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One-parameter group

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in kinematics and dynamics of relativity theory. Since rapidity is unbounded, the one-parameter group it stands upon is non-compact. The rapidity concept was introduced by
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is an infinitely small transformation of the one-parameter group that it generates. It is these infinitesimal transformations that generate a
1418:{\displaystyle \left.{\frac {d\varphi (t)}{dt}}\right|_{t=0}=\left.{\frac {d}{dt}}\right|_{t=0}e^{tX}=\left.(Xe^{tX})\right|_{t=0}=Xe^{0}=X} 42: 1665: 1709: 1687: 108: 89: 61: 46: 68: 336: 145: 1794: 385: 75: 1429:
This result can be used, for example, to show that any continuous homomorphism between matrix Lie groups is smooth.
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Any connected 1-dimensional Lie group is analytically isomorphic either to the additive group of real numbers
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was reduced to arbitrariness of which diameter of the unit hyperbola was used to determine a
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had all employed in their writings an equivalent mapping of the Cartesian plane by operator
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is differentiable, even though this was not an assumption of the theorem. The matrix
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In that case the induced topology may not be the standard one of the real line.
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provided a calculus of relative motion with the one-parameter group indexed by
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matrices with complex entries. In that case, a basic result is the following:
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of the vector field. The local flow of a vector field is used to define the
348: 252: 180: 1660:, Graduate Texts in Mathematics, vol. 222 (2nd ed.), Springer, 1658:
Lie Groups, Lie Algebras, and Representations: An Elementary Introduction
740: 654:. In particular, every 1-dimensional Lie group is locally isomorphic to 1731:, page 58, Cambridge Tracts in Mathematics and Mathematical Physics #46 686: 366:- a one parameter group of local diffeomorphisms, sending points along 760: 1742:
Applied Functional Analysis: Main Principles and Their Applications
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to calibrate spatio-temporal measurements has become common since
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the next year. The rapidity parameter amounts to the length of a
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An important example in the theory of Lie groups arises when
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is a one-parameter group. Then there exists a unique
