Emergence of curved momentum-spacetime and its effect on the cyclotron motion in the antiferromagnetic quantum critical metal
arXiv:2305.02833 · doi:10.1103/PhysRevB.108.245112
Abstract
We show that anisotropic quantum corrections can dynamically give rise to curved momentum-spacetimes for quasiparticles in metals. In the (2+1)-dimensional antiferromagnetic quantum critical metal, a curved momentum-spacetime arises as the critical spin fluctuations generate red shift that dilates frequency of electron unevenly on the Fermi surface. As the disparity of the momentum-dependent red shift is controlled by the shape of the Fermi surface, the momentum-spacetime geometry that emerges at low energies depends on the bare nesting angle of the Fermi surface. With increasing nesting angle, the region in which electron motion is slowed down by critical spin fluctuations shrinks. On the other hand, the increasing nesting angle makes the red shift stronger near the hot spots due to the weakened screening of the interaction. These competing effects result in a non-monotonic dependence of the cyclotron frequency of electron on the nesting angle of the Fermi surface. The red shift that becomes more singular at the hot spots with increasing nesting angle creates a possibility of realizing a momentum-space black hole horizon beyond a critical nesting angle : the electron motion becomes `perpetually' slowed down as it approaches a hot spot in the same way that the motion of a free falling object freezes near the event horizon of a black hole with respect to an asymptotic observer. However, the analogous horizon in momentum space does not lead to a vanishing cyclotron frequency because the metric singularity at the hot spots is cut off by thermal effects present above the non-zero superconducting transition temperature.
22 pages
References in corpus (21)
- Quantum oscillations and the Fermi surface in an underdoped high-Tc superconductor
- Hidden Magnetism and Quantum Criticality in the Heavy Fermion Superconductor CeRhIn5
- Quantum phase transitions of metals in two spatial dimensions: II. Spin density wave order
- A Sharp Peak of the Zero-Temperature Penetration Depth at Optimal Composition in BaFe2(As1-xPx)2
- Effects of topological defects and local curvature on the electronic properties of planar graphene
- A multi-component Fermi surface in the vortex state of an underdoped high-Tc superconductor
- Quasiparticle mass enhancement approaching optimal doping in a high-Tc superconductor
- Geometry, mechanics and electronics of singular structures and wrinkles in graphene
- Evidence of Flat Bands and Correlated States in Buckled Graphene Superlattices
- Sign-problem-free quantum Monte Carlo of the onset of antiferromagnetism in metals
- Quasi-Local Strange Metal
- Magnetic Breakdown in the electron-doped cuprate superconductor NdCeCuO: the reconstructed Fermi surface survives in the strongly overdoped regime
- Quantum critical properties of a metallic spin density wave transition
- Symmetry-enforced topological nodal planes at the Fermi surface of a chiral magnet
- Quantum criticality of reconstructing Fermi surfaces in antiferromagnetic metals
- Field-theoretic functional renormalization group formalism for non-Fermi liquids and its application to the antiferromagnetic quantum critical metal in two dimensions
- Evolution of the cyclotron mass with doping in LaSrCuO
- Non-Hertz-Millis scaling of the antiferromagnetic quantum critical metal via scalable Hybrid Monte Carlo
- Effective masses in a strongly anisotropic Fermi liquid
- Tunable superconductivity and Möbius Fermi surfaces in an inversion-symmetric twisted van der Waals heterostructure
- Geodesic geometry of 2+1-D Dirac materials subject to artificial, quenched gravitational singularities