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20:
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28:
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systems. In such systems, a quantum dot with at least one unpaired electron behaves as a magnetic impurity, and when the dot is coupled to a metallic conduction band, the conduction electrons can scatter off the dot. This is completely analogous to the more traditional case of a magnetic impurity in
459:
and B. Voigt observed that the resistivity of nominally pure gold reaches a minimum at 10 K, and similarly for nominally pure Cu at 2 K. Similar results were discovered in other metals. Kondo described the three puzzling aspects that frustrated previous researchers who tried to explain the effect:
610:
In 2017, teams from the Vienna
University of Technology and Rice University conducted experiments into the development of new materials made from the metals cerium, bismuth and palladium in specific combinations and theoretical work experimenting with models of such structures, respectively. The
524:, the Fermi velocity, experiencing only a mild antiferromagnetic correlation in the vicinity of the impurity. In contrast, as the temperature tends to zero the impurity magnetic moment and one conduction electron moment bind very strongly to form an overall non-magnetic state.
493:
resulting in a divergence as the temperature approaches 0 K, but later methods used non-perturbative techniques to refine his result. These improvements produced a finite resistivity but retained the feature of a resistance minimum at a non-zero temperature. One defines the
513:, it was shown that the Kondo model lies in the strong coupling regime of the Anderson impurity model. The Schrieffer–Wolff transformation projects out the high energy charge excitations in the Anderson impurity model, obtaining the Kondo model as an effective Hamiltonian.
568:
materials, the non-perturbative growth of the interaction leads to quasi-electrons with masses up to thousands of times the free electron mass, i.e., the electrons are dramatically slowed by the interactions. In a number of instances they are
532:, i.e. a situation where the coupling becomes non-perturbatively strong at low temperatures and low energies. In the Kondo problem, the coupling refers to the interaction between the localized magnetic impurities and the itinerant electrons.
264:
1230:
Neupane, Madhab; Alidoust, Nasser; Belopolski, Ilya; Bian, Guang; Xu, Su-Yang; Kim, Dae-Jeong; Shibayev, Pavel P.; Sanchez, Daniel S.; Zheng, Hao; Chang, Tay-Rong; Jeng, Horng-Tay; et al. (2015-09-18).
73:). Kondo's calculation predicted that the scattering rate and the resulting part of the resistivity should increase logarithmically as the temperature approaches 0 K. Extended to a lattice of
471:
of the phonons, below which the phonons. However, in the AuFe alloy, the resistivity continues to rise sharply below 0.01 K, yet there seemed to be no energy gap in AuFe alloy that small.
1460:
Buccheri, F.; Bruce, G. D.; Trombettoni, A.; Cassettari, D.; Babujian, H.; Korepin, V. E.; Sodano, P. (2016-01-01). "Holographic optical traps for atom-based topological Kondo devices".
520:
Schematic of the weakly coupled high temperature situation in which the magnetic moments of conduction electrons in the metal host pass by the impurity magnetic moment at speeds of v
486:
showed that phenomenon was caused by magnetic impurity in nominally pure metals. When Kondo sent a preview of his paper to
Sarachik, Sarachik confirmed the data fit the theory.
447:
are constants independent of temperature. Jun Kondo derived the third term with logarithmic dependence on temperature and the experimentally observed concentration dependence.
294:
1657:
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1178:
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The resistivity of a truly pure metal is expected to decrease monotonically, because with lower temperature, the probability of electron-phonon scattering decreases.
358:
324:
425:
135:
445:
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378:
155:
611:
results of the experiments were published in
December 2017 and, together with the theoretical work, lead to the discovery of a new state, a correlation-driven
1010:
2351:
1707:. Cambridge studies in magnetism (1. paperback ed. (with corr.), transferred to digital printing 2003 ed.). Cambridge: Cambridge Univ. Press.