997: 964: 922: 902: 852: 832: 781: 660: 634: 610: 586: 539: 445: 422: 388: 312: 292: 261: 237: 217: 188: 148: 49:. Unsourced material may be challenged and removed. 1613: 1593: 1573: 1550: 1538:is injective. Think for example of the case where 1530: 1510: 1484: 1460: 1417: 1228: 1208: 1188: 1164: 1132: 1085: 1065: 1039: 976: 950: 908: 874: 838: 818: 731:. Using the parametrization of the hyperbola with 668: 646: 620: 596: 545: 493: 428: 408: 320: 298: 278: 243: 223: 196: 169:{\displaystyle \varphi :\mathbb {R} \rightarrow G} 168: 1601:is constructed by winding a straight line round 358:of a one-parameter group on a set is known as a 892:Stone's theorem on one-parameter unitary groups 563:Stone's theorem on one-parameter unitary groups 409:{\displaystyle \phi :\mathbb {R} \rightarrow G} 951:{\displaystyle \mathrm {GL} (n;\mathbb {C} )} 8: 16:Lie group homomorphism from the real numbers 494:{\displaystyle \phi (t)\phi (s)=\phi (s+t)} 1606: 1586: 1566: 1543: 1523: 1504: 1503: 1501: 1477: 1451: 1450: 1442: 1403: 1381: 1364: 1337: 1321: 1302: 1283: 1250: 1244: 1221: 1201: 1181: 1158: 1157: 1149: 1121: 1100: 1078: 1052: 1030: 1029: 1012: 1005: 1004: 996: 963: 941: 940: 923: 921: 901: 857: 851: 831: 808: 791: 780: 662: 661: 659: 640: 639: 633: 612: 611: 609: 588: 587: 585: 538: 444: 421: 396: 395: 387: 374:of tensor fields along the vector field. 314: 313: 311: 291: 269: 268: 260: 236: 216: 190: 189: 187: 156: 155: 147: 109:Learn how and when to remove this message 1688:Vorlesungen ĂĽber Continuierliche Gruppen 331:One-parameter groups were introduced by 1676: 1461:{\displaystyle \varphi (\mathbb {R} )} 819:{\displaystyle (\cosh {a}+r\sinh {a})} 279:{\displaystyle \varphi (\mathbb {R} )} 628:, the additive group of real numbers 7: 1765: 1753: 520:Lie group–Lie algebra correspondence 416:is called one-parameter subgroup of 47:adding citations to reliable sources 613: 589: 522:is the basis of a science begun by 286:, the image, will be a subgroup of 1133:{\displaystyle \varphi (t)=e^{tX}} 1016: 1013: 927: 924: 529:Another important case is seen in 14: 1518:; this may happen in cases where 1437:A technical complication is that 1176:It follows from this result that 1165:{\displaystyle t\in \mathbb {R} } 689:, one-parameter groups describe 23: 1702:Geometry, topology, and physics 635: 621:{\displaystyle {\mathfrak {T}}} 597:{\displaystyle {\mathfrak {R}}} 436:if it satisfies the condition 34:needs additional citations for 1455: 1447: 1373: 1354: 1265: 1259: 1111: 1105: 1034: 1020: 1009: 945: 931: 813: 782: 488: 476: 467: 461: 455: 449: 400: 273: 265: 160: 1: 1492:may carry a topology that is 337:infinitesimal transformations 1511:{\displaystyle \mathbb {R} } 846:is the hyperbolic angle and 669:{\displaystyle \mathbb {R} } 576:gave the following theorem: 341:infinitesimal transformation 321:{\displaystyle \mathbb {R} } 197:{\displaystyle \mathbb {R} } 1216:can then be recovered from 347:that is used to describe a 1811: 1704:. CRC Press. p. 232. 958:, the group of invertible 889: 723:discussed it in 1908. The 1066:{\displaystyle n\times n} 977:{\displaystyle n\times n} 1621:at an irrational slope. 1594:{\displaystyle \varphi } 1531:{\displaystyle \varphi } 1229:{\displaystyle \varphi } 1189:{\displaystyle \varphi } 875:{\displaystyle r^{2}=+1} 769:William Kingdon Clifford 244:{\displaystyle \varphi } 1656:Hall, Brian C. (2015), 1639:One-parameter semigroup 725:principle of relativity 339:. According to Lie, an 1615: 1595: 1575: 1552: 1532: 1512: 1486: 1462: 1419: 1230: 1210: 1190: 1166: 1134: 1087: 1067: 1041: 978: 952: 910: 876: 840: 820: 755:in 1910, and named by 670: 648: 647:{\displaystyle \mod 1} 622: 598: 547: 495: 430: 410: 328:as an additive group. 