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Dark state

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that determine which transitions are allowed and which are not. Often these selection rules can be boiled down to conservation of angular momentum (the photon has angular momentum). In most cases we only consider an atom interacting with the electric dipole field of the photon. Then some transitions
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of the atom no longer interacts with the laser simply because no photons of the right frequency are present to induce a transition to a different level. In practice, the term dark state is often used for a state that is not accessible by the specific laser in use even though transitions from this
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This means that when the atoms are in this state, they will stay in this state indefinitely. This is a dark state, because it can not absorb or emit any photons from the applied fields. It is, therefore, effectively transparent to the probe laser, even when the laser is exactly resonant with the
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state can not decay to the ground state by emitting a single photon. It can only decay by collisions with other atoms or by emitting multiple photons. Since these events are rare, the atom can remain in this excited state for a very long time, such an excited state is called a
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can result in an atom being in this dark state or another coherent state, known as a bright state. Therefore, in a collection of atoms, over time, decay into the dark state will inevitably result in the system being "trapped" coherently in that state, a phenomenon known as
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superposition of two states, both of which are coupled by lasers at the right frequency to a third state. With the system in a particular superposition of the two states, the system can be made dark to both lasers as the probability of absorbing a photon goes to 0.
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light to induce transitions between energy levels, when atoms can spontaneously decay into a state that is not coupled to any other level by the laser light, preventing the atom from absorbing or emitting light from that state.
1724: 3106: 1199: 2841: 667: 1477: 1622: 1552: 599: 557: 515: 2227: 1879: 2849: 2773:{\displaystyle c_{3}(t)=-ic_{1}(0){\frac {\Omega _{p}}{\Omega }}\sin {\frac {\Omega t}{2}}-ic_{2}(0){\frac {\Omega _{c}}{\Omega }}\sin {\frac {\Omega t}{2}}+c_{3}(0)\cos {\frac {\Omega t}{2}}} 171: 1187: 1147: 3253:{\displaystyle \cos \theta ={\frac {\Omega _{c}}{\sqrt {\Omega _{p}^{2}+\Omega _{c}^{2}}}},\qquad \sin \theta ={\frac {\Omega _{p}}{\sqrt {\Omega _{p}^{2}+\Omega _{c}^{2}}}}.