What does this equation mean?

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.