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Many-body localization

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434:, and the MBL phenomenon was shown to survive. In 2005 and 2006, this was extended to high orders in perturbation theory in high dimensional systems. MBL was argued to survive at least at low energy density. A series of numerical works provided further evidence for the phenomenon in one dimensional systems, at all energy densities (“infinite temperature”). Finally, in 2014 Imbrie presented a proof of MBL for certain one dimensional spin chains with strong disorder, with the localization being stable to arbitrary local perturbations – i.e. the systems were shown to be in a many body localized phase. 27: 381:. A system in a many body localized phase exhibits MBL, and continues to exhibit MBL even when subject to arbitrary local perturbations. Eigenstates of systems exhibiting MBL do not obey the ETH, and generically follow an "area law" for entanglement entropy (i.e. the entanglement entropy scales with the surface area of subregion 99:). The process of thermalization erases local memory of the initial conditions. In textbooks, thermalization is ensured by coupling the system to an external environment or "reservoir," with which the system can exchange energy. What happens if the system is isolated from the environment, and evolves according to its own 892: 418:
MBL was first proposed by P.W. Anderson in 1958 as a possibility that could arise in strongly disordered quantum systems. The basic idea was that if particles all live in a random energy landscape, then any rearrangement of particles would change the energy of the system. Since energy is a conserved
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Quantum mechanical time evolution is unitary and formally preserves all information about the initial condition in the quantum state at all times. However, a quantum system generically contains a macroscopic number of degrees of freedom, but can only be probed through few-body measurements which are
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Many body localized systems exhibit a phenomenon known as emergent integrability. In a non-interacting Anderson insulator, the occupation number of each localized single particle orbital is separately a local integral of motion. It was conjectured (and proven by Imbrie) that a similar extensive set
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approaches a thermal density matrix at a temperature set by the energy density in the state, then the system has "thermalized," and no local information about the initial condition can be extracted from local measurements. This process of "quantum thermalization" may be understood in terms of
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Choi, Soonwon; Choi, Joonhee; Landig, Renate; Kucsko, Georg; Zhou, Hengyun; Isoya, Junichi; Jelezko, Fedor; Onoda, Shinobu; Sumiya, Hitoshi; Khemani, Vedika; von Keyserlingk, Curt; Yao, Norman Y.; Demler, Eugene; Lukin, Mikhail D. (2017).
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In thermalizing systems, entanglement entropy grows as a power law in time starting from low entanglement initial conditions. In MBL systems, entanglement entropy grows logarithmically in time starting from low entanglement initial
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Schreiber, M.; Hodgman, S. S.; Bordia, P.; Luschen, H. P.; Fischer, M. H.; Vosk, R.; Altman, E.; Schneider, U.; Bloch, I. (2015). "Observation of many-body localization of interacting fermions in a quasirandom optical lattice".
426:), the existence of the phenomenon for many particle systems remained a conjecture for decades. In 1980 Fleishman and Anderson demonstrated the phenomenon survived the addition of interactions to lowest order in 3012:
Zhang, J.; Hess, P. W.; Kyprianidis, A.; Becker, P.; Lee, A.; Smith, J.; Pagano, G.; Potirniche, I.-D.; Potter, A. C.; Vishwanath, A.; Yao, N. Y.; Monroe, C. (2017). "Observation of a discrete time crystal".
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In thermalizing systems, a memory of initial conditions is not accessible in local observables at long times. In MBL systems, memory of initial conditions remains accessible in local observables at long
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Choi, J.-y.; Hild, S.; Zeiher, J.; Schauss, P.; Rubio-Abadal, A.; Yefsah, T.; Khemani, V.; Huse, D. A.; Bloch, I.; Gross, C. (2016). "Exploring the many-body localization transition in two dimensions".
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In thermalizing systems, the dynamics of out-of-time-ordered correlators forms a linear light cone which reflects the ballistic propagation of information. In MBL systems, the light cone is logarithmic.
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Smith, J.; Lee, A.; Richerme, P.; Neyenhuis, B.; Hess, P. W.; Hauke, P.; Heyl, M.; Huse, D. A.; Monroe, C. (2016). "Many-body localization in a quantum simulator with programmable random disorder".