} 47:. However, not all transitions between arbitrary states are allowed. A state that cannot absorb an incident photon is called a dark state. This can occur in experiments using 211: 656: 432: 379: 326: 1107: 1080: 1049: 1022: 3290: 3009: 987:{\displaystyle H_{1}=-{\frac {\hbar }{2}}\left(\Omega _{p}e^{+i\omega _{p}t}|1\rangle \langle 3|+\Omega _{c}e^{+i\omega _{c}t}|2\rangle \langle 3|\right)+{\mbox{H.c.}},} 276: 248: 3029: 95: 3350: 122: 1734: 283:
are not allowed at all, others are only allowed for photons of a certain polarization. Consider for example the hydrogen atom. The transition from the state
1628: 3306: 1406:{\displaystyle |\psi (t)\rangle =c_{1}(t)e^{-i\omega _{1}t}|1\rangle +c_{2}(t)e^{-i\omega _{2}t}|2\rangle +c_{3}(t)e^{-i\omega _{3}t}|3\rangle .} 3037: 173:. However, the atom can still decay spontaneously into a third state by emitting a photon of a different frequency. The new state with energy 278:
is allowed often depends on how detailed the model is that we use for the atom-light interaction. From a particular model follow a set of
801:{\displaystyle H_{0}=\hbar \omega _{1}|1\rangle \langle 1|+\hbar \omega _{2}|2\rangle \langle 2|+\hbar \omega _{3}|3\rangle \langle 3|,} 2786: 1422: 1558: 1488: 606: 2562:{\displaystyle c_{2}(t)=c_{1}(0)\left+c_{2}(0)\left\quad -ic_{3}(0){\frac {\Omega _{c}}{\Omega }}\sin {\frac {\Omega t}{2}}} 2214:{\displaystyle c_{1}(t)=c_{1}(0)\left+c_{2}(0)\left\quad -ic_{3}(0){\frac {\Omega _{p}}{\Omega }}\sin {\frac {\Omega t}{2}}} 2973:{\displaystyle c_{1}(0)={\frac {\Omega _{c}}{\Omega }},\qquad c_{2}(0)=-{\frac {\Omega _{p}}{\Omega }},\qquad c_{3}(0)=0,} 562: 520: 478: 602: 127: 1152: 1112: 97:(meaning the photons have a specific energy), so they only couple one set of states with a particular energy 2983:
which gives a time-independent solution to these equations with no probability of the system being in state
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is only allowed for light with polarization along the z axis (quantization axis) of the atom. The state
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Experiments in atomic physics are often done with a laser of a specific frequency
1719:{\displaystyle {\dot {c}}_{3}={\frac {i}{2}}(\Omega _{p}c_{1}+\Omega _{c}c_{2}).} 35:
that cannot absorb (or emit) photons. All atoms and molecules are described by
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therefore appears dark for light of other polarizations. Transitions from the
32: 3101:{\displaystyle |D\rangle =\cos \theta |1\rangle -\sin \theta |2\rangle } 44: 1193:
of the entire expression. We will write the atomic wave function as
