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Resolvent formalism

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1197: 320: 526: 1505: 933: 763: 1405: 1453: 570: 145: 944: 1538: 1262: 1360: 419: 214: 1334: 1297: 1558: 1593: 787:
is a generalization of the first resolvent identity, above, useful for comparing the resolvents of two distinct operators. Given operators
233: 438: 1733: 1462: 824: 654: 1777: 1755: 1676: 1373: 1410: 1563: 54: 24: 1800: 182: 42: 1805: 1598: 1192:{\displaystyle (A-zI)^{-1}-(B-zI)^{-1}=(A-zI)^{-1}((B-zI)-(A-zI))(B-zI)^{-1}=(A-zI)^{-1}(B-A)(B-zI)^{-1}\,.} 1588: 585: 534: 155: 78: 225: 151: 1510: 53:
and more general spaces. Formal justification for the manipulations can be found in the framework of
1795: 1232: 341: 65: 1343: 382: 192: 1310: 46: 361: 1267: 769: 8: 349: 326: 20: 1685: 1541: 1208: 1689: 1773: 1765: 1751: 1729: 1721: 1672: 1664: 1578: 430: 345: 1704: 1573: 1300: 166: 38: 1583: 1568: 597: 64:
captures the spectral properties of an operator in the analytic structure of the
1660: 1789: 1553: 1223: 637: 608: 589: 1367: 50: 1717: 30: 1743: 1709: 333: 315:{\displaystyle -{\frac {1}{2\pi i}}\oint _{C_{\lambda }}(A-zI)^{-1}~dz} 178: 150:
Among other uses, the resolvent may be used to solve the inhomogeneous
780:, instead, so that the formula above differs in sign from theirs.) 580:
The first major use of the resolvent operator as a series in
521:{\displaystyle R(z;A)=\int _{0}^{\infty }e^{-zt}U(t)~dt,} 379:
is a one-parameter group of unitary operators. Whenever
189:. That is, suppose there exists a simple closed curve 1513: 1465: 1413: 1376: 1346: 1313: 1270: 1235: 947: 827: 657: 537: 441: 385: 236: 195: 165:
can be used to directly obtain information about the
154:; a commonly used approach is a series solution, the 81: 1500:{\displaystyle \{\lambda _{i}\}_{i\in \mathbb {N} }} 1532: 1499: 1447: 1399: 1354: 1328: 1291: 1256: 1191: 928:{\displaystyle R(z;A)-R(z;B)=R(z;A)(B-A)R(z;B)\,.} 927: 758:{\displaystyle R(z;A)-R(w;A)=(z-w)R(z;A)R(w;A)\,.} 757: 564: 520: 413: 314: 208: 139: 1787: 1750:(2nd ed.), New York, NY: Springer-Verlag, 1659: 1594:Decomposition of spectrum (functional analysis) 1559:Stone's theorem on one-parameter unitary groups 1400:{\displaystyle \sigma (A)\subset \mathbb {R} } 795:, both defined on the same linear space, and 1728:, Providence: American Mathematical Society, 1716: 1634:Dunford and Schwartz, Vol I, Lemma 6, p. 568. 1448:{\displaystyle \{v_{i}\}_{i\in \mathbb {N} }} 1527: 1514: 1480: 1466: 1428: 1414: 408: 402: 1690:"Sur une classe d'equations fonctionnelles" 1625:Hille and Phillips, Theorem 11.4.1, p. 341 531:where the integral is taken along the ray 37:is a technique for applying concepts from 1708: 1643:Hille and Phillips, Theorem 4.8.2, p. 126 1491: 1439: 1393: 1348: 1185: 921: 751: 1748:Perturbation Theory for Linear Operators 1684: 648:(also called Hilbert's identity) holds: 1669:Linear Operators, Part I General Theory 1788: 1764: 1407:and there exists an orthonormal basis 348:to an integral over the one-parameter 216:in the complex plane that separates 614: 565:{\displaystyle \arg t=-\arg \lambda } 1742: 1307:has compact resolvent. The spectrum 1202: 140:{\displaystyle R(z;A)=(A-zI)^{-1}~.