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Spontaneous emission

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2441:), one needs to solve the time evolution of the wavefunction with an appropriate Hamiltonian. To solve for the transition amplitude, one needs to average over (integrate over) all the vacuum modes, since one must consider the probabilities that the emitted photon occupies various parts of phase space equally. The "spontaneously" emitted photon has infinite different modes to propagate into, thus the probability of the atom re-absorbing the photon and returning to the original state is negligible, making the atomic decay practically irreversible. Such irreversible time evolution of the atom-vacuum system is responsible for the apparent spontaneous decay of an excited atom. If one were to keep track of all the vacuum modes, the combined atom-vacuum system would undergo unitary time evolution, making the decay process reversible. 1281: 1877:, in which the electronic energy levels were quantized, but the electromagnetic field was not. Given that the eigenstates of an atom are properly diagonalized, the overlap of the wavefunctions between the excited state and the ground state of the atom is zero. Thus, in the absence of a quantized electromagnetic field, the excited state atom cannot decay to the ground state. In order to explain spontaneous transitions, quantum mechanics must be extended to a 2470:. The rate of emission depends on two factors: an 'atomic part', which describes the internal structure of the light source and a 'field part', which describes the density of electromagnetic modes of the environment. The atomic part describes the strength of a transition between two states in terms of transition moments. In a homogeneous medium, such as 2678: 2395:, which are the wavenumber and polarization of the emitted photon, respectively. As mentioned above, the emitted photon has a chance to be emitted with different wavenumbers and polarizations, and the resulting wavefunction is a superposition of these possibilities. To calculate the probability of the atom at the ground state ( 1908:
Although there is only one electronic transition from the excited state to ground state, there are many ways in which the electromagnetic field may go from the ground state to a one-photon state. That is, the electromagnetic field has infinitely more degrees of freedom, corresponding to the different
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only occurs under emission of light. In this case one speaks of full radiative decay and this means that the quantum efficiency is 100%. Besides radiative decay, which occurs under the emission of light, there is a second decay mechanism; nonradiative decay. To determine the total decay rate
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of the combined system of the atom plus electromagnetic field. In particular, the electron transition from the excited state to the electronic ground state mixes with the transition of the electromagnetic field from the ground state to an excited state, a field state with one photon in it.
919:. Spontaneous emission is ultimately responsible for most of the light we see all around us; it is so ubiquitous that there are many names given to what is essentially the same process. If atoms (or molecules) are excited by some means other than heating, the spontaneous emission is called 990:
interacting with a quantized field mode (i.e. the vacuum) within an optical cavity. It gave the nonintuitive prediction that the rate of spontaneous emission could be controlled depending on the boundary conditions of the surrounding vacuum field. These experiments gave rise to
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in 1930 in a landmark paper. The Weisskopf-Wigner calculation remains the standard approach to spontaneous radiation emission in atomic and molecular physics. Dirac had also developed the same calculation a couple of years prior to the paper by Wigner and Weisskopf.
2108: 2480: 2805: 3537:), electrons move quickly from a high energy level to a meta-stable level via small nonradiative transitions and then make the final move down to the bottom level via an optical or radiative transition. This final transition is the transition over the 3520: 1917:
In the presence of electromagnetic vacuum modes, the combined atom-vacuum system is explained by the superposition of the wavefunctions of the excited state atom with no photon and the ground state atom with a single emitted photon:
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stands for position operator. (This approximation breaks down in the case of inner shell electrons in high-Z atoms.) The above equation clearly shows that the rate of spontaneous emission in free space increases proportionally to
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A. F. van Driel, G. Allan, C. Delerue, P. Lodahl, W. L. Vos and D. Vanmaekelbergh, Frequency-dependent spontaneous emission rate from CdSe and CdTe nanocrystals: Influence of dark states, Physical Review Letters, 95, 236804
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offered by the electromagnetic field is infinitely larger than that offered by the atom. This infinite degree of freedom for the emission of the photon results in the apparent irreversible decay, i.e., spontaneous emission.
3366: 108: 1610: 3533:. Nonradiative relaxation occurs when the energy difference between the levels is very small, and these typically occur on a much faster time scale than radiative transitions. For many materials (for instance, 1433: 3117: 1863: 3632: 2673:{\displaystyle \Gamma _{\text{rad}}(\omega )={\frac {\omega ^{3}n|\mu _{12}|^{2}}{3\pi \varepsilon _{0}\hbar c^{3}}}={\frac {4\alpha \omega ^{3}n|\langle 1|\mathbf {r} |2\rangle |^{2}}{3c^{2}}}} 1924: 3040: 2686: 3150: 1159: 1692: 3450: 3423: 3396: 3310: 1770: 1218: 2218: 2910: 2353: 3458: 1743: 1104: 3192: 2145: 3254: 3220: 2307: 2439: 1797: 2879: 2257: 970:
by several decades. Later, after the formal discovery of quantum mechanics in 1926, the rate of spontaneous emission was accurately described from first principles by
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and is fundamentally a quantum process. According to the American Physical Society, the first person to correctly predict the phenomenon of spontaneous emission was
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Sharafiev, Aleksei; Juan, Mathieu L.; Gargiulo, Oscar; Zanner, Maximilian; Wögerer, Stephanie; García-Ripoll, Juan José; Kirchmair, Gerhard (2021-06-10).
4201: 1896:, which can mix with the excited stationary states of the atom. As a result of this interaction, the "stationary state" of the atom is no longer a true 1881:, wherein the electromagnetic field is quantized at every point in space. The quantum field theory of electrons and electromagnetic fields is known as 4181:
Phys. Rev. Lett. 95, 236804 (2005) - Frequency-Dependent Spontaneous Emission Rate from CdSe and CdTe Nanocrystals: Influence of Dark States (aps.org)
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the nonradiative decay rate. The quantum efficiency (QE) is defined as the fraction of emission processes in which emission of light is involved:
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Jaynes, E. T.; Cummings, F. W. (1963). "Comparison of quantum and semiclassical radiation theories with application to the beam maser".
3553:. Specifically, since electrons decay slowly from them, they can be deliberately piled up in this state without too much loss and then 935:. Sometimes molecules have a metastable level and continue to fluoresce long after the exciting radiation is turned off; this is called 4122: 1361: 923:. For example, fireflies are luminescent. And there are different forms of luminescence depending on how excited atoms are produced ( 3045: 126: 1805: 1492:
is a proportionality constant for this particular transition in this particular light source. The constant is referred to as the
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Welton, Theodore Allen (1948). "Some observable effects of the quantum-mechanical fluctuations of the electromagnetic field".
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of the photon in spontaneous emission is random as is the direction in which the photon propagates. This is not true for
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generally cannot support large vibrations without destroying bonds (which generally doesn't happen for relaxation).
978:. Contemporary physicists, when asked to give a physical explanation for spontaneous emission, generally invoke the 210: 3924: 868: 317: 297: 165: 3122: 1112: 2442: 992: 557: 287: 1667: 4198: 3768: 597: 335: 235: 3428: 2445:
is one such system where the vacuum modes are modified resulting in the reversible decay process, see also
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B. Henderson and G. Imbusch, Optical Spectroscopy of Inorganic Solids (Clarendon Press, Oxford, UK, 1989).