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operators, and the coefficients fall off exponentially with distance. This Hamiltonian manifestly contains an extensive number of localized integrals of motion or "l-bits" (the operators
623: 373:, then the system retains forever a memory of its initial condition in local observables. This latter possibility is referred to as "many body localization," and involves 371: 335: 215: 2199:
Basko, D.M.; Aleiner, I.L.; Altshuler, B.L. (2006). "Metal–insulator transition in a weakly interacting many-electron system with localized single-particle states".
887:{\displaystyle H=\sum _{i}h_{i}^{\prime }\tau _{i}^{z}+\sum _{ij}J_{ij}\tau _{i}^{z}\tau _{j}^{z}+\sum _{ijk}K_{ijk}\tau _{i}^{z}\tau _{j}^{z}\tau _{k}^{z}+\cdots ,} 431: 903:
are Pauli operators that are related to the physical Pauli operators by a local unitary transformation, the ... indicates additional terms which only involve
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A number of experiments have been reported observing the MBL phenomenon. Most of these experiments involve synthetic quantum systems, such as assemblies of
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In thermalizing systems, energy eigenstates have volume law entanglement entropy. In MBL systems, energy eigenstates have area law entanglement entropy.
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Altshuler, Boris L.; Gefen, Yuval; Kamenev, Alex; Levitov, Leonid S. (1997). "Quasiparticle Lifetime in a Finite System: A Nonperturbative Approach".
918:, which all commute with the Hamiltonian). If the original Hamiltonian is perturbed, the l-bits get redefined, but the integrable structure survives. 1954:
Chen, Xiao; Zhou, Tianci; Huse, David A.; Fradkin, Eduardo (July 2017). "Out-of-time-order correlations in many-body localized and thermal phases".
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Nandkishore, Rahul; Gopalakrishnan, Sarang; Huse, David A. (2014). "Spectral features of a many-body-localized system weakly coupled to a bath".
1633:Žnidarič, Marko; Prosen, Tomaž; Prelovšek, Peter (February 25, 2008). "Many-body localization in the Heisenberg XXZ magnet in a random field". 437:
It is now believed that MBL can arise also in periodically driven "Floquet" systems where energy is conserved only modulo the drive frequency.
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Gornyi, I. V.; Mirlin, A. D.; Polyakov, D. G. (2005). "Interacting Electrons in Disordered Wires: Anderson Localization and Low-TTransport".
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of local integrals of motion should also exist in the MBL phase. Consider for specificity a one dimensional spin-1/2 chain with Hamiltonian
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Rigol, Marcos; Dunjko, Vanja; Olshanii, Maxim (April 2008). "Thermalization and its mechanism for generic isolated quantum systems".
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Serbyn, Maksym; Papić, Z.; Abanin, Dmitry A. (2013). "Local Conservation Laws and the Structure of the Many-Body Localized States".
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MBL enables the formation of exotic forms of quantum order that could not arise in thermal equilibrium, through the phenomenon of
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Deutsch, J. M.; Li, Haibin; Sharma, Auditya (April 30, 2013). "Microscopic origin of thermodynamic entropy in isolated systems".
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quantity in quantum mechanics, such a process can only be virtual and cannot lead to any transport of particle number or energy.
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He, Rong-Qiang; Lu, Zhong-Yi (February 10, 2017). "Characterizing many-body localization by out-of-time-ordered correlation".
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While localization for single particle systems was demonstrated already in Anderson's original paper (coming to be known as
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of a thermalizing system in a pure state plays the role of thermal entropy. Thermalizing systems therefore generically have
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fails to approach a thermal density matrix even in the long time limit, and remains instead close to its initial condition
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D’Alessio, Luca; Polkovnikov, Anatoli (2013). "Many-body energy localization transition in periodically driven systems".
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Nandkishore, Rahul; Huse, David A. (2015). "Many-Body Localization and Thermalization in Quantum Statistical Mechanics".
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local in real space. The meaningful question then becomes whether accessible local measurements display thermalization.
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Lazarides, Achilleas; Das, Arnab; Moessner, Roderich (2015). "Fate of Many-Body Localization Under Periodic Driving".