} 1726:Functional Analysis and Semi-groups 1671:, Hoboken, NJ: Wiley-Interscience, 13: 938:A one-line proof goes as follows: 473: 72:, the resolvent may be defined as 14: 1817: 1772:, New York, NY: Springer-Verlag, 772:, cited, define the resolvent as 220:from the rest of the spectrum of 1770:Partial Differential Equations I 1616:Taylor, section 9 of Appendix A. 1533:{\displaystyle \{\lambda _{i}\}} 352:of transformations generated by 344:relates the resolvent through a 1564:Holomorphic functional calculus 55:holomorphic functional calculus 25:Holomorphic functional calculus 1646: 1637: 1628: 1619: 1610: 1386: 1380: 1323: 1317: 1286: 1274: 1251: 1245: 1173: 1157: 1154: 1142: 1130: 1114: 1099: 1083: 1080: 1077: 1062: 1056: 1041: 1038: 1026: 1010: 995: 979: 964: 948: 918: 906: 900: 888: 885: 873: 864: 852: 843: 831: 818:the following identity holds, 748: 736: 730: 718: 712: 700: 694: 682: 673: 661: 592:, in a landmark 1903 paper in 503: 497: 457: 445: 395: 387: 291: 275: 119: 103: 97: 85: 1: 1604: 1599:Limiting absorption principle 1257:{\displaystyle z\in \rho (A)} 596:that helped establish modern 1355:{\displaystyle \mathbb {C} } 414:{\displaystyle |z|>\|A\|} 209:{\displaystyle C_{\lambda }} 7: 1547: 152:Fredholm integral equations 10: 1822: 1329:{\displaystyle \sigma (A)} 575: 18: 785:second resolvent identity 356:. Thus, for example, if 1589:Liouvilleā€“Neumann series 1340:is a discrete subset of 646:first resolvent identity 586:Liouvilleā€“Neumann series 429:can be expressed as the 156:Liouvilleā€“Neumann series 16:Technique in mathematics 1207:When studying a closed 173:. For example, suppose 1534: 1501: 1449: 1401: 1356: 1330: 1293: 1292:{\displaystyle R(z;A)} 1258: 1193: 929: 759: 566: 522: 415: 316: 210: 167:spectral decomposition 141: 1801:Formalism (deductive) 1535: 1502: 1450: 1402: 1357: 1331: 1294: 1259: 1194: 930: 760: 567: 523: 416: 362:skew-Hermitian matrix 317: 211: 142: 19:Further information: 1806:Mathematical physics 1511: 1507:respectively. Also, 1463: 1455:of eigenvectors of 1411: 1374: 1344: 1311: 1268: 1233: 945: 825: 770:Dunford and Schwartz 655: 535: 439: 383: 342:Hilleā€“Yosida theorem 234: 193: 79: 68:. Given an operator 41:to the study of the 644:, we have that the 477: 421:, the resolvent of 327:projection operator 35:resolvent formalism 21:Frobenius covariant 1766:Taylor, Michael E. 1722:Phillips, Ralph S. 1710:10.1007/bf02421317 1665:Schwartz, Jacob T. 1542:accumulation point 1530: 1497: 1445: 1397: 1352: 1326: 1289: 1254: 1229:, if there exists 1209:unbounded operator 1189: 925: 755: 615:Resolvent identity 562: 518: 463: 411: 312: 206: 137: 1735:978-0-8218-1031-6 1686:Fredholm, Erik I. 1579:Laplace transform 1459:with eigenvalues 1362:. If furthermore 1203:Compact resolvent 508: 431:Laplace transform 346:Laplace transform 305: 256: 161:The resolvent of 133: 1813: 1782: 1760: 1738: 1713: 1712: 1697:Acta Mathematica 1694: 1681: 1653: 1650: 1644: 1641: 1635: 1632: 1626: 1623: 1617: 1614: 1574:Compact operator 1539: 1537: 1536: 1531: 1526: 1525: 1506: 1504: 1503: 1498: 1496: 1495: 1494: 1478: 1477: 1458: 1454: 1452: 1451: 1446: 1444: 1443: 1442: 1426: 1425: 1406: 1404: 1403: 1398: 1396: 1365: 1361: 1359: 1358: 1353: 1351: 1339: 1335: 1333: 1332: 1327: 1306: 1301:compact operator 1298: 1296: 1295: 1290: 1263: 1261: 1260: 1255: 1228: 1221: 1217: 1213: 1198: 1196: 1195: 1190: 1184: 1183: 1141: 1140: 1110: 1109: 1037: 1036: 1006: 1005: 975: 974: 934: 932: 931: 926: 817: 798: 794: 