Knowledge (XXG)

Light dressed state

Source đź“ť

33: 1380:
in eq. (2) can be regarded as the number of photons absorbed from (or emitted to) the laser field. In order to prove this statement, we clarify the correspondence between the solution (2), which is derived from the classical expression of the electromagnetic field where there is no concept of
833: 1252: 317: 957: 1076: 435: 707: 719: 1090: 1312: 516: 486: 650: 381: 355: 1314:
is the frequency of the laser field. This expression (2) reveals that a quantum state of the system governed by the Hamiltonian (1) can be specified by a real number
1431: 981: 572: 544: 1452: 1404: 1378: 1354: 1333: 593: 456: 1538:
Guérin, S; Monti, F; Dupont, J-M; Jauslin, H R (1997). "On the relation between cavity-dressed states, Floquet states, RWA and semiclassical models".
156: 844: 986: 54: 1655: 1629: 76: 595:
is the speed of light. By virtue of this time-periodicity of the laser field, the total Hamiltonian is also periodic in time as
1673: 145: 386: 828:{\displaystyle i\hbar {\frac {\partial }{\partial t}}\psi (\{\mathbf {r} _{i}\},t)=H(t)\psi (\{\mathbf {r} _{i}\},t)} 47: 41: 662: 1247:{\displaystyle \psi (\{\mathbf {r} _{i}\},t)=\exp\sum _{n=-\infty }^{\infty }\exp\phi _{n}(\{\mathbf {r} _{i}\})} 58: 1501:
Sambe, Hideo (1973). "Steady States and Quasienergies of a Quantum-Mechanical System in an Oscillating Field".
1693: 1688: 1612:
Guérin, S.; Jauslin, H. R. (2003). "Control of Quantum Dynamics by Laser Pulses: Adiabatic Floquet Theory".
710: 1273: 491: 461: 1584: 1547: 1510: 1473: 1382: 117: 1464:
Shirley, Jon H. (1965). "Solution of the Schrödinger Equation with a Hamiltonian Periodic in Time".
601: 364: 338: 1651: 1635: 1625: 1600: 1563: 1526: 1489: 1409: 94: 965: 549: 521: 1617: 1592: 1555: 1518: 1481: 358: 656: 133: 1436: 1388: 1362: 1338: 1317: 577: 440: 1588: 1551: 1514: 1477: 1668: 1575:
Cardoso, G.C.; Tabosa, J.W.R. (2000). "Four-wave mixing in dressed cold cesium atoms".
1079: 90: 1596: 1559: 1682: 106: 148:
of a system of charged particles interacting with a laser light can be expressed as
1406:
is equal to the expectation value of the absorbed photon number at the limit of
312:{\displaystyle H=\sum _{i}{\frac {1}{2m_{i}}}\left^{2}+V(\{\mathbf {r} _{i}\}),} 952:{\displaystyle \psi (\{\mathbf {r} _{i}\},t)=\exp\phi (\{\mathbf {r} _{i}\},t)} 1381:
photons, and one which is derived from a quantized electromagnetic field (see
1071:{\displaystyle \phi (\{\mathbf {r} _{i}\},t+T)=\phi (\{\mathbf {r} _{i}\},t).} 17: 1639: 1604: 1567: 1530: 1493: 1485: 1522: 1621: 125: 129: 98: 113: 110: 121: 26: 518:, respectively, while its mass and charge are symbolized as 136:
in differential equations with periodic coefficients.