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etc.). If the excitation is effected by the absorption of radiation the spontaneous emission is called
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are the atomic excited state-electromagnetic vacuum wavefunction and its probability amplitude,
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Berman, Paul R.; Ford, George W. (2010-01-01), Arimondo, E.; Berman, P. R.; Lin, C. C. (eds.),
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R. Loudon, The Quantum Theory of Light, 3rd ed. (Oxford University Press Inc., New York, 2001).
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Straumann, Norbert (23 Mar 2017). "Einstein in 1916: "On the Quantum Theory of Radiation"".
3256:-frequency dependence of the spontaneous emission rate as described by Fermi's golden rule. 2919: 1468: 1441: 1167: 4043:"Visualizing the emission of a single photon with frequency and time resolved spectroscopy" 3861: 3818: 3783: 3733: 3586: 3229:
can be tuned continuously by changing their size. This property has been used to check the
1878: 1276:. An energy level diagram illustrating the process of spontaneous emission is shown below: 1033: 1006: 562: 474: 200: 157: 4210: 2150: 1718:. After one lifetime, the number of excited states decays to 36.8% of its original value ( 1618: 1309: 1247: 806: 8: 3571: 3566: 3554: 2913: 2851: 2449:. The theory of the spontaneous emission under the QED framework was first calculated by 1902: 1273: 1030:, it may spontaneously decay to a lower lying level (e.g., the ground state) with energy 944: 924: 661: 469: 387: 215: 195: 147: 4083: 3865: 3822: 3787: 3737: 2262: 4134: 4054: 4042: 3834: 3663: 3541:
in semiconductors. Large nonradiative transitions do not occur frequently because the
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in his quantum theory of radiation, the precursor to the theory which he later called
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In the rate-equation above, it is assumed that decay of the number of excited states
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directions in which the photon can be emitted. Equivalently, one might say that the
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The rate of spontaneous emission (i.e., the radiative rate) can be described by
3979:"Berechnung der natĂĽrlichen Linienbreite auf Grund der Diracschen Lichttheorie" 3809:
Weisskopf, Viktor (1935). "Probleme der neueren Quantentheorie des Elektrons".
3596: 3361:{\displaystyle \Gamma _{\text{tot}}=\Gamma _{\text{rad}}+\Gamma _{\text{nrad}}} 2961: 995:(CQED), the study of effects of mirrors and cavities on radiative corrections. 967: 781: 741: 721: 691: 671: 621: 587: 437: 427: 220: 4068: 962:. Einstein's quantum theory of radiation anticipated ideas later expressed in 958:
in a series of papers starting in 1916, culminating in what is now called the
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is the radiative decay rate of the transition. The number of excited states
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Spontaneous transitions were not explainable within the framework of the
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start via spontaneous emission, then during continuous operation work by
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Detail calculation of the Spontaneous Emission: Weisskopf-Wigner Theory
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form a very important feature that is exploited in the construction of
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In quantum electrodynamics (or QED), the electromagnetic field has a
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If a light source ('the atom') is in an excited state with energy
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In contrast with atoms, which have a discrete emission spectrum,
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is the initial number of light sources in the excited state,
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Stenholm, Stig Torsten; Suominen, Kalle-Antti (1998-04-27).
1858:{\displaystyle A_{21}=\Gamma _{21}={\frac {1}{\tau _{21}}}.} 1286:
If the number of light sources in the excited state at time
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Spontaneous emission and laser oscillation in microcavities
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Einstein and the Quantum: The Quest of the Valiant Swabian
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stands for the definition of the transition dipole moment
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is the rate of spontaneous emission. In the rate-equation
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Radiative and nonradiative decay: the quantum efficiency
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are the ground state atom with a single photon (of mode
