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1 rsionless lasing, polariton condensation and superfluidity.
2 rts a new kind of parity-preserving skyrmion superfluidity.
3 hases, such as interlayer pairing and p-wave superfluidity.
4 s lies at the heart of superconductivity and superfluidity.
5 al calculations on the stability of resonant superfluidity.
6 er in the solid plays a key role in enabling superfluidity.
7 es are particularly dramatic consequences of superfluidity.
8 g-and possibly to search for exotic forms of superfluidity.
9 increase the critical temperature for s-wave superfluidity.
10 ermion-pair condensates and high-temperature superfluidity.
11 he normal state, known as the Pauli limit of superfluidity.
12 rmi gas that provide definitive evidence for superfluidity.
13 sed in liquid helium are excellent probes of superfluidity.
14  to the realization of exciton circuitry and superfluidity.
15 ropagation is the evidence for IX condensate superfluidity.
16 sical behaviors and quantum devices that use superfluidity.
17  version is considered to be the hallmark of superfluidity.
18 hydrodynamics(2-4), superconductivity(5) and superfluidity(6,7) observed in graphene heterostructures
19  controversy has surrounded the stability of superfluidity against an imbalance between the two spin
20 ights into quantum turbulence, vortices, and superfluidity and also explore the similarities and diff
21 ena in physics, including superconductivity, superfluidity and Bose-Einstein condensation.
22         Bosonic [Formula: see text] exhibits superfluidity and Bose-Einstein condensation.
23  of nonlinear quantum hydrodynamics, such as superfluidity and Cerenkov flow, which is a consequence
24 lvin precision, will facilitate the study of superfluidity and give rise to tunnelling and a large ra
25 e quantum fluids that simultaneously realize superfluidity and magnetism, both of which are associate
26 ase, featuring both intermediate temperature superfluidity and possible pair density wave ground stat
27 n condensates, such as long-range coherence, superfluidity and quantized vorticity.
28 quences for the fundamental understanding of superfluidity and superconductivity and opens up new app
29                                              Superfluidity and superconductivity have been widely stu
30 n-dominated matter, deconfined quark matter, superfluidity and superconductivity with critical temper
31  a quantum liquid leads to phenomena such as superfluidity and superconductivity.
32        Quantized vortices play a key role in superfluidity and superconductivity.
33              This crossover between BCS-type superfluidity and the BEC limit has long been of theoret
34 nomena as ferromagnetism, superconductivity, superfluidity and the Higgs mechanism.
35         Furthermore, it is as fundamental to superfluidity (and superconductivity) as quantized persi
36 nomena of atomic Bose-Einstein condensation, superfluidity, and photon lasing.
37 na such as Bose-Einstein condensates (BECs), superfluidity, and strongly interacting quantum gases(3)
38 ts include a low temperature (0.37 K), their superfluidity, and the ability to easily add a wide vari
39  investigation of the resulting breakdown of superfluidity, and we observe directly the decay of the
40 ch are characterized by quantized vorticity, superfluidity, and, at finite temperatures, two-fluid be
41 how exotic spin transport phenomena, such as superfluidity arising from pairing of spins induced by s
42                      One of the hallmarks of superfluidity, as predicted by the two-fluid model(3,4)
43 ng the importance of small fermion pairs for superfluidity at high critical temperatures.
44 ude collective modes, as well as the loss of superfluidity at high flow velocities.
45 xcitons are expected to condense and exhibit superfluidity at sufficiently low temperatures.
46 ent with the data, and predicts the onset of superfluidity at the observed transition point.
47 uch as (4)He and (3)He-B, which display pure superfluidity at zero temperature and two-fluid behavior
48 where collective interlayer pairing and pair superfluidity can be clearly observed.
49                     Here we demonstrate that superfluidity can be completely restored for specific, a
50 r anomalous Hall effect, whereas the exciton superfluidity can be detected by voltage-drop quantizati
51                                              Superfluidity corresponds to frictionless flow of the ma
52                    Finally, we map effective superfluidity effects to identities among fermionic obse
53 ystems, particularly interesting in 2D where superfluidity emerges via the Berezinskii-Kosterlitz-Tho
54                                              Superfluidity, first discovered in liquid (4)He, is clos
55                                              Superfluidity has been a subject of intense studies and
56 ltracold atomic gases where high-temperature superfluidity has been observed.
57 cial-that intrinsically exhibits topological superfluidity has been ongoing since the discovery of th
58              In atomic Fermi gas experiments superfluidity has not yet been demonstrated; however, lo
59                           The realization of superfluidity in a dilute gas of fermionic atoms, analog
60                               We established superfluidity in a two-state mixture of ultracold fermio
61                                              Superfluidity in Bose-Einstein condensates of excitons c
62 al for understanding many phenomena, such as superfluidity in flat bands(5), orbital magnetic suscept
63 y investigate the excitonic bound states and superfluidity in flat-band insulators pumped with light.
64                                              Superfluidity in its various forms has been of interest
65 densed matter physics since the discovery of superfluidity in liquid (3)He.
66 ies can in principle allow the appearance of superfluidity in the solid.
67 rmi gas is relevant for the quest to observe superfluidity in this system.
68 e hallmark of Bose-Einstein condensation and superfluidity in trapped, weakly interacting Bose gases
69                                  Topological superfluidity is an important concept in electronic mate
70                                 The onset of superfluidity is observed in the compressibility, the ch
71  provide a satisfactory explanation, whereas superfluidity is plausible.
72 rconducting UGe2), the superconductivity (or superfluidity) is actually mediated by magnetic interact
73 s as diverse as cosmology, particle physics, superfluidity, liquid crystals, and metallurgy.
74 many important effects in superconductivity, superfluidity, magnetism, liquid crystals, and plasticit
75 t, thus providing direct evidence of bilayer superfluidity mediated by interlayer coupling.
76 ons preclude long-range order(8,9); however, superfluidity nevertheless emerges at a non-zero critica
77  In fermionic systems, superconductivity and superfluidity occur through the condensation of fermion
78          Examples include superconductivity, superfluidity of (3)He, the anomalous rotation of neutro
79 y then, at lower temperatures, into complete superfluidity of both layers.
80      This behavior discriminates between the superfluidity of interlayer bound pairs and independent
81 ly bound pairs and Bardeen-Cooper-Schrieffer superfluidity of long-range Cooper pairs, and a "pseudo-
82 w route to realizing finite angular momentum superfluidity of spin-polarized fermions in optical latt
83                              We observe that superfluidity often survives when these systems are stir
84    Our results enable the study of polariton superfluidity on a par with other superfluids, as well a
85 perties governed by quantum effects, such as superfluidity or superconductivity.
86 es were consistent with predictions assuming superfluidity, proof of superfluid behaviour has been el
87        This increased complexity arises from superfluidity, quantization of circulation, and, at fini
88 and many-body physics, encompassing phonons, superfluidity, quantized vortices, Josephson junctions a
89                                    Fermionic superfluidity requires the formation of particle pairs,
90 This correlation indicates that the onset of superfluidity requires the pinning and stiffening of the
91 ce of broken time-reversal symmetry, whereas superfluidity results from broken gauge invariance.
92 e crossover is associated with a new form of superfluidity that may provide insights into high-transi
93 nt phenomena from the birth of our cosmos to superfluidity transition.
94 ong interactions, near a Feshbach resonance, superfluidity was observed for a broad range of populati
95                               Indicators for superfluidity were condensates of fermion pairs and vort
96  examples are Bose-Einstein condensation and superfluidity, which have been tested experimentally in
97           The method offers ways of studying superfluidity with molecular nanoprobes under variable t