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Gyromagnetic ratio

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3275: 1400: 2988: 3270:{\displaystyle \omega =2\pi \,f={\frac {1}{\,J\,\sin {\phi }\,}}\,\left|{\frac {\,{\rm {{d}\,\mathbf {J} \,}}}{\,{\rm {{d}\,t\,}}}}\right|={\frac {\,\left|\mathbf {T} \right|\,}{\,J\,\sin {\phi }\,}}={\frac {\,\left|\mathbf {m} \times \mathbf {B} \right|\,}{\,J\,\sin {\phi }\,}}={\frac {\,m\,B\sin {\phi }\,}{\,J\,\sin {\phi }\,}}={\frac {\,m\,B\,}{J}}=\gamma \,B~.} 106:
body rotating about an axis of symmetry. According to the laws of classical physics, it has both a magnetic dipole moment due to the movement of charge and an angular momentum due to the movement of mass arising from its rotation. It can be shown that as long as its charge and mass density and flow
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of a gyroscope. The earth's gravitational attraction applies a force or torque to the gyroscope in the vertical direction, and the angular momentum vector along the axis of the gyroscope rotates slowly about a vertical line through the pivot. In the place of the gyroscope imagine a sphere spinning
511: 1539: 373:. While an electron's spin is sometimes visualized as a literal rotation about an axis, it cannot be attributed to mass distributed identically to the charge. The above classical relation does not hold, giving the wrong result by the absolute value of the electron's 844: 943: 359: 2524: 392: 2604: 613: 1426:, which gives rise to a gyromagnetic ratio as above. The ratio is conventionally written in terms of the proton mass and charge, even for neutrons and for other nuclei, for the sake of simplicity and consistency. The formula is: 2874: 2335: 3334: 1670: 729: 722: 1432: 2740: 848: 1275: 2750:
around the axis and with its center on the pivot of the gyroscope, and along the axis of the gyroscope two oppositely directed vectors both originated in the center of the sphere, upwards
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The derivation of this relation is as follows. It suffices to demonstrate this for an infinitesimally narrow circular ring within the body, as the general result then follows from an
146: 2635: 1707: 1814: 1571: 2934: 2461: 3827: 2980: 2898: 2824: 2662: 2412: 535: 2795: 2770: 2684: 2434: 2374: 2290: 2268: 1768: 1604: 3401:, the resonance frequency of an ionized plasma being under the influence of a static finite magnetic field, when we superimpose a high frequency electromagnetic field. 2956: 2640:
The model of the spinning electron we use in the derivation has an evident analogy with a gyroscope. For any rotating body the rate of change of the angular momentum
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The identity of the functional form of the stationary electric and magnetic fields has led to defining the magnitude of the magnetic dipole moment equally well as
193: 171: 2529: 2830: 3458: 2295: 3453: 661: 506:{\displaystyle \gamma _{\mathrm {e} }={\frac {-e}{2m_{\mathrm {e} }}}\,|g_{\mathrm {e} }|={\frac {g_{\mathrm {e} }\mu _{\mathrm {B} }}{\hbar }}\,,} 3651: 3283: 1735:
Most common nuclei such as H and C have positive gyromagnetic ratios. Approximate values for some common nuclei are given in the table below.
1616: 1534:{\displaystyle \gamma _{\text{n}}={\frac {e}{\,2m_{\text{p}}\,}}\,g_{\rm {n}}=g_{\rm {n}}\,{\frac {\,\mu _{\mathrm {N} }\,}{\hbar }}~,} 1363: 100: 2692: 2248:
The derivation of this relation is as follows: First we must prove that the torque resulting from subjecting a magnetic moment
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puts a positive sign on the quantity; however, to be consistent with the formulas in this article, a negative sign is put on
1728:, which is simply the product of the gyromagnetic ratio with the magnetic field strength. With this phenomenon, the sign of 1407:, determines the sense of precession. While the magnetic moments (the black arrows) are oriented the same for both cases of 3691: 4152: 1068: 839:{\displaystyle \gamma _{\mathrm {e} }=\mathrm {-1.760\,859\,630\,23(53)\times 10^{11}\,rad{\cdot }s^{-1}{\cdot }T^{-1}} } 2382:
of an electric dipole: The magnetic dipole can be represented by a needle of a compass with fictitious magnetic charges
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Since a gyromagnetic factor equal to 2 follows from Dirac's equation, it is a frequent misconception to think that a
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2 is a consequence of relativity; it is not. The factor 2 can be obtained from the linearization of both the
938:{\displaystyle {\frac {\gamma _{\mathrm {e} }}{2\pi }}=\mathrm {-28\,024.951\,4242(85)\,MHz{\cdot }T^{-1}} .} 113: 3658:. PoincarĂ© Seminar. Progress in Mathematical Physics. Vol. 30. Paris, FR: BirkhĂ€user (published 2003). 2609: 1675: 3791: 1775: 1547: 2903: 3669: 2439: 1717: 1713: 3795: 2961: 2879: 2800: 2643: 3434: 2385: 1023: 981: 3471: 999:
of the minimal coupling and of the fact of having the same order of derivatives for space and time.
2775: 1411:, the precession is in opposite directions. Spin and magnetic moment are in the same direction for 655: 2753: 2667: 2417: 2340: 2273: 2251: 4147: 3881: 1746: 1580: 636: 977: 3914: 2939: 1308: 957: 354:{\displaystyle \mu =IA={\frac {qv}{2\pi r}}\,\pi r^{2}={\frac {q}{2m}}\,mvr={\frac {q}{2m}}L~.} 2519:{\displaystyle \,{\boldsymbol {\mathrm {T} }}=q_{\rm {m}}(\mathbf {d} \times \mathbf {B} )\,.} 529:
The gyromagnetic ratio due to electron spin is twice that due to the orbiting of an electron.
