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Weak localization

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each other exactly and these (otherwise random in sign) quantum interference terms survive disorder averaging. Since it is much more likely to find a self-crossing trajectory in low dimensions, the weak localization effect manifests itself much more strongly in low-dimensional systems (films and wires).
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The weak localization correction can be shown to come mostly from quantum interference between self-crossing paths in which an electron can propagate in the clock-wise and counter-clockwise direction around a loop. Due to the identical length of the two paths along a loop, the quantum phases cancel
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part (individual probabilities of diffusive paths) and a number of interference terms (products of the amplitudes corresponding to different paths). These interference terms effectively make it more likely that a carrier will "wander around in a circle" than it would otherwise, which leads to an
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tells us that to find the total probability we have to sum up the quantum-mechanical amplitudes of the paths rather than the probabilities themselves. Therefore, the correct (quantum-mechanical) formula for the probability for an electron to move from a point A to a point B includes the classical
108:, the spin of a carrier is coupled to its momentum. The spin of the carrier rotates as it goes around a self-intersecting path, and the direction of this rotation is opposite for the two directions about the loop. Because of this, the two paths along any loop interfere 78:
of the system is related to the probability of an electron to propagate between two given points in space. Classical physics assumes that the total probability is just the sum of the probabilities of the paths connecting the two points. However
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The strength of either weak localization or weak anti-localization falls off quickly in the presence of a magnetic field, which causes carriers to acquire an additional phase as they move around paths.
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In two dimensions the change in conductivity from applying a magnetic field, due to either weak localization or weak anti-localization can be described by the Hikami-Larkin-Nagaoka equation:
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motion is diffusive rather than ballistic. That is, an electron does not move along a straight line, but experiences a series of random scatterings off impurities which results in a
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is the elastic characteristic field. The characteristic fields are better understood in terms of their corresponding characteristic lengths which are deduced from
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Altshuler, B. L.; D. Khmel'nitzkii; A. I. Larkin; P. A. Lee (1980). "Magnetoresistance and Hall effect in a disordered two-dimensional electron gas".
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can be thought of as the distance traveled before the spin of the electron undergoes the effect of the spin–orbit interaction, and finally
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Poole, D A; Pepper, M; Hughes, A (1982-11-20). "Spin-orbit coupling and weak localisation in the 2D inversion layer of indium phosphide".
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is a physical effect which occurs in disordered electronic systems at very low temperatures. The effect manifests itself as a
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is the spin–orbit characteristic field which can be considered a measure of the strength of the spin–orbit interaction and
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is the phase coherence characteristic field, which is roughly the magnetic field required to destroy phase coherence,
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The effect is quantum-mechanical in nature and has the following origin: In a disordered electronic system, the
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can then be understood as the distance traveled by an electron before it loses phase coherence,
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in the net resistivity. The usual formula for the conductivity of a metal (the so-called
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Bergman, Gerd (1982-04-12). "Influence of Spin-Orbit Coupling on Weak Localization".
2481: 2400: 80: 2516: 2473: 2444: 2425:"Spin–Orbit Interaction and Magnetoresistance in the Two-Dimensional Random System" 2377: 1858: 2359: 2520: 2292:{\displaystyle \sigma (B)-\sigma (0)=\alpha {e^{2} \over 2\pi ^{2}\hbar }\left} 24: 2542: 2528: 2485: 2381: 89: 48: 1400:{\displaystyle \sigma (B)-\sigma (0)=+{e^{2} \over 2\pi ^{2}\hbar }\left} 802:{\displaystyle \sigma (B)-\sigma (0)=-{e^{2} \over 2\pi ^{2}\hbar }\left} 410:{\displaystyle \sigma (B)-\sigma (0)=-{e^{2} \over 2\pi ^{2}\hbar }\left} 75: 68: 40: 51:. The name emphasizes the fact that weak localization is a precursor of 28:
Weak localization is due primarily to self-intersecting scattering paths
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is spin-orbit scattering. Under some condition, this can be rewritten:
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is -1 for weak antilocalization and +1/2 for weak localization.