4123:"P. A. M. Dirac and the discovery of quantum mechanics" 939:. Figurines that glow in the dark are phosphorescent. 3525:
In nonradiative relaxation, the energy is released as
4084:"Weisskopf-Wigner decay of excited oscillator states" 3461: 3431: 3404: 3377: 3321: 3312:, radiative and nonradiative rates should be summed: 3291: 3270: 3235: 3201: 3178: 3158: 3125: 3048: 2994: 2970: 2946: 2922: 2891: 2860: 2836: 2816: 2689: 2483: 2401: 2381: 2361: 2315: 2288: 2265: 2226: 2182: 2153: 2119: 1927: 1808: 1778: 1751: 1724: 1700: 1670: 1650: 1621: 1507: 1471: 1444: 1364: 1341: 1312: 1292: 1250: 1226: 1194: 1170: 1115: 1089: 1066: 1036: 1009: 41: 4022:Advances In Atomic, Molecular, and Optical Physics 3514: 3444: 3417: 3390: 3360: 3304: 3276: 3248: 3214: 3186: 3164: 3144: 3111: 3035:{\displaystyle |\langle 1|\mathbf {r} |2\rangle |} 3034: 2976: 2952: 2928: 2904: 2873: 2842: 2822: 2799: 2672: 2433: 2387: 2367: 2347: 2301: 2274: 2251: 2212: 2168: 2139: 2102: 1857: 1791: 1764: 1737: 1706: 1686: 1656: 1636: 1604: 1484: 1457: 1427: 1347: 1327: 1298: 1256: 1232: 1212: 1176: 1153: 1098: 1072: 1049: 1022: 102: 2355:is the frequency of the photon. The sum is over 1676: 1586: 4217: 4081: 3950:Marian O Scully & M. Suhail Zubairy (1997). 1901:Spontaneous emission in free space depends upon 1714:thus decays exponentially with time, similar to 3976: 2461: 3886: 3689:(First ed.). Princeton University Press. 2282:) wavefunction and its probability amplitude, 869: 3101: 3077: 3024: 3000: 2782: 2758: 2637: 2613: 2207: 2134: 2097: 2003: 1945: 950:Spontaneous emission cannot be explained by 97: 71: 982:of the electromagnetic field. In 1963, the 4015: 3923:Hiroyuki Yokoyama & Ujihara K (1995). 3145:{\displaystyle \mathbf {d} =q\mathbf {r} } 1772:is inversely proportional to the lifetime 1154:{\displaystyle E_{2}-E_{1}=\hbar \omega ,} 876: 862: 4138: 4120: 4058: 3916: 3808: 3759: 3757: 3745: 3667: 3661: 986:was developed describing the system of a 4211:Britney's Guide to Semiconductor Physics 3977:Weisskopf, V.; Wigner, E. (1930-01-01). 3655: 3630: 3557:can be used to boost an optical signal. 2309:is the atomic transition frequency, and 1687:{\displaystyle \Gamma _{\!{\text{rad}}}} 3943: 3763: 3715: 3713: 4218: 3851: 3754: 3719: 3682: 3445:{\displaystyle \Gamma _{\text{nrad}}} 3929:. Boca Raton: CRC Press. p. 6. 3710: 3683:Stone, A. Douglas (6 October 2013). 3676: 3418:{\displaystyle \Gamma _{\text{rad}}} 3391:{\displaystyle \Gamma _{\text{tot}}} 3305:{\displaystyle \Gamma _{\text{tot}}} 1765:{\displaystyle \Gamma _{\text{rad}}} 3720:Dirac, Paul Adrien Maurice (1927). 1213:{\displaystyle \hbar \omega =h\nu } 911:to a lower energy state (e.g., its 13: 3624: 3497: 3484: 3473: 3433: 3406: 3379: 3349: 3336: 3323: 3293: 2485: 1823: 1753: 1672: 1582: 1385: 1368: 408:Sum-over-histories (path integral) 94: 68: 24:Part of a series of articles about 14: 4252: 4192: 2735: 2567: 2213:{\displaystyle |g;1_{ks}\rangle } 1745:-time). The radiative decay rate 1142: 45: 3425:is the radiative decay rate and 3180: 3138: 3127: 3089: 3012: 2905:{\displaystyle \varepsilon _{0}} 2770: 2625: 2348:{\displaystyle \omega _{k}=c|k|} 1279: 952:classical electromagnetic theory 4172: 4163: 4114: 4075: 4034: 4009: 3970: 3631:Tretkoff, Ernie (August 2005). 998: 16:Quantum mechanical state change 4121:Gottfried, Kurt (2011-03-01). 3907: 3880: 3845: 3802: 3637:American Physical Society News 3105: 3094: 3084: 3073: 3065: 3050: 3028: 3017: 3007: 2996: 2787: 2775: 2765: 2754: 2710: 2694: 2642: 2630: 2620: 2609: 2539: 2523: 2500: 2494: 2443:Cavity quantum electrodynamics 2421: 2416: 2410: 2403: 2341: 2333: 2246: 2240: 2184: 2163: 2157: 2121: 2074: 2044: 2038: 1990: 1960: 1954: 1942: 1936: 1929: 1738:{\displaystyle {\frac {1}{e}}} 1631: 1625: 1570: 1564: 1532: 1526: 1517: 1511: 1419: 1413: 1380: 1374: 1322: 1316: 993:cavity quantum electrodynamics 558:Relativistic quantum mechanics 90: 83: 64: 1: 3617: 3172:is the elementary charge and 1099:{\displaystyle \hbar \omega } 598:Quantum statistical mechanics 3187:{\displaystyle \mathbf {r} } 2462:Rate of spontaneous emission 2140:{\displaystyle |e;0\rangle } 7: 4127:American Journal of Physics 3769:"Why spontaneous emission?" 