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factors of the spin 1/2 particles in the (1/2-1/2-1/2) triad of the four-vector spinor,
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This relationship also explains an apparent contradiction between the two equivalent terms,
4048:"Tritium Solid State NMR Spectroscopy at PNNL for Evaluation of Hydrogen Storage Materials" 3757: 3530: 3410: 3508: 8: 3396: 2599:{\displaystyle \,q_{\rm {m}}\mathbf {d} =I\pi r^{2}{\hat {\mathbf {d} }}=\mathbf {m} \,,} 2121:
Any free system with a constant gyromagnetic ratio, such as a rigid system of charges, a
176: 154: 4086: 4025: 3761: 3534: 608:{\displaystyle g_{\mathrm {e} }=-2\left(1+{\frac {\alpha }{\,2\pi \,}}+\cdots \right)~,} 3773: 3747: 3554: 3520: 1607: 989: 970: 374: 77: 3985: 3632: 1720:(MRI). These procedures rely on the fact that bulk magnetization due to nuclear spins 369:
An isolated electron has an angular momentum and a magnetic moment resulting from its
4064: 4003: 3947: 3918: 3907: 3885: 3856: 3777: 3701: 3659: 3558: 3546: 3463: 3371: 2869:{\displaystyle {\frac {\,\operatorname {d} \mathbf {J} \,}{\,\operatorname {d} t\,}}} 2116: 4126: 4109: 3967: 3420: 4121: 4110:"Explorations of Magnetic Properties of Noble Gases: The Past, Present, and Future" 3765: 3614: 3572: 3542: 3538: 3363: 1725: 1574: 107:
are distributed identically and rotationally symmetric, its gyromagnetic ratio is
40: 4157: 3697: 3429: 3347: 2330:{\displaystyle \,{\boldsymbol {\mathrm {T} }}=\mathbf {m} \times \mathbf {B} \,.} 2139: 103: 36: 3415: 3389: 3355: 2130: 2122: 1019: 370: 3769: 3724:
Delgado Acosta, E.G.; Banda GuzmĂĄn, V.M.; Kirchbach, M. (2015). "Gyromagnetic
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The angular precession frequency has an important physical meaning: It is the
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and the vertical. Hence the angular velocity of the rotation of the spin is
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Fan, X.; Myers, T. G.; Sukra, B. A. D.; Gabrielse, G. (13 February 2023).
964: 3329:{\displaystyle f={\frac {\gamma }{\,2\pi \,}}\,B~.\quad {\text{q.e.d.}}} 3674: 2746: 2143: 2040: 3607: 3943: 2147: 1983: 1948: 1882: 996: 1732:
determines the sense (clockwise vs counterclockwise) of precession.
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stand for the Lorentz group generators in the Dirac space, and the
199: 66: 1665:{\displaystyle \,{\frac {\gamma _{n}}{\,2\pi \,g_{\rm {n}}\,}}\,,} 1895: 1721: 62: 20: 3565: 3838: 1821: 1419: 985: 717:{\displaystyle g_{\mathrm {e} }=-2.002\,319\,304\,361\,18(27).} 72:
The term "gyromagnetic ratio" is often used as a synonym for a
54: 3652:"The anomalous magnetic moments of the electron and the muon" 2229: 2154: 44: 32: 3989: 3971: 3832: 3636: 3618: 3582: 3576: 654:-factor is known to twelve decimal places by measuring the 87:-factor only differs from the gyromagnetic ratio in being 3604:
Also note that the units of radians are added for clarity.
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ratio: whereas it is a ratio of a magnetic property (i.e.
2735:{\displaystyle {\frac {d\mathbf {J} }{dt}}=\mathbf {T} ~.} 1391:
and consequently to behave as a truly quadratic fermion.