1439: 1412: 1391: 1365: 1341: 1320: 1276: 1093: 989: 968: 847: 722: 665: 604: 580: 552: 524: 494: 464: 443: 389: 367: 341: 159: 109:
of an atomic or molecular system interacting with a
1446: 1425: 1398: 1372: 1348: 1327: 1306: 1246: 1070: 983:has the same time-periodicity as the Hamiltonian, 975: 951: 827: 701: 644: 587: 566: 538: 510: 480: 450: 429: 375: 349: 311: 430:{\displaystyle \mathbf {A} (t+T)=\mathbf {A} (t)} 261: 240: 1540:Journal of Physics A: Mathematical and General 702:{\displaystyle \psi (\{\mathbf {r} _{i}\},t)} 8: 1238: 1223: 1115: 1100: 1053: 1038: 1011: 996: 937: 922: 869: 854: 813: 798: 765: 750: 687: 672: 300: 285: 361:of the electromagnetic field of the laser; 1078:Therefore, this part can be expanded in a 1454:is the initial number of total photons.) 1443: 1438: 1422: 1411: 1395: 1390: 1369: 1364: 1345: 1340: 1324: 1319: 1303: 1292: 1275: 1232: 1227: 1214: 1180: 1166: 1151: 1109: 1104: 1092: 1047: 1042: 1005: 1000: 988: 972: 967: 931: 926: 905: 863: 858: 846: 807: 802: 759: 754: 729: 721: 681: 676: 664: 638: 603: 584: 579: 563: 557: 551: 535: 529: 523: 507: 501: 496: 493: 477: 471: 466: 463: 447: 442: 413: 390: 388: 368: 366: 342: 340: 294: 289: 270: 249: 244: 236: 225: 219: 210: 205: 189: 176: 170: 158: 77:Learn how and when to remove this message 40:This article includes a list of general 1156: 910: 726: 132:. The Floquet picture is based on the 7: 1084: 150: 1307:{\displaystyle \omega (=2\pi /T)\,} 437:. The position and momentum of the 1181: 1176: 735: 731: 511:{\displaystyle \mathbf {p} _{i}\,} 481:{\displaystyle \mathbf {r} _{i}\,} 46:it lacks sufficient corresponding 25: 1648:Theory of Multiphoton Processes, 1228: 1105: 1043: 1001: 927: 859: 803: 755: 677: 497: 467: 414: 391: 369: 343: 290: 258: 255: 250: 245: 237: 206: 31: 1674:Hamiltonian (quantum mechanics) 713:with this type of Hamiltonian, 1300: 1280: 1241: 1220: 1207: 1192: 1159: 1136: 1124: 1097: 1062: 1035: 1026: 993: 946: 919: 913: 890: 878: 851: 822: 795: 789: 783: 774: 747: 696: 669: 645:{\displaystyle H(t+T)=H(t)\,.} 635: 629: 620: 608: 424: 418: 407: 395: 303: 282: 1: 1597:10.1016/S0030-4018(00)01033-6 1385:). (It can be verified that 838:can be expressed in the form 659:guarantees that any solution 458:-th particle are denoted as 1614:Advances in Chemical Physics 376:{\displaystyle \mathbf {A} } 350:{\displaystyle \mathbf {A} } 1560:10.1088/0305-4470/30/20/020 1710: 1486:10.1103/PhysRev.138.B979 1426:{\displaystyle n\ll N\,} 140:Mathematical formulation 1650:Plenum (New York) 1987 1523:10.1103/PhysRevA.7.2203 976:{\displaystyle \phi \,} 567:{\displaystyle z_{i}\,} 539:{\displaystyle m_{i}\,} 383:is periodic in time as 120:, i.e. roughly like an 61:more precise citations. 1622:10.1002/0471428027.ch3 1448: 1427: 1400: 1374: 1350: 1329: 1308: 1248: 1185: 1072: 977: 953: 829: 703: 646: 589: 568: 540: 512: 482: 452: 431: 377: 351: 313: 1577:Optics Communications 1449: 1428: 1401: 1375: 1351: 1330: 1309: 1249: 1162: 1073: 978: 954: 830: 704: 647: 590: 569: 541: 513: 483: 453: 432: 378: 352: 314: 1616:. pp. 147–267. 