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There are many possible scattering paths in a disordered system
1114:{\displaystyle H_{4}={2 \over 3}H_{S}+{4 \over 3}H_{SO}+H_{i}} 967:{\displaystyle H_{2}={4 \over 3}H_{SO}+{2 \over 3}H_{S}+H_{i}} 44: 2422: 2308: 2136: 2093: 2063: 2036: 2009: 1948: 1921: 1894: 1867: 1843: 1621: 1428: 1244: 1211: 1184: 1157: 1130: 1038: 981: 891: 821: 538: 472: 426: 133: 1816:{\displaystyle -{3e^{2} \over 2\pi ^{2}\hbar }\left} 518:{\displaystyle \tau ,\tau _{1},\tau _{2},\tau _{3}} 2507:(15). American Physical Society (APS): 1046–1049. 2314: 2291: 2119: 2076: 2049: 2022: 1995: 1934: 1907: 1880: 1849: 1815: 1581:{\displaystyle +{e^{2} \over \pi ^{2}\hbar }\left} 1580: 1399: 1227: 1197: 1170: 1143: 1113: 1023: 966: 876: 801: 517: 458: 409: 2463: 2540: 2423:Hikami, S.; A. I Larkin; Y. Nagaoka (1980). 2325: 2087:In the limit of strong spin–orbit coupling 2397:Electronic Transport in Mesoscopic Systems 2120:{\displaystyle B_{\text{SO}}\gg B_{\phi }} 1996:{\displaystyle {B_{i}=\hbar /4el_{i}^{2}}} 2466:Journal of Physics C: Solid State Physics 2448: 99: 2418: 2416: 877:{\displaystyle H_{1}=H_{0}+H_{SO}+H_{s}} 23: 15: 2498: 2559:Electric and magnetic fields in matter 2541: 2413: 2394: 812:Where the characteristic fields are: 119: 58: 2472:(32). IOP Publishing: L1137–L1145. 55:, which occurs at strong disorder. 13: 1024:{\displaystyle H_{3}=2H_{S}+H_{i}} 14: 2570: 2196: 2127:, the equation above reduces to: 1963: 1656: 1455: 1304: 598: 450: 193: 2429:Progress of Theoretical Physics 2492: 2457: 2399:. Cambridge University Press. 2388: 2353: 2161: 2155: 2146: 2140: 1771: 1757: 1694: 1680: 1269: 1263: 1254: 1248: 791: 758: 739: 706: 687: 654: 645: 612: 563: 557: 548: 542: 459:{\displaystyle a=4DeH/\hbar c} 399: 361: 342: 304: 285: 247: 238: 207: 158: 152: 143: 137: 1: 2346: 2050:{\displaystyle l_{\text{SO}}} 1908:{\displaystyle B_{\text{SO}}} 1205:is magnetic scattering, and 7: 2521:10.1103/physrevlett.48.1046 2478:10.1088/0022-3719/15/32/005 2334: 10: 2575: 2084:is the mean free path. 2326:Magnetic field dependence 2023:{\displaystyle l_{\phi }} 1881:{\displaystyle B_{\phi }} 1178:is inelastic scattering, 1151:is potential scattering, 2554:Condensed matter physics 2382:10.1103/PhysRevB.22.5142 2501:Physical Review Letters 2341:Coherent backscattering 2315:{\displaystyle \alpha } 2316: 2293: 2121: 2078: 2051: 2024: 1997: 1936: 1909: 1882: 1851: 1817: 1582: 1401: 1229: 1228:{\displaystyle H_{SO}} 1199: 1172: 1145: 1115: 1025: 968: 878: 803: 519: 460: 411: 100:Weak anti-localization 29: 21: 2317: 2294: 2122: 2079: 2077:{\displaystyle l_{e}} 2052: 2025: 1998: 1937: 1935:{\displaystyle B_{e}} 1910: 