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Huse, David A.; Nandkishore, Rahul; Oganesyan, Vadim (2014). "Phenomenology of fully many-body-localized systems".
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Dymarsky, Anatoly; Lashkari, Nima; Liu, Hong (January 25, 2018). "Subsystem eigenstate thermalization hypothesis".
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Kim, Hyungwon; Huse, David A. (2013). "Ballistic Spreading of Entanglement in a Diffusive Nonintegrable System".
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Thermalizing systems generically have non-zero thermal conductivity. MBL systems have zero thermal conductivity.
930:. A form of localization-protected quantum order, arising only in periodically driven systems, is the Floquet 3488: 92: 1909:
Swingle, Brian; Chowdhury, Debanjan (February 21, 2017). "Slow scrambling in disordered quantum systems".
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In thermalizing systems, energy eigenstates obey ETH. In MBL systems, energy eigenstates do not obey ETH.
2587: 674:) that all eigenstates are localized, then there exists a local unitary transformation to new variables 3483: 452: 2366:
Serbyn, Maksym; Papić, Z.; Abanin, D. A. (2014). "Quantum quenches in the many-body localized phase".
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Oganesyan, Vadim; Huse, David A. (2007). "Localization of interacting fermions at high temperature".
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or "volume law" entanglement entropy at any non-zero temperature. They also generically obey the
100: 44: 1780: 385:). A brief list of properties differentiating thermalizing and MBL systems is provided below. 1738: 1020: 423: 37: 402:
Thermalizing systems have continuous local spectra. MBL systems have discrete local spectra.
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Huse, David A.; Nandkishore, Rahul; Oganesyan, Vadim; Pal, Arijeet; Sondhi, S. L. (2013).
8: 3085:"Observation of discrete time-crystalline order in a disordered dipolar many-body system" 427: 3439: 3376: 3303: 3110: 3036: 2980: 2907: 2844: 2785: 2222: 2100: 2012: 1478: 1417: 1356: 1086: 1063:
Deutsch, J M (July 26, 2010). "Thermodynamic entropy of a many-body energy eigenstate".
1012: 430:. In a 1998 study, the analysis was extended to all orders in perturbation theory, in a 3459: 3425: 3362: 3331: 3289: 3261: 3227: 3171: 3135: 3096: 3084: 3064: 3022: 2966: 2935: 2893: 2830: 2771: 2740: 2714: 2687: 2653: 2626: 2568: 2534: 2507: 2481: 2454: 2428: 2401: 2348: 2322: 2295: 2269: 2242: 2208: 2181: 2147: 2120: 2086: 1981: 1963: 1936: 1891: 1873: 1834: 1803: 1761: 1691: 1660: 1642: 1612: 1578: 1551: 1525: 1498: 1464: 1437: 1403: 1376: 1343:
Deutsch, J. M. (February 1, 1991). "Quantum statistical mechanics in a closed system".
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This question can be formalized by considering the quantum mechanical density matrix
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Fleishman, L.; Anderson, P. W. (1980). "Interactions and the Anderson transition".
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Khemani, Vedika; Lazarides, Achilleas; Moessner, Roderich; Sondhi, S. L. (2016).
1739:"Entanglement dynamics in critical random quantum Ising chain with perturbations" 52: 16:
Phenomenon of isolated many-body quantum systems not reaching thermal equilibrium
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Pal, Arijeet; Huse, David A. (2010). "Many-body localization phase transition".
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Else, Dominic V.; Bauer, Bela; Nayak, Chetan (2016). "Floquet Time Crystals".
2495: 2442: 2230: 1757: 1240: 1213: 3477: 3455: 3394: 3319: 3249: 3195: 3126: 3052: 2998: 2923: 2862: 2803: 2736: 2675: 2614: 2556: 2503: 2450: 2419:
Imbrie, John Z. (2016). "On Many-Body Localization for Quantum Spin Chains".
