Chemically driven surface effects in polar intermetallic topological insulators A3Bi

2018 ◽  
Vol 20 (41) ◽  
pp. 26372-26385 ◽  
Author(s):  
I. P. Rusinov ◽  
P. Golub ◽  
I. Yu. Sklyadneva ◽  
A. Isaeva ◽  
T. V. Menshchikova ◽  
...  

Surface electronic spectra, surface and bulk properties as well as the underlying chemical bonding characteristics in topological insulators with complex bonding patterns are considered for the example of cubic, polar intermetallics KNa2Bi, K3Bi and Rb3Bi (with the general formula A3Bi, A – alkali metal).

2018 ◽  
Vol 29 (2) ◽  
pp. 1805972 ◽  
Author(s):  
Hyewon Ryoo ◽  
Sang-Gil Lee ◽  
Jin-Gyu Kim ◽  
Sung-Yoon Chung

2013 ◽  
Vol 1517 ◽  
Author(s):  
Gordon J. Miller ◽  
Srinivasa Thimmaiah ◽  
Volodymyr Smetana ◽  
Andriy Palasyuk ◽  
Qisheng Lin

ABSTRACTRecent exploratory syntheses of polar intermetallic compounds containing gold have established gold’s tremendous ability to stabilize new phases with diverse and fascinating structural motifs. In particular, Au-rich polar intermetallics contain Au atoms condensed into tetrahedra and diamond-like three-dimensional frameworks. In Au-poor intermetallics, on the other hand, Au atoms tend to segregate, which maximizes the number of Au-heteroatom contacts. Lastly, among polar intermetallics with intermediate Au content, complex networks of icosahedra have emerged, including discovery of the first sodium-containing, Bergman-type, icosahedral quasicrystal. Gold’s behavior in this metal-rich chemistry arises from its various atomic properties, which influence the chemical bonding features of gold with its environment in intermetallic compounds. Thus, the structural versatility of gold and the accessibility of various Au fragments within intermetallics are opening new insights toward elucidating relationships among metal-rich clusters and bulk solids.


2018 ◽  
Vol 6 (7) ◽  
pp. 1651-1658 ◽  
Author(s):  
Dong Fan ◽  
Shaohua Lu ◽  
Yundong Guo ◽  
Xiaojun Hu

We identify two B–C bonding patterns: pyramidal-geometry tetra-coordinated and hexa-coordinated sp2carbon moiety; B4C3has an ultrahigh Young's modulus that can even outperform graphene; the B2C sheet is metallic with a relatively high superconducting transition temperature (Tc≈ 21.20 K).


1976 ◽  
Vol 54 (24) ◽  
pp. 3839-3849 ◽  
Author(s):  
J. Corish ◽  
Brenda M. C. Parker ◽  
P. W. M. Jacobs

Various models for the interionic potential in the alkali metal chlorides have been examined. The parameters in these potentials have been determined by fitting the equilibrium, elastic and dielectric properties of each substance. The potentials are compared graphically with each other, with the theoretically derived potentials of Kim and Gordon (1,2) and with a potential derived earlier by Catlow, Diller, and Norgett (3) by fitting the properties of sixteen alkali halides simultaneously. Intrinsic defect properties of the four chlorides have been calculated from these potentials. The results show that while it is possible to derive adequate two-body potentials for these salts from fitting their bulk properties, it is concluded, as found earlier by Catlow, Diller, and Norgett (3), that such potentials need to have the anion–cation interaction hardened by neglecting completely the Van der Waals interaction between nearest neighbours. Inclusion of non-central forces does not improve the potential, as judged by the criterion of the results of defect calculations.


1993 ◽  
Vol 32 (22) ◽  
pp. 4708-4713 ◽  
Author(s):  
Jordi Mestres ◽  
Miquel Duran ◽  
Pedro Martin-Zarza ◽  
Eduardo Medina de la Rosa ◽  
Pedro Gili

2006 ◽  
Vol 632 (8-9) ◽  
pp. 1423-1431 ◽  
Author(s):  
Frank Haarmann ◽  
Daniel Grüner ◽  
Viktor Bezugly ◽  
Helge Rosner ◽  
Yuri Grin

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