Steady-state dynamical mean field theory based on influence functional matrix product states
Source abstract
Abstract
We implement the recently developed influence functional matrix product states approach as impurity solver in equilibrium and nonequilibrium dynamical mean field theory (DMFT) calculations of the single-band Hubbard model. The method yields numerically exact descriptions of metallic states without sharp spectral features, at a moderate numerical cost. Systems with narrow quasiparticle or spin-polaron peaks, as well as low-temperature Mott insulators provide more challenges, since these simulations require long time contours or high bond dimensions. A promising field of application is the DMFT simulation of nonequilibrium steady states, which we demonstrate with results for photo-doped Mott systems with long-lived doublon and holon populations.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Quantum many-body systems · Physics of Superconductivity and Magnetism · Theoretical and Computational Physics
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
University of Fribourg
University of Geneva
Max Planck Institute for the Physics of Complex Systems
Princeton University
École Polytechnique Fédérale de Lausanne (EPFL)
Funding
Université de Fribourg · Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung · European Research Council
References (70)
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1. 10.1103/RevModPhys.68.1310.1103/RevModPhys.68.13 ↗
2. 10.1103/PhysRevLett.62.32410.1103/PhysRevLett.62.324 ↗
3. 10.1007/BF0131139710.1007/BF01311397 ↗
4. 10.1103/PhysRevD.24.227810.1103/PhysRevD.24.2278 ↗
5. 10.1103/PhysRevB.72.03512210.1103/PhysRevB.72.035122 ↗
6. 10.1103/PhysRevLett.97.07640510.1103/PhysRevLett.97.076405 ↗
7. 10.1103/RevModPhys.83.34910.1103/RevModPhys.83.349 ↗
8. 10.1103/RevModPhys.80.39510.1103/RevModPhys.80.395 ↗
9. 10.1103/PhysRevLett.99.07640210.1103/PhysRevLett.99.076402 ↗
10. 10.1103/PhysRevB.60.33510.1103/PhysRevB.60.335 ↗
11. 10.1103/PhysRevB.77.07511610.1103/PhysRevB.77.075116 ↗
12. 10.1103/PhysRevB.92.15513210.1103/PhysRevB.92.155132 ↗
13. 10.1103/PhysRevB.90.04514410.1103/PhysRevB.90.045144 ↗
14. 10.1103/PhysRevX.7.03101310.1103/PhysRevX.7.031013 ↗
15. 10.1103/PhysRevB.76.10450910.1103/PhysRevB.76.104509 ↗
16. 10.1103/PhysRevB.93.15516110.1103/PhysRevB.93.155161 ↗
17. 10.1103/PhysRevLett.101.16640510.1103/PhysRevLett.101.166405 ↗
18. 10.1088/1367-2630/11/2/02502110.1088/1367-2630/11/2/025021 ↗
19. 10.1146/annurev-conmatphys-020911-12504510.1146/annurev-conmatphys-020911-125045 ↗
20. 10.1103/PhysRevLett.90.08640210.1103/PhysRevLett.90.086402 ↗
21. 10.1103/PhysRevMaterials.1.04380310.1103/PhysRevMaterials.1.043803 ↗
22. 10.1103/PhysRevLett.97.26640810.1103/PhysRevLett.97.266408 ↗