466: 48: 2836:{\displaystyle \Omega ={\sqrt {\Omega _{c}^{2}+\Omega _{p}^{2}}}} 3011:. This state can also be expressed in terms of a mixing angle 1472:{\displaystyle i\hbar |{\dot {\psi }}\rangle =H|\psi \rangle } 1617:{\displaystyle {\dot {c}}_{2}={\frac {i}{2}}\Omega _{c}c_{3}} 1547:{\displaystyle {\dot {c}}_{1}={\frac {i}{2}}\Omega _{p}c_{3}} 2843:. We observe that we can choose the initial conditions 3332:
Fundamentals of Quantum Optics and Quantum Information
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Lambropoulos & D. Petrosyan (2007). 3271: 3269: 3238: 3233: 3220: 3215: 3204: 3198: 3173: 3168: 3155: 3150: 3139: 3133: 3119: 3087: 3064: 3041: 3039: 3016: 2990: 2988: 2946: 2927: 2921: 2900: 2881: 2875: 2857: 2851: 2825: 2820: 2807: 2802: 2796: 2788: 2755: 2734: 2712: 2695: 2689: 2674: 2649: 2632: 2626: 2611: 2583: 2577: 2544: 2527: 2521: 2506: 2475: 2461: 2451: 2446: 2440: 2429: 2419: 2414: 2408: 2388: 2361: 2347: 2336: 2326: 2319: 2308: 2297: 2287: 2280: 2257: 2235: 2229: 2196: 2179: 2173: 2158: 2127: 2113: 2102: 2092: 2085: 2074: 2063: 2053: 2046: 2023: 1996: 1982: 1972: 1967: 1961: 1950: 1940: 1935: 1929: 1909: 1887: 1881: 1846: 1831: 1813: 1798: 1780: 1765: 1738: 1736: 1704: 1694: 1681: 1671: 1654: 1645: 1634: 1633: 1630: 1608: 1598: 1584: 1575: 1564: 1563: 1560: 1538: 1528: 1514: 1505: 1494: 1493: 1490: 1458: 1438: 1437: 1432: 1424: 1389: 1378: 1367: 1348: 1330: 1319: 1308: 1289: 1271: 1260: 1249: 1230: 1203: 1201: 1173: 1160: 1154: 1133: 1120: 1114: 1093: 1087: 1066: 1060: 1035: 1029: 1008: 1002: 974: 961: 944: 933: 922: 912: 900: 883: 872: 861: 851: 832: 820: 814: 790: 773: 767: 752: 735: 729: 714: 697: 691: 675: 669: 642: 629: 617: 580: 566: 564: 538: 524: 522: 496: 482: 480: 414: 410: 400: 394: 361: 357: 347: 341: 308: 304: 294: 288: 257: 255: 229: 227: 197: 184: 178: 166:{\displaystyle E_{2}=E_{1}+\hbar \omega } 148: 135: 129: 108: 102: 82: 3307:Electromagnetically induced transparency 1189:, respectively, and H.c. stands for the 124:to another set of states with an energy 3322: 1873:we can solve these equations to obtain 1429: 1182:{\displaystyle \omega _{2}-\omega _{3}} 1142:{\displaystyle \omega _{1}-\omega _{3}} 1082:) and the coupling field (of frequency 834: 760: 722: 684: 157: 55:A dark state can also be the result of 3351:Atomic, molecular, and optical physics 3264:transition. Spontaneous emission from 7: 559:are dipole-allowed transitions and 3230: 3212: 3201: 3165: 3147: 3136: 2933: 2924: 2887: 2878: 2817: 2799: 2790: 2758: 2715: 2701: 2692: 2652: 2638: 2629: 2547: 2533: 2524: 2478: 2458: 2443: 2426: 2411: 2364: 2344: 2333: 2323: 2305: 2294: 2284: 2199: 2185: 2176: 2130: 2110: 2099: 2089: 2071: 2060: 2050: 1999: 1979: 1964: 1947: 1932: 1691: 1668: 1595: 1525: 1032: 1005: 909: 848: 450:level are not allowed at all. The 14: 1055:of the probe field (of frequency 214:state are in principle allowed. 