Upper bound of a band complex

被引:2
|
作者
Li, Si [1 ,2 ]
Zhang, Zeying [3 ,4 ]
Feng, Xukun [4 ]
Wu, Weikang [4 ,5 ]
Yu, Zhi-Ming [6 ,7 ]
Zhao, Y. X. [8 ,9 ,10 ]
Yao, Yugui [6 ,7 ]
Yang, Shengyuan A. [4 ]
机构
[1] Northwest Univ, Sch Phys, Xian 710127, Peoples R China
[2] Shaanxi Key Lab Theoret Phys Frontiers, Xian 710127, Peoples R China
[3] Beijing Univ Chem Technol, Coll Math & Phys, Beijing 100029, Peoples R China
[4] Singapore Univ Technol & Design, Res Lab Quantum Mat, Singapore 487372, Singapore
[5] Shandong Univ, Key Lab Liquid Solid Struct Evolut & Proc Mat, Minist Educ, Jinan 250061, Peoples R China
[6] Beijing Inst Technol, Beijing Key Lab Nanophoton & Ultrafine Optoelect, Key Lab Adv Optoelect Quantum Architecture & Meas, Beijing 100081, Peoples R China
[7] Beijing Inst Technol, Sch Phys, Beijing 100081, Peoples R China
[8] Nanjing Univ, Natl Lab Solid State Microstruct, Nanjing 210093, Peoples R China
[9] Nanjing Univ, Dept Phys, Nanjing 210093, Peoples R China
[10] Nanjing Univ, Collaborat Innovat Ctr Adv Microstruct, Nanjing 210093, Peoples R China
关键词
BILBAO CRYSTALLOGRAPHIC SERVER;
D O I
10.1103/PhysRevB.107.235145
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The band structure for a crystal generally consists of connected components in energy-momentum space, known as band complexes. Here, we explore a fundamental aspect regarding the maximal number of bands that can be accommodated in a single band complex. We show that, in principle, a band complex can have no finite upper bound for certain space groups. This means infinitely many bands can entangle together, forming a connected pattern stable against symmetry-preserving perturbations. This is demonstrated by our developed inductive construction procedure, through which a given band complex can always be grown into a larger one by gluing a basic building block to it. As a by-product, we demonstrate the existence of arbitrarily large accordiontype band structures containing N-C = 4n bands, with n is an element of N.
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页数:6
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