2397: 2344: 2291: 2238: 2169: 2116: 2063: 2055: 2028: 2020: 1715: 1600: 1547: 1364: 1028: 3311: 3241: 1425: 3402: 3327: 3257: 3203: 3160:"Disorder-Induced Localization in a Strongly Correlated Atomic Hubbard Gas" 3144: 3060: 2955:"Absolute stability and spatiotemporal long-range order in Floquet systems" 2931: 2870: 2683: 2622: 2564: 2177: 1999:
Anderson, P. W. (1958). "Absence of Diffusion in Certain Random Lattices".
1977: 1799: 1723: 1608: 1494: 1286: 1190: 1145: 969: 959: 931: 1433: 1372: 2274: 2213: 2152: 2091: 1931: 1408: 1277: 947: 3118: 3044: 2586:
Ponte, Pedro; Papić, Z.; Huveneers, François; Abanin, Dmitry A. (2015).
2388: 1486: 3447: 1680:"Unbounded Growth of Entanglement in Models of Many-Body Localization" 1394:
Srednicki, Mark (August 1, 1994). "Chaos and quantum thermalization".
76: 3349:
Wei, Ken Xuan; Ramanathan, Chandrasekhar; Cappellaro, Paola (2018).
1108:
Santos, Lea F.; Polkovnikov, Anatoli; Rigol, Marcos (July 5, 2012).
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Fan, Ruihua; Zhang, Pengfei; Shen, Huitao; Zhai, Hui (May 2017).
1302:"Universal eigenstate entanglement of chaotic local Hamiltonians" 1781:"Out-of-time-ordered correlators in many-body localized systems" 2953:
von Keyserlingk, C. W.; Khemani, Vedika; Sondhi, S. L. (2016).
283:{\displaystyle S=-\operatorname {Tr} (\rho _{A}\log \rho _{A})} 2816: 79:
quantum systems. It is characterized by the system failing to
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are random variables drawn from a distribution of some width
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Bardarson, Jens H.; Pollmann, Frank; Moore, Joel E. (2012).
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Kondov, S. S.; McGehee, W. R.; Xu, W.; DeMarco, B. (2015).
2757: 3011: 2946: 1823:"Out-of-time-order correlation for many-body localization" 3415: 2585: 1779:
Huang, Yichen; Zhang, Yong-Liang; Chen, Xie (July 2017).
174:{\displaystyle \rho _{A}=\operatorname {Tr} _{B}\rho (t)} 114:
of the system. If the system is divided into a subregion
2704: 2465: 3348: 2588:"Many-Body Localization in Periodically Driven Systems" 1632: 1214:"Does a Single Eigenstate Encode the Full Hamiltonian?" 3157: 1677: 1107: 3278: 2198: 2035: 1671: 1628: 1626: 689: 455: 343: 307: 232: 187: 132: 3210: 3081: 2810: 2524: 2471: 2137: 1212:
Garrison, James R.; Grover, Tarun (April 30, 2018).
2751: 2698: 1953: 1454: 1254: 2070: 1623: 982: 886: 617: 365: 329: 282: 209: 173: 86: 3342: 3151: 2643: 2365: 2253: 2041: 3475: 2518: 2192: 2131: 1908: 1820: 226:. In this perspective, the entanglement entropy 95:assumes that systems go to thermal equilibrium ( 75:is a dynamical phenomenon occurring in isolated 3351:"Exploring Localization in Nuclear Spin Chains" 2637: 2359: 1158: 1110:"Weak and strong typicality in quantum systems" 988: 126:alone is encoded in the reduced density matrix 2883: 2579: 1778: 1211: 3005: 2877: 2259: 118:(the region being probed) and its complement 3409: 3272: 3075: 1992: 937: 2819:"Phase Structure of Driven Quantum Systems" 2306: 1562: 2412: 3429: 3384: 3366: 3293: 3231: 3185: 3175: 3134: 3100: 3026: 2988: 2970: 2897: 2852: 2834: 2793: 2775: 2718: 2657: 2538: 2485: 2432: 2387: 2326: 2273: 2212: 2151: 2090: 1967: 1930: 1877: 1848: 1838: 1705: 1695: 1646: 1582: 1529: 1468: 1407: 1393: 1327: 1317: 1276: 1239: 1229: 1172: 1135: 1125: 1076: 1002: 991:Annual Review of Condensed Matter Physics 440: 1998: 1021:10.1146/annurev-conmatphys-031214-014726 2312: 1568: 1342: 1062: 3476: 2760:"Localization-protected quantum order" 2418: 661:. When the disorder is strong enough ( 1736: 1299: 1863: 928:localization-protected quantum order 296:eigenstate thermalization hypothesis 103:? Does the system still thermalize? 