790: 779: 764: 762: 761: 756: 643: 640:of an operator 635: 624: 594:Acta Mathematica 583: 571: 569: 568: 563: 527: 525: 524: 519: 506: 493: 492: 476: 471: 420: 418: 417: 412: 398: 390: 378: 359: 355: 339: 332: 321: 319: 318: 313: 303: 302: 301: 274: 273: 272: 271: 257: 255: 241: 223: 219: 215: 213: 212: 207: 205: 204: 188: 176: 172: 164: 146: 144: 143: 138: 131: 130: 129: 71: 39:complex analysis 1821: 1820: 1816: 1815: 1814: 1812: 1811: 1810: 1796:Fredholm theory 1786: 1785: 1780: 1758: 1736: 1692: 1679: 1661:Dunford, Nelson 1656: 1652:Taylor, p. 515. 1651: 1647: 1642: 1638: 1633: 1629: 1624: 1620: 1615: 1611: 1607: 1584:Fredholm theory 1569:Spectral theory 1550: 1521: 1517: 1512: 1509: 1508: 1490: 1483: 1479: 1473: 1469: 1464: 1461: 1460: 1456: 1438: 1431: 1427: 1421: 1417: 1412: 1409: 1408: 1392: 1375: 1372: 1371: 1363: 1347: 1345: 1342: 1341: 1337: 1312: 1309: 1308: 1304: 1303:, we say that 1269: 1266: 1265: 1234: 1231: 1230: 1226: 1219: 1215: 1211: 1205: 1176: 1172: 1133: 1129: 1102: 1098: 1029: 1025: 998: 994: 967: 963: 946: 943: 942: 826: 823: 822: 800: 796: 792: 788: 773: 656: 653: 652: 641: 626: 620: 617: 598:operator theory 581: 578: 536: 533: 532: 482: 478: 472: 467: 440: 437: 436: 394: 386: 384: 381: 380: 365: 357: 353: 337: 330: 294: 290: 267: 263: 262: 258: 245: 240: 235: 232: 231: 221: 217: 200: 196: 194: 191: 190: 186: 177:is an isolated 174: 170: 162: 122: 118: 80: 77: 76: 69: 27: 17: 12: 11: 5: 1819: 1809: 1808: 1803: 1798: 1784: 1783: 1778: 1762: 1756: 1740: 1734: 1714: 1682: 1677: 1655: 1654: 1645: 1636: 1627: 1618: 1608: 1606: 1603: 1602: 1601: 1596: 1591: 1586: 1581: 1576: 1571: 1566: 1561: 1556: 1549: 1546: 1540:has no finite 1529: 1524: 1520: 1516: 1493: 1489: 1486: 1482: 1476: 1472: 1468: 1441: 1437: 1434: 1430: 1424: 1420: 1416: 1395: 1391: 1388: 1385: 1382: 1379: 1350: 1325: 1322: 1319: 1316: 1288: 1285: 1282: 1279: 1276: 1273: 1253: 1250: 1247: 1244: 1241: 1238: 1204: 1201: 1200: 1199: 1188: 1182: 1179: 1175: 1171: 1168: 1165: 1162: 1159: 1156: 1153: 1150: 1147: 1144: 1139: 1136: 1132: 1128: 1125: 1122: 1119: 1116: 1113: 1108: 1105: 1101: 1097: 1094: 1091: 1088: 1085: 1082: 1079: 1076: 1073: 1070: 1067: 1064: 1061: 1058: 1055: 1052: 1049: 1046: 1043: 1040: 1035: 1032: 1028: 1024: 1021: 1018: 1015: 1012: 1009: 1004: 1001: 997: 993: 990: 987: 984: 981: 978: 973: 970: 966: 962: 959: 956: 953: 950: 936: 935: 924: 920: 917: 914: 911: 908: 905: 902: 899: 896: 893: 890: 887: 884: 881: 878: 875: 872: 869: 866: 863: 860: 857: 854: 851: 848: 845: 842: 839: 836: 833: 830: 808:) āˆ©  766: 765: 754: 750: 747: 744: 741: 738: 735: 732: 729: 726: 723: 720: 717: 714: 711: 708: 705: 702: 699: 696: 693: 690: 687: 684: 681: 678: 675: 672: 669: 666: 663: 660: 616: 613: 577: 574: 561: 558: 555: 552: 549: 546: 543: 540: 529: 528: 517: 514: 511: 505: 502: 499: 496: 491: 488: 485: 481: 475: 470: 466: 462: 459: 456: 453: 450: 447: 444: 410: 407: 404: 401: 397: 393: 389: 323: 322: 311: 308: 300: 297: 293: 289: 286: 283: 280: 277: 270: 266: 261: 254: 251: 248: 244: 239: 203: 199: 148: 147: 136: 128: 125: 121: 117: 114: 111: 108: 105: 102: 99: 96: 93: 90: 87: 84: 15: 9: 6: 4: 3: 2: 1818: 1807: 1804: 1802: 1799: 1797: 1794: 1793: 1791: 1781: 1779:7-5062-4252-4 1775: 1771: 1767: 1763: 1759: 1757:0-387-07558-5 1753: 1749: 1745: 1741: 1737: 1731: 1727: 1723: 1719: 1715: 1711: 1706: 1702: 1698: 