3560: 3249:{\displaystyle \omega ^{3}} 3215:{\displaystyle \omega ^{3}} 3119:for dipole moment operator 2830:is the emission frequency, 2302:{\displaystyle \omega _{0}} 568:Quantum information science 10: 4257: 2434:{\displaystyle |b(t)|^{2}} 1792:{\displaystyle \tau _{21}} 891:is the process in which a 4236:Electromagnetic radiation 4069:10.22331/q-2021-06-10-474 3529:, more commonly known as 3398:is the total decay rate, 2874:{\displaystyle \mu _{12}} 2252:{\displaystyle b_{ks}(t)} 1868: 2883:transition dipole moment 603:Quantum machine learning 356:Wheeler's delayed-choice 3889:Proceedings of the IEEE 3874:10.1103/PhysRev.74.1157 3607:Vacuum Rabi oscillation 2986:fine-structure constant 2977:{\displaystyle \alpha } 2938:reduced Planck constant 2823:{\displaystyle \omega } 1883:quantum electrodynamics 1186:reduced Planck constant 1073:{\displaystyle \omega } 976:quantum electrodynamics 964:quantum electrodynamics 313:Leggett–Garg inequality 3983:Zeitschrift fĂĽr Physik 3901:10.1109/PROC.1963.1664 3747:10.1098/rspa.1927.0039 3516: 3446: 3419: 3392: 3362: 3306: 3278: 3250: 3216: 3188: 3166: 3146: 3113: 3036: 2978: 2954: 2930: 2929:{\displaystyle \hbar } 2906: 2875: 2844: 2824: 2801: 2674: 2435: 2389: 2369: 2349: 2303: 2276: 2253: 2214: 2170: 2141: 2104: 1859: 1793: 1766: 1739: 1708: 1688: 1658: 1638: 1606: 1495:Einstein A coefficient 1486: 1485:{\displaystyle A_{21}} 1459: 1458:{\displaystyle A_{21}} 1429: 1349: 1329: 1300: 1258: 1234: 1214: 1178: 1177:{\displaystyle \hbar } 1155: 1100: 1074: 1051: 1024: 960:Einstein A Coefficient 104: 3612:Jaynes–Cummings model 3517: 3447: 3420: 3393: 3363: 3307: 3279: 3251: 3217: 3189: 3167: 3147: 3114: 3037: 2979: 2955: 2931: 2907: 2876: 2845: 2825: 2802: 2675: 2436: 2390: 2370: 2350: 2304: 2277: 2254: 2215: 2171: 2142: 2105: 1860: 1794: 1767: 1740: 1709: 1689: 1659: 1639: 1607: 1487: 1460: 1430: 1350: 1330: 1301: 1259: 1235: 1215: 1179: 1156: 1101: 1075: 1052: 1050:{\displaystyle E_{1}} 1025: 1023:{\displaystyle E_{2}} 984:Jaynes–Cummings model 298:Elitzur–Vaidman 288:Davisson–Germer 105: 3587:Atomic spectral line 3459: 3429: 3402: 3375: 3319: 3289: 3268: 3233: 3199: 3176: 3156: 3123: 3046: 2992: 2968: 2944: 2920: 2889: 2858: 2834: 2814: 2687: 2481: 2399: 2379: 2359: 2313: 2286: 2263: 2224: 2180: 2169:{\displaystyle a(t)} 2151: 2117: 1925: 1879:quantum field theory 1875:Schrödinger equation 1806: 1776: 1749: 1722: 1698: 1668: 1648: 1637:{\displaystyle N(0)} 1619: 1505: 1469: 1442: 1362: 1339: 1335:, the rate at which 1328:{\displaystyle N(t)} 1310: 1290: 1257:{\displaystyle \nu } 1248: 1224: 1192: 1168: 1113: 1087: 1064: 1034: 1007: 909:excited energy state 889:Spontaneous emission 563:Quantum field theory 475:Consistent histories 112:Schrödinger equation 39: 4100:10.1364/OE.2.000378 3866:1948PhRv...74.1157W 3823:1935NW.....23..631W 3811:Naturwissenschaften 3788:1984AmJPh..52..340M 3738:1927RSPSA.114..243D 3572:Stimulated emission 3567:Absorption (optics) 3555:stimulated emission 2914:vacuum permittivity 2852:index of refraction 2468:Fermi's golden rule 1903:vacuum fluctuations 1274:stimulated emission 945:stimulated emission 925:electroluminescence 907:) transits from an 351:Stern–Gerlach 148:Classical mechanics 4226:Physical phenomena 4204:2016-03-04 at the 3995:10.1007/BF01336768 3831:10.1007/BF01492012 3547:Meta-stable states 3512: 3442: 3415: 3388: 3358: 3302: 3274: 3246: 3212: 3184: 3162: 3142: 3109: 3032: 2974: 2950: 2926: 2902: 2871: 2840: 2820: 2797: 2670: 2431: 2385: 2365: 2345: 2299: 2275:{\displaystyle ks} 2272: 2249: 2210: 2166: 2137: 2100: 2024: 1855: 1789: 1762: 1735: 1704: 1684: 1654: 1634: 1602: 1482: 1455: 1425: 1345: 1325: 1296: 1254: 1230: 1210: 1174: 1151: 1096: 1070: 1047: 1020: 905:subatomic particle 895:system (such as a 893:quantum mechanical 539:Von Neumann–Wigner 519:Objective-collapse 318:Mach–Zehnder 308:Leggett inequality 303:Franck–Hertz 153:Old quantum theory 100: 4149:10.1119/1.3536639 3765:Milonni, Peter W. 3577:Emission spectrum 3543:crystal structure 3507: 3503: 3490: 3479: 3465: 3439: 3412: 3385: 3355: 3342: 3329: 3299: 3277:{\displaystyle N} 3165:{\displaystyle q} 2988:. The expression 2953:{\displaystyle c} 2843:{\displaystyle n} 2742: 2668: 2581: 2491: 2388:{\displaystyle s} 2368:{\displaystyle k} 2009: 1850: 1759: 1733: 1716:radioactive decay 1707:{\displaystyle N} 1680: 1657:{\displaystyle t} 1590: 1392: 1348:{\displaystyle N} 1299:{\displaystyle t} 1233:{\displaystyle h} 1059:angular frequency 980:zero-point energy 929:chemiluminescence 886: 885: 593:Scattering theory 573:Quantum computing 346:Schrödinger's cat 278:Bell's inequality 86: 61: 30:Quantum mechanics 4248: 4183: 4176: 4170: 4167: 4161: 4160: 4142: 4118: 4112: 4111: 4079: 4073: 4072: 4062: 4038: 4032: 4031: 4030: 4029: 4013: 4007: 4006: 3974: 3968: 3967: 3947: 3941: 3940: 3920: 3914: 3911: 3905: 3904: 3884: 3878: 3877: 3849: 3843: 3842: 3806: 3800: 3799: 3773: 3761: 3752: 3751: 3749: 3732:(767): 243–265. 