1286:
Neupane, M.; Alidoust, N.; Xu, S.-Y.; Kondo, T.; Ishida, Y.; Kim, D. J.; Liu, Chang; Belopolski, I.; Jo, Y. J.; Chang, T.-R.; Jeng, H.-T. (2013).
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Dzsaber, S.; Prochaska, L.; Sidorenko, A.; Eguchi, G.; Svagera, R.; Waas, M.; Prokofiev, A.; Si, Q.; Paschen, S. (2017-06-16).
2764:
2533:
1731:
1712:
1692:
1378:
886:
573:. It is believed that a manifestation of the Kondo effect is necessary for understanding the unusual metallic delta-phase of
1359:"Topological Insulators, Topological Dirac semimetals, Topological Crystalline Insulators, and Topological Kondo Insulators"
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2344:
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510:
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1873:
23:
Kondo effect: How gold with a small amount of what were probably iron impurities behaves at low temperatures
2893:
2769:
2419:
1808:
509:
theory were an important contribution to understanding the underlying physics of the problem. Based on the
994:
2958:
2888:
2682:
1288:"Surface electronic structure of the topological Kondo-insulator candidate correlated electron system SmB
1074:
Schrieffer, J.R.; Wolff, P.A. (September 1966). "Relation between the
Anderson and Kondo Hamiltonians".
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2053:
1962:
868:
821:
2630:
2002:
1977:
1724:
Exotic Kondo effects in metals: magnetic ions in a crystalline electric field and tunnelling centres
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1216:
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2172:
1926:
1916:
1772:
775:"Messungen mit Hilfe von flĂĽssigem Helium XI Widerstand der reinen Metalle in tiefen Temperaturen"
728:"Messungen mit Hilfe von flĂĽssigem Helium XI Widerstand der reinen Metalle in tiefen Temperaturen"
2738:
2594:
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2538:
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2018:
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272:
54:
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2707:
2640:
2543:
2507:
2497:
2452:
2069:
2048:
1982:
1203:
588:
Band-structure hybridization and flat band topology in Kondo insulators have been imaged in
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967:
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833:
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739:
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657:
403:
120:
46:
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Extended to a lattice of magnetic ions, the Kondo effect likely explains the formation of
430:
8:
2883:
2849:
2784:
2702:
2692:
2487:
1992:
1972:
1957:
1906:
1658:"Scientists discover entirely new material that cannot be explained by classical physics"
490:
62:
1615:
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1140:
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1052:
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1967:
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1434:
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1339:
1331:
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1002:
955:
936:
882:
867:
Kondo, J. (1970-01-01), Seitz, Frederick; Turnbull, David; Ehrenreich, Henry (eds.),
849:
802:
755:
600:
503:
483:
50:
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1446:
1103:
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2217:
2109:
2089:
2084:
2079:
2074:
1931:
1911:
1868:
1833:
1803:
1738:
Monograph on newer versions of the Kondo effect in non-magnetic contexts especially
1629:
1619:
1557:
1552:
1522:
1487:
1430:
1426:
1399:
BĂ©ri, B.; Cooper, N. R. (2012). "Topological Kondo Effect with
Majorana Fermions".
1366:
1321:
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1144:
1091:
1056:
975:
928:
874:
841:
794:
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665:
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in intermetallic compounds, especially those involving rare earth elements such as
456:
89:
in intermetallic compounds, especially those involving rare earth elements such as
2861:
2599:
2548:
2242:
2197:
1863:
1780:
1233:"Fermi surface topology and hot spot distribution in the Kondo lattice system CeB
1148:
595:
In 2012, Beri and Cooper proposed a topological Kondo effect could be found with
570:
545:
506:
479:
84:
908:
2804:
2779:
2558:
2305:
2252:
2134:
2023:
1594:
Proceedings of the
National Academy of Sciences of the United States of America
1271:
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604:
66:
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2028:
1997:
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1335:
1006:
940:
853:
806:
798:
759:
751:
565:
541:
78:
1624:
1095:
467:
The resistivity should rapidly plateau when the temperature drops below the
259:{\displaystyle \rho (T)=\rho _{0}+aT^{2}+c_{m}\ln {\frac {\mu }{T}}+bT^{5},}
2844:
2754:
2472:
2414:
2399:
2114:
1838:
1741:
1643:
1574:
1438:
1343:
1060:
553:
327:
94:
1523:"Kondo Insulator to Semimetal Transformation Tuned by Spin-Orbit Coupling"
1156:
2502:
2329:
2234:
1952:
1921:
1901:
1848:
1131:
581:
468:
106:
70:
822:"The electrical resistance of gold, copper and lead at low temperatures"
474:
The phenomenon is universal, so any explanation should apply in general.
