2022
DOI: 10.1016/j.aop.2022.168914
|View full text |Cite
|
Sign up to set email alerts
|

Quantum magnetic billiards: boundary conditions and gauge transformations

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2022
2022
2023
2023

Publication Types

Select...
2

Relationship

1
1

Authors

Journals

citations
Cited by 2 publications
(2 citation statements)
references
References 27 publications
0
2
0
Order By: Relevance
“…Despite the fact that many physically observable quantities, such as the spectrum of H A , are independent of the gauge choice [50], such a choice is needed in order to perform calculations. More importantly, one should be aware that, generally, even boundary conditions depend on the gauge choice: see [51] for a detailed discussion. For the Hall strip (1)-(2), a profitable choice is the Landau gauge A = (−By, 0) , (8) which clearly satisfies equation (5).…”
Section: The Hall Hamiltonianmentioning
confidence: 99%
See 1 more Smart Citation
“…Despite the fact that many physically observable quantities, such as the spectrum of H A , are independent of the gauge choice [50], such a choice is needed in order to perform calculations. More importantly, one should be aware that, generally, even boundary conditions depend on the gauge choice: see [51] for a detailed discussion. For the Hall strip (1)-(2), a profitable choice is the Landau gauge A = (−By, 0) , (8) which clearly satisfies equation (5).…”
Section: The Hall Hamiltonianmentioning
confidence: 99%
“…where α 0 , α 1 ∈ R (see e.g. [51] for a discussion of its physical significance); note in particular that chiral conditions reduce to Robin conditions if α 1 = 0. The above expression is manifestly invariant under longitudinal translations, which are indeed generated by the longitudinal momentum operator p x = −iℏ∂/∂ x .…”
Section: Data Availability Statementmentioning
confidence: 99%