3717: 3708: 3707: 3705: 3703: 3680: 3674: 3673: 3671: 3659: 3653: 3652: 3650: 3648: 3628: 3602:Photonic crystal 3521: 3519: 3518: 3513: 3508: 3506: 3505: 3504: 3501: 3492: 3491: 3488: 3481: 3480: 3477: 3471: 3466: 3463: 3451: 3449: 3448: 3443: 3441: 3440: 3437: 3424: 3422: 3421: 3416: 3414: 3413: 3410: 3397: 3395: 3394: 3389: 3387: 3386: 3383: 3367: 3365: 3364: 3359: 3357: 3356: 3353: 3344: 3343: 3340: 3331: 3330: 3327: 3311: 3309: 3308: 3303: 3301: 3300: 3297: 3283: 3281: 3280: 3275: 3255: 3253: 3252: 3247: 3245: 3244: 3221: 3219: 3218: 3213: 3211: 3210: 3193: 3191: 3190: 3185: 3183: 3171: 3169: 3168: 3163: 3151: 3149: 3148: 3143: 3141: 3130: 3118: 3116: 3115: 3110: 3108: 3097: 3092: 3087: 3076: 3068: 3063: 3062: 3053: 3041: 3039: 3038: 3033: 3031: 3020: 3015: 3010: 2999: 2983: 2981: 2980: 2975: 2959: 2957: 2956: 2951: 2935: 2933: 2932: 2927: 2911: 2909: 2908: 2903: 2901: 2900: 2880: 2878: 2877: 2872: 2870: 2869: 2849: 2847: 2846: 2841: 2829: 2827: 2826: 2821: 2806: 2804: 2803: 2798: 2796: 2795: 2790: 2778: 2773: 2768: 2757: 2743: 2741: 2734: 2733: 2720: 2719: 2718: 2713: 2707: 2706: 2697: 2691: 2679: 2677: 2676: 2671: 2669: 2667: 2666: 2665: 2652: 2651: 2650: 2645: 2633: 2628: 2623: 2612: 2604: 2603: 2587: 2582: 2580: 2579: 2578: 2566: 2565: 2549: 2548: 2547: 2542: 2536: 2535: 2526: 2518: 2517: 2507: 2493: 2492: 2489: 2451:Victor Weisskopf 2440: 2438: 2437: 2432: 2430: 2429: 2424: 2406: 2394: 2392: 2391: 2386: 2374: 2372: 2371: 2366: 2354: 2352: 2351: 2346: 2344: 2336: 2325: 2324: 2308: 2306: 2305: 2300: 2298: 2297: 2281: 2279: 2278: 2273: 2258: 2256: 2255: 2250: 2239: 2238: 2219: 2217: 2216: 2211: 2206: 2205: 2187: 2175: 2173: 2172: 2167: 2146: 2144: 2143: 2138: 2124: 2109: 2107: 2106: 2101: 2096: 2095: 2077: 2072: 2071: 2067: 2066: 2037: 2036: 2023: 1993: 1988: 1987: 1983: 1982: 1932: 1905:to get started. 1864: 1862: 1861: 1856: 1851: 1849: 1848: 1836: 1831: 1830: 1818: 1817: 1798: 1796: 1795: 1790: 1788: 1787: 1771: 1769: 1768: 1763: 1761: 1760: 1757: 1744: 1742: 1741: 1736: 1734: 1726: 1713: 1711: 1710: 1705: 1693: 1691: 1690: 1685: 1683: 1682: 1681: 1678: 1664:is the time and 1663: 1661: 1660: 1655: 1643: 1641: 1640: 1635: 1611: 1609: 1608: 1603: 1598: 1597: 1593: 1592: 1591: 1588: 1557: 1556: 1552: 1551: 1491: 1489: 1488: 1483: 1481: 1480: 1464: 1462: 1461: 1456: 1454: 1453: 1434: 1432: 1431: 1426: 1409: 1408: 1393: 1391: 1383: 1366: 1354: 1352: 1351: 1346: 1334: 1332: 1331: 1326: 1305: 1303: 1302: 1297: 1283: 1263: 1261: 1260: 1255: 1239: 1237: 1236: 1231: 1219: 1217: 1216: 1211: 1183: 1181: 1180: 1175: 1160: 1158: 1157: 1152: 1138: 1137: 1125: 1124: 1105: 1103: 1102: 1097: 1079: 1077: 1076: 1071: 1056: 1054: 1053: 1048: 1046: 1045: 1029: 1027: 1026: 1021: 1019: 1018: 878: 871: 864: 505:Superdeterminism 158:Bra–ket notation 109: 107: 106: 101: 93: 88: 87: 79: 67: 62: 60: 49: 21: 20: 4256: 4255: 4251: 4250: 4249: 4247: 4246: 4245: 4241:Charge carriers 4216: 4215: 4206:Wayback Machine 4195: 4189: 4187: 4186: 4177: 4173: 4168: 4164: 4119: 4115: 4080: 4076: 4039: 4035: 4027: 4025: 4014: 4010: 3975: 3971: 3964: 3948: 3944: 3937: 3921: 3917: 3912: 3908: 3885: 3881: 3850: 3846: 3817:(37): 631–637. 3807: 3803: 3796:10.1119/1.13886 3771: 3762: 3755: 3718: 3711: 3701: 3699: 3697: 3681: 3677: 3660: 3656: 3646: 3644: 3629: 3625: 3620: 3563: 3500: 3496: 3487: 3483: 3482: 3476: 3472: 3470: 3462: 3460: 3457: 3456: 3436: 3432: 3430: 3427: 3426: 3409: 3405: 3403: 3400: 3399: 3382: 3378: 3376: 3373: 3372: 3352: 3348: 3339: 3335: 3326: 3322: 3320: 3317: 3316: 3296: 3292: 3290: 3287: 3286: 3269: 3266: 3265: 3262: 3240: 3236: 3234: 3231: 3230: 3206: 3202: 3200: 3197: 3196: 3179: 3177: 3174: 3173: 3157: 3154: 3153: 3137: 3126: 3124: 3121: 3120: 3104: 3093: 3088: 3083: 3072: 3064: 3058: 3054: 3049: 3047: 3044: 3043: 3027: 3016: 3011: 3006: 2995: 2993: 2990: 2989: 2969: 2966: 2965: 2945: 2942: 2941: 2921: 2918: 2917: 2896: 2892: 2890: 2887: 2886: 2865: 2861: 2859: 2856: 2855: 2835: 2832: 2831: 2815: 2812: 2811: 2791: 2786: 2785: 2774: 2769: 2764: 2753: 2729: 2725: 2721: 2714: 2709: 2708: 2702: 2698: 2693: 2692: 2690: 2688: 2685: 2684: 2661: 2657: 2653: 2646: 2641: 2640: 2629: 2624: 2619: 2608: 2599: 2595: 2588: 2586: 2574: 2570: 2561: 2557: 2550: 2543: 2538: 2537: 2531: 2527: 2522: 2513: 2509: 2508: 2506: 2488: 2484: 2482: 2479: 2478: 2464: 2447:Quantum revival 2425: 2420: 2419: 2402: 2400: 2397: 2396: 2380: 2377: 2376: 2360: 2357: 2356: 2340: 2332: 2320: 2316: 2314: 2311: 2310: 2293: 2289: 2287: 2284: 2283: 2264: 2261: 2260: 2231: 2227: 2225: 2222: 2221: 2198: 2194: 2183: 2181: 2178: 2177: 2152: 2149: 2148: 2120: 2118: 2115: 2114: 2088: 2084: 2073: 2062: 2058: 2051: 2047: 2029: 2025: 2013: 1989: 1978: 1974: 1967: 1963: 1928: 1926: 1923: 1922: 1871: 1844: 1840: 1835: 1826: 1822: 1813: 1809: 1807: 1804: 1803: 1783: 1779: 1777: 1774: 1773: 1756: 1752: 1750: 1747: 1746: 1725: 1723: 1720: 1719: 1699: 1696: 1695: 1677: 1675: 1671: 1669: 1666: 1665: 1649: 1646: 1645: 1620: 1617: 1616: 1587: 1585: 1581: 1577: 1573: 1547: 1543: 1539: 1535: 1506: 1503: 1502: 1476: 1472: 1470: 1467: 1466: 1449: 1445: 1443: 1440: 1439: 1404: 1400: 1384: 1367: 1365: 1363: 1360: 1359: 1340: 1337: 1336: 1311: 1308: 1307: 1291: 1288: 1287: 1249: 1246: 1245: 1242:Planck constant 1225: 1222: 1221: 1193: 1190: 1189: 1169: 1166: 1165: 1133: 1129: 1120: 1116: 1114: 1111: 1110: 1088: 1085: 1084: 1065: 1062: 1061: 1041: 1037: 1035: 1032: 1031: 1014: 1010: 1008: 1005: 1004: 1001: 956:Albert Einstein 937:phosphorescence 882: 853: 852: 851: 616: 608: 607: 553: 552:Advanced topics 545: 544: 543: 495:Hidden-variable 485:de Broglie–Bohm 464: 462:Interpretations 454: 453: 452: 422: 414: 413: 412: 370: 362: 361: 360: 327: 283:CHSH inequality 272: 264: 263: 262: 191:Complementarity 185: 177: 176: 175: 143: 114: 89: 78: 77: 63: 53: 48: 40: 37: 36: 17: 12: 11: 5: 4254: 4244: 4243: 4238: 4233: 4228: 4214: 4213: 4208: 4194: 4193:External links 4191: 4185: 4184: 4171: 4162: 4133:(3): 261–266. 