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particles which cannot be described by the linear gauged
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represents the linear velocity of the pike of the arrow
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is found to be equal to 2; Therefore, the factor 2 is a
639:. Here the small corrections to the relativistic result 2414:
on the two poles and vector distance between the poles
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come from the quantum field theory calculations of the
50: 3937: 3654:. In Duplantier, Bertrand; Rivasseau, Vincent (eds.). 3506: 1366:. This particle has been shown to be characterized by 965:
Gyromagnetic factor not as a consequence of relativity
234:. Then the magnitude of the magnetic dipole moment is 3798: 3286: 2991: 2964: 2942: 2906: 2882: 2833: 2803: 2778: 2756: 2695: 2670: 2646: 2612: 2532: 2469: 2442: 2420: 2388: 2343: 2298: 2276: 2254: 2166: 1778: 1749: 1678: 1619: 1583: 1550: 1435: 1071: 851: 732: 664: 621: 538: 395: 243: 179: 157: 116: 31:
in other disciplines) of a particle or system is the
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By classical mechanics the torque on this needle is
1712:
The gyromagnetic ratio of a nucleus plays a role in
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In the framework of relativistic quantum mechanics,
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Quantities, Units and Symbols in Physical Chemistry
2436:under the influence of the magnetic field of earth 1270:{\displaystyle \left\;\psi \;=\;0~,\quad g\neq 2~.} 3913:. San Diego, CA: Elsevier Academic Press. p.  3821: 3719: 3717: 3328: 3269: 2974: 2950: 2928: 2892: 2868: 2818: 2797:Replace the gravity with a magnetic flux density 2789: 2764: 2734: 2678: 2656: 2629: 2598: 2518: 2455: 2428: 2406: 2368: 2329: 2284: 2262: 2196: 2138:(measured in teslas) that is not aligned with its 1808: 1762: 1701: 1664: 1598: 1565: 1533: 1269: 937: 838: 716: 627: 607: 505: 353: 187: 165: 140: 3875: 3454:International Union of Pure and Applied Chemistry 1613:of the nucleon or nucleus in question. The ratio 4139: 3905:Bernstein, M.A.; King, K.F.; Zhou, X.J. (2004). 2376:, or in the following way, imitating the moment 94: 3844: 3714: 2157:), that is proportional to the external field: 1321:. An example for such a particle, is the spin 4087:"shielded helion gyromagnetic ratio in MHz/T" 4026:"shielded proton gyromagnetic ratio in MHz/T" 3509:"Measurement of the Electron Magnetic Moment" 3850: 2197:{\displaystyle f={\frac {\gamma }{2\pi }}B.} 988:is obtained and for both linearizations the 984:(which leads to Dirac's). In both cases a 4- 955:are in excellent agreement with theory; see 61:(rad⋅s⋅T) or, equivalently, the 16:Ratio of magnetic moment to angular momentum 3491: 364: 3597: 3462:, 2nd edition, Oxford: Blackwell Science. 1241: 1237: 1233: 4125: 3751: 3740:International Journal of Modern Physics E 3524: 3310: 3306: 3299: 3257: 3244: 3240: 3236: 3226: 3214: 3210: 3207: 3192: 3188: 3178: 3166: 3162: 3159: 3135: 3125: 3113: 3109: 3106: 3092: 3076: 3072: 3064: 3059: 3053: 3045: 3037: 3033: 3021: 3017: 3004: 2971: 2965: 2947: 2943: 2922: 2907: 2889: 2883: 2862: 2852: 2849: 2837: 2804: 2653: 2647: 2592: 2533: 2512: 2470: 2449: 2443: 2323: 2299: 1724:in a magnetic field at a rate called the 1658: 1654: 1641: 1634: 1620: 1518: 1505: 1501: 1473: 1469: 1455: 1364:representation space of the Lorentz group 1227: 1200: 1186: 1182: 1178: 1171: 1149: 1145: 1123: 1107: 1103: 1093: 1077: 903: 890: 886: 789: 763: 759: 755: 698: 694: 690: 686: 584: 577: 499: 440: 314: 282: 4107: 1398: 43:, and it is often denoted by the symbol 3938:Weast, R.C.; Astle, M.J., eds. (1982). 