TY - JOUR
T1 - Erratum
T2 - Valley magnetism, nematicity, and density wave orders in twisted bilayer graphene (Physical Review B (2020) 102 (125120) DOI: 10.1103/PhysRevB.102.125120)
AU - Chichinadze, Dmitry
AU - Classen, Laura
AU - Chubukov, Andrey V.
N1 - Publisher Copyright:
© 2021 American Physical Society. All rights reserved.
PY - 2021/1/4
Y1 - 2021/1/4
N2 - In the original paper, we erroneously neglected the interaction between fermionic densities in different valleys in the diagrams for intravalley charge orders. Although this interaction does not change the hierarchy of previously reported ordered states, it introduces an additional attraction in the s ± charge Pomeranchuk channel (a density order with the opposite sign in the two valleys). The correct result is that in both six-patch and twelve-patch models, the coupling in the s ± charge Pomeranchuk channel is degenerate with the one in the s -wave spin Pomeranchuk channel, responsible for valley magnetism. Our discussion of the Landau free energy for spin Pomeranchuk order is not affected as the system develops either spin or charge (valley) order, but not both. In practical terms, the coupling matrix CPom , 0 in Eq. (21) for the six-patch model should be revised to so that the eigenvalues are now,ntravalley charge orders in the 12-patch model also receive additional corrections, and Eqs. (72) and (75)–(78) must be revised accordingly. The outcome is the same as in the six-patch model: The hierarchy of leading instabilities remains the same, but the coupling in the s ± charge Pomeranchuk channel becomes degenerate with the one in the s -wave spin Pomeranchuk channel, and the eigenvalues in some CDW and SDW channels become degenerate.
AB - In the original paper, we erroneously neglected the interaction between fermionic densities in different valleys in the diagrams for intravalley charge orders. Although this interaction does not change the hierarchy of previously reported ordered states, it introduces an additional attraction in the s ± charge Pomeranchuk channel (a density order with the opposite sign in the two valleys). The correct result is that in both six-patch and twelve-patch models, the coupling in the s ± charge Pomeranchuk channel is degenerate with the one in the s -wave spin Pomeranchuk channel, responsible for valley magnetism. Our discussion of the Landau free energy for spin Pomeranchuk order is not affected as the system develops either spin or charge (valley) order, but not both. In practical terms, the coupling matrix CPom , 0 in Eq. (21) for the six-patch model should be revised to so that the eigenvalues are now,ntravalley charge orders in the 12-patch model also receive additional corrections, and Eqs. (72) and (75)–(78) must be revised accordingly. The outcome is the same as in the six-patch model: The hierarchy of leading instabilities remains the same, but the coupling in the s ± charge Pomeranchuk channel becomes degenerate with the one in the s -wave spin Pomeranchuk channel, and the eigenvalues in some CDW and SDW channels become degenerate.
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U2 - 10.1103/PhysRevB.103.039901
DO - 10.1103/PhysRevB.103.039901
M3 - Comment/debate
AN - SCOPUS:85099460951
SN - 2469-9950
VL - 103
JO - Physical Review B
JF - Physical Review B
IS - 3
M1 - 039901
ER -