4113: 4088:Optics Express 4074: 4033: 4008: 3969: 3962: 3953:Quantum optics 3942: 3935: 3915: 3906: 3879: 3844: 3801: 3753: 3709: 3696:978-0691139685 3695: 3675: 3654: 3622: 3621: 3619: 3616: 3615: 3614: 3609: 3604: 3599: 3597:Purcell effect 3594: 3589: 3584: 3579: 3574: 3569: 3562: 3559: 3535:semiconductors 3523: 3522: 3511: 3499: 3495: 3486: 3475: 3469: 3435: 3408: 3381: 3369: 3368: 3351: 3347: 3338: 3334: 3325: 3295: 3273: 3261: 3258: 3243: 3239: 3209: 3205: 3182: 3161: 3140: 3136: 3133: 3129: 3107: 3103: 3100: 3096: 3091: 3086: 3082: 3079: 3075: 3071: 3067: 3061: 3057: 3052: 3030: 3026: 3023: 3019: 3014: 3009: 3005: 3002: 2998: 2973: 2962:speed of light 2960:is the vacuum 2949: 2925: 2899: 2895: 2868: 2864: 2839: 2819: 2808: 2807: 2794: 2789: 2784: 2781: 2777: 2772: 2767: 2763: 2760: 2756: 2752: 2749: 2746: 2740: 2737: 2732: 2728: 2724: 2717: 2712: 2705: 2701: 2696: 2681: 2680: 2664: 2660: 2656: 2649: 2644: 2639: 2636: 2632: 2627: 2622: 2618: 2615: 2611: 2607: 2602: 2598: 2594: 2591: 2585: 2577: 2573: 2569: 2564: 2560: 2556: 2553: 2546: 2541: 2534: 2530: 2525: 2521: 2516: 2512: 2505: 2502: 2499: 2496: 2487: 2463: 2460: 2428: 2423: 2418: 2415: 2412: 2409: 2405: 2384: 2364: 2343: 2339: 2335: 2331: 2328: 2323: 2319: 2296: 2292: 2271: 2268: 2248: 2245: 2242: 2237: 2234: 2230: 2209: 2204: 2201: 2197: 2193: 2190: 2186: 2165: 2162: 2159: 2156: 2136: 2133: 2130: 2127: 2123: 2111: 2110: 2099: 2094: 2091: 2087: 2083: 2080: 2076: 2070: 2065: 2061: 2057: 2054: 2050: 2046: 2043: 2040: 2035: 2032: 2028: 2022: 2019: 2016: 2012: 2008: 2005: 2002: 1999: 1996: 1992: 1986: 1981: 1977: 1973: 1970: 1966: 1962: 1959: 1956: 1953: 1950: 1947: 1944: 1941: 1938: 1935: 1931: 1870: 1867: 1866: 1865: 1854: 1847: 1843: 1839: 1834: 1829: 1825: 1821: 1816: 1812: 1786: 1782: 1755: 1732: 1729: 1703: 1674: 1653: 1633: 1630: 1627: 1624: 1613: 1612: 1601: 1596: 1584: 1580: 1576: 1572: 1569: 1566: 1563: 1560: 1555: 1550: 1546: 1542: 1538: 1534: 1531: 1528: 1525: 1522: 1519: 1516: 1513: 1510: 1479: 1475: 1452: 1448: 1436: 1435: 1424: 1421: 1418: 1415: 1412: 1407: 1403: 1399: 1396: 1390: 1387: 1382: 1379: 1376: 1373: 1370: 1344: 1324: 1321: 1318: 1315: 1295: 1264:is the linear 1253: 1229: 1209: 1206: 1203: 1200: 1197: 1173: 1162: 1161: 1150: 1147: 1144: 1141: 1136: 1132: 1128: 1123: 1119: 1095: 1092: 1069: 1044: 1040: 1017: 1013: 1000: 997: 988:two-level atom 968:quantum optics 884: 883: 881: 880: 873: 866: 858: 855: 854: 850: 849: 844: 839: 834: 829: 824: 819: 814: 809: 804: 799: 794: 789: 784: 779: 774: 769: 764: 759: 754: 749: 744: 739: 734: 729: 724: 719: 714: 709: 704: 699: 694: 689: 684: 679: 674: 669: 664: 659: 654: 649: 644: 639: 634: 629: 624: 618: 617: 614: 613: 610: 609: 606: 605: 600: 595: 590: 588:Density matrix 585: 580: 575: 570: 565: 560: 554: 551: 550: 547: 546: 542: 541: 536: 531: 526: 521: 516: 511: 510: 509: 508: 507: 492: 487: 482: 477: 472: 466: 465: 460: 459: 456: 455: 451: 450: 445: 440: 435: 430: 424: 423: 420: 419: 416: 415: 411: 410: 405: 400: 395: 390: 385: 379: 378: 377: 371: 368: 367: 364: 363: 359: 358: 353: 348: 342: 341: 340: 339: 338: 336:Delayed-choice 331:Quantum eraser 326: 325: 320: 315: 310: 305: 300: 295: 290: 285: 280: 274: 273: 270: 269: 266: 265: 261: 260: 259: 258: 248: 243: 238: 233: 228: 223: 221:Quantum number 218: 213: 208: 203: 198: 193: 187: 186: 183: 182: 179: 178: 174: 173: 168: 162: 161: 160: 155: 150: 144: 141: 140: 137: 136: 135: 134: 129: 124: 116: 115: 110: 99: 96: 92: 85: 82: 76: 73: 70: 66: 59: 56: 52: 47: 44: 33: 32: 26: 25: 15: 9: 6: 4: 3: 2: 4253: 4242: 4239: 4237: 4234: 4232: 4231:Laser science 4229: 4227: 4224: 4223: 4221: 4212: 4209: 4207: 4203: 4200: 4197: 4196: 4190: 4182: 4175: 4166: 4158: 4154: 4150: 4146: 4141: 4136: 4132: 4128: 4124: 4117: 4109: 4105: 4101: 4097: 4093: 4089: 4085: 4078: 4070: 4066: 4061: 4056: 4052: 4048: 4044: 4037: 4023: 4019: 4012: 4004: 4000: 3996: 3992: 3988: 3985:(in German). 3984: 3980: 3973: 3965: 3963:0-521-43595-1 3959: 3955: 3954: 3946: 3938: 3936:0-8493-3786-0 3932: 3928: 3927: 3919: 3910: 3902: 3898: 3895:(1): 89–109. 