1883: 1852: 1850:{\displaystyle \psi } 1818: 1583: 1402: 1230: 1200: 1198:{\displaystyle H_{S}} 1173: 1171:{\displaystyle H_{i}} 1146: 1144:{\displaystyle H_{0}} 1116: 1026: 969: 879: 804: 520: 461: 412: 53:Anderson localization 27: 19: 2306: 2134: 2091: 2061: 2034: 2007: 1946: 1919: 1892: 1865: 1841: 1619: 1426: 1242: 1209: 1182: 1155: 1128: 1036: 979: 889: 819: 536: 470: 424: 131: 2513:1982PhRvL..48.1046B 2441:1980PThPh..63..707H 2374:1980PhRvB..22.5142A 1991: 106:spin–orbit coupling 2549:Mesoscopic physics 2450:10.1143/PTP.63.707 2395:Datta, S. (1995). 2312: 2289: 2117: 2074: 2047: 2020: 1993: 1977: 1932: 1905: 1878: 1847: 1813: 1578: 1397: 1225: 1195: 1168: 1141: 1111: 1021: 964: 874: 799: 515: 456: 407: 116:net resistivity. 39:correction to the 30: 22: 2302:In this equation 2277: 2257: 2232: 2200: 2101: 2044: 1902: 1801: 1781: 1749: 1724: 1704: 1660: 1566: 1546: 1531: 1506: 1486: 1459: 1385: 1365: 1340: 1308: 1083: 1060: 939: 913: 789: 769: 753: 737: 717: 701: 685: 665: 643: 623: 602: 397: 372: 356: 340: 315: 299: 283: 258: 236: 218: 197: 120:In two dimensions 112:which leads to a 104:In a system with 81:quantum mechanics 59:General principle 33:Weak localization 2566: 2533: 2532: 2496: 2490: 2489: 2461: 2455: 2454: 2452: 2420: 2411: 2410: 2392: 2386: 2385: 2357: 2321: 2319: 2318: 2313: 2298: 2296: 2295: 2290: 2288: 2284: 2283: 2279: 2278: 2273: 2272: 2263: 2258: 2250: 2237: 2233: 2228: 2227: 2218: 2201: 2199: 2195: 2194: 2181: 2180: 2171: 2126: 2124: 2123: 2118: 2116: 2115: 2103: 2102: 2099: 2083: 2081: 2080: 2075: 2073: 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Rev. B 2361: 2355: 2329: 2301: 2086: 1837: 1123: 811: 525:are various 419: 123: 113: 109: 103: 94: 85: 73: 62: 36: 32: 31: 76:resistivity 69:random walk 41:resistivity 2543:Categories 2347:References 2529:0031-9007 2486:0022-3719 2310:α 2270:ϕ 2242:ψ 2239:− 2225:ϕ 2211:⁡ 2197:ℏ 2188:π 2168:α 2153:σ 2150:− 2138:σ 2113:ϕ 2105:≫ 2016:ϕ 1964:ℏ 1874:ϕ 1845:ψ 1793:ϕ 1734:ψ 1731:− 1716:ϕ 1671:⁡ 1657:ℏ 1648:π 1623:− 1516:ψ 1513:− 1470:⁡ 1456:ℏ 1447:π 1378:ϕ 1350:ψ 1347:− 1333:ϕ 1319:⁡ 1305:ℏ 1296:π 1261:σ 1258:− 1246:σ 756:ψ 743:− 704:ψ 652:ψ 649:− 610:ψ 599:ℏ 590:π 570:− 555:σ 552:− 540:σ 507:τ 494:τ 481:τ 474:τ 451:ℏ 385:τ 359:ψ 346:− 328:τ 302:ψ 271:τ 245:ψ 242:− 230:τ 205:ψ 194:ℏ 185:π 165:− 150:σ 147:− 135:σ 2335:See also 86:increase 65:electron 37:positive 2509:Bibcode 2437:Bibcode 2370:Bibcode 1857:is the 2527:  2484:  2403:  1124:Where 466:, and 420:Where 114:lower 45:metal 43:of a 2525:ISSN 2482:ISSN 2401:ISBN 74:The 2517:doi 2474:doi 2445:doi 2378:doi 47:or 2545:: 2523:. 2515:. 2505:48 2503:. 2480:. 2470:15 2468:. 2443:. 2433:63 2431:. 2427:. 