31:refers to a state of an atom or 3185: 2941: 2895: 2495: 2147: 3272: 3088: 3065: 3042: 2991: 2958: 2952: 2912: 2906: 2869: 2863: 2746: 2740: 2686: 2680: 2623: 2617: 2595: 2589: 2518: 2512: 2400: 2394: 2269: 2263: 2247: 2241: 2170: 2164: 2035: 2029: 1921: 1915: 1899: 1893: 1847: 1843: 1837: 1814: 1810: 1804: 1781: 1777: 1771: 1752: 1746: 1739: 1710: 1664: 1459: 1433: 1390: 1360: 1354: 1331: 1301: 1295: 1272: 1242: 1236: 1217: 1211: 1204: 962: 945: 901: 884: 791: 774: 753: 736: 715: 698: 581: 577: 567: 539: 535: 525: 497: 493: 483: 258: 230: 206:{\displaystyle E_{3}<E_{2}} 1: 3334:. Berlin; New York: Springer. 651:{\displaystyle H=H_{0}+H_{1}} 3295:coherent population trapping 1728:Using the initial condition 427:{\displaystyle 2^{2}P_{3/2}} 374:{\displaystyle 2^{2}P_{3/2}} 321:{\displaystyle 1^{2}S_{1/2}} 1102:{\displaystyle \omega _{c}} 1075:{\displaystyle \omega _{p}} 1044:{\displaystyle \Omega _{c}} 1017:{\displaystyle \Omega _{p}} 603:rotating wave approximation 471:A three-state Λ-type system 3372: 3285:{\displaystyle |3\rangle } 3004:{\displaystyle |3\rangle } 1479:, we obtain the solutions 271:{\displaystyle |2\rangle } 243:{\displaystyle |1\rangle } 15: 3024:{\displaystyle \theta } 90:{\displaystyle \omega } 16:For the 2021 film, see 3312:List of laser articles 3286: 3254: 3102: 3025: 3005: 2974: 2837: 2774: 2563: 2215: 1864: 1720: 1618: 1548: 1473: 1407: 1183: 1143: 1103: 1076: 1045: 1018: 988: 802: 652: 595: 553: 511: 472: 428: 375: 322: 272: 244: 207: 167: 118: 91: 3287: 3255: 3103: 3026: 3006: 2975: 2838: 2775: 2564: 2216: 1865: 1721: 1619: 1549: 1474: 1408: 1184: 1144: 1104: 1077: 1046: 1019: 989: 803: 653: 605:, the semi-classical 601:is forbidden. In the 596: 554: 512: 470: 429: 376: 323: 273: 245: 208: 168: 119: 117:{\displaystyle E_{1}} 92: 3268: 3118: 3038: 3015: 2987: 2850: 2787: 2576: 2228: 1880: 1735: 1629: 1559: 1489: 1423: 1418:Schrödinger equation 1200: 1153: 1113: 1086: 1059: 1028: 1001: 813: 668: 616: 563: 521: 479: 393: 340: 287: 254: 226: 177: 128: 101: 81: 57:quantum interference 3243: 3225: 3178: 3160: 2830: 2812: 2456: 2424: 1977: 1945: 1191:Hermitian conjugate 463:Three-level systems 3282: 3250: 3229: 3211: 3164: 3146: 3098: 3021: 3001: 2970: 2833: 2816: 2798: 2770: 2559: 2442: 2410: 2211: 1963: 1931: 1860: 1716: 1614: 1544: 1469: 1403: 1179: 1139: 1099: 1072: 1041: 1014: 984: 979: 798: 648: 591: 549: 507: 473: 424: 371: 318: 268: 240: 203: 163: 114: 87: 3245: 3244: 3180: 3179: 2936: 2890: 2831: 2768: 2725: 2704: 2662: 2641: 2557: 2536: 2488: 2467: 2435: 2374: 2353: 2314: 2209: 2188: 2140: 2119: 2080: 2009: 1988: 1956: 1662: 1642: 1592: 1572: 1522: 1502: 1446: 978: 840: 68:Two-level systems 18:Dark State (film) 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1138: 1137: 1125: 1124: 1108: 1106: 1105: 1100: 1098: 1097: 1081: 1079: 1078: 1073: 1071: 1070: 1053:Rabi frequencies 1050: 1048: 1047: 1042: 1040: 1039: 1023: 1021: 1020: 1015: 1013: 1012: 993: 991: 990: 985: 980: 976: 