3689: 3589:here. Indeed, many references say that 2243: 141:{\displaystyle \gamma ={\frac {q}{2m}}} 4140: 3649: 3633:"electron gyromagnetic ratio in MHz/T" 3986:"proton gyromagnetic ratio over 2 pi" 3643: 2630:{\displaystyle {\hat {\mathbf {d} }}} 1702:{\displaystyle \mu _{\mathrm {N} }/h} 4065:"shielded helion gyromagnetic ratio" 4004:"shielded proton gyromagnetic ratio" 3486:Physics for Scientists and Engineers 3483: 2236:(Hz/T), are often quoted instead of 2110: 1403:The sign of the gyromagnetic ratio, 1809:{\displaystyle \gamma _{n}/(2\pi )} 1566:{\displaystyle \mu _{\mathrm {N} }} 726:The electron gyromagnetic ratio is 13: 3805: 3693:Quantum Mechanics: An introduction 3690:Greiner, Walter (4 October 2000). 3073: 3068: 3049: 2929:{\displaystyle \,J\sin {\phi }\,,} 2853: 2838: 2540: 2487: 2398: 1685: 1648: 1590: 1557: 1512: 1495: 1480: 1422:, neutrons, and many nuclei carry 1130: 1084: 919: 910: 907: 904: 860: 823: 805: 796: 793: 790: 739: 671: 545: 487: 475: 452: 431: 402: 76:but closely related quantity, the 14: 4169: 3940:Handbook of Chemistry and Physics 3738:, irreducibility and linearity". 2606:so the desired formula comes up. 2456:{\displaystyle \,\mathbf {B} \,.} 1709:, is 7.622593285(47) MHz/T. 1520: 494: 3822:{\displaystyle \mu _{\rm {N}}/h} 3650:Knecht, Marc (12 October 2002). 3150: 3142: 3098: 3055: 2975:{\displaystyle \,\mathbf {J} \,} 2967: 2893:{\displaystyle \,\mathbf {J} \,} 2885: 2845: 2819:{\displaystyle \,\mathbf {B} ~.} 2806: 2780: 2758: 2722: 2703: 2672: 2657:{\displaystyle \,\mathbf {J} \,} 2649: 2617: 2588: 2574: 2547: 2505: 2497: 2473: 2445: 2422: 2319: 2311: 2302: 2278: 2256: 1394: 648:anomalous magnetic dipole moment 4127:10.3390/magnetochemistry6040065 4101: 4079: 4057: 4040: 4018: 3996: 3978: 3960: 3931: 3909:Handbook of MRI Pulse Sequences 3898: 3784: 3600:Electron Paramagnetic Resonance 3320: 2900:along a circle whose radius is 2407:{\displaystyle \pm q_{\rm {m}}} 1251: 4108:Makulski, Wlodzimierz (2020). 3683: 3596:for an electron; for example, 3543:10.1103/PhysRevLett.130.071801 3500: 3492:Tipler, P.A.; Llewellyn, R.A. 3476: 3447: 2621: 2578: 2509: 2493: 1803: 1794: 1319:electromagnetic four-potential 900: 894: 773: 767: 708: 702: 459: 442: 202:. Suppose the ring has radius 1: 3855:. John Wiley & Sons Ltd. 3615:"electron gyromagnetic ratio" 3573:"electron gyromagnetic ratio" 3488:(3rd ed.). p. 1017; 3440: 2790:{\displaystyle \mathbf {m} .} 2637:is the unit distance vector. 2129:, when placed in an external 658:in a one-electron cyclotron: 95:For a classical rotating body 27:(also sometimes known as the 3792:"Nuclear magneton in MHz/T: 3496:(4th ed.). p. 309. 3372:angular precession frequency 2765:{\displaystyle \mathbf {J} } 2679:{\displaystyle \mathbf {T} } 2429:{\displaystyle \mathbf {d} } 2369:{\displaystyle m=I\pi r^{2}} 2285:{\displaystyle \mathbf {B} } 2263:{\displaystyle \mathbf {m} } 7: 3968:"proton gyromagnetic ratio" 3404: 3398:angular cyclotron frequency 2207:For this reason, values of 1763:{\displaystyle \gamma _{n}} 1599:{\displaystyle g_{\rm {n}}} 10: 4174: 4153:Nuclear magnetic resonance 3876:Palmer, Arthur G. (2007). 3598:Weil & Bolton (2007). 2664:equals the applied torque 2114: 1718:magnetic resonance imaging 1714:nuclear magnetic resonance 3770:10.1142/S0218301315500603 3710:– via Google Books. 3435:Proton gyromagnetic ratio 3362:, "turn") property (i.e. 3359: 2951:{\displaystyle \,\phi \,} 2526:But as previously stated 3927:– via archive.org. 3878:Protein NMR Spectroscopy 1415:> 0 (as for protons). 656:electron magnetic moment 365:For an isolated electron 3882:Elsevier Academic Press 3513:Physical Review Letters 2745:Note as an example the 637:fine-structure constant 628:{\displaystyle \alpha } 224:, and angular momentum 3823: 3370:, a ratio between the 3330: 3271: 2976: 2952: 2930: 2894: 2870: 2820: 2791: 2766: 2736: 2680: 2658: 2631: 2600: 2520: 2457: 2430: 2408: 2370: 2331: 2286: 2264: 2198: 1810: 1764: 1703: 1666: 1600: 1567: 1535: 1416: 1309:electromagnetic tensor 1271: 958:Precision tests of QED 939: 840: 718: 629: 609: 507: 355: 189: 167: 142: 3851:Levitt, M.H. (2008). 