2149:
1987:
1823:
1326:
1287:
873:, Solid State Physics, vol. 23, Academic Press, pp. 183–281,
1117:
Cronenwett, Sara M. (1998). "A Tunable Kondo Effect in
Quantum Dots".
932:
711:
686:
69:
conduction electrons off d-orbital electrons localized at impurities (
2635:
2207:
2033:
1818:
641:
620:
574:
557:
98:
58:
31:
498:
as the energy scale limiting the validity of the Kondo results. The
2733:
1539:
1474:
1606:
1459:
1413:
1308:
1253:
2257:
2224:
2202:
2182:
561:
102:
57:
with temperature. The cause of the effect was first explained by
38:
954:
Sarachik, M. P.; Corenzwit, E.; Longinotti, L. D. (1964-08-17).
2192:
2187:
1793:
1679:- special issue of the Journal of the Physical Society of Japan
1520:
820:
de Haas, W. J.; de Boer, J.; van dën Berg, G. J. (1934-05-01).
549:
90:
19:
2167:
1788:
1229:
27:
1073:
953:
819:
516:
1798:
1687:. Cambridge ; New York: Cambridge University Press.
53:, resulting in a characteristic change i.e. a minimum in
956:"Resistivity of Mo-Nb and Mo-Re Alloys Containing 1% Fe"
1357:
Hasan, M. Zahid; Xu, Su-Yang; Neupane, Madhab (2015),
1285:
433:
406:
386:
366:
336:
302:
275:
166:
143:
123:
1588:
Lai, H.H.; Grefe, S.E.; Paschen, S.; Si, Q. (2012).
528:
The Kondo effect can be considered as an example of
77:, the Kondo effect likely explains the formation of
439:
419:
392:
372:
352:
318:
288:
258:
149:
129:
1587:
2935:
1365:, John Wiley & Sons, Ltd., pp. 55–100,
1590:"Weyl–Kondo semimetal in heavy-fermion systems"
639:
1356:
687:"Resistance Minimum in Dilute Magnetic Alloys"
2345:
1757:
1721:
772:
725:
105:. The Kondo effect has also been observed in
1771:
157:, including the Kondo effect, is written as
65:to the problem to account for scattering of
1677:Kondo Effect - 40 Years after the Discovery
2359:
2352:
2338:
1847:
1764:
1750:
1398:
1116:
995:"Myriam Sarachik Never Gave Up on Physics"
1633:
1623:
1605:
1556:
1538:
1473:
1412:
1325:
1307:
1270:
1252:
1130:
710:
669:
590:angle-resolved photoemission spectroscopy
1031:
913:Journal of the Physical Society of Japan
773:Meissner, W.; Voigt, B. (January 1930).
726:Meissner, W.; Voigt, B. (January 1930).
515:
26:
18:
2954:Electric and magnetic fields in matter
2936:
2430:Two-dimensional conformal field theory
1702:
580:The Kondo effect has been observed in
296:is the residual resistivity, the term
2944:Electrical resistance and conductance
2333:
1745:
1685:The physics of dilute magnetic alloys
1682:
1034:"Localized Magnetic States in Metals"
992:
906:
866:
684:
16:Physical phenomenon due to impurities
2288:
1013:from the original on August 31, 2020
2312:
1722:Cox, D. L.; Zawadowski, A. (1999).