970: 966: 965: 948: 943: 942: 938: 937: 917: 916: 904: 887: 882: 881: 877: 876: 856: 855: 841: 833: 825: 824: 807: 805: 804: 799: 794: 777: 772: 771: 756: 739: 734: 733: 718: 701: 696: 695: 680: 679: 657: 655: 654: 649: 647: 646: 634: 633: 600: 598: 597: 592: 584: 570: 558: 556: 555: 550: 542: 528: 516: 514: 513: 508: 500: 486: 457:metastable state 433: 431: 430: 425: 423: 422: 418: 405: 404: 380: 378: 377: 372: 370: 369: 365: 352: 351: 327: 325: 324: 319: 317: 316: 312: 299: 298: 277: 275: 274: 269: 261: 249: 247: 246: 241: 233: 212: 210: 209: 204: 202: 201: 189: 188: 172: 170: 169: 164: 153: 152: 140: 139: 123: 121: 120: 115: 113: 112: 96: 94: 93: 88: 3371: 3370: 3366: 3365: 3364: 3362: 3361: 3360: 3341: 3340: 3339: 3329: 3328: 3324: 3320: 3303: 3266: 3265: 3200: 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284: 280:selection rules 252: 251: 224: 223: 220: 193: 180: 175: 174: 144: 131: 126: 125: 104: 99: 98: 79: 78: 75: 70: 21: 12: 11: 5: 3369: 3367: 3359: 3358: 3353: 3343: 3342: 3338: 3337: 3321: 3319: 3316: 3315: 3314: 3309: 3302: 3299: 3281: 3278: 3274: 3261: 3260: 3249: 3241: 3236: 3232: 3228: 3223: 3218: 3214: 3207: 3203: 3197: 3194: 3191: 3188: 3184: 3176: 3171: 3167: 3163: 3158: 3153: 3149: 3142: 3138: 3132: 3129: 3126: 3123: 3109: 3108: 3097: 3094: 3090: 3086: 3083: 3080: 3077: 3074: 3071: 3067: 3063: 3060: 3057: 3054: 3051: 3048: 3044: 3020: 3000: 2997: 2993: 2981: 2980: 2969: 2966: 2963: 2960: 2957: 2954: 2949: 2945: 2940: 2935: 2930: 2926: 2920: 2917: 2914: 2911: 2908: 2903: 2899: 2894: 2889: 2884: 2880: 2874: 2871: 2868: 2865: 2860: 2856: 2828: 2823: 2819: 2815: 2810: 2805: 2801: 2795: 2792: 2781: 2780: 2767: 2763: 2760: 2754: 2751: 2748: 2745: 2742: 2737: 2733: 2729: 2724: 2720: 2717: 2711: 2708: 2703: 2698: 2694: 2688: 2685: 2682: 2677: 2673: 2669: 2666: 2661: 2657: 2654: 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1859: 1856: 1853: 1849: 1845: 1842: 1839: 1834: 1830: 1826: 1823: 1820: 1816: 1812: 1809: 1806: 1801: 1797: 1793: 1790: 1787: 1783: 1779: 1776: 1773: 1768: 1764: 1760: 1757: 1754: 1751: 1748: 1745: 1741: 1715: 1712: 1707: 1703: 1697: 1693: 1689: 1684: 1680: 1674: 1670: 1666: 1661: 1658: 1653: 1648: 1641: 1638: 1611: 1607: 1601: 1597: 1591: 1588: 1583: 1578: 1571: 1568: 1541: 1537: 1531: 1527: 1521: 1518: 1513: 1508: 1501: 1498: 1484: 1483: 1468: 1465: 1461: 1457: 1454: 1451: 1445: 1442: 1435: 1431: 1428: 1414: 1413: 1402: 1399: 1396: 1392: 1386: 1381: 1377: 1373: 1370: 1366: 1362: 1359: 1356: 1351: 1347: 1343: 1340: 1337: 1333: 1327: 1322: 1318: 1314: 1311: 1307: 1303: 1300: 1297: 1292: 1288: 1284: 1281: 1278: 1274: 1268: 1263: 1259: 1255: 1252: 1248: 1244: 1241: 1238: 1233: 1229: 1225: 1222: 1219: 1216: 1213: 1210: 1206: 1176: 1172: 1168: 1163: 1159: 1136: 1132: 1128: 1123: 1119: 1096: 1092: 1069: 1065: 1038: 1034: 1011: 1007: 995: 994: 983: 