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Overlap fermion

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Initially introduced by Neuberger in 1998, they were quickly taken up for a variety of numerical simulations. By now overlap fermions are well established and regularly used in non-perturbative fermion simulations, for instance in
707: 158: 375: 482: 550: 40: 577: 422: 1218: 739: 747: 609: 505: 395: 322: 147: 123: 621: 1291: 1143: 294:{\displaystyle D_{\text{ov}}={\frac {1}{a}}\left(\left(1+am\right)\mathbf {1} +\left(1-am\right)\gamma _{5}\mathrm {sign} \right)\,} 58: 1313: 327: 854: 91: 434: 510: 612: 1247: 1070: 944: 1082: 1027: 962: 901: 75: 858: 555: 425: 1233: 1212: 1172: 1149: 1051: 1017: 986: 952: 925: 891: 400: 1122:. Cambridge Lecture Notes in Physics. Cambridge: Cambridge University Press. pp. 211–212. 1318: 1287: 1200: 1139: 1098: 1043: 978: 917: 840:{\displaystyle D_{\text{ov}}={\frac {1}{a}}+m+i\,{p\!\!\!/}{\frac {1}{1-s}}+{\mathcal {O}}(a)} 715: 1279: 1190: 1182: 1131: 1123: 1090: 1035: 970: 909: 87: 1260: 585: 126: 1086: 1031: 966: 905: 1195: 490: 380: 307: 150: 132: 108: 1117: 974: 913: 1307: 1186: 1153: 929: 1055: 990: 879: 702:{\displaystyle D_{\text{ov}}=m+i\,{p\!\!\!/}{\frac {1}{1+s}}+{\mathcal {O}}(a)\,} 1005: 424:-hermitian. The sign-function usually has to be calculated numerically, e.g. by 99: 1039: 1283: 1135: 1094: 1127: 1102: 1047: 982: 921: 1204: 611:
the overlap Dirac operator recovers the correct continuum form (using the
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FLAG Working Group; Aoki, S.; et al. (2014). "A.1 Lattice actions".
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Gattringer, C.; Lang, C.B. (2009). "7 Chiral symmetry on the lattice".
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Quantum Chromodynamics on the Lattice: An Introductory Presentation
1177: 945:"Overlap and domainwall fermions: what is the price of chirality?" 1169:
Review of Lattice Results Concerning Low-Energy Particle Physics
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is a free parameter that can be tuned to optimise locality of
15: 1278:. Lecture Notes in Physics 788. Springer. pp. 177–182. 823: 684: 1232:
Kennedy, A.D. (2012). "Algorithms for Dynamical Fermions".
36: 861:(obeying the Ginsparg–Wilson equation) and locality. 750: 718: 624: 588: 558: 513: 493: 437: 403: 383: 330: 310: 161: 135: 111: 1071:"Going chiral: twisted mass versus overlap fermions" 370:{\displaystyle \gamma _{5}A=A^{\dagger }\gamma _{5}} 1171:. Eur. Phys. J. C. Vol. 74. pp. 116–117. 1006:"An introduction to chiral symmetry on the lattice" 31:
may be too technical for most readers to understand