1705:The Kondo problem to heavy fermions
489:Kondo's solution was derived using
13:
1670:
993:Chang, Kenneth (August 31, 2020).
117:The dependence of the resistivity
14:
2970:
2925:Template:Quantum mechanics topics
607:may also demonstrate the effect.
2920:
2919:
2311:
2299:
2287:
2276:
2275:
1726:. London: Taylor & Francis.
870:Theory of Dilute Magnetic Alloys
560:, and actinide elements such as
360:is from the lattice vibrations:
326:shows the contribution from the
101:, and actinide elements such as
1650:
1581:
1514:
1453:
1392:
1350:
1279:
1223:
1171:
1110:
1067:
1025:
691:Progress of Theoretical Physics
599:, while it has been shown that
511:Schrieffer–Wolff transformation
1558:10.1103/PhysRevLett.118.246601
1431:10.1103/PhysRevLett.109.156803
986:
947:
900:
860:
813:
766:
719:
678:
633:
176:
170:
1:
1874:Spontaneous symmetry breaking
1703:Hewson, Alexander C. (2003).
1699:. Monograph by Kondo himeslf.
1492:10.1088/1367-2630/18/7/075012
879:10.1016/S0081-1947(08)60616-5
846:10.1016/S0031-8914(34)80310-2
626:
1149:10.1126/science.281.5376.540
478:Experiments in the 1960s by
45:describes the scattering of
7:
2889:Quantum information science
907:Kondo, Jun (January 2005).
615:. The team dubbed this new
535:
10:
2975:
2054:Spin gapless semiconductor
1963:Nearly free electron model
1272:10.1103/PhysRevB.92.104420
450:
61:, who applied third-order
2914:
2797:
2747:
2726:
2675:
2649:
2613:
2577:
2526:
2445:
2438:
2367:
2271:
2233:
2158:
2102:
2062:
2011:
2003:Density functional theory
1978:electronic band structure
1945:
1894:
1887:
1856:
1845:
1779:
1371:10.1002/9783527681594.ch4
980:10.1103/PhysRev.135.A1041
671:10.4249/scholarpedia.7529
330:properties, and the term
289:{\displaystyle \rho _{0}}
112:
2173:Bogoliubov quasiparticle
1917:Quantum spin Hall effect
1809:Bose–Einstein condensate
1773:Condensed matter physics
799:10.1002/andp.19303990803
752:10.1002/andp.19303990702
2585:2D free massless scalar
2478:Quantum electrodynamics
2405:QFT in curved spacetime
1625:10.1073/pnas.1715851115
1527:Physical Review Letters
1401:Physical Review Letters
1096:10.1103/PhysRev.149.491
500:Anderson impurity model
2906:Quantum thermodynamics
2830:On shell and off shell
2825:Loop quantum cosmology
2667:N = 4 super Yang–Mills
2626:N = 1 super Yang–Mills
2493:Scalar electrodynamics
2483:Quantum chromodynamics
2385:Conformal field theory
2361:Quantum field theories
1462:New Journal of Physics
1363:Topological Insulators
1211:Cite journal requires
1179:"Revival of the Kondo"
1061:10.1103/PhysRev.124.41
525:
441:
421:
394:
374:
354:
353:{\displaystyle bT^{5}}
320:
319:{\displaystyle aT^{2}}
290:
260:
151:
131:
55:electrical resistivity
34:
24:
2879:Quantum hydrodynamics
2874:Quantum hadrodynamics
2498:Scalar chromodynamics
2049:Topological insulator
1983:Anderson localization
1656:Gabbatiss, J. (2017)
1296:Nature Communications
1032:Anderson, P. (1961).