1691: 1687: 1683: 1680: 1678:0-471-60848-3 1674: 1670: 1666: 1662: 1658: 1657: 1649: 1640: 1631: 1622: 1613: 1609: 1600: 1597: 1595: 1592: 1590: 1587: 1585: 1582: 1580: 1577: 1575: 1572: 1570: 1567: 1565: 1562: 1560: 1557: 1555: 1554:Resolvent set 1552: 1551: 1545: 1543: 1522: 1518: 1487: 1484: 1474: 1470: 1435: 1432: 1422: 1418: 1389: 1383: 1377: 1369: 1320: 1314: 1302: 1283: 1280: 1277: 1271: 1248: 1242: 1239: 1236: 1225: 1224:Hilbert space 1210: 1186: 1180: 1177: 1169: 1166: 1163: 1160: 1151: 1148: 1145: 1137: 1134: 1126: 1123: 1120: 1117: 1111: 1106: 1103: 1095: 1092: 1089: 1086: 1074: 1071: 1068: 1065: 1059: 1053: 1050: 1047: 1044: 1033: 1030: 1022: 1019: 1016: 1013: 1007: 1002: 999: 991: 988: 985: 982: 976: 971: 968: 960: 957: 954: 951: 941: 940: 939: 922: 915: 912: 909: 903: 897: 894: 891: 882: 879: 876: 870: 867: 861: 858: 855: 849: 846: 840: 837: 834: 828: 821: 820: 819: 815: 811: 807: 803: 786: 781: 777: 771: 752: 745: 742: 739: 733: 727: 724: 721: 715: 709: 706: 703: 697: 691: 688: 685: 679: 676: 670: 667: 664: 658: 651: 650: 649: 647: 639: 638:resolvent set 633: 629: 623: 612: 610: 609:David Hilbert 607:was given by 606: 601: 599: 595: 591: 590:Ivar Fredholm 587: 573: 559: 556: 553: 550: 547: 544: 541: 538: 515: 512: 509: 500: 494: 489: 486: 483: 479: 468: 464: 460: 454: 451: 448: 442: 435: 434: 433: 432: 428: 424: 405: 399: 391: 376: 372: 368: 363: 351: 347: 343: 335: 328: 309: 306: 298: 295: 287: 284: 281: 278: 268: 264: 259: 252: 249: 246: 242: 237: 230: 229: 228: 227: 201: 197: 184: 180: 168: 159: 157: 153: 134: 126: 123: 115: 112: 109: 106: 100: 94: 91: 88: 82: 75: 74: 73: 67: 63: 58: 56: 52: 51:Banach spaces 48: 44: 40: 36: 32: 26: 22: 1769: 1747: 1725: 1718:Hille, Einar 1700: 1696: 1668: 1648: 1639: 1630: 1621: 1612: 1368:self-adjoint 1206: 937: 813: 809: 805: 801: 784: 782: 775: 767: 645: 631: 627: 621: 618: 604: 602: 593: 579: 530: 426: 422: 374: 370: 366: 324: 160: 149: 61: 59: 34: 28: 1744:Kato, Tosio 1703:: 365ā€“390, 768:(Note that 224:. Then the 31:mathematics 1790:Categories 1605:References 1264:such that 334:eigenspace 329:onto the 325:defines a 179:eigenvalue 66:functional 1519:λ 1488:∈ 1471:λ 1436:∈ 1390:⊂ 1378:σ 1336:of such 1315:σ 1243:ρ 1240:∈ 1178:− 1164:− 1149:− 1135:− 1121:− 1104:− 1090:− 1069:− 1060:− 1048:− 1031:− 1017:− 1000:− 986:− 977:− 969:− 955:− 895:− 847:− 707:− 677:− 605:resolvent 603:The name 588:) was by 560:λ 557:⁡ 551:− 542:⁡ 484:− 474:∞ 465:∫ 409:‖ 403:‖ 296:− 282:− 269:λ 260:∮ 250:π 238:− 202:λ 124:− 110:− 62:resolvent 47:operators 1768:(1996), 1746:(1980), 1724:(1957), 1688:(1903), 1667:(1988), 1548:See also 619:For all 373:) = exp( 183:spectrum 181:in the 43:spectrum 1370:, then 576:History 364:, then 340:. 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Index

Frobenius covariant
Holomorphic functional calculus
mathematics
complex analysis
spectrum
operators
Banach spaces
holomorphic functional calculus
functional
Fredholm integral equations
Liouvilleā€“Neumann series
spectral decomposition
eigenvalue
spectrum
residue
projection operator
eigenspace
Hilleā€“Yosida theorem
Laplace transform
group
skew-Hermitian matrix
Laplace transform
Liouvilleā€“Neumann series
Ivar Fredholm
operator theory
David Hilbert
resolvent set
Dunford and Schwartz
unbounded operator
Hilbert space

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