1437: 1410: 1389: 1383:quantum field theory 1363: 1339: 1318: 1274: 1091: 987: 966: 845: 720: 711:Schrödinger equation 663: 602: 578: 550: 522: 492: 462: 441: 387: 365: 339: 157: 1589:2000OptCo.185..353C 1552:1997JPhA...30.7193G 1515:1973PhRvA...7.2203S 1478:1965PhRv..138..979S 1447:{\displaystyle N\,} 1399:{\displaystyle n\,} 1373:{\displaystyle n\,} 1349:{\displaystyle n\,} 1328:{\displaystyle E\,} 588:{\displaystyle c\,} 451:{\displaystyle i\,} 103:light dressed state 1444: 1423: 1396: 1370: 1346: 1325: 1304: 1244: 1068: 973: 949: 825: 699: 642: 585: 564: 536: 508: 478: 448: 427: 373: 347: 309: 175: 101:science, the term 1546:(20): 7193–7215. 1503:Physical Review A 1472:(4B): B979–B987. 1268: 1267: 742: 574:, respectively. 333: 332: 234: 196: 166: 89:In the fields of 87: 86: 79: 16:(Redirected from 1701: 1643: 1608: 1583:(4–6): 353–358. 1571: 1534: 1509:(6): 2203–2213. 1497: 1453: 1451: 1450: 1445: 1432: 1430: 1429: 1424: 1405: 1403: 1402: 1397: 1379: 1377: 1376: 1371: 1355: 1353: 1352: 1347: 1334: 1332: 1331: 1326: 1313: 1311: 1310: 1305: 1296: 1262: 1253: 1251: 1250: 1245: 1237: 1236: 1231: 1219: 1218: 1184: 1179: 1155: 1114: 1113: 1108: 1085: 1077: 1075: 1074: 1069: 1052: 1051: 1046: 1010: 1009: 1004: 982: 980: 979: 974: 958: 956: 955: 950: 936: 935: 930: 909: 868: 867: 862: 834: 832: 831: 826: 812: 811: 806: 764: 763: 758: 743: 741: 730: 708: 706: 705: 700: 686: 685: 680: 651: 649: 648: 643: 594: 592: 591: 586: 573: 571: 570: 565: 562: 561: 545: 543: 542: 537: 534: 533: 517: 515: 514: 509: 506: 505: 500: 487: 485: 484: 479: 476: 475: 470: 457: 455: 454: 449: 436: 434: 433: 428: 417: 394: 382: 380: 379: 374: 372: 359:vector potential 356: 354: 353: 348: 346: 327: 318: 316: 315: 310: 299: 298: 293: 275: 274: 269: 265: 264: 254: 253: 248: 235: 230: 229: 220: 215: 214: 209: 197: 195: 194: 193: 177: 174: 151: 116:in terms of the 82: 75: 71: 68: 62: 57:this article by 48:inline citations 35: 34: 27: 21: 1709: 1708: 1704: 1703: 1702: 1700: 1699: 1698: 1679: 1678: 1665: 1646:F.H.M. Faisal, 1632: 1611: 1574: 1537: 1500: 1466:Physical Review 1463: 1460: 1435: 1434: 1408: 1407: 1387: 1386: 1361: 1360: 1337: 1336: 1335:and an integer 1316: 1315: 1272: 1271: 1260: 1226: 1210: 1103: 1089: 1088: 1041: 999: 985: 984: 964: 963: 925: 857: 843: 842: 801: 753: 734: 718: 717: 675: 661: 660: 657:Floquet theorem 600: 599: 576: 575: 553: 548: 547: 525: 520: 519: 495: 490: 489: 465: 460: 459: 439: 438: 385: 384: 363: 362: 337: 336: 325: 288: 243: 221: 204: 203: 199: 198: 185: 181: 155: 154: 142: 134:Floquet theorem 118:Floquet picture 83: 72: 66: 63: 53:Please help to 52: 36: 32: 23: 22: 15: 12: 11: 5: 1707: 1705: 1697: 1696: 1694:Quantum states 1691: 1689:Quantum optics 1681: 1680: 1677: 1676: 1671: 1669:Quantum