3824: 3656:PoincarĂ© Seminar 2002 3602:. Wiley. p. 578. 3331: 3272: 2977: 2958:is the angle between 2953: 2931: 2895: 2871: 2821: 2792: 2767: 2737: 2681: 2659: 2632: 2601: 2521: 2458: 2431: 2409: 2371: 2332: 2287: 2265: 2199: 1811: 1765: 1704: 1667: 1601: 1568: 1536: 1402: 1272: 1024:Klein–Gordon equation 982:Klein–Gordon equation 980:and the relativistic 940: 841: 719: 630: 610: 508: 356: 190: 168: 143: 3841:-recommended values) 3796: 3411:Charge-to-mass ratio 3284: 2989: 2962: 2940: 2904: 2880: 2831: 2801: 2776: 2754: 2693: 2668: 2644: 2610: 2530: 2467: 2440: 2418: 2386: 2341: 2296: 2274: 2270:to a magnetic field 2252: 2244:Heuristic derivation 2164: 1776: 1747: 1676: 1617: 1581: 1548: 1433: 1311:respectively, while 1069: 978:Schrödinger equation 849: 730: 662: 619: 536: 393: 241: 177: 155: 114: 3762:2015IJMPE..2450060D 3679:on 15 October 2005. 3535:2023PhRvL.130g1801F 3472:Electronic version. 1062:term according to, 1022:satisfy the gauged 380:, which is denoted 188:{\displaystyle {m}} 166:{\displaystyle {q}} 3942:. Boca Raton, FL: 3819: 3482:For example, see: 3354:(rotational, from 3326: 3267: 2972: 2948: 2926: 2890: 2866: 2816: 2787: 2762: 2732: 2676: 2654: 2627: 2596: 2516: 2453: 2426: 2404: 2366: 2327: 2282: 2260: 2194: 1806: 1760: 1699: 1662: 1596: 1563: 1531: 1417: 1337:companion to spin 1267: 935: 836: 714: 625: 605: 503: 351: 185: 173:is its charge and 163: 138: 29:magnetogyric ratio 25:gyromagnetic ratio 3324: 3316: 3308: 3263: 3249: 3228: 3180: 3127: 3080: 3035: 2864: 2812: 2728: 2716: 2624: 2581: 2186: 2117:Larmor precession 2111:Larmor precession 2108: 2107: 1656: 1527: 1523: 1471: 1466: 1443: 1263: 1247: 1184: 874: 601: 586: 497: 438: 347: 340: 312: 280: 136: 4165: 4132: 4131: 4129: 4114:Magnetochemistry 4105: 4099: 4098: 4096: 4094: 4083: 4077: 4076: 4074: 4072: 4061: 4055: 4054: 4053:. November 2015. 4052: 4044: 4038: 4037: 4035: 4033: 4022: 4016: 4015: 4013: 4011: 4000: 3994: 3993: 3982: 3976: 3975: 3964: 3958: 3957: 3935: 3929: 3928: 3912: 3902: 3896: 3895: 3873: 3867: 3866: 3848: 3842: 3836: 3828: 3826: 3825: 3820: 3815: 3810: 3809: 3808: 3788: 3782: 3781: 3755: 3737: 3727: 3721: 3712: 3711: 3687: 3681: 3680: 3678: 3668:. Archived from 3647: 3641: 3640: 3629: 3623: 3622: 3611: 3605: 3603: 3595: 3593: 3588: 3580: 3569: 3563: 3562: 3528: 3504: 3498: 3497: 3489: 3480: 3474: 3451: 3424: 3387: 3368:at the same time 3364:angular momentum 3361: 3335: 3333: 3332: 3327: 3325: 3322: 3314: 3309: 3307: 3294: 3276: 3274: 3273: 3268: 3261: 3250: 3245: 3234: 3229: 3227: 3225: 3208: 3206: 3186: 3181: 3179: 3177: 3160: 3158: 3154: 3153: 3145: 3133: 3128: 3126: 3124: 3107: 3105: 3101: 3090: 3085: 3081: 3079: 3078: 3077: 3071: 3062: 3061: 3060: 3058: 3052: 3043: 3036: 3034: 3032: 3012: 2981: 2979: 2978: 2973: 2970: 2957: 2955: 2954: 2949: 2935: 2933: 2932: 2927: 2921: 2899: 2897: 2896: 2891: 2888: 2875: 2873: 2872: 2867: 2865: 2863: 2850: 2848: 2835: 2825: 2823: 2822: 2817: 2810: 2809: 2796: 2794: 2793: 2788: 2783: 2771: 2769: 2768: 2763: 2761: 2741: 2739: 2738: 2733: 2726: 2725: 2717: 2715: 2707: 2706: 2697: 2685: 2683: 2682: 2677: 2675: 2663: 2661: 2660: 2655: 2652: 2636: 2634: 2633: 2628: 2626: 2625: 2620: 2615: 2605: 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1532: 1525: 1524: 1519: 1517: 1516: 1515: 1503: 1500: 1499: 1498: 1485: 1484: 1483: 1472: 1470: 1468: 1467: 1464: 1450: 1445: 1444: 1441: 1414: 1410: 1406: 1390: 1389: 1387: 1386: 1383: 1380: 1376: 1370: 1362: 1352: 1350: 1349: 1346: 1343: 1336: 1334: 1333: 1330: 1327: 1316: 1306: 1300: 1296: 1294: 1293: 1290: 1287: 1276: 1274: 1273: 1268: 1261: 1245: 1232: 1228: 1226: 1225: 1213: 1212: 1199: 1198: 1185: 1183: 1173: 1164: 1160: 1159: 1158: 1138: 1137: 1122: 1118: 1117: 1116: 1092: 1091: 1061: 1060: 1048: 1046: 1045: 1042: 1039: 1030: 1026:extended by the 1017: 