322: 306:that is isomorphic to 300: 280: 245: 225: 198: 170: 131:one-parameter subgroup 1616: 1596: 1576: 1553: 1533: 1513: 1487: 1463: 1420: 1231: 1211: 1191: 1167: 1135: 1088: 1068: 1042: 979: 953: 911: 877: 841: 821: 671: 649: 623: 599: 548: 496: 431: 411: 323: 301: 281: 246: 226: 199: 171: 58:"One-parameter group" 1605: 1585: 1565: 1542: 1522: 1500: 1476: 1441: 1243: 1220: 1200: 1180: 1148: 1099: 1077: 1051: 995: 962: 920: 900: 850: 830: 779: 773:Alexander Macfarlane 658: 632: 608: 584: 537: 443: 420: 386: 310: 290: 259: 235: 215: 186: 146: 43:improve this article 1740:Zeidler, E. (1995) 553:being the group of 531:functional analysis 127:one-parameter group 1795:Topological groups 1611: 1591: 1571: 1548: 1528: 1508: 1482: 1458: 1415: 1226: 1206: 1186: 1162: 1130: 1083: 1063: 1037: 974: 948: 906: 872: 836: 816: 737:special relativity 702:conserved quantity 700:, then there is a 666: 644: 618: 594: 543: 491: 426: 406: 351:of any dimension. 335:in 1893 to define 318: 296: 276: 241: 221: 194: 166: 138:group homomorphism 1644:Noether's theorem 1614:{\displaystyle T} 1574:{\displaystyle T} 1551:{\displaystyle G} 1485:{\displaystyle G} 1315: 1277: 1209:{\displaystyle X} 1086:{\displaystyle X} 909:{\displaystyle G} 839:{\displaystyle a} 761:hyperbolic versor 721:Hermann Minkowski 706:Noether's theorem 691:dynamical systems 568:In his monograph 555:unitary operators 546:{\displaystyle G} 429:{\displaystyle G} 299:{\displaystyle G} 224:{\displaystyle G} 210:topological group 119: 118: 111: 93: 1802: 1769: 1763: 1757: 1751: 1745: 1738: 1732: 1722: 1716: 1715: 1697: 1691: 1681: 1670: 1620: 1618: 1617: 1612: 1600: 1598: 1597: 1592: 1580: 1578: 1577: 1572: 1557: 1555: 1554: 1549: 1537: 1535: 1534: 1529: 1517: 1515: 1514: 1509: 1507: 1491: 1489: 1488: 1483: 1467: 1465: 1464: 1459: 1454: 1424: 1422: 1421: 1416: 1408: 1407: 1392: 1391: 1380: 1376: 1372: 1371: 1345: 1344: 1332: 1331: 1320: 1316: 1314: 1303: 1294: 1293: 1282: 1278: 1276: 1268: 1251: 1235: 1233: 1232: 1227: 1215: 1213: 1212: 1207: 1195: 1193: 1192: 1187: 1171: 1169: 1168: 1163: 1161: 1139: 1137: 1136: 1131: 1129: 1128: 1092: 1090: 1089: 1084: 1072: 1070: 1069: 1064: 1046: 1044: 1043: 1038: 1033: 1019: 1008: 983: 981: 980: 975: 957: 955: 954: 949: 944: 930: 915: 913: 912: 907: 881: 879: 878: 873: 862: 861: 845: 843: 842: 837: 825: 823: 822: 817: 812: 795: 735:, the theory of 733:hyperbolic angle 711:In the study of 675: 673: 672: 667: 665: 653: 651: 650: 645: 627: 625: 624: 619: 617: 616: 603: 601: 600: 595: 593: 592: 552: 550: 549: 544: 500: 498: 497: 492: 435: 433: 432: 427: 415: 413: 412: 407: 399: 327: 325: 324: 319: 317: 305: 303: 302: 297: 285: 283: 282: 277: 272: 250: 248: 247: 242: 230: 228: 227: 222: 208:) to some other 203: 201: 200: 195: 193: 175: 173: 172: 167: 159: 133:usually means a 114: 107: 103: 100: 94: 92: 51: 27: 19: 1810: 1809: 1805: 1804: 1803: 1801: 1800: 1799: 1775: 1774: 1773: 1772: 1764: 1760: 1752: 1748: 1744:Springer-Verlag 1739: 1735: 1723: 1719: 1712: 1699: 1698: 1694: 1682: 1678: 1668: 1655: 1652: 