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Superfluidity

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Lev Landau
Soviet theoretical physicist (1908–1968)
Pyotr Kapitsa
Soviet physicist
Anthony James Leggett
British physicist (1938–2026)
superfluidity
thumb|right|Helium#Helium II|Helium II will "creep" along surfaces in order to find its own level—after a short while, the levels in the two containers will equalize. The [[Rollin film also covers the interior of the larger container; if it were not sealed, the helium II would creep out and escape.]] thumb|right|The liquid helium is in the superfluid phase. A thin invisible film creeps up the inside wall of the bowl and down on the outside. A drop forms. It will fall off into the liquid helium below. This will repeat until the cup is empty—provided the liquid remains superfluid.
Douglas Osheroff
American physicist
Nikolai Bogolyubov
Soviet mathematician and theoretical physicist (1909-1992)
metallic hydrogen
phase of hydrogen
helium-3
thumb|alt=The nucleus is depicted by two red circles with inscribed plus symbols and one purple circle with no inscription. Around the nucleus there is a black ring - a symbol of an electron shell. On it are two teal circles with inscribed minus symbols, depicting electrons.|Diagram of a Helium-3 atom Helium-3 (3He see also helion) is a light, stable isotope of helium with two protons and one neutron (in contrast to the more common isotope, helium-4, which has two protons and two neutrons.) Helium-3 and hydrogen-1 are the only stable nuclides with more protons than neutrons. It was discovered
liquid helium
liquid state of the element helium
perfect fluid
fluid fully characterized by its density and isotropic pressure
fermionic condensate
non-classical state of matter
Isaak Khalatnikov
university teacher at Leiden University (1919–2021)
lambda point
fluid/superfluid transition point of helium
roton
thumb|Roton dispersion relation, showing the quasiparticle energy E(p) as a function of momentum p. A quasiparticle with momentum generated in the local energy minimum is called a roton. In theoretical physics, a roton is an elementary excitation, or quasiparticle, seen in superfluid helium-4 and Bose–Einstein condensates with long-range dipolar interactions or spin-orbit coupling. The dispersion relation of elementary excitations in this superfluid shows a linear increase from the origin, but exhibits first a maximum and then a minimum in energy as the momentum increases. Excitations with mom
Inviscid flow
flow of fluids with zero viscosity (superfluids)
Gross–Pitaevskii equation
describes the ground state of a quantum system of identical bosons using the Hartree–Fock approximation and the pseudopotential interaction model
Second sound
quantum mechanical phenomenon in which heat transfer occurs by wave-like motion
quantum vortex
quantized flux circulation of some physical quantity
superfluid helium-4
superfluid form of the helium-4 isotope
Weyl semimetal
concept in quantum physics
superglass
REDIRECT Supersolid#Superglass
John F. Allen
Canadian physicist (1908–2001)
color superconductivity
phenomenon in quark matter where matter carries color charge without loss
superfluid vacuum theory
theory of fundamental physics