20: 1053:. Menlo Park, CA: Benjamin/Cummings 13: 716: 553: 377:failing to act as a reservoir for 14: 3500: 618:{\displaystyle H=\sum _{i}\left,} 921: 25: 1947: 1902: 1857: 1814: 1772: 1730: 1448: 1387: 1329:10.1016/j.nuclphysb.2018.09.013 87:Thermalization and localization 3386:10.1103/PhysRevLett.120.070501 3187:10.1103/PhysRevLett.114.083002 2916:10.1103/PhysRevLett.117.090402 2854:10.1103/PhysRevLett.116.250401 2668:10.1103/PhysRevLett.111.127201 2607:10.1103/PhysRevLett.114.140401 2549:10.1103/PhysRevLett.115.030402 2421:Journal of Statistical Physics 1707:10.1103/PhysRevLett.109.017202 1593:10.1103/PhysRevLett.111.127205 1336: 1300:Huang, Yichen (January 2019). 1293: 1248: 1205: 1152: 1101: 1056: 1043: 360: 354: 324: 318: 277: 248: 204: 198: 181:. If, in the long time limit, 168: 162: 1: 2162:10.1103/PhysRevLett.95.206603 1087:10.1088/1367-2630/12/7/075021 975: 93:quantum statistical mechanics 51:in tone and meet Knowledge's 366:{\displaystyle \rho _{A}(0)} 330:{\displaystyle \rho _{A}(T)} 210:{\displaystyle \rho _{A}(t)} 73:Many-body localization (MBL) 7: 2109:10.1103/PhysRevLett.78.2803 953: 10: 3505: 2990:10.1103/PhysRevB.94.085112 2795:10.1103/PhysRevB.88.014206 2729:10.1103/PhysRevB.90.174202 2380:10.1103/PhysRevB.90.174302 2337:10.1103/PhysRevB.82.174411 2284:10.1103/PhysRevB.75.155111 1923:10.1103/PhysRevB.95.060201 1888:10.1103/PhysRevB.95.054201 1850:10.1016/j.scib.2017.04.011 1737:Huang, Yichen (May 2017). 1657:10.1103/PhysRevB.77.064426 1540:10.1103/PhysRevB.90.064203 1269:10.1103/PhysRevE.97.012140 1183:10.1103/PhysRevE.87.042135 1137:10.1103/PhysRevE.86.010102 413: 222:acting as a reservoir for 2496:10.1016/j.aop.2013.02.011 2443:10.1007/s10955-016-1508-x 2231:10.1016/j.aop.2005.11.014 1758:10.1016/j.aop.2017.02.018 1241:10.1103/PhysRevX.8.021026 938:Experimental realizations 646:are Pauli operators, and 81:reach thermal equilibrium 2056:10.1103/PhysRevB.21.2366 2021:10.1103/PhysRev.109.1492 1365:10.1103/PhysRevA.43.2046 1051:Modern Quantum Mechanics 3355:Physical Review Letters 3312:10.1126/science.aaf8834 3242:10.1126/science.aaa7432 3164:Physical Review Letters 2886:Physical Review Letters 2823:Physical Review Letters 2646:Physical Review Letters 2595:Physical Review Letters 2527:Physical Review Letters 2140:Physical Review Letters 2079:Physical Review Letters 1684:Physical Review Letters 1571:Physical Review Letters 1426:10.1103/PhysRevE.50.888 432:zero-dimensional system 1978:10.1002/andp.201600332 1800:10.1002/andp.201600318 1065:New Journal of Physics 888: 619: 441:Emergent integrability 367: 331: 284: 211: 175: 889: 620: 424:Anderson localization 368: 332: 285: 212: 176: 3489:Quantum chaos theory 687: 453: 341: 305: 230: 185: 130: 101:Schrödinger equation 45:improve this article 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Index

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