optics 1664: 1661: 1660: 1659: 1644: 1630: 1609: 1572: 1535: 1498: 1459: 1456: 1442: 1421: 1418: 1415: 1394: 1368: 1344: 1323: 1302: 1299: 1295: 1291: 1288: 1285: 1282: 1279: 1266: 1265: 1256: 1254: 1243: 1240: 1235: 1230: 1225: 1222: 1217: 1213: 1209: 1206: 1203: 1200: 1197: 1194: 1191: 1188: 1183: 1178: 1175: 1172: 1169: 1165: 1161: 1158: 1154: 1150: 1147: 1144: 1141: 1138: 1135: 1132: 1129: 1126: 1123: 1120: 1117: 1112: 1107: 1102: 1099: 1096: 1080:Fourier series 1067: 1064: 1061: 1058: 1055: 1050: 1045: 1040: 1037: 1034: 1031: 1028: 1025: 1022: 1019: 1016: 1013: 1008: 1003: 998: 995: 992: 971: 960: 959: 948: 945: 942: 939: 934: 929: 924: 921: 918: 915: 912: 908: 904: 901: 898: 895: 892: 889: 886: 883: 880: 877: 874: 871: 866: 861: 856: 853: 850: 836: 835: 824: 821: 818: 815: 810: 805: 800: 797: 794: 791: 788: 785: 782: 779: 776: 773: 770: 767: 762: 757: 752: 749: 746: 740: 737: 733: 728: 725: 698: 695: 692: 689: 684: 679: 674: 671: 668: 653: 652: 641: 637: 634: 631: 628: 625: 622: 619: 616: 613: 610: 607: 583: 560: 556: 532: 528: 504: 499: 474: 469: 446: 426: 423: 420: 416: 412: 409: 406: 403: 400: 397: 393: 371: 345: 331: 330: 321: 319: 308: 305: 302: 297: 292: 287: 284: 281: 278: 273: 268: 263: 260: 257: 252: 247: 242: 239: 233: 228: 224: 218: 213: 208: 202: 192: 188: 184: 180: 173: 169: 165: 162: 141: 138: 85: 84: 39: 37: 30: 24: 18:Dressed states 14: 13: 10: 9: 6: 4: 3: 2: 1706: 1695: 1692: 1690: 1687: 1686: 1684: 1675: 1672: 1670: 1667: 1666: 1662: 1657: 1656:0-306-42317-0 1653: 1649: 1645: 1641: 1637: 1633: 1631:9780471214526 1627: 1623: 1619: 1615: 1610: 1606: 1602: 1598: 1594: 1590: 1586: 1582: 1578: 1573: 1569: 1565: 1561: 1557: 1553: 1549: 1545: 1541: 1536: 1532: 1528: 1524: 1520: 1516: 1512: 1508: 1504: 1499: 1495: 1491: 1487: 1483: 1479: 1475: 1471: 1467: 1462: 1461: 1457: 1455: 1440: 1419: 1416: 1413: 1392: 1384: 1366: 1357: 1342: 1321: 1297: 1293: 1289: 1286: 1283: 1277: 1264: 1257: 1255: 1233: 1215: 1211: 1204: 1201: 1198: 1195: 1189: 1186: 1173: 1170: 1167: 1163: 1152: 1148: 1145: 1142: 1139: 1133: 1130: 1127: 1121: 1118: 1110: 1094: 1087: 1086: 1083: 1081: 1065: 1059: 1056: 1048: 1032: 1029: 1023: 1020: 1017: 1014: 1006: 990: 969: 943: 940: 932: 916: 906: 902: 899: 896: 893: 887: 884: 881: 875: 872: 864: 848: 841: 840: 839: 819: 816: 808: 792: 786: 780: 777: 771: 768: 760: 744: 738: 723: 716: 715: 714: 712: 693: 690: 682: 666: 658: 639: 632: 626: 623: 617: 614: 611: 605: 598: 597: 596: 581: 558: 554: 530: 526: 502: 472: 444: 421: 410: 404: 401: 398: 360: 329: 322: 320: 306: 295: 279: 276: 271: 266: 231: 226: 222: 216: 211: 200: 190: 186: 182: 178: 171: 167: 163: 160: 153: 152: 149: 147: 139: 137: 135: 131: 127: 123: 119: 115: 112: 108: 107:quantum state 104: 100: 96: 92: 81: 78: 70: 60: 56: 50: 49: 43: 38: 29: 28: 19: 1647: 1613: 1580: 1576: 1543: 1539: 1506: 1502: 1469: 1465: 1359:The integer 1358: 1269: 1258: 1082:, obtaining 