1630: 1603: 1602: 1583: 1582: 1563: 1562: 1540: 1539: 1520: 1519: 1498: 1497: 1474: 1473: 1439: 1438: 1435: 1399: 1360: 1353: 1350: 1349: 1333: 1307: 1299: 1298: 1269: 1252: 1247: 1246: 1241: 1240: 1218: 1217: 1198: 1197: 1178: 1177: 1146: 1145: 1117: 1097: 1096: 1075: 1074: 1049: 1048: 993: 992: 960: 959: 918: 917: 916:is taken to be 898: 897: 894: 888: 853: 848: 847: 828: 827: 777: 776: 715:the use of the 683: 656: 655: 630: 629: 606: 605: 582: 581: 535: 534: 508: 441: 440: 418: 417: 384: 383: 380: 368:integral curves 308: 307: 288: 287: 257: 256: 233: 232: 213: 212: 184: 183: 144: 143: 115: 104: 98: 95: 52: 50: 40: 28: 17: 12: 11: 5: 1808: 1806: 1798: 1797: 1792: 1787: 1777: 1776: 1771: 1770: 1768:Corollary 3.50 1758: 1746: 1733: 1717: 1710: 1692: 1675: 1674: 1673: 1672: 1667:978-3319134666 1666: 1651: 1648: 1647: 1646: 1641: 1636: 1634:Integral curve 1629: 1626: 1610: 1590: 1570: 1547: 1527: 1506: 1481: 1457: 1453: 1449: 1446: 1434: 1431: 1427: 1426: 1414: 1411: 1406: 1402: 1398: 1395: 1390: 1387: 1384: 1379: 1375: 1370: 1367: 1363: 1359: 1356: 1352: 1348: 1343: 1340: 1336: 1330: 1327: 1324: 1319: 1313: 1310: 1306: 1301: 1297: 1292: 1289: 1286: 1281: 1275: 1272: 1267: 1264: 1261: 1258: 1255: 1249: 1225: 1205: 1185: 1174: 1173: 1160: 1156: 1153: 1142: 1141: 1140: 1127: 1124: 1120: 1116: 1113: 1110: 1107: 1104: 1082: 1062: 1059: 1056: 1036: 1032: 1028: 1025: 1022: 1018: 1015: 1011: 1007: 1003: 1000: 973: 970: 967: 947: 943: 939: 936: 933: 929: 926: 905: 887: 884: 871: 868: 865: 860: 856: 835: 815: 811: 807: 804: 801: 798: 794: 790: 787: 784: 753:E.T. Whittaker 717:unit hyperbola 695:differentiable 682: 679: 678: 677: 664: 643: 638: 615: 591: 542: 526:in the 1890s. 507: 504: 503: 502: 490: 487: 484: 481: 478: 475: 472: 469: 466: 463: 460: 457: 454: 451: 448: 425: 405: 402: 398: 394: 391: 379: 376: 372:Lie derivative 316: 295: 275: 271: 267: 264: 240: 220: 206:additive group 192: 177: 176: 165: 162: 158: 154: 151: 117: 116: 31: 29: 22: 15: 13: 10: 9: 6: 4: 3: 2: 1807: 1796: 1793: 1791: 1788: 1786: 1783: 1782: 1780: 1767: 1762: 1759: 1755: 1750: 1747: 1743: 1737: 1734: 1730: 1726: 1721: 1718: 1713: 1711:9780750306065 1707: 1703: 1696: 1693: 1689: 1685: 1680: 1677: 1669: 1663: 1659: 1654: 1653: 1649: 1645: 1642: 1640: 1637: 1635: 1632: 1631: 1627: 1625: 1622: 1608: 1588: 1568: 1561: 1545: 1525: 1496:than that on 1495: 1479: 1471: 1444: 1432: 1430: 1412: 1409: 1404: 1400: 1396: 1393: 1388: 1385: 1382: 1377: 1368: 1365: 1361: 1357: 1346: 1341: 1338: 1334: 1328: 1325: 1322: 1317: 1311: 1308: 1304: 1295: 1290: 1287: 1284: 1279: 1273: 1270: 1262: 1256: 1253: 1239: 1238: 1237: 1223: 1203: 1183: 1154: 1151: 1143: 1125: 1122: 1118: 1114: 1108: 1102: 1095: 1094: 1080: 1060: 1057: 1054: 1026: 1023: 1001: 998: 990: 987: 986: 985: 971: 968: 965: 937: 934: 903: 893: 885: 883: 869: 866: 863: 858: 854: 833: 809: 805: 802: 799: 796: 792: 788: 785: 774: 770: 766: 762: 758: 754: 750: 747:replaces the 746: 742: 738: 734: 730: 726: 722: 718: 714: 709: 707: 703: 699: 696: 692: 688: 680: 641: 636: 579: 578: 577: 575: 571: 566: 564: 560: 559:Hilbert space 556: 540: 532: 527: 525: 521: 517: 513: 505: 485: 482: 479: 473: 470: 464: 458: 452: 446: 439: 438: 437: 423: 403: 392: 389: 