909:"Sticking to My Bush"
519:
442:
422:
420:{\displaystyle c_{m}}
395:
375:
355:
321:
291:
261:
152:
132:
130:{\displaystyle \rho }
30:
22:
2949:Correlated electrons
2850:Quantum fluctuations
2820:Loop quantum gravity
2390:Lattice field theory
1927:Aharonov–Bohm effect
1814:Fermionic condensate
440:{\displaystyle \mu }
431:
404:
384:
364:
334:
300:
273:
164:
141:
121:
47:conduction electrons
2884:Quantum information
2488:Quartic interaction
2318:Physics WikiProject
1993:tight binding model
1973:Fermi liquid theory
1958:Free electron model
1907:Quantum Hall effect
1888:Electrons in solids
1683:KondĹŤ, Jun (2012).
1616:2018PNAS..115...93L
1549:2017PhRvL.118x6601D
1484:2016NJPh...18g5012B
1423:2012PhRvL.109o6803B
1318:2013NatCo...4.2991N
1263:2015PhRvB..92j4420N
1141:1998Sci...281..540C
1088:1966PhRv..149..491S
1053:1961PhRv..124...41A
972:1964PhRv..135.1041S
966:(4A): A1041–A1045.
925:2005JPSJ...74....1K
838:1934Phy.....1.1115D
791:1930AnP...399..892M
744:1930AnP...399..761M
703:1964PThPh..32...37K
685:Kondo, Jun (1964).
662:2009SchpJ...4.7529H
601:quantum simulations
491:perturbation theory
75:magnetic impurities
63:perturbation theory
51:magnetic impurities
2959:Physical phenomena
2770:Nambu–Jona-Lasinio
2698:Higher dimensional
2605:Wess–Zumino–Witten
2395:Noncommutative QFT
1879:Critical phenomena
1327:10.1038/ncomms3991
999:The New York Times
779:Annalen der Physik
732:Annalen der Physik
530:asymptotic freedom
526:
437:
417:
390:
370:
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316:
286:
256:
147:
127:
49:in a metal due to
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25:
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2326:
2213:Exciton-polariton
2098:
2097:
2070:Thermoelectricity
1733:978-0-7484-0889-4
1714:978-0-521-59947-4
1694:978-1-107-02418-2
1380:978-3-527-68159-4
1241:Physical Review B
1125:(5376): 540–544.
933:10.1143/JPSJ.74.1
888:978-0-12-607723-0
712:10.1143/PTP.32.37
597:Majorana fermions
502:and accompanying
496:Kondo temperature
484:Bell Laboratories
469:Debye temperature
393:{\displaystyle b}
373:{\displaystyle a}
235:
150:{\displaystyle T}
2966:
2923:
2922:
2840:Quantum dynamics
2513:Yang–Mills–Higgs
2468:Non-linear sigma
2458:Euler–Heisenberg
2443:
2442:
2354:
2347:
2340:
2331:
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2315:
2314:
2303:
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2279:
2278:
2218:Phonon polariton
2110:Amorphous magnet
2090:Electrostriction
2085:Flexoelectricity
2080:Ferroelectricity
2075:Piezoelectricity
1932:Josephson effect
1912:Spin Hall effect
1892:
1891:
1869:Phase transition
1851:
1834:Luttinger liquid
1781:States of matter
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1214:
1209:
1207:
1199:
1197:
1196:
1190:
1184:. Archived from
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1132:cond-mat/9804211
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864:
858:
857:
832:(7): 1115–1124.
