4.8 Article

Gyrotropic Magnetic Effect and the Magnetic Moment on the Fermi Surface

Journal

PHYSICAL REVIEW LETTERS
Volume 116, Issue 7, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.116.077201

Keywords

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Funding

  1. DOE LBL Quantum Materials Program
  2. Simons Foundation
  3. Spanish Ministerio de Economia y Competitividad [MAT2012-33720]
  4. European Commission [CIG-303602]
  5. [NSF DMR-1507141]
  6. Direct For Mathematical & Physical Scien [1507141] Funding Source: National Science Foundation
  7. Division Of Materials Research [1507141] Funding Source: National Science Foundation

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The current density j(B) induced in a clean metal by a slowly-varying magnetic field B is formulated as the low-frequency limit of natural optical activity, or natural gyrotropy. Working with a multiband Pauli Hamiltonian, we obtain from the Kubo formula a simple expression for alpha(GME)(ij) = j(i)(B)/B-j in terms of the intrinsic magnetic moment (orbital plus spin) of the Bloch electrons on the Fermi surface. An alternate semiclassical derivation provides an intuitive picture of the effect, and takes into account the influence of scattering processes in dirty metals. This gyrotropic magnetic effect is fundamentally different from the chiral magnetic effect driven by the chiral anomaly and governed by the Berry curvature on the Fermi surface, and the two effects are compared for a minimal model of a Weyl semimetal. Like the Berry curvature, the intrinsic magnetic moment should be regarded as a basic ingredient in the Fermi-liquid description of transport in broken-symmetry metals.

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