1015: 1014: 1011: 1008: 992: 973: 954: 950: 944: 942: 941: 936: 931: 930: 929: 917: 875: 873: 865: 864: 863: 853: 845: 843: 842: 837: 835: 834: 833: 821: 816: 815: 803: 788: 787: 744: 743: 742: 723: 721: 720: 715: 676: 675: 674: 653: 645: 634: 632: 631: 626: 614: 612: 611: 606: 599: 598: 594: 587: 585: 572: 550: 549: 548: 521: 512: 510: 509: 504: 498: 493: 492: 491: 490: 480: 479: 478: 467: 462: 457: 456: 455: 445: 439: 437: 436: 435: 434: 420: 412: 407: 406: 405: 388: 377: 360: 358: 357: 352: 345: 341: 339: 328: 313: 311: 300: 295: 294: 281: 279: 268: 260: 233: 223: 219: 215: 205: 194: 192: 191: 186: 184: 172: 170: 169: 164: 162: 147: 145: 144: 139: 137: 135: 124: 86: 80: 47: 41:angular momentum 4173: 4172: 4168: 4167: 4166: 4164: 4163: 4162: 4138: 4137: 4136: 4135: 4106: 4102: 4092: 4090: 4085: 4084: 4080: 4070: 4068: 4063: 4062: 4058: 4050: 4046: 4045: 4041: 4031: 4029: 4024: 4023: 4019: 4009: 4007: 4002: 4001: 3997: 3984: 3983: 3979: 3966: 3965: 3961: 3954: 3946:. p. E66. 3936: 3932: 3925: 3903: 3899: 3892: 3874: 3870: 3863: 3849: 3845: 3811: 3804: 3803: 3799: 3797: 3794: 3793: 3790: 3789: 3785: 3736: 3732: 3730: 3725: 3722: 3715: 3708: 3698:Springer Verlag 3688: 3684: 3672: 3666: 3648: 3644: 3631: 3630: 3626: 3613: 3612: 3608: 3591: 3590: 3586: 3571: 3570: 3566: 3505: 3501: 3484:Giancoli, D.C. 3481: 3477: 3452: 3448: 3443: 3430:Larmor equation 3422: 3407: 3379: 3366:), it is also, 3321: 3298: 3293: 3285: 3282: 3281: 3235: 3233: 3221: 3209: 3202: 3187: 3185: 3173: 3161: 3149: 3141: 3140: 3136: 3134: 3132: 3120: 3108: 3097: 3093: 3091: 3089: 3067: 3066: 3065: 3063: 3054: 3048: 3047: 3046: 3044: 3042: 3038: 3028: 3016: 3011: 2990: 2987: 2986: 2966: 2963: 2960: 2959: 2941: 2938: 2937: 2917: 2905: 2902: 2901: 2884: 2881: 2878: 2877: 2851: 2844: 2836: 2834: 2832: 2829: 2828: 2805: 2802: 2799: 2798: 2779: 2777: 2774: 2773: 2757: 2755: 2752: 2751: 2721: 2708: 2702: 2698: 2696: 2694: 2691: 2690: 2671: 2669: 2666: 2665: 2648: 2645: 2642: 2641: 2616: 2614: 2613: 2611: 2608: 2607: 2587: 2573: 2571: 2570: 2564: 2560: 2546: 2539: 2538: 2534: 2531: 2528: 2527: 2504: 2496: 2486: 2485: 2481: 2472: 2471: 2468: 2465: 2464: 2444: 2441: 2438: 2437: 2421: 2419: 2416: 2415: 2397: 2396: 2392: 2387: 2384: 2383: 2378: 2360: 2356: 2342: 2339: 2338: 2318: 2310: 2301: 2300: 2297: 2294: 2293: 2277: 2275: 2272: 2271: 2255: 2253: 2250: 2249: 2246: 2237: 2221: 2219: 2216: 2212: 2211: 2210: 2208: 2178: 2173: 2165: 2162: 2161: 2150: 2140:magnetic moment 2134: 2119: 2113: 2100: 2098: 2091: 2089: 1928: 1925: 1923: 1916: 1913: 1911: 1873: 1870: 1868: 1861: 1859: 1855: 1843: 1840: 1838: 1831: 1828: 1826: 1789: 1783: 1779: 1777: 1774: 1773: 1754: 1750: 1748: 1745: 1744: 1729: 1691: 1684: 1683: 1679: 1677: 1674: 1673: 1647: 1646: 1642: 1633: 1627: 1623: 1621: 1618: 1615: 1614: 1608: 1589: 1588: 1584: 1582: 1579: 1578: 1556: 1555: 1551: 1549: 1546: 1545: 1511: 1510: 1506: 1504: 1502: 1494: 1493: 1489: 1479: 1478: 1474: 1463: 1459: 1454: 1449: 1440: 1436: 1434: 1431: 1430: 1412: 1408: 1404: 1397: 1384: 1381: 1378: 1377: 1374: 1372: 1368: 1367: 1354: 1347: 1344: 1341: 1340: 1338: 1331: 1328: 1325: 1324: 1322: 1312: 1302: 1291: 1288: 1285: 1284: 1282: 1281: 1221: 1217: 1205: 1201: 1191: 1187: 1177: 1172: 1154: 1150: 1133: 1129: 1128: 1124: 1112: 1108: 1087: 1083: 1082: 1078: 1076: 1072: 1070: 1067: 1066: 1059: 1043: 1040: 1035: 1034: 1032: 1031: 1028: 1027: 1012: 1009: 1006: 1005: 1003: 990: 971: 967: 952: 948: 922: 918: 913: 879: 866: 859: 858: 854: 852: 850: 847: 846: 826: 822: 817: 808: 804: 799: 783: 779: 748: 738: 737: 733: 731: 728: 727: 670: 669: 665: 663: 660: 659: 651: 650:. The electron 640: 620: 617: 616: 576: 571: 564: 560: 544: 543: 539: 537: 534: 533: 520: 514: 486: 485: 481: 474: 473: 469: 468: 466: 458: 451: 450: 446: 441: 430: 429: 425: 421: 413: 411: 401: 400: 396: 394: 391: 390: 387: 381: 375: 367: 332: 327: 304: 299: 290: 286: 269: 261: 259: 242: 239: 238: 225: 221: 217: 207: 203: 180: 178: 175: 174: 158: 156: 153: 152: 128: 123: 115: 112: 111: 97: 84: 78: 57:per second per 45: 37:magnetic moment 17: 12: 11: 5: 4171: 4161: 4160: 4155: 4150: 4148:Atomic physics 4134: 4133: 4100: 4078: 4056: 4039: 4017: 3995: 3977: 3959: 3952: 3930: 3923: 3897: 3891:978-0121644918 3890: 3868: 3862:978-0470511176 3861: 3843: 3818: 3814: 3807: 3802: 3783: 3746:(7): 1550060. 