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"8 Chiral symmetry". 545:{\displaystyle s\in \left(-1,1\right)} 712:whereas the unphysical doublers near 41:make it understandable to non-experts 7: 428:. A common choice for the kernel is 507:is the massless Dirac operator and 90:problem. They are a realisation of 262: 259: 256: 253: 14: 857:because they explicitly violate 454: 213: 20: 1075:Computer Physics Communications 1187:10.1140/epjc/s10052-014-2890-7 834: 828: 741:are suppressed by a high mass 695: 689: 470: 458: 282: 266: 71:Lattice fermion discretisation 1: 975:10.1016/S0920-5632(01)01660-7 914:10.1016/s0370-2693(97)01368-3 890:(1–2). Elsevier BV: 141–144. 572:{\displaystyle D_{\text{ov}}} 1004:Chandrasekharan, S. (2004). 1016:(2). Elsevier BV: 373–418. 417:{\displaystyle \gamma _{5}} 105:Overlap fermions with mass 1335: 1040:10.1016/j.ppnp.2004.05.003 1284:10.1007/978-3-642-01850-3 1095:10.1016/j.cpc.2005.03.080 1128:10.1017/CBO9780511583971 855:Nielsen–Ninomiya theorem 92:Ginsparg–Wilson fermions 734:{\displaystyle pa=\pi } 426:rational approximations 1255:Cite journal requires 878:Neuberger, H. (1998). 841: 735: 703: 613:Feynman slash notation 605: 573: 546: 501: 478: 418: 391: 371: 318: 295: 143: 119: 842: 736: 704: 606: 574: 547: 502: 479: 419: 392: 372: 319: 296: 144: 129:lattice with spacing 120: 1314:Lattice field theory 951:. 106–107: 191–192. 748: 716: 622: 604:{\displaystyle pa=0} 586: 556: 511: 491: 435: 401: 381: 328: 308: 159: 133: 109: 76:lattice field theory 1087:2005CoPhC.169..362J 1069:Jansen, K. (2005). 1032:2004PrPNP..53..373C 967:2002NuPhS.106..191J 943:Jansen, K. (2002). 906:1998PhLB..417..141N 127:Euclidean spacetime 1136:20.500.12657/64022 837: 731: 699: 601: 569: 542: 497: 474: 414: 387: 367: 314: 291: 139: 115: 884:Physics Letters B 816: 772: 758: 677: 632: 566: 500:{\displaystyle D} 390:{\displaystyle A} 317:{\displaystyle A} 183: 169: 142:{\displaystyle a} 125:are defined on a 118:{\displaystyle m} 69: 68: 61: 1326: 1298: 1297: 1271: 1265: 1264: 1258: 1253: 1251: 1243: 1241: 1229: 1223: 1222: 1216: 1208: 1198: 1180: 1164: 1158: 1157: 1113: 1107: 1106: 1066: 1060: 1059: 1025: 1001: 995: 994: 960: 940: 934: 933: 899: 875: 846: 844: 843: 838: 827: 826: 817: 815: 801: 799: 798: 773: 765: 760: 759: 756: 740: 738: 737: 732: 708: 706: 705: 700: 688: 687: 678: 676: 662: 660: 659: 634: 633: 630: 610: 608: 607: 602: 578: 576: 575: 570: 568: 567: 564: 551: 549: 548: 543: 541: 537: 506: 504: 503: 498: 483: 481: 480: 475: 457: 423: 421: 420: 415: 413: 412: 396: 394: 393: 388: 376: 374: 373: 368: 366: 365: 356: 355: 340: 339: 323: 321: 320: 315: 300: 298: 297: 292: 289: 285: 278: 277: 265: 251: 250: 241: 237: 216: 211: 207: 184: 176: 171: 170: 167: 148: 146: 145: 140: 124: 122: 121: 116: 88:fermion doubling 80:overlap fermions 64: 57: 53: 50: 44: 24: 23: 16: 1334: 1333: 1329: 1328: 1327: 1325: 1324: 1323: 1304: 1303: 1302: 1301: 1294: 1273: 1272: 1268: 1254: 1244: 1239:hep-lat/0607038 1231: 1230: 1226: 1209: 1166: 1165: 1161: 1146: 1115: 1114: 1110: 1068: 1067: 1063: 1023:hep-lat/0405024 1003: 1002: 998: 958:hep-lat/0111062 942: 941: 937: 897:hep-lat/9707022 877: 876: 872: 867: 859:chiral symmetry 805: 751: 746: 745: 714: 713: 666: 625: 620: 619: 584: 583: 559: 554: 553: 524: 520: 509: 508: 489: 488: 433: 432: 404: 399: 398: 379: 378: 357: 347: 331: 326: 325: 306: 305: 269: 242: 224: 220: 194: 190: 189: 185: 162: 157: 156: 149:by the overlap 131: 130: 107: 106: 72: 65: 54: 48: 45: 37:help improve it 34: 25: 21: 12: 11: 5: 1332: 1330: 1322: 1321: 1316: 1306: 1305: 1300: 1299: 1293:978-3642018497 1292: 1266: 1257:|journal= 1224: 1159: 1144: 1108: 1081:(1): 362–364. 