Kosterlitz-Thouless signatures in the low-temperature phase of layered three-dimensional systems
Source abstract
Abstract
We study the quasi-two-dimensional quantum O(2) model, a quantum generalization of the Lawrence-Doniach model, within the nonperturbative renormalization-group approach and propose a generic phase diagram for layered three-dimensional systems with an O(2)-symmetric order parameter. Below the transition temperature we identify a wide region of the phase diagram where the renormalization-group flow is quasi-two-dimensional for length scales smaller than a Josephson length ${l}J$, leading to signatures of Kosterlitz-Thouless physics in the temperature dependence of physical observables. In particular the order parameter varies as a power law of the interplane coupling with an exponent which depends on the anomalous dimension (itself related to the stiffness) of the strictly two-dimensional low-temperature Kosterlitz-Thouless phase.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Physics of Superconductivity and Magnetism · Quantum many-body systems · Quantum and electron transport phenomena
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (49)
Show source-provided references
1. V. L. Berezinskii · Sov. Phys. JETP · 1970 · 32 · 493
2. V. L. Berezinskii · Sov. Phys. JETP · 1971 · 34 · 610
3. 10.1088/0022-3719/6/7/01010.1088/0022-3719/6/7/010 ↗
4. 10.1088/0022-3719/7/6/00510.1088/0022-3719/7/6/005 ↗
5. 10.1103/PhysRevB.16.121710.1103/PhysRevB.16.1217 ↗
6. 10.1103/PhysRevB.21.180610.1103/PhysRevB.21.1806 ↗
7. 10.1103/RevModPhys.59.100110.1103/RevModPhys.59.1001 ↗
8. 10.1103/PhysRevLett.39.120110.1103/PhysRevLett.39.1201 ↗
9. 10.1103/PhysRevB.24.252610.1103/PhysRevB.24.2526 ↗
10. 10.1038/nphys237810.1038/nphys2378 ↗
11. 10.1103/PhysRevLett.113.02040410.1103/PhysRevLett.113.020404 ↗
12. V. L. Berezinskii · Sov. Phys. JETP · 1973 · 37 · 369
13. V. L. Pokrovskii · Sov. Phys. JETP · 1974 · 38 · 847
14. 10.1143/PTP.63.38710.1143/PTP.63.387 ↗
15. 10.1103/PhysRevB.42.1067310.1103/PhysRevB.42.10673 ↗
16. 10.1103/PhysRevB.44.450310.1103/PhysRevB.44.4503 ↗
17. 10.1007/BF0130927810.1007/BF01309278 ↗
18. 10.1103/PhysRevB.45.1307610.1103/PhysRevB.45.13076 ↗
19. 10.1103/PhysRevB.45.1303510.1103/PhysRevB.45.13035 ↗
20. 10.1016/0921-4534(93)90023-J10.1016/0921-4534(93)90023-J ↗
21. 10.1103/PhysRevLett.72.40010.1103/PhysRevLett.72.400 ↗
22. 10.1103/PhysRevB.51.912910.1103/PhysRevB.51.9129 ↗
23. 10.1103/PhysRevB.51.666310.1103/PhysRevB.51.6663 ↗
24. 10.1103/PhysRevB.51.63210.1103/PhysRevB.51.632 ↗
25. 10.1209/0295-5075/99/6600110.1209/0295-5075/99/66001 ↗
26. 10.1103/PhysRevB.94.14440310.1103/PhysRevB.94.144403 ↗
27. 10.1103/PhysRevLett.98.11700810.1103/PhysRevLett.98.117008 ↗
28. W. E. Lawrence · 1970
29. 10.1103/PhysRevA.96.04362310.1103/PhysRevA.96.043623 ↗
30. 10.1103/PhysRevE.90.06210510.1103/PhysRevE.90.062105 ↗
31. 10.1103/PhysRevE.93.06214510.1103/PhysRevE.93.062145 ↗
32. 10.1103/PhysRevB.95.08511310.1103/PhysRevB.95.085113 ↗
33. 10.1103/PhysRevE.96.04210710.1103/PhysRevE.96.042107 ↗
34. 10.1103/PhysRevB.96.17450510.1103/PhysRevB.96.174505 ↗
35. 10.1103/PhysRevLett.75.37810.1103/PhysRevLett.75.378 ↗
36. 10.1103/PhysRevB.64.05451310.1103/PhysRevB.64.054513 ↗
37. 10.1016/j.physleta.2007.03.02810.1016/j.physleta.2007.03.028 ↗
38. 10.1103/PhysRevE.82.04112810.1103/PhysRevE.82.041128 ↗
39. 10.1103/PhysRevA.79.01360110.1103/PhysRevA.79.013601 ↗
40. 10.1103/PhysRevA.85.06360710.1103/PhysRevA.85.063607 ↗
41. 10.1209/0295-5075/104/1600210.1209/0295-5075/104/16002 ↗
42. 10.1103/PhysRevB.89.21441810.1103/PhysRevB.89.214418 ↗
43. 10.1016/S0370-1573(01)00098-910.1016/S0370-1573(01)00098-9 ↗
44. Bertrand Delamotte · 2012
45. P. Kopietz · 201010.1007/978-3-642-05094-7 ↗
46. 10.1016/0370-2693(93)90726-X10.1016/0370-2693(93)90726-X ↗
47. 10.1103/PhysRevE.88.01211310.1103/PhysRevE.88.012113 ↗
48. 10.1103/PhysRevB.40.505610.1103/PhysRevB.40.5056 ↗
49. 10.1007/JHEP08(2016)03610.1007/JHEP08(2016)036 ↗