23. 10.1103/RevModPhys.86.77910.1103/RevModPhys.86.779 ↗
24. 10.1103/PhysRevB.100.23511710.1103/PhysRevB.100.235117 ↗
25. 10.1103/PhysRevB.88.16511510.1103/PhysRevB.88.165115 ↗
26. 10.1103/PhysRevB.81.11513110.1103/PhysRevB.81.115131 ↗
27. 10.1103/PhysRevLett.100.17640310.1103/PhysRevLett.100.176403 ↗
28. 10.1103/PhysRevB.79.03532010.1103/PhysRevB.79.035320 ↗
29. 10.1063/1.166029310.1063/1.1660293 ↗
30. 10.1103/PhysRevB.24.442010.1103/PhysRevB.24.4420 ↗
31. 10.1007/BF0131139110.1007/BF01311391 ↗
32. 10.1103/PhysRevB.82.11511510.1103/PhysRevB.82.115115 ↗
33. 10.1103/PhysRevLett.105.14640410.1103/PhysRevLett.105.146404 ↗
34. 10.1103/PhysRevB.98.07510210.1103/PhysRevB.98.075102 ↗
35. 10.1103/PhysRevLett.121.05740510.1103/PhysRevLett.121.057405 ↗
36. 10.1103/PhysRevLett.115.26680210.1103/PhysRevLett.115.266802 ↗
37. 10.1103/RevModPhys.59.84510.1103/RevModPhys.59.845 ↗
38. 10.1103/PhysRevLett.132.17650110.1103/PhysRevLett.132.176501 ↗
39. 10.1016/j.laa.2009.07.02410.1016/j.laa.2009.07.024 ↗
40. 10.1103/PhysRevX.12.04101810.1103/PhysRevX.12.041018 ↗
41. 10.1103/PhysRevB.111.12512010.1103/PhysRevB.111.125120 ↗
42. 10.1103/PhysRevB.103.04513310.1103/PhysRevB.103.045133 ↗
43. 10.1016/0003-4916(63)90068-X10.1016/0003-4916(63)90068-X ↗
44. 10.1103/PhysRevB.107.19510110.1103/PhysRevB.107.195101 ↗
45. 10.1103/PhysRevB.107.L20111510.1103/PhysRevB.107.L201115 ↗
46. 10.1103/PhysRevB.107.12510310.1103/PhysRevB.107.125103 ↗
47. 10.1103/PhysRevB.110.16511410.1103/PhysRevB.110.165114 ↗
48. 10.1103/PhysRevB.109.04514010.1103/PhysRevB.109.045140 ↗
49. 10.1103/PhysRev.124.4110.1103/PhysRev.124.41 ↗
50. J. W. Negele · 1988
51. 10.1103/PhysRevB.92.07513210.1103/PhysRevB.92.075132 ↗
52. 10.1016/j.aam.2012.12.00110.1016/j.aam.2012.12.001 ↗
53. 10.1103/PhysRevLett.91.14790210.1103/PhysRevLett.91.147902 ↗
54. 10.1103/PhysRevLett.93.04050210.1103/PhysRevLett.93.040502 ↗
55. 10.1103/PhysRevLett.102.24060310.1103/PhysRevLett.102.240603 ↗
56. 10.1103/PhysRevA.91.03230610.1103/PhysRevA.91.032306 ↗
57. 10.1103/PhysRevB.107.L06030510.1103/PhysRevB.107.L060305 ↗
58. 10.1103/PhysRevB.45.647910.1103/PhysRevB.45.6479 ↗
59. 10.1103/PhysRevB.108.20511010.1103/PhysRevB.108.205110 ↗
60. N. Blümer · 2003
61. 10.1103/PhysRev.121.94210.1103/PhysRev.121.942 ↗
62. 10.1016/0370-1573(95)00074-710.1016/0370-1573(95)00074-7 ↗
63. 10.1002/sapm194625126110.1002/sapm1946251261 ↗
64. 10.1103/PhysRevLett.83.13610.1103/PhysRevLett.83.136 ↗
65. 10.1103/PhysRevLett.110.13640410.1103/PhysRevLett.110.136404 ↗
66. 10.1103/PhysRevB.46.1385210.1103/PhysRevB.46.13852 ↗
67. 10.1103/PhysRevB.82.22430210.1103/PhysRevB.82.224302 ↗
68. 10.1103/PhysRevLett.110.12640110.1103/PhysRevLett.110.126401 ↗
69. 10.5281/zenodo.1561116310.5281/zenodo.15611163 ↗
70. 10.1103/PhysRevLett.119.23640210.1103/PhysRevLett.119.236402 ↗