817:
811:
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770:
764:
763:
723:
717:
716:
714:
682:
676:
675:
673:
640:Hewson, Alex C;
637:
617:quantum material
546:Kondo insulators
457:Walther Meissner
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86:Kondo insulators
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2862:Quantum gravity
2789:
2748:Particle theory
2743:
2722:
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2645:
2609:
2573:
2527:Low dimensional
2522:
2463:Ginzburg–Landau
2434:
2425:Topological QFT
2363:
2358:
2328:
2323:
2267:
2248:Granular matter
2243:Amorphous solid
2229:
2154:
2140:Antiferromagnet
2130:Superparamagnet
2103:Magnetic phases
2094:
2058:
2007:
1968:Bloch's theorem
1941:
1883:
1864:Order parameter
1857:Phase phenomena
1852:
1843:
1775:
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1671:Further reading
1668:
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1662:The Independent
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1076:Physical Review
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960:Physical Review
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767:
724:
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605:ultracold atoms
571:superconductors
538:
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507:renormalization
480:Myriam Sarachik
453:
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2805:Casimir effect
2801:
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2787:
2782:
2780:Standard Model
2777:
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2650:Superconformal
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2631:Seiberg–Witten
2628:
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2617:
2615:
2614:Supersymmetric
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2306:Physics Portal
2297:
2285:
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2255:
2253:Liquid crystal
2250:
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2120:Superdiamagnet
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2044:Superconductor
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2024:Mott insulator
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2015:
2013:
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1665:
1649:
1580:
1533:(24): 246601.
1513:
1452:
1407:(15): 156803.
1391:
1379:
1349:
1289:
1278:
1247:(10): 104420.
1234:
1222:
1213:|journal=
1170:
1109:
1082:(2): 491–492.
1066:
1024:
985:
946:
899:
887:
859:
812:
785:(8): 892–936.
765:
738:(7): 761–797.
718:
677:
646:"Kondo effect"
631:
630:
628:
625:
613:Weyl semimetal
542:heavy fermions
537:
534:
521:
476:
475:
472:
465:
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80:heavy fermions
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2902:
2901:Quantum logic
2899:
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2835:Quantum chaos
2833:
2831:
2828:
2826:
2823:
2821:
2818:
2816:
2813:
2811:
2810:Cosmic string
2808:
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2800:
2796:
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2701:
2699:
2696:
2694:
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2689:
2686:
2684:
2683:Pure 4D N = 1
2681:
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2674:
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2564:Thirring–Wess
2562:
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2557:
2555:
2552:
2550:
2547:
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2540:
2539:Bullough–Dodd
2537:
2535:
2534:2D Yang–Mills
2532:
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2410:String theory
2408:
2406:
2403:
2401:
2398:
2396:
2393:
2391:
2388:
2386:
2383:
2381:
2380:Axiomatic QFT
2378:
2376:
2375:Algebraic QFT
2373:
2372:
2370:
2366:
2362:
2355:
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2029:Semiconductor
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2020:
2017:
2016:
2014:
2010:
2004:
2001:
1999:
1998:Hubbard model
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1501:
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1481:
1476:
1471:
1468:(7): 075012.
1467:
1463:
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1432:
1428:
1424:
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1218:
1205:
1191:on 2017-05-17
1187:
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655:
651:
647:
643:
636:
632:
624:
622:
618:
614:
608:
606:
602:
598:
593:
592:experiments.
591:
586:
583:
578:
576:
572:
567:
566:heavy fermion
563:
559:
555:
551:
547:
543:
533:
531:
518:
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512:
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497:
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329:
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110:
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81:
76:
72:
68:
64:
60:
56:
52:
48:
44:
40:
33:
29:
21:
2916:
2845:Quantum foam
2785:Stueckelberg
2739:Chern–Simons
2676:Supergravity
2415:Supergravity
2400:Gauge theory
2316:
2304:
2292:
2280:
2198:Pines' demon
1937:Kondo effect
1936:
1839:Time crystal
1723:
1704:
1684:
1661:
1652:
1600:(1): 93–97.
1597:
1593:
1583:
1530:
1526:
1516:
1465:
1461:
1455:
1404:
1400:
1394:
1384:, retrieved
1362:
1352:
1299:
1295:
1281:
1244:
1240:
1225:
1204:cite journal
1193:. Retrieved
1186:the original
1173:
1122:
1118:
1112:
1079:
1075:
1069:
1047:(1): 41–53.
