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  2. Weyl semimetal - Wikipedia

    en.wikipedia.org/wiki/Weyl_semimetal

    A Weyl semimetal is a solid state crystal whose low energy excitations are Weyl fermions that carry electrical charge even at room temperatures. [ 11 ] [ 12 ] [ 13 ] A Weyl semimetal enables realization of Weyl fermions in electronic systems. [ 9 ]

  3. Acoustic metamaterial - Wikipedia

    en.wikipedia.org/wiki/Acoustic_metamaterial

    An acoustic metamaterial, sonic crystal, or phononic crystal is a material designed to manipulate sound waves or phonons in gases, liquids, and solids (crystal lattices).By carefully controlling properties such as the bulk modulus β, density ρ, and chirality, these materials can be tailored to interact with sound in specific ways, such as transmitting, trapping, or amplifying waves at ...

  4. Phonon - Wikipedia

    en.wikipedia.org/wiki/Phonon

    The ground state, also called the "vacuum state", is the state composed of no phonons. Hence, the energy of the ground state is 0. Hence, the energy of the ground state is 0. When a system is in the state | n 1 n 2 n 3 … , we say there are n α phonons of type α , where n α is the occupation number of the phonons.

  5. Quasiparticle - Wikipedia

    en.wikipedia.org/wiki/Quasiparticle

    Solids are made of only three kinds of particles: electrons, protons, and neutrons. None of these are quasiparticles; instead a quasiparticle is an emergent phenomenon that occurs inside the solid. Therefore, while it is quite possible to have a single particle (electron, proton, or neutron) floating in space, a quasiparticle can only exist ...

  6. Dirac matter - Wikipedia

    en.wikipedia.org/wiki/Dirac_matter

    The unique transport properties and the semimetallic state of graphene are the result of the delocalized electrons occupying these p z orbitals. [ 12 ] The semimetallic state corresponds to a linear crossing of energy bands at the K {\displaystyle K} and K ′ {\displaystyle K'} points of graphene's hexagonal Brillouin zone .

  7. Majorana fermion - Wikipedia

    en.wikipedia.org/wiki/Majorana_fermion

    The concept goes back to Majorana's suggestion in 1937 [2] that electrically neutral spin-⁠ 1 / 2 ⁠ particles can be described by a real-valued wave equation (the Majorana equation), and would therefore be identical to their antiparticle, because the wave functions of particle and antiparticle are related by complex conjugation, which leaves the Majorana wave equation unchanged.

  8. Dirac cone - Wikipedia

    en.wikipedia.org/wiki/Dirac_cone

    The three first are Type-I Weyl semimetals, the last one is a Type-II Weyl semimetal. In quantum mechanics , Dirac cones are a kind of crossing-point which electrons avoid , [ 8 ] where the energy of the valence and conduction bands are not equal anywhere in two dimensional lattice k -space , except at the zero dimensional Dirac points.

  9. Phonon polariton - Wikipedia

    en.wikipedia.org/wiki/Phonon_polariton

    Phonon polaritons only result from coupling of transverse optical phonons, this is due to the particular form of the dispersion relation of the phonon and photon and their interaction. Photons consist of electromagnetic waves, which are always transverse. Therefore, they can only couple with transverse phonons in crystals.

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