2415:^ 2376:. 2366:22 2364:. 2208:ln 2100:SO 2043:SO 2003:. 1901:SO 1861:. 1780:SO 1703:SO 1668:ln 1545:SO 1485:SO 1467:ln 1316:ln 71:. 2531:. 2519:: 2511:: 2488:. 2476:: 2453:. 2447:: 2439:: 2409:. 2384:. 2380:: 2372:: 2286:] 2281:) 2275:B 2266:B 2260:+ 2255:2 2252:1 2246:( 2235:) 2230:B 2221:B 2215:( 2204:[ 2192:2 2184:2 2178:2 2174:e 2165:= 2162:) 2159:0 2156:( 2147:) 2144:B 2141:( 2109:B 2096:B 2070:e 2066:l 2039:l 2012:l 1988:2 1983:i 1979:l 1975:e 1972:4 1968:/ 1961:= 1956:i 1952:B 1928:e 1924:B 1897:B 1870:B 1810:] 1805:) 1799:B 1789:B 1785:+ 1776:B 1772:) 1769:3 1765:/ 1761:4 1758:( 1752:+ 1747:2 1744:1 1738:( 1727:) 1722:B 1712:B 1708:+ 1699:B 1695:) 1692:3 1688:/ 1684:4 1681:( 1675:( 1664:[ 1652:2 1644:2 1637:2 1633:e 1629:3 1575:] 1570:) 1564:B 1558:e 1554:B 1550:+ 1541:B 1534:+ 1529:2 1526:1 1520:( 1509:) 1504:B 1498:e 1494:B 1490:+ 1481:B 1474:( 1463:[ 1451:2 1440:2 1436:e 1430:+ 1394:] 1389:) 1383:B 1374:B 1368:+ 1363:2 1360:1 1354:( 1343:) 1338:B 1329:B 1323:( 1312:[ 1300:2 1292:2 1286:2 1282:e 1276:+ 1273:= 1270:) 1267:0 1264:( 1255:) 1252:B 1249:( 1221:O 1218:S 1214:H 1191:S 1187:H 1164:i 1160:H 1137:0 1133:H 1107:i 1103:H 1099:+ 1094:O 1091:S 1087:H 1081:3 1078:4 1073:+ 1068:S 1064:H 1058:3 1055:2 1050:= 1045:4 1041:H 1017:i 1013:H 1009:+ 1004:S 1000:H 996:2 993:= 988:3 984:H 960:i 956:H 952:+ 947:S 943:H 937:3 934:2 929:+ 924:O 921:S 917:H 911:3 908:4 903:= 898:2 894:H 870:s 866:H 862:+ 857:O 854:S 850:H 846:+ 841:0 837:H 833:= 828:1 824:H 796:] 792:) 787:H 782:4 778:H 772:+ 767:2 764:1 759:( 751:2 748:1 740:) 735:H 730:3 726:H 720:+ 715:2 712:1 707:( 699:2 696:1 691:+ 688:) 683:H 678:2 674:H 668:+ 663:2 660:1 655:( 646:) 641:H 636:1 632:H 626:+ 621:2 618:1 613:( 606:[ 594:2 586:2 580:2 576:e 567:= 564:) 561:0 558:( 549:) 546:B 543:( 511:3 503:, 498:2 490:, 485:1 477:, 454:c 447:/ 443:H 440:e 437:D 434:4 431:= 428:a 404:] 400:) 394:a 389:3 380:1 375:+ 370:2 367:1 362:( 354:2 351:1 343:) 337:a 332:2 323:1 318:+ 313:2 310:1 305:( 297:2 294:1 289:+ 286:) 280:a 275:1 266:1 261:+ 256:2 253:1 248:( 239:) 233:a 226:1 221:+ 216:2 213:1 208:( 201:[ 189:2 181:2 175:2 171:e 162:= 159:) 156:0 153:( 144:) 141:B 138:(

Index



resistivity
metal
semiconductor
Anderson localization
electron
random walk
resistivity
quantum mechanics
Drude formula
spin–orbit coupling
relaxation times
digamma function
Coherent backscattering
Bibcode
1980PhRvB..22.5142A
doi
10.1103/PhysRevB.22.5142
ISBN
978-0521599436


"Spin–Orbit Interaction and Magnetoresistance in the Two-Dimensional Random System"
Bibcode
1980PThPh..63..707H
doi
10.1143/PTP.63.707
doi
10.1088/0022-3719/15/32/005

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