3894: 3890: 3883: 3875: 3871: 3867: 3863: 3859: 3855: 3848: 3840: 3836: 3832: 3828: 3824: 3820: 3816: 3812: 3805: 3797: 3793: 3789: 3785: 3781: 3777: 3770: 3766: 3760: 3758: 3748: 3743: 3739: 3735: 3731: 3727: 3723: 3716: 3714: 3698: 3692: 3688: 3687: 3679: 3670: 3665: 3658: 3642: 3638: 3634: 3627: 3623: 3613: 3610: 3608: 3605: 3603: 3600: 3598: 3595: 3593: 3592:Laser science 3590: 3588: 3585: 3583: 3582:Spectral line 3580: 3578: 3575: 3573: 3570: 3568: 3565: 3564: 3558: 3556: 3552: 3548: 3544: 3540: 3536: 3532: 3528: 3509: 3493: 3467: 3455: 3454: 3453: 3345: 3332: 3315: 3314: 3313: 3271: 3257: 3241: 3237: 3228: 3223: 3207: 3203: 3159: 3134: 3131: 3098: 3080: 3069: 3059: 3055: 3021: 3003: 2987: 2971: 2963: 2947: 2939: 2923: 2915: 2897: 2893: 2884: 2866: 2862: 2853: 2837: 2817: 2792: 2779: 2761: 2750: 2747: 2744: 2738: 2730: 2726: 2722: 2715: 2703: 2699: 2683: 2682: 2662: 2658: 2654: 2647: 2634: 2616: 2605: 2600: 2596: 2592: 2589: 2583: 2575: 2571: 2562: 2558: 2554: 2551: 2544: 2532: 2528: 2519: 2514: 2510: 2503: 2497: 2477: 2476: 2475: 2473: 2469: 2459: 2456: 2455:Eugene Wigner 2452: 2448: 2444: 2426: 2413: 2407: 2382: 2362: 2337: 2329: 2326: 2321: 2317: 2294: 2290: 2269: 2266: 2243: 2235: 2232: 2228: 2202: 2199: 2195: 2191: 2188: 2160: 2154: 2131: 2128: 2125: 2092: 2089: 2085: 2081: 2078: 2068: 2063: 2059: 2055: 2052: 2048: 2041: 2033: 2030: 2026: 2020: 2017: 2014: 2010: 2006: 2000: 1997: 1994: 1984: 1979: 1975: 1971: 1968: 1964: 1957: 1951: 1948: 1939: 1933: 1921: 1920: 1919: 1915: 1912: 1906: 1904: 1899: 1895: 1891: 1886: 1884: 1880: 1876: 1852: 1845: 1841: 1837: 1832: 1827: 1819: 1814: 1810: 1802: 1801: 1800: 1784: 1780: 1730: 1727: 1717: 1701: 1651: 1628: 1622: 1599: 1594: 1578: 1574: 1567: 1561: 1558: 1553: 1548: 1544: 1540: 1536: 1529: 1523: 1520: 1514: 1508: 1501: 1500: 1499: 1497: 1496: 1477: 1473: 1450: 1446: 1422: 1416: 1410: 1405: 1401: 1397: 1394: 1388: 1377: 1371: 1358: 1357: 1356: 1342: 1319: 1313: 1293: 1284: 1282: 1277: 1275: 1271: 1267: 1251: 1243: 1227: 1207: 1204: 1201: 1198: 1195: 1187: 1171: 1148: 1145: 1139: 1134: 1130: 1126: 1121: 1117: 1109: 1108: 1107: 1093: 1090: 1083: 1067: 1060: 1042: 1038: 1015: 1011: 996: 994: 989: 985: 981: 977: 973: 969: 965: 961: 957: 953: 948: 946: 942: 938: 934: 930: 926: 922: 918: 914: 910: 906: 902: 898: 894: 890: 879: 874: 872: 867: 865: 860: 859: 857: 856: 848: 845: 843: 840: 838: 835: 833: 830: 828: 825: 823: 820: 818: 815: 813: 810: 808: 805: 803: 800: 798: 795: 793: 790: 788: 785: 783: 780: 778: 775: 773: 770: 768: 765: 763: 760: 758: 755: 753: 750: 748: 745: 743: 740: 738: 735: 733: 730: 728: 725: 723: 720: 718: 715: 713: 710: 708: 705: 703: 700: 698: 695: 693: 690: 688: 685: 683: 680: 678: 675: 673: 670: 668: 665: 663: 660: 658: 655: 653: 650: 648: 645: 643: 640: 638: 635: 633: 630: 628: 625: 623: 620: 619: 612: 611: 604: 601: 599: 596: 594: 591: 589: 586: 584: 581: 579: 578:Quantum chaos 576: 574: 571: 569: 566: 564: 561: 559: 556: 555: 549: 548: 540: 537: 535: 534:Transactional 532: 530: 527: 525: 524:Quantum logic 522: 520: 517: 515: 512: 506: 503: 502: 501: 498: 497: 496: 493: 491: 488: 486: 483: 481: 478: 476: 473: 471: 468: 467: 463: 458: 457: 449: 446: 444: 441: 439: 436: 434: 431: 429: 426: 425: 418: 417: 409: 406: 404: 401: 399: 396: 394: 391: 389: 386: 384: 381: 380: 376: 373: 372: 366: 365: 357: 354: 352: 349: 347: 344: 343: 337: 334: 333: 332: 329: 328: 324: 321: 319: 316: 314: 311: 309: 306: 304: 301: 299: 296: 294: 291: 289: 286: 284: 281: 279: 276: 275: 268: 267: 257: 254: 253: 252: 251:Wave function 249: 247: 244: 242: 239: 237: 234: 232: 231:Superposition 229: 227: 224: 222: 219: 217: 214: 212: 209: 207: 204: 202: 199: 197: 194: 192: 189: 188: 181: 180: 172: 169: 167: 164: 163: 159: 156: 154: 151: 149: 146: 145: 139: 138: 133: 130: 128: 125: 123: 120: 119: 118: 117: 113: 80: 74: 57: 54: 50: 42: 35: 34: 31: 28: 27: 23: 22: 19: 4188: 4174: 4165: 4130: 4126: 4116: 4091: 4087: 4077: 4050: 4046: 4036: 4026:, retrieved 4021: 4011: 3989:(1): 54–73. 3986: 3982: 3972: 3952: 3945: 3925: 3918: 3909: 3892: 3888: 3882: 3857: 3853: 3847: 3814: 3810: 3804: 3779: 3775: 3729: 3726:Proc. R. Soc 3725: 3700:. Retrieved 3685: 3678: 3657: 3645:. Retrieved 3640: 3636: 3626: 3524: 3370: 3263: 3227:quantum dots 3224: 2809: 2465: 2112: 1916: 1907: 1890:ground state 1887: 1872: 1614: 1493: 1437: 1306:is given by 1285: 1278: 1163: 1002: 999:Introduction 949: 933:fluorescence 921:luminescence 913:ground state 888: 887: 433:Klein–Gordon 369:Formulations 206:Energy level 201:Entanglement 184:Fundamentals 171:Interference 122:Introduction 18: 3860:(9): 1157. 3776:Am. J. Phys 1911:phase space 1355:decays is: 822:von Neumann 807:Schrödinger 583:EPR paradox 514:Many-worlds 448:Schrödinger 403:Schrödinger 398:Phase-space 388:Interaction 293:Double-slit 271:Experiments 246:Uncertainty 216:Nonlocality 211:Measurement 196:Decoherence 166:Hamiltonian 4220:Categories 4094:(9): 378. 4060:2001.09737 4028:2024-06-21 3782:(4): 340. 