973: 969: 964: 960: 957: 954: 951: 947: 941: 936: 932: 928: 925: 921: 915: 911: 907: 903: 899: 896: 893: 890: 886: 880: 875: 871: 867: 864: 860: 854: 850: 845: 839: 836: 831: 828: 823: 819: 808: 797: 793: 789: 786: 783: 780: 776: 770: 766: 762: 759: 755: 751: 748: 745: 742: 738: 732: 728: 724: 721: 717: 713: 710: 707: 704: 700: 694: 690: 686: 683: 678: 674: 659: 658: 645: 641: 637: 632: 628: 624: 621: 590: 587: 583: 579: 576: 573: 569: 548: 545: 541: 537: 534: 531: 527: 506: 503: 499: 495: 492: 489: 485: 464: 461: 437: 421: 417: 413: 409: 403: 399: 384: 368: 364: 360: 356: 350: 346: 331: 315: 311: 307: 303: 297: 293: 267: 264: 260: 239: 236: 232: 219: 216: 200: 196: 192: 187: 183: 162: 159: 156: 151: 147: 143: 138: 134: 111: 107: 86: 74: 71: 69: 66: 37:quantum states 25:atomic physics 13: 10: 9: 6: 4: 3: 2: 3368: 3357: 3354: 3352: 3349: 3348: 3346: 3333: 3326: 3323: 3317: 3313: 3310: 3308: 3305: 3304: 3300: 3298: 3296: 3276: 3247: 3239: 3234: 3226: 3221: 3216: 3205: 3195: 3192: 3189: 3186: 3182: 3174: 3169: 3161: 3156: 3151: 3140: 3130: 3127: 3124: 3121: 3114: 3113: 3112: 3092: 3084: 3081: 3078: 3075: 3069: 3061: 3058: 3055: 3052: 3046: 3034: 3033: 3032: 3018: 2995: 2967: 2964: 2961: 2955: 2947: 2943: 2938: 2928: 2918: 2915: 2909: 2901: 2897: 2892: 2882: 2872: 2866: 2858: 2854: 2846: 2845: 2844: 2826: 2821: 2813: 2808: 2803: 2793: 2765: 2761: 2752: 2749: 2743: 2735: 2731: 2727: 2722: 2718: 2709: 2706: 2696: 2683: 2675: 2671: 2667: 2664: 2659: 2655: 2646: 2643: 2633: 2620: 2612: 2608: 2604: 2601: 2598: 2592: 2584: 2580: 2572: 2571: 2554: 2550: 2541: 2538: 2528: 2515: 2507: 2503: 2499: 2496: 2491: 2485: 2481: 2472: 2469: 2462: 2452: 2447: 2437: 2430: 2420: 2415: 2404: 2397: 2389: 2385: 2381: 2377: 2371: 2367: 2358: 2355: 2348: 2337: 2327: 2316: 2309: 2298: 2288: 2277: 2273: 2266: 2258: 2254: 2250: 2244: 2236: 2232: 2224: 2223: 2206: 2202: 2193: 2190: 2180: 2167: 2159: 2155: 2151: 2148: 2143: 2137: 2133: 2124: 2121: 2114: 2103: 2093: 2082: 2075: 2064: 2054: 2043: 2039: 2032: 2024: 2020: 2016: 2012: 2006: 2002: 1993: 1990: 1983: 1973: 1968: 1958: 1951: 1941: 1936: 1925: 1918: 1910: 1906: 1902: 1896: 1888: 1884: 1876: 1875: 1874: 1857: 1851: 1840: 1832: 1828: 1824: 1818: 1807: 1799: 1795: 1791: 1785: 1774: 1766: 1762: 1758: 1749: 1743: 1731: 1730: 1729: 1726: 1713: 1705: 1701: 1695: 1687: 1682: 1678: 1672: 1659: 1656: 1651: 1646: 1639: 1636: 1624: 1609: 1605: 1599: 1589: 1586: 1581: 1576: 1569: 1566: 1554: 1539: 1535: 1529: 1519: 1516: 1511: 1506: 1499: 1496: 1482: 1481: 1480: 1463: 1455: 1452: 1443: 1440: 1426: 1419: 1400: 1394: 1384: 1379: 1375: 1371: 1368: 1364: 1357: 1349: 1345: 1341: 1335: 1325: 1320: 1316: 1312: 1309: 1305: 1298: 1290: 1286: 1282: 1276: 1266: 1261: 1257: 1253: 1250: 1246: 1239: 1231: 1227: 1223: 1214: 1208: 1196: 1195: 1194: 1192: 1174: 1170: 1166: 1161: 1157: 1134: 