961: 837: 654: 334: 323: 143: 105:refers to a 102: 88: 73: 64: 45: 146:Hamiltonian 59:introducing 1683:Categories 1458:References 67:April 2021 42:references 1640:1934-4791 1605:0030-4018 1568:0305-4470 1531:0556-2791 1494:0031-899X 1417:≪ 1290:π 1278:ω 1212:ϕ 1202:ω 1190:⁡ 1182:∞ 1177:∞ 1174:− 1164:∑ 1157:ℏ 1140:− 1134:⁡ 1095:ψ 1033:ϕ 991:ϕ 970:ϕ 917:ϕ 911:ℏ 894:− 888:⁡ 849:ψ 793:ψ 745:ψ 736:∂ 732:∂ 727:ℏ 667:ψ 217:− 168:∑ 95:molecular 1663:See also 1433:, where 709:of the 126:molecule 1585:Bibcode 1548:Bibcode 1511:Bibcode 1474:Bibcode 357:is the 128:plus a 99:optical 55:improve 1654:  1638:  1628:  1603:  1566:  1529:  1492:  1270:where 962:where 335:where 130:photon 97:, and 91:atomic 44:, but 124:or a 114:light 111:laser 1652:ISBN 1636:ISSN 1626:ISBN 1601:ISSN 1564:ISSN 1527:ISSN 1490:ISSN 655:The 546:and 488:and 144:The 122:atom 1618:doi 1593:doi 1581:185 1556:doi 1519:doi 1482:doi 1470:138 1187:exp 1131:exp 885:exp 1685:: 1634:. 1624:. 1599:. 1591:. 1579:. 1562:. 1554:. 1544:30 1542:. 1525:. 1517:. 1505:. 1488:. 1480:. 1468:. 1356:. 93:, 1658:. 1642:. 1620:: 1607:. 1595:: 1587:: 1570:. 1558:: 1550:: 1533:. 1521:: 1513:: 1507:7 1496:. 1484:: 1476:: 1441:N 1420:N 1414:n 1393:n 1367:n 1343:n 1322:E 1301:) 1298:T 1294:/ 1287:2 1284:= 1281:( 1263:) 1261:2 1259:( 1242:) 1239:} 1234:i 1229:r 1224:{ 1221:( 1216:n 1208:] 1205:t 1199:n 1196:i 1193:[ 1171:= 1168:n 1160:] 1153:/ 1149:t 1146:E 1143:i 1137:[ 1128:= 1125:) 1122:t 1119:, 1116:} 1111:i 1106:r 1101:{ 1098:( 1066:. 1063:) 1060:t 1057:, 1054:} 1049:i 1044:r 1039:{ 1036:( 1030:= 1027:) 1024:T 1021:+ 1018:t 1015:, 1012:} 1007:i 1002:r 997:{ 994:( 947:) 944:t 941:, 938:} 933:i 928:r 923:{ 920:( 914:] 907:/ 903:t 900:E 897:i 891:[ 882:= 879:) 876:t 873:, 870:} 865:i 860:r 855:{ 852:( 823:) 820:t 817:, 814:} 809:i 804:r 799:{ 796:( 790:) 787:t 784:( 781:H 778:= 775:) 772:t 769:, 766:} 761:i 756:r 751:{ 748:( 739:t 724:i 697:) 694:t 691:, 688:} 683:i 678:r 673:{ 670:( 640:. 636:) 633:t 630:( 627:H 624:= 621:) 618:T 615:+ 612:t 609:( 606:H 582:c 559:i 555:z 531:i 527:m 503:i 498:p 473:i 468:r 445:i 425:) 422:t 419:( 415:A 411:= 408:) 405:T 402:+ 399:t 396:( 392:A 370:A 344:A 328:) 326:1 324:( 307:, 304:) 301:} 296:i 291:r 286:{ 283:( 280:V 277:+ 272:2 267:] 262:) 259:t 256:, 251:i 246:r 241:( 238:A 232:c 227:i 223:z 212:i 207:p 201:[ 191:i 187:m 183:2 179:1 172:i 164:= 161:H 80:) 74:( 69:) 65:( 51:. 20:)

Index

Dressed states
references
inline citations
improve
introducing
Learn how and when to remove this message
atomic
molecular
optical
quantum state
laser
light
Floquet picture
atom
molecule
photon
Floquet theorem
Hamiltonian
vector potential
Floquet theorem
Schrödinger equation
Fourier series
quantum field theory
Bibcode
1965PhRv..138..979S
doi
10.1103/PhysRev.138.B979
ISSN
0031-899X
Bibcode

Text is available under the Creative Commons Attribution-ShareAlike License. Additional terms may apply.

↑