates show the presence of new electronic energy bands. Our measurements suggest that superlattice structure on the same scale as the unit cell results in a band structure significantly different from that of a random alloy.


1997 ◽  
Vol 494 ◽  
Author(s):  
T. Saitoh ◽  
D. S. Dessau ◽  
C.-H. Park ◽  
Z.-X. Shen ◽  
P. Villella ◽  
...  

ABSTRACTWe have studied the fc-dependent electronic structure of the layered colossal magnetoresistive manganite La1.2Sr1.8Mn2O7 using high-resolution angle-resolved photoemission spectroscopy. We found dispersive energy bands as a function of the crystal momentum k near the Fermi level (EF). We have also performed local spin density approximation (LSDA)+U band-structure calculations on the current system. The overall experimental dispersion relation is basically in agreement with the band-structure calculations yet close to EF there is a significant deviation from the predicted dispersions. Instead of clear Fermi-surface (FS) crossings, we observe a depression of the features as the FS is approached as if there is a “pseudo” gap in the excitation spectrum. The pseudogap continuously opens with temperature and does not show further significant opening above Tc, corresponding to the metal-insulator transition. Those unusual aspects of the spectra has been discussed from the viewpoint of the strong electron-lattice coupling model.


Author(s):  
Igor Vurgaftman ◽  
Matthew P. Lumb ◽  
Jerry R. Meyer

III–V semiconductors form crystalline structures with three-dimensional periodic arrangements of the atoms. In this chapter, we will explore the nature of the crystal lattice starting from lower dimensions and progressing to real semiconductor crystals. We also learn why we expect distinct energy bands to form in the solids that crystallize in such lattices. The carrier statistics and occupation of the bands will also be examined.


2007 ◽  
Vol 244 (4) ◽  
pp. 1318-1336 ◽  
Author(s):  
D. M. Bercha ◽  
K. E. Glukhov ◽  
M. Sznajder
Keyword(s):  

1996 ◽  
Vol 10 (19) ◽  
pp. 931-937 ◽  
Author(s):  
H.F. HU ◽  
K.L. YAO

Starting from the extensional model Hückel Hamiltonian containing the next-neighbor hopping interactions, the energy band structure and their variation have been studied for polydiacetylenes (PDA’s). With the increase of the next-neighbor hopping interaction parameter ρ the results show that: (1) the electronic state symmetry is broken, (2) the locations and the widths of energy bands have been changed, and (3) the energy gap becomes narrower and the total bandwidth broader. Finally, the effect of the nextneighbor hopping interactions on the band-structure is discussed.


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