1044:
1040:
1027:
1015:. Retrieved
998:
988:
963:
959:
949:
916:
912:
902:
892:, retrieved
869:
862:
829:
825:
815:
782:
778:
768:
735:
731:
721:
697:(1): 37–49.
694:
690:
680:
653:
650:Scholarpedia
649:
635:
609:
594:
587:
579:
554:praseodymium
539:
527:
495:
488:
477:
454:
328:Fermi liquid
268:
116:
95:praseodymium
85:
79:
74:
43:Kondo effect
42:
36:
2727:Topological
2641:Wess–Zumino
2554:Sine-Gordon
2544:Gross–Neveu
2453:Born–Infeld
2420:Thermal QFT
2235:Soft matter
2135:Ferromagnet
1953:Drude model
1922:Berry phase
1902:Hall effect
1302:(1): 2991.
1017:October 13,
656:(3): 7529.
619:Weyl-Kondo
582:quantum dot
107:quantum dot
71:Kondo model
2938:Categories
2508:Yang–Mills
2150:Spin glass
2145:Metamagnet
2125:Paramagnet
2012:Conduction
1988:BCS theory
1829:Superfluid
1824:Supersolid
1540:1612.03972
1475:1511.06574
1386:2020-04-26
1195:2016-08-19
919:(1): 1–3.
894:2024-06-01
627:References
2917:See also:
2636:Super QCD
2590:Liouville
2578:Conformal
2549:Schwinger
2208:Polariton
2115:Diamagnet
2063:Couplings
2039:Conductor
2034:Semimetal
2019:Insulator
1895:Phenomena
1819:Fermi gas
1607:1206.2224
1567:0031-9007
1508:118610269
1500:1367-2630
1414:1206.2224
1336:2041-1723
1309:1312.1979
1254:1411.0302
1007:0362-4331
941:0031-9015
854:0031-8914
807:0003-3804
760:0003-3804
642:Jun Kondo
621:semimetal
585:a metal.
575:plutonium
558:ytterbium
504:Wilsonian
455:In 1930,
435:μ
278:ρ
230:μ
225:
184:ρ
168:ρ
125:ρ
109:systems.
99:ytterbium
67:s-orbital
59:Jun Kondo
32:Jun Kondo
2713:Type IIB
2708:Type IIA
2693:4D N = 8
2688:4D N = 1
2657:6D (2,0)
2621:4D N = 1
2600:Polyakov
2559:Thirring
2368:Theories
2282:Category
2263:Colloids
1644:29255021
1575:28665644
1447:45712589
1439:23102351
1344:24346502
1104:55838235
1011:Archived
644:(2009).
536:Examples
2815:History
2798:Related
2595:Minimal
2446:Regular
2294:Commons
2258:Polymer
2225:Polaron
2203:Plasmon
2183:Exciton
1635:5776817
1612:Bibcode
1545:Bibcode
1480:Bibcode
1419:Bibcode
1314:Bibcode
1259:Bibcode
1165:5139144
1157:9677192
1137:Bibcode
1119:Science
1084:Bibcode
1049:Bibcode
968:Bibcode
921:Bibcode
834:Bibcode
826:Physica
787:Bibcode
740:Bibcode
699:Bibcode
658:Bibcode
562:uranium
451:History
103:uranium
39:physics
2755:Chiral
2703:Type I
2518:Yukawa
2439:Models
2193:Phonon
2188:Magnon
1946:Theory
1804:Plasma
1794:Liquid
1730:
1711:
1691:
1642:
1632:
1573:
1565:
1506:
1498:
1445:
1437:
1377:
1342:
1334:
1163:
1155:
1102:
1005:
939:
885:
852:
805:
758:
556:, and
550:cerium
269:where
113:Theory
97:, and
91:cerium
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