3734: 3728: 3713: 3706: 3682: 3664: 3642: 3624: 3606: 3564: 3499: 3494:Modern Physics 3475: 3470:. p. 21. 3445: 3444: 3442: 3439: 3438: 3437: 3432: 3427: 3418: 3416:Chemical shift 3413: 3406: 3403: 3390:magnetic field 3319: 3313: 3305: 3302: 3297: 3292: 3289: 3280:Consequently, 3278: 3277: 3266: 3260: 3256: 3253: 3248: 3243: 3239: 3232: 3224: 3220: 3217: 3213: 3205: 3201: 3198: 3195: 3191: 3184: 3176: 3172: 3169: 3165: 3157: 3152: 3148: 3144: 3139: 3131: 3123: 3119: 3116: 3112: 3104: 3100: 3096: 3088: 3084: 3075: 3070: 3057: 3051: 3041: 3031: 3027: 3024: 3020: 3015: 3010: 3007: 3003: 3000: 2997: 2994: 2969: 2946: 2925: 2920: 2916: 2913: 2910: 2887: 2861: 2858: 2855: 2847: 2843: 2840: 2815: 2808: 2786: 2782: 2772:and downwards 2760: 2743: 2742: 2731: 2724: 2720: 2714: 2711: 2705: 2701: 2674: 2651: 2623: 2619: 2595: 2590: 2586: 2580: 2576: 2567: 2563: 2559: 2556: 2553: 2549: 2542: 2537: 2515: 2511: 2507: 2503: 2499: 2495: 2489: 2484: 2480: 2475: 2452: 2447: 2424: 2400: 2395: 2391: 2363: 2359: 2355: 2352: 2349: 2346: 2326: 2321: 2317: 2313: 2309: 2304: 2280: 2258: 2245: 2242: 2228:, in units of 2205: 2204: 2193: 2190: 2184: 2181: 2177: 2172: 2169: 2131:magnetic field 2115:Main article: 2112: 2109: 2106: 2105: 2096: 2087: 2083: 2082: 2079: 2076: 2072: 2071: 2068: 2065: 2061: 2060: 2057: 2054: 2050: 2049: 2046: 2043: 2037: 2036: 2033: 2030: 2026: 2025: 2022: 2019: 2015: 2014: 2011: 2008: 2004: 2003: 2000: 1997: 1993: 1992: 1989: 1986: 1980: 1979: 1976: 1973: 1969: 1968: 1965: 1962: 1958: 1957: 1954: 1951: 1945: 1944: 1941: 1938: 1934: 1933: 1921: 1909: 1905: 1904: 1901: 1898: 1892: 1891: 1888: 1885: 1879: 1878: 1866: 1857: 1853: 1849: 1848: 1836: 1824: 1818: 1817: 1805: 1802: 1799: 1796: 1792: 1786: 1782: 1771: 1757: 1753: 1742: 1698: 1694: 1687: 1682: 1661: 1650: 1645: 1640: 1637: 1630: 1626: 1592: 1587: 1559: 1554: 1542: 1541: 1530: 1522: 1514: 1509: 1497: 1492: 1488: 1482: 1477: 1462: 1458: 1453: 1448: 1439: 1396: 1393: 1278: 1277: 1266: 1260: 1257: 1254: 1250: 1244: 1240: 1236: 1231: 1224: 1220: 1216: 1211: 1208: 1204: 1197: 1194: 1190: 1181: 1176: 1170: 1167: 1163: 1157: 1153: 1148: 1144: 1141: 1136: 1132: 1127: 1121: 1115: 1111: 1106: 1102: 1099: 1096: 1090: 1086: 1081: 1075: 1055: 1020:Dirac equation 1002:Physical spin 966: 963: 934: 928: 925: 921: 916: 912: 909: 906: 902: 899: 896: 893: 889: 885: 882: 878: 872: 869: 862: 857: 832: 829: 825: 820: 814: 811: 807: 802: 798: 795: 792: 786: 782: 778: 775: 772: 769: 766: 762: 758: 754: 751: 747: 741: 736: 713: 710: 707: 704: 701: 697: 693: 689: 685: 682: 679: 673: 668: 624: 604: 597: 593: 590: 583: 580: 575: 570: 567: 563: 559: 556: 553: 547: 542: 518: 502: 496: 489: 484: 477: 472: 465: 461: 454: 449: 444: 433: 428: 424: 419: 416: 410: 404: 399: 385: 366: 363: 362: 361: 350: 344: 338: 335: 331: 326: 323: 320: 317: 310: 307: 303: 298: 293: 289: 285: 278: 275: 272: 267: 264: 258: 255: 252: 249: 246: 183: 161: 149: 148: 134: 131: 127: 122: 119: 96: 93: 69:(C⋅kg). 15: 9: 6: 4: 3: 2: 4170: 4159: 4156: 4154: 4151: 4149: 4146: 4145: 4143: 4128: 4123: 4119: 4115: 4111: 4104: 4088: 4082: 4066: 4060: 4049: 4043: 4027: 4021: 4005: 3999: 3991: 3987: 3981: 3973: 3969: 3963: 3955: 3953:0-8493-0463-6 3949: 3945: 3941: 3934: 3926: 3924:0-12-092861-2 3920: 3916: 3911: 3910: 3901: 3893: 3887: 3883: 3879: 3872: 3864: 3858: 3854: 3853:Spin Dynamics 3847: 3840: 3834: 3830: 3816: 3812: 3800: 3787: 3779: 3775: 3771: 3767: 3763: 3759: 3754: 3749: 3745: 3741: 3720: 3718: 3709: 3707:9783540674580 3703: 3699: 3695: 3694: 3686: 3676: 3671: 3667: 3665:3-7643-0579-7 3661: 3657: 3653: 3646: 3638: 3634: 3628: 3620: 3616: 3610: 3601: 3584: 3578: 3574: 3568: 3560: 3556: 3552: 3548: 3544: 3540: 3536: 3532: 3527: 3522: 3519:(7): 071801. 