ライフサイエンスコーパス: superfluidity

1 rts a new kind of parity-preserving skyrmion superfluidity.

2 s lies at the heart of superconductivity and superfluidity.

3 al calculations on the stability of resonant superfluidity.

4 er in the solid plays a key role in enabling superfluidity.

5 g-and possibly to search for exotic forms of superfluidity.

6 increase the critical temperature for s-wave superfluidity.

7 ermion-pair condensates and high-temperature superfluidity.

8 he normal state, known as the Pauli limit of superfluidity.

9 rmi gas that provide definitive evidence for superfluidity.

10 rsionless lasing, polariton condensation and superfluidity.

11 controversy has surrounded the stability of superfluidity against an imbalance between the two spin

12 ights into quantum turbulence, vortices, and superfluidity and also explore the similarities and diff

13 ena in physics, including superconductivity, superfluidity and Bose-Einstein condensation.

14 e quantum fluids that simultaneously realize superfluidity and magnetism, both of which are associate

15 ase, featuring both intermediate temperature superfluidity and possible pair density wave ground stat

16 n condensates, such as long-range coherence, superfluidity and quantized vorticity.

17 quences for the fundamental understanding of superfluidity and superconductivity and opens up new app

18 Superfluidity and superconductivity have been widely stu

19 n-dominated matter, deconfined quark matter, superfluidity and superconductivity with critical temper

20 a quantum liquid leads to phenomena such as superfluidity and superconductivity.

21 Quantized vortices play a key role in superfluidity and superconductivity.

22 This crossover between BCS-type superfluidity and the BEC limit has long been of theoret

23 nomena as ferromagnetism, superconductivity, superfluidity and the Higgs mechanism.

24 Furthermore, it is as fundamental to superfluidity (and superconductivity) as quantized persi

25 nomena of atomic Bose-Einstein condensation, superfluidity, and photon lasing.

26 ts include a low temperature (0.37 K), their superfluidity, and the ability to easily add a wide vari

27 investigation of the resulting breakdown of superfluidity, and we observe directly the decay of the

28 ch are characterized by quantized vorticity, superfluidity, and, at finite temperatures, two-fluid be

29 ng the importance of small fermion pairs for superfluidity at high critical temperatures.

30 ude collective modes, as well as the loss of superfluidity at high flow velocities.

31 ent with the data, and predicts the onset of superfluidity at the observed transition point.

32 Here we demonstrate that superfluidity can be completely restored for specific, a

33 Finally, we map effective superfluidity effects to identities among fermionic obse

34 Superfluidity has been a subject of intense studies and

35 ltracold atomic gases where high-temperature superfluidity has been observed.

36 In atomic Fermi gas experiments superfluidity has not yet been demonstrated; however, lo

37 The realization of superfluidity in a dilute gas of fermionic atoms, analog

38 We established superfluidity in a two-state mixture of ultracold fermio

39 ies can in principle allow the appearance of superfluidity in the solid.

40 rmi gas is relevant for the quest to observe superfluidity in this system.

41 e hallmark of Bose-Einstein condensation and superfluidity in trapped, weakly interacting Bose gases

42 The onset of superfluidity is observed in the compressibility, the ch

43 provide a satisfactory explanation, whereas superfluidity is plausible.

44 rconducting UGe2), the superconductivity (or superfluidity) is actually mediated by magnetic interact

45 s as diverse as cosmology, particle physics, superfluidity, liquid crystals, and metallurgy.

46 many important effects in superconductivity, superfluidity, magnetism, liquid crystals, and plasticit

47 Examples include superconductivity, superfluidity of (3)He, the anomalous rotation of neutro

48 We observe that superfluidity often survives when these systems are stir

49 perties governed by quantum effects, such as superfluidity or superconductivity.

50 es were consistent with predictions assuming superfluidity, proof of superfluid behaviour has been el

51 and many-body physics, encompassing phonons, superfluidity, quantized vortices, Josephson junctions a

52 Fermionic superfluidity requires the formation of particle pairs,

53 This correlation indicates that the onset of superfluidity requires the pinning and stiffening of the

54 ce of broken time-reversal symmetry, whereas superfluidity results from broken gauge invariance.

55 e crossover is associated with a new form of superfluidity that may provide insights into high-transi

56 nt phenomena from the birth of our cosmos to superfluidity transition.

57 ong interactions, near a Feshbach resonance, superfluidity was observed for a broad range of populati

58 Indicators for superfluidity were condensates of fermion pairs and vort

59 examples are Bose-Einstein condensation and superfluidity, which have been tested experimentally in