3669:1703.08176 3618:References 2472:free space 1898:eigenstate 1894:QED vacuum 817:Sommerfeld 732:Heisenberg 727:Gutzwiller 667:de Broglie 615:Scientists 529:Relational 480:Copenhagen 383:Heisenberg 241:Tunnelling 142:Background 4157:0002-9505 4140:1006.4610 4108:1094-4087 4003:0044-3328 3854:Phys. Rev 3498:Γ 3485:Γ 3474:Γ 3434:Γ 3407:Γ 3380:Γ 3350:Γ 3337:Γ 3324:Γ 3294:Γ 3238:ω 3204:ω 3102:⟩ 3078:⟨ 3056:μ 3025:⟩ 3001:⟨ 2972:α 2924:ℏ 2894:ε 2863:μ 2818:ω 2783:⟩ 2759:⟨ 2751:α 2736:ℏ 2727:ε 2723:π 2700:μ 2638:⟩ 2614:⟨ 2597:ω 2593:α 2568:ℏ 2559:ε 2555:π 2529:μ 2511:ω 2498:ω 2486:Γ 2318:ω 2291:ω 2208:⟩ 2135:⟩ 2098:⟩ 2060:ω 2053:− 2011:∑ 2004:⟩ 1976:ω 1969:− 1946:⟩ 1934:ψ 1842:τ 1824:Γ 1781:τ 1754:Γ 1673:Γ 1583:Γ 1579:− 1541:− 1398:− 1386:∂ 1369:∂ 1266:frequency 1252:ν 1208:ν 1199:ω 1196:ℏ 1188:. Note: 1172:ℏ 1146:ω 1143:ℏ 1127:− 1094:ω 1091:ℏ 1068:ω 847:Zeilinger 692:Ehrenfest 421:Equations 98:⟩ 95:Ψ 84:^ 72:⟩ 69:Ψ 46:ℏ 4202:Archived 3767:(1984). 3561:See also 3152:, where 1220:, where 1080:and an 897:molecule 772:Millikan 697:Einstein 682:Davisson 637:Blackett 622:Aharonov 490:Ensemble 470:Bayesian 375:Overview 256:Collapse 236:Symmetry 127:Glossary 4179:(2005). 4053:: 474. 4047:Quantum 3862:Bibcode 3839:6780937 3819:Bibcode 3784:Bibcode 3734:Bibcode 3539:bandgap 3527:phonons 2984:is the 2936:is the 2912:is the 2881:is the 2850:is the 1268:. The 1240:is the 1184:is the 812:Simmons 802:Rydberg 767:Moseley 747:Kramers 737:Hilbert 722:Glauber 717:Feynman 702:Everett 672:Compton 443:Rydberg 132:History 4155:  4106:  4001:  3960:  3933:  3837:  3702:1 June 3693:  3647:1 June 3551:lasers 3371:where 2964:, and 2810:where 2113:where 1892:, the 1869:Theory 1615:where 1438:where 1164:where 1082:energy 941:Lasers 917:photon 842:Zeeman 837:Wigner 787:Planck 757:Landau 742:Jordan 393:Matrix 323:Popper 4135:arXiv 4055:arXiv 3835:S2CID 3772:(PDF) 3664:arXiv 1270:phase 972:Dirac 903:or a 899:, an 797:Raman 782:Pauli 777:Onnes 712:Fermi 687:Debye 677:Dirac 642:Bloch 632:Bethe 500:Local 438:Pauli 428:Dirac 226:State 4153:ISSN 4104:ISSN 3999:ISSN 3958:ISBN 3931:ISBN 3730:A114 3704:2022 3691:ISBN 3649:2022 3531:heat 3489:nrad 3438:nrad 3354:nrad 2453:and 2375:and 2220:and 2147:and 1244:and 966:and 901:atom 832:Wien 827:Weyl 792:Rabi 762:Laue 752:Lamb 707:Fock 662:Bose 657:Born 652:Bohr 647:Bohm 627:Bell 4145:doi 4096:doi 4065:doi 3991:doi 3897:doi 3870:doi 3827:doi 3792:doi 3742:doi 3643:(8) 3502:rad 3478:rad 3411:rad 3384:tot 3341:rad 3328:tot 3298:tot 2490:rad 1758:rad 1679:rad 1589:rad 4222:: 4151:. 4143:. 4131:79 4129:. 4125:. 4102:. 4090:. 4086:. 4063:. 4049:. 4045:. 4020:, 3997:. 3987:63 3981:. 3893:51 3891:. 3868:. 3858:74 3856:. 3833:. 3825:. 3815:23 3813:. 3790:. 3780:52 3778:. 3774:. 3756:^ 3740:. 3728:. 3724:. 3712:^ 3641:14 3639:. 3635:. 3464:QE 3222:. 3060:12 2940:, 2916:, 2885:, 2867:12 2854:, 2704:12 2533:12 1885:. 1846:21 1828:21 1815:21 1799:: 1785:21 1549:21 1478:21 1451:21 1406:21 1106:: 947:. 927:, 4159:. 4147:: 4137:: 4110:. 4098:: 4092:2 4071:. 4067:: 4057:: 4051:5 4005:. 3993:: 3966:. 3939:. 3903:. 3899:: 3876:. 3872:: 3864:: 3841:. 3829:: 3821:: 3798:. 3794:: 3786:: 3750:. 3744:: 3736:: 3706:. 3672:. 3666:: 3651:. 3510:. 3494:+ 3468:= 3346:+ 3333:= 3272:N 3242:3 3208:3 3181:r 3160:q 3139:r 3135:q 3132:= 3128:d 3106:| 3099:2 3095:| 3090:d 3085:| 3081:1 3074:| 3070:= 3066:| 3051:| 3029:| 3022:2 3018:| 3013:r 3008:| 3004:1 2997:| 2948:c 2898:0 2838:n 2793:2 2788:| 2780:2 2776:| 2771:r 2766:| 2762:1 2755:| 2748:4 2745:= 2739:c 2731:0 2716:2 2711:| 2695:| 2663:2 2659:c 2655:3 2648:2 2643:| 2635:2 2631:| 2626:r 2621:| 2617:1 2610:| 2606:n 2601:3 2590:4 2584:= 2576:3 2572:c 2563:0 2552:3 2545:2 2540:| 2524:| 2520:n 2515:3 2504:= 2501:) 2495:( 2427:2 2422:| 2417:) 2414:t 2411:( 2408:b 2404:| 2383:s 2363:k 2342:| 2338:k 2334:| 2330:c 2327:= 2322:k 2295:0 2270:s 2267:k 2247:) 2244:t 2241:( 2236:s 2233:k 2229:b 2203:s 2200:k 2196:1 2192:; 2189:g 2185:| 2164:) 2161:t 2158:( 2155:a 2132:0 2129:; 2126:e 2122:| 2093:s 2090:k 2086:1 2082:; 2079:g 2075:| 2069:t 2064:k 2056:i 2049:e 2045:) 2042:t 2039:( 2034:s 2031:k 2027:b 2021:s 2018:, 2015:k 2007:+ 2001:0 1998:; 1995:e 1991:| 1985:t 1980:0 1972:i 1965:e 1961:) 1958:t 1955:( 1952:a 1949:= 1943:) 1940:t 1937:( 1930:| 1853:. 1838:1 1833:= 1820:= 1811:A 1731:e 1728:1 1702:N 1652:t 1632:) 1629:0 1626:( 1623:N 1600:, 1595:t 1575:e 1571:) 1568:0 1565:( 1562:N 1559:= 1554:t 1545:A 1537:e 1533:) 1530:0 1527:( 1524:N 1521:= 1518:) 1515:t 1512:( 1509:N 1474:A 1447:A 1423:, 1420:) 1417:t 1414:( 1411:N 1402:A 1395:= 1389:t 1381:) 1378:t 1375:( 1372:N 1343:N 1323:) 1320:t 1317:( 1314:N 1294:t 1228:h 1205:h 1202:= 1149:, 1140:= 1135:1 1131:E 1122:2 1118:E 1043:1 1039:E 1016:2 1012:E 877:e 870:t 863:v 91:| 81:H 75:= 65:| 58:t 55:d 51:d 43:i

Index

Quantum mechanics
Schrödinger equation
Introduction
Glossary
History
Classical mechanics
Old quantum theory
Bra–ket notation
Hamiltonian
Interference
Complementarity
Decoherence
Entanglement
Energy level
Measurement
Nonlocality
Quantum number
State
Superposition
Symmetry
Tunnelling
Uncertainty
Wave function
Collapse
Bell's inequality
CHSH inequality
Davisson–Germer
Double-slit
Elitzur–Vaidman
Franck–Hertz

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