25:
1423:
1045:
1242:
174:
414:
956:
499:
1466:
824:
284:
1138:
1170:
626:
602:
751:
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
1516:
891:
674:
562:
326:
202:
1071:
982:
1599:
1536:
1234:
1194:
880:
249:
652:
1619:
1579:
1556:
1490:
1214:
1091:
914:
844:
551:
434:
304:
229:
519:
994:
343:
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.
919:
701:
35:
442:
57:
768:
580:
Any connected 1-dimensional Lie group is analytically isomorphic either to the additive group of real numbers
1638:
1440:
778:
724:
258:
1098:
764:
355:
134:
1147:
1643:
772:
705:
607:
583:
1789:
1784:
530:
1499:
657:
309:
185:
736:
359:
137:
82:
1050:
961:
1705:
1661:
1584:
1521:
1469:
1219:
1179:
849:
720:
690:
234:
209:
727:
was reduced to arbitrariness of which diameter of the unit hyperbola was used to determine a
775:
had all employed in their writings an equivalent mapping of the
Cartesian plane by operator
732:
631:
554:
1633:
1604:
1564:
1541:
1493:
1475:
1199:
1076:
899:
829:
752:
716:
697:
536:
419:
371:
367:
289:
214:
1778:
1196:
is differentiable, even though this was not an assumption of the theorem. The matrix
558:
205:
693:. Furthermore, whenever a system of physical laws admits a one-parameter group of
514:, one-parameter groups correspond to one-dimensional subspaces of the associated
1624:
In that case the induced topology may not be the standard one of the real line.
756:
515:
344:
122:
24:
739:
provided a calculus of relative motion with the one-parameter group indexed by
1683:
1040:{\displaystyle \varphi :\mathbb {R} \rightarrow \mathrm {GL} (n;\mathbb {C} )}
984:
matrices with complex entries. In that case, a basic result is the following:
728:
694:
573:
523:
511:
332:
1690:, English translation by D.H. Delphenich, §8, link from Neo-classical Physics
1724:
712:
370:
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
1559:
719:
to calibrate spatio-temporal measurements has become common since
759:
the next year. The rapidity parameter amounts to the length of a
763:, a concept of the nineteenth century. Mathematical physicists
18:
896:
An important example in the theory of Lie groups arises when
362:. A smooth vector field on a manifold, at a point, induces a
1351:
1300:
1248:
1607:
1587:
1567:
1544:
1524:
1502:
1478:
1443:
1245:
1222:
1202:
1182:
1150:
1101:
1079:
1053:
1047:
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: –
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:.
Text is available under the Creative Commons Attribution-ShareAlike License. Additional terms may apply.