377: 375: 373: 369: 365: 361: 357: 352: 350: 346: 342: 338: 334: 329: 293: 262: 254: 238: 218: 211: 207: 182: 163: 152: 149: 142: 141: 140: 139: 136: 132: 128: 124: 113: 110: 102: 91: 88: 84: 81: 77: 74: 70: 67: 63: 60: â€“  59: 55: 54:Find sources: 48: 44: 38: 37: 32:This article 30: 26: 21: 20: 1761: 1756:Theorem 2.14 1749: 1741: 1736: 1728: 1720: 1701: 1695: 1679: 1657: 1623: 1436: 1428: 1175: 988: 895: 765:James Cockle 748: 744: 710: 684: 569: 567: 528: 509: 381: 363: 353: 340: 330: 178: 130: 126: 120: 105: 99:January 2015 96: 86: 79: 72: 65: 53: 41:Please help 36:verification 33: 757:Alfred Robb 516:Lie algebra 345:Lie algebra 123:mathematics 1790:1 (number) 1785:Lie groups 1779:Categories 1729:Lie Groups 1700:Nakahara. 1684:Sophus Lie 1650:References 1093:such that 991:: Suppose 890:See also: 886:In GL(n,C) 729:world-line 698:symmetries 574:P. M. Cohn 570:Lie Groups 524:Sophus Lie 512:Lie theory 378:Definition 364:local flow 333:Sophus Lie 135:continuous 69:newspapers 1766:Hall 2015 1754:Hall 2015 1725:Paul Cohn 1589:φ 1526:φ 1445:φ 1257:φ 1224:φ 1184:φ 1155:∈ 1103:φ 1058:× 1010:→ 999:φ 969:× 806:⁡ 789:⁡ 713:spacetime 474:ϕ 459:ϕ 447:ϕ 401:→ 390:ϕ 349:Lie group 263:φ 253:injective 239:φ 181:real line 179:from the 161:→ 150:φ 1628:See also 1470:subspace 1433:Topology 1144:for all 826:, where 749:velocity 745:rapidity 741:rapidity 604:, or to 506:Examples 382:A curve 1727:(1957) 1686:(1893) 1494:coarser 1073:matrix 989:Theorem 687:physics 681:Physics 533:, with 204:(as an 83:scholar 1708:  1664:  1581:, and 771:, and 743:. The 561:. See 518:. The 356:action 231:. If 85:  78:  71:  64:  56:  1560:torus 1558:is a 1468:as a 704:, by 557:on a 255:then 90:JSTOR 76:books 1706:ISBN 1662:ISBN 803:sinh 786:cosh 360:flow 354:The 125:, a 62:news 1472:of 1236:as 685:In 637:mod 510:In 251:is 129:or 121:In 45:by 1781:: 882:. 767:, 708:. 572:, 565:. 1714:. 1671:. 1609:T 1569:T 1546:G 1505:R 1480:G 1456:) 1452:R 1448:( 1425:. 1413:X 1410:= 1405:0 1401:e 1397:X 1394:= 1389:0 1386:= 1383:t 1378:| 1374:) 1369:X 1366:t 1362:e 1358:X 1355:( 1347:= 1342:X 1339:t 1335:e 1329:0 1326:= 1323:t 1318:| 1312:t 1309:d 1305:d 1296:= 1291:0 1288:= 1285:t 1280:| 1274:t 1271:d 1266:) 1263:t 1260:( 1254:d 1204:X 1172:. 1159:R 1152:t 1126:X 1123:t 1119:e 1115:= 1112:) 1109:t 1106:( 1081:X 1061:n 1055:n 1035:) 1031:C 1027:; 1024:n 1021:( 1017:L 1014:G 1006:R 1002:: 972:n 966:n 946:) 942:C 938:; 935:n 932:( 928:L 925:G 904:G 870:1 867:+ 864:= 859:2 855:r 834:a 814:) 810:a 800:r 797:+ 793:a 783:( 676:. 663:R 642:1 614:T 590:R 541:G 501:. 489:) 486:t 483:+ 480:s 477:( 471:= 468:) 465:s 462:( 456:) 453:t 450:( 424:G 404:G 397:R 393:: 315:R 294:G 274:) 270:R 266:( 219:G 191:R 164:G 157:R 153:: 112:) 106:( 101:) 97:( 87:· 80:· 73:· 66:· 39:.

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"One-parameter group"
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mathematics
continuous
group homomorphism
real line
additive group
topological group
injective
Sophus Lie
infinitesimal transformations
Lie algebra
Lie group
action
flow
integral curves
Lie derivative
Lie theory
Lie algebra
Lie group–Lie algebra correspondence
Sophus Lie

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