1130: 1126: 1121: 1117: 1094: 1090: 1067: 1063: 1054: 1036: 1009: 981: 971: 967: 958: 949: 939: 934: 930: 926: 923: 919: 913: 905: 897: 888: 878: 873: 869: 865: 862: 858: 852: 843: 837: 829: 826: 821: 817: 809: 795: 787: 778: 768: 764: 757: 749: 740: 730: 726: 719: 711: 702: 692: 688: 681: 676: 672: 664: 663: 662: 643: 639: 635: 630: 626: 622: 619: 612: 611: 610: 608: 604: 585: 571: 543: 529: 501: 487: 469: 462: 460: 458: 453: 449: 446:level to the 445: 441: 419: 415: 411: 407: 401: 397: 388: 366: 362: 358: 354: 348: 344: 336:to the state 335: 313: 309: 305: 301: 295: 291: 281: 262: 234: 217: 215: 198: 194: 190: 185: 181: 160: 154: 149: 145: 141: 136: 132: 109: 105: 84: 72: 67: 65: 62: 58: 53: 50: 46: 42: 38: 34: 30: 26: 19: 3331: 3325: 3294: 3262: 3110: 2982: 2782: 1872: 1727: 1625: 1555: 1485: 1416:Solving the 1415: 996: 660: 609:is given by 474: 451: 447: 443: 435: 382: 329: 250:and a state 221: 76: 54: 41:energy level 28: 22: 607:Hamiltonian 73:In practice 3345:Categories 3318:References 29:dark state 3356:Photonics 3280:⟩ 3231:Ω 3213:Ω 3202:Ω 3193:θ 3190:⁡ 3166:Ω 3148:Ω 3137:Ω 3128:θ 3125:⁡ 3096:⟩ 3085:θ 3082:⁡ 3076:− 3073:⟩ 3062:θ 3059:⁡ 3050:⟩ 3019:θ 2999:⟩ 2934:Ω 2925:Ω 2919:− 2888:Ω 2879:Ω 2818:Ω 2800:Ω 2791:Ω 2759:Ω 2753:⁡ 2716:Ω 2710:⁡ 2702:Ω 2693:Ω 2665:− 2653:Ω 2647:⁡ 2639:Ω 2630:Ω 2602:− 2548:Ω 2542:⁡ 2534:Ω 2525:Ω 2497:− 2479:Ω 2473:⁡ 2459:Ω 2444:Ω 2427:Ω 2412:Ω 2365:Ω 2359:⁡ 2345:Ω 2334:Ω 2324:Ω 2306:Ω 2295:Ω 2285:Ω 2278:− 2200:Ω 2194:⁡ 2186:Ω 2177:Ω 2149:− 2131:Ω 2125:⁡ 2111:Ω 2100:Ω 2090:Ω 2072:Ω 2061:Ω 2051:Ω 2044:− 2000:Ω 1994:⁡ 1980:Ω 1965:Ω 1948:Ω 1933:Ω 1855:⟩ 1822:⟩ 1789:⟩ 1756:⟩ 1744:ψ 1692:Ω 1669:Ω 1640:˙ 1596:Ω 1570:˙ 1526:Ω 1500:˙ 1467:⟩ 1464:ψ 1450:⟩ 1444:˙ 1441:ψ 1430:ℏ 1398:⟩ 1376:ω 1369:− 1339:⟩ 1317:ω 1310:− 1280:⟩ 1258:ω 1251:− 1221:⟩ 1209:ψ 1171:ω 1167:− 1158:ω 1131:ω 1127:− 1118:ω 1091:ω 1064:ω 1033:Ω 1006:Ω 956:⟨ 953:⟩ 931:ω 910:Ω 895:⟨ 892:⟩ 870:ω 849:Ω 835:ℏ 830:− 785:⟨ 782:⟩ 765:ω 761:ℏ 747:⟨ 744:⟩ 727:ω 723:ℏ 709:⟨ 706:⟩ 689:ω 685:ℏ 589:⟩ 578:↔ 575:⟩ 547:⟩ 536:↔ 533:⟩ 505:⟩ 494:↔ 491:⟩ 266:⟩ 238:⟩ 218:In theory 161:ω 158:ℏ 85:ω 3301:See also 1051:are the 61:coherent 33:molecule 45:photons 997:where 3111:with 2783:with 661:with 440:=-1/2 434:with 387:=-1/2 381:with 334:=-1/2 328:with 49:laser 1149:and 1024:and 977:H.c. 517:and 191:< 27:, a 3187:sin 3122:cos 3079:sin 3056:cos 3031:as 2750:cos 2707:sin 2644:sin 2539:sin 2470:cos 2356:cos 2191:sin 2122:cos 1991:cos 23:In 3347:: 3297:. 459:. 452:2S 448:1S 444:2S 3277:3 3273:| 3248:. 