Journal article
Exact electromagnetic response of Landau level electrons
- Abstract:
- We present a simple method that allows us to calculate the electromagnetic response of noninteracting electrons in a strong magnetic field to arbitrary order in the gradients of external electric and magnetic fields. We illustrate the method on both nonrelativistic and massless Dirac electrons filling N Landau levels. First, we derive an exact relation between the electromagnetic response of the nonrelativistic and Dirac electrons in the lowest Landau level. Next, we obtain a closed form expression for the polarization operator in the large- N (or weak magnetic field) limit. We explicitly show that in the large- N limit the random phase approximation (RPA) computation of the polarization tensor agrees—in leading and subleading order in N —with a Fermi liquid computation to all orders in the gradient expansion and for arbitrary value of the g factor. Finally, we show that in the large- N limit the nonrelativistic polarization tensor agrees with Dirac's in the leading and subleading orders in N , provided that the Berry phase of the Dirac cone is taken into account via replacement N ⟶ N + 1 / 2 .
- Publication status:
- Published
- Peer review status:
- Peer reviewed
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- Files:
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(Preview, Accepted manuscript, pdf, 545.9KB, Terms of use)
-
- Publisher copy:
- 10.1103/PhysRevB.95.085151
Authors
- Publisher:
- American Physical Society
- Journal:
- Physical Review B More from this journal
- Volume:
- 95
- Issue:
- 8
- Article number:
- 085151
- Publication date:
- 2018-02-28
- DOI:
- EISSN:
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2469-9969
- ISSN:
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2469-9950
- Pubs id:
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pubs:842342
- UUID:
-
uuid:771523f9-1f53-4902-b086-ce53e7f7fc7c
- Local pid:
-
pubs:842342
- Source identifiers:
-
842342
- Deposit date:
-
2018-04-20
Terms of use
- Copyright holder:
- ©2017 American Physical Society
- Copyright date:
- 2018
- Notes:
- This is the author accepted manuscript following peer review version of the article. The final version is available online from American Physical Society at: 10.1103/PhysRevB.95.085151
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