Equation 5 · A Strained Crystal Is a Designer Spacetime
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Symbol H
H is part of the quantity the equation computes from the expression on the right.
Symbol boldsymbolσ
boldsymbolσ is one of the signed contributions combined to compute the quantity on the left.
Symbol W
W is one of the signed contributions combined to compute the quantity on the left.
Symbol x
x is one of the signed contributions combined to compute the quantity on the left.
=
The expressions on both sides represent the same quantity under the stated assumptions.
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subscript
The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.
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What the article says around this equation
The tilt is where the geometry stops being a figure of speech. Once the tilt varies smoothly from place to place across a crystal, an electron propagating through it is, at leading order in the standard low-energy expansion, equivalent to a particle moving through a curved effective spacetime of the same mathematical form — a Painlevé–Gullstrand metric — that describes an object falling into a black hole, with the tilt itself playing the role of the metric’s off-diagonal, “flow” components. The paper writes the whole statement as a single Hamiltonian, fixing the Fermi velocity , the Pauli matrices acting on the electron’s internal degree of freedom, the momentum-space…
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The tilt is where the geometry stops being a figure of speech. Once the tilt varies smoothly from place to place across a crystal, an electron propagating through it is, at leading order in the standard low-energy expansion, equivalent to a particle moving through a curved effective spacetime of the same mathematical form — a Painlevé–Gullstrand metric — that describes an object falling into a black hole, with the tilt itself playing the role of the metric’s off-diagonal, “flow” components. The paper writes the whole statement as a single Hamiltonian, fixing the Fermi velocity , the Pauli matrices acting on the electron’s internal degree of freedom, the momentum-space shift , and the tilt vector W(x) : . The first term is ordinary tilted-free Weyl physics, shifted by the strain-induced gauge field. The second term is the one that matters here: it multiplies the momentum by the tilt and by the identity matrix, so it does not distinguish between the electron’s two internal states the way the first term does — it simply drags the whole cone in one direction, by an amount that depends on position through W(x) . Where |W| crosses the value 1, the type-I/type-II boundary, the cone tips over far enough that one branch of carriers can only move one way past that line, in exactly the sense that nothing can move outward past an event horizon. That correspondence between an over-tilted Weyl cone and a horizon is not this paper’s invention — it descends from Grigory Volovik’s 2016 observation that a type-II Weyl semimetal could in principle host a Hawking-radiating horizon at room temperature if the tilted region were made small enough, stated as a symbolic relation between the Hawking temperature and the velocity gradient at the horizon, with no material, no computed number, and no fabrication route attached [ 15 ] . What the new paper adds is everything Volovik’s ancestor claim left as a symbol: a specific material, a specific device geometry, and a computed temperature.
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