3240:2 3235:c 3227:+ 3222:2 3217:p 3206:p 3196:= 3183:, 3175:2 3170:c 3162:+ 3157:2 3152:p 3141:c 3131:= 3093:2 3089:| 3070:1 3066:| 3053:= 3047:D 3043:| 2996:3 2992:| 2968:, 2965:0 2962:= 2959:) 2956:0 2953:( 2948:3 2944:c 2939:, 2929:p 2916:= 2913:) 2910:0 2907:( 2902:2 2898:c 2893:, 2883:c 2873:= 2870:) 2867:0 2864:( 2859:1 2855:c 2827:2 2822:p 2814:+ 2809:2 2804:c 2794:= 2766:2 2762:t 2747:) 2744:0 2741:( 2736:3 2732:c 2728:+ 2723:2 2719:t 2697:c 2687:) 2684:0 2681:( 2676:2 2672:c 2668:i 2660:2 2656:t 2634:p 2624:) 2621:0 2618:( 2613:1 2609:c 2605:i 2599:= 2596:) 2593:t 2590:( 2585:3 2581:c 2555:2 2551:t 2529:c 2519:) 2516:0 2513:( 2508:3 2504:c 2500:i 2492:] 2486:2 2482:t 2463:2 2453:2 2448:c 2438:+ 2431:2 2421:2 2416:p 2405:[ 2401:) 2398:0 2395:( 2390:2 2386:c 2382:+ 2378:] 2372:2 2368:t 2349:2 2338:c 2328:p 2317:+ 2310:2 2299:c 2289:p 2274:[ 2270:) 2267:0 2264:( 2259:1 2255:c 2251:= 2248:) 2245:t 2242:( 2237:2 2233:c 2207:2 2203:t 2181:p 2171:) 2168:0 2165:( 2160:3 2156:c 2152:i 2144:] 2138:2 2134:t 2115:2 2104:c 2094:p 2083:+ 2076:2 2065:c 2055:p 2040:[ 2036:) 2033:0 2030:( 2025:2 2021:c 2017:+ 2013:] 2007:2 2003:t 1984:2 1974:2 1969:p 1959:+ 1952:2 1942:2 1937:c 1926:[ 1922:) 1919:0 1916:( 1911:1 1907:c 1903:= 1900:) 1897:t 1894:( 1889:1 1885:c 1858:, 1852:3 1848:| 1844:) 1841:0 1838:( 1833:3 1829:c 1825:+ 1819:2 1815:| 1811:) 1808:0 1805:( 1800:2 1796:c 1792:+ 1786:1 1782:| 1778:) 1775:0 1772:( 1767:1 1763:c 1759:= 1753:) 1750:0 1747:( 1740:| 1714:. 1711:) 1706:2 1702:c 1696:c 1688:+ 1683:1 1679:c 1673:p 1665:( 1660:2 1657:i 1652:= 1647:3 1637:c 1610:3 1606:c 1600:c 1590:2 1587:i 1582:= 1577:2 1567:c 1540:3 1536:c 1530:p 1520:2 1517:i 1512:= 1507:1 1497:c 1460:| 1456:H 1453:= 1434:| 1427:i 1401:. 1395:3 1391:| 1385:t 1380:3 1372:i 1365:e 1361:) 1358:t 1355:( 1350:3 1346:c 1342:+ 1336:2 1332:| 1326:t 1321:2 1313:i 1306:e 1302:) 1299:t 1296:( 1291:2 1287:c 1283:+ 1277:1 1273:| 1267:t 1262:1 1254:i 1247:e 1243:) 1240:t 1237:( 1232:1 1228:c 1224:= 1218:) 1215:t 1212:( 1205:| 1175:3 1162:2 1135:3 1122:1 1095:c 1068:p 1037:c 1010:p 982:, 972:+ 968:) 963:| 959:3 950:2 946:| 940:t 935:c 927:i 924:+ 920:e 914:c 906:+ 902:| 898:3 889:1 885:| 879:t 874:p 866:i 863:+ 859:e 853:p 844:( 838:2 827:= 822:1 818:H 796:, 792:| 788:3 779:3 775:| 769:3 758:+ 754:| 750:2 741:2 737:| 731:2 720:+ 716:| 712:1 703:1 699:| 693:1 682:= 677:0 673:H 644:1 640:H 636:+ 631:0 627:H 623:= 620:H 586:2 582:| 572:1 568:| 544:3 540:| 530:2 526:| 502:3 498:| 488:1 484:| 438:j 436:m 420:2 416:/ 412:3 408:P 402:2 398:2 385:j 383:m 367:2 363:/ 359:3 355:P 349:2 345:2 332:j 330:m 314:2 310:/ 306:1 302:S 296:2 292:1 263:2 259:| 235:1 231:| 199:2 195:E 186:3 182:E 155:+ 150:1 146:E 142:= 137:2 133:E 110:1 106:E 20:.

Index

Dark State (film)
atomic physics
molecule
quantum states
energy level
photons
laser
quantum interference
coherent
selection rules
metastable state

rotating wave approximation
Hamiltonian
Rabi frequencies
Hermitian conjugate
Schrödinger equation
Electromagnetically induced transparency
List of laser articles
Categories
Atomic, molecular, and optical physics
Photonics

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