1061: 996: 935: 869: 868: 866: 863: 850:and decouple. 848: 847: 836: 833: 830: 825: 820: 814: 811: 808: 804: 797: 790: 785: 782: 779: 776: 771: 768: 763: 754: 730: 727: 724: 721: 710: 709: 697: 694: 691: 686: 681: 675: 672: 669: 665: 658: 651: 646: 643: 640: 637: 628: 600: 597: 594: 591: 562: 540: 536: 533: 530: 527: 523: 519: 516: 496: 485: 484: 472: 469: 466: 463: 460: 456: 452: 449: 446: 443: 440: 411: 407: 386: 364: 360: 354: 350: 346: 343: 338: 334: 313: 302: 301: 288: 284: 281: 276: 272: 268: 264: 261: 258: 255: 249: 245: 240: 236: 233: 230: 227: 223: 219: 215: 210: 206: 203: 200: 197: 193: 188: 182: 179: 174: 165: 151:Dirac operator 138: 114: 70: 67: 66: 49:September 2023 28: 26: 19: 13: 10: 9: 6: 4: 3: 2: 1331: 1320: 1317: 1315: 1312: 1311: 1309: 1295: 1289: 1285: 1281: 1277: 1270: 1267: 1262: 1249: 1240: 1235: 1228: 1225: 1220: 1214: 1206: 1202: 1197: 1192: 1188: 1184: 1179: 1174: 1170: 1163: 1160: 1155: 1151: 1147: 1145:9780511583971 1141: 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18: 17: 1275: 1269: 1248:cite journal 1227: 1168: 1162: 1118: 1111: 1078: 1074: 1064: 1013: 1009: 999: 948: 938: 887: 883: 873: 852: 849: 711: 581: 486: 303: 104: 96: 79: 73: 55: 46: 30: 100:lattice QCD 1308:Categories 865:References 1213:cite book 1178:1310.8555 1154:116214756 1103:0010-4655 1048:0146-6410 983:0920-5632 930:119372020 922:0370-2693 810:− 729:π 526:− 518:∈ 451:− 406:γ 359:γ 353:† 333:γ 271:γ 244:γ 229:− 1319:Fermions 1205:25972762 1056:17473067 1196:4410391 1083:Bibcode 1028:Bibcode 991:2547180 963:Bibcode 902:Bibcode 377:, i.e. 84:fermion 35:Please 1290:  1203:  1193:  1152:  1142:  1101:  1054:  1046:  989:  981:  928:  920:  487:where 304:where 82:are a 1234:arXiv 1173:arXiv 1150:S2CID 1052:S2CID 1018:arXiv 987:S2CID 953:arXiv 926:S2CID 892:arXiv 582:Near 1288:ISBN 1261:help 1219:link 1201:PMID 1140:ISBN 1099:ISSN 1044:ISSN 979:ISSN 918:ISSN 1280:doi 1191:PMC 1183:doi 1132:hdl 1124:doi 1091:doi 1079:169 1036:doi 971:doi 910:doi 888:417 397:is 74:In 39:to 1310:: 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Index

help improve it
make it understandable to non-experts
Learn how and when to remove this message
lattice field theory
fermion
fermion doubling
Ginsparg–Wilson fermions
lattice QCD
Euclidean spacetime
Dirac operator
rational approximations
Feynman slash notation
Nielsen–Ninomiya theorem
chiral symmetry
"Exactly massless quarks on the lattice"
arXiv
hep-lat/9707022
Bibcode
1998PhLB..417..141N
doi
10.1016/s0370-2693(97)01368-3
ISSN
0370-2693
S2CID
119372020
"Overlap and domainwall fermions: what is the price of chirality?"
arXiv
hep-lat/0111062
Bibcode
2002NuPhS.106..191J

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