3518: 3514: 3510: 3503: 3495: 3487: 3479: 3473: 3469: 3468:0-632-03583-8 3465: 3461: 3460: 3455: 3450: 3446: 3436: 3433: 3431: 3428: 3426: 3419: 3417: 3414: 3412: 3409: 3408: 3402: 3400: 3399: 3393: 3391: 3386: 3382: 3377: 3373: 3369: 3365: 3357: 3353: 3349: 3348:dipole moment 3345: 3342:ratio versus 3341: 3336: 3317: 3311: 3303: 3300: 3295: 3290: 3287: 3264: 3258: 3254: 3251: 3246: 3241: 3237: 3230: 3222: 3218: 3215: 3211: 3203: 3199: 3196: 3193: 3189: 3182: 3174: 3170: 3167: 3163: 3155: 3146: 3137: 3129: 3121: 3117: 3114: 3110: 3102: 3094: 3086: 3082: 3039: 3029: 3025: 3022: 3018: 3013: 3008: 3005: 3001: 2998: 2995: 2992: 2985: 2984: 2983: 2944: 2923: 2918: 2914: 2911: 2908: 2859: 2856: 2841: 2826: 2813: 2784: 2748: 2729: 2718: 2712: 2709: 2699: 2689: 2688: 2687: 2638: 2593: 2584: 2565: 2561: 2557: 2554: 2551: 2535: 2513: 2501: 2482: 2478: 2450: 2393: 2389: 2381: 2361: 2357: 2353: 2350: 2347: 2344: 2324: 2315: 2307: 2241: 2235: 2231: 2191: 2188: 2182: 2179: 2175: 2170: 2167: 2160: 2159: 2158: 2156: 2153:(measured in 2149: 2145: 2141: 2137: 2132: 2128: 2124: 2118: 2097: 2088: 2085: 2084: 2080: 2077: 2074: 2073: 2069: 2066: 2063: 2062: 2058: 2055: 2052: 2051: 2047: 2044: 2042: 2039: 2038: 2034: 2031: 2028: 2027: 2023: 2020: 2017: 2016: 2012: 2009: 2006: 2005: 2001: 1998: 1995: 1994: 1990: 1987: 1985: 1982: 1981: 1977: 1974: 1971: 1970: 1966: 1963: 1960: 1959: 1955: 1952: 1950: 1947: 1946: 1942: 1939: 1936: 1935: 1922: 1910: 1907: 1906: 1902: 1899: 1897: 1894: 1893: 1889: 1886: 1884: 1881: 1880: 1867: 1858: 1851: 1850: 1837: 1825: 1823: 1820: 1819: 1800: 1797: 1790: 1784: 1780: 1772: 1770:(10 rad⋅s⋅T) 1755: 1751: 1743: 1740: 1739: 1736: 1733: 1727: 1723: 1719: 1715: 1710: 1696: 1692: 1680: 1659: 1643: 1638: 1635: 1628: 1624: 1612: 1585: 1576: 1552: 1528: 1507: 1490: 1486: 1475: 1460: 1456: 1451: 1446: 1437: 1429: 1428: 1427: 1425: 1421: 1401: 1395:For a nucleus 1392: 1365: 1361: 1357: 1320: 1315: 1310: 1305: 1299: 1264: 1258: 1255: 1252: 1248: 1242: 1238: 1234: 1229: 1222: 1218: 1214: 1209: 1206: 1202: 1195: 1192: 1188: 1179: 1174: 1168: 1165: 1161: 1155: 1151: 1146: 1142: 1139: 1134: 1125: 1119: 1113: 1109: 1104: 1100: 1097: 1094: 1088: 1079: 1073: 1065: 1064: 1063: 1058: 1054: 1051: 1038: 1025: 1021: 1000: 998: 994: 987: 983: 979: 975: 962: 961:for details. 960: 959: 947:The electron 945: 932: 926: 923: 914: 897: 891: 887: 883: 880: 876: 870: 867: 855: 830: 827: 818: 812: 809: 800: 784: 780: 776: 770: 764: 760: 756: 752: 749: 745: 734: 724: 711: 705: 699: 695: 691: 687: 683: 680: 677: 666: 657: 649: 643: 638: 622: 602: 595: 591: 588: 581: 578: 573: 568: 565: 561: 557: 554: 551: 540: 530: 527: 525: 524:Bohr magneton 517: 500: 482: 470: 463: 447: 426: 422: 417: 414: 408: 397: 384: 379: 372: 348: 342: 336: 333: 329: 324: 321: 318: 315: 308: 305: 301: 296: 291: 287: 283: 276: 273: 270: 265: 262: 256: 253: 250: 247: 244: 237: 236: 235: 232: 228: 214: 210: 201: 196: 195:is its mass. 181: 159: 132: 129: 125: 120: 117: 110: 109: 108: 105: 102: 101:nonconductive 92: 90: 89:dimensionless 82: 75: 70: 68: 64: 60: 56: 52: 49:, gamma. Its 48: 42: 38: 34: 30: 26: 22: 4117: 4113: 4103: 4091:. Retrieved 4081: 4069:. Retrieved 4059: 4042: 4030:. Retrieved 4020: 4008:. Retrieved 3998: 3980: 3962: 3939: 3933: 3908: 3900: 3877: 3871: 3852: 3846: 3786: 3743: 3739: 3692: 3685: 3670:the original 3655: 3645: 3627: 3609: 3599: 3567: 3516: 3512: 3502: 3493: 3485: 3478: 3457: 3449: 3397: 3394: 3384: 3380: 3375: 3367: 3351: 3344:magnetogyric 3343: 3340:gyromagnetic 3339: 3337: 3279: 2827: 2744: 2639: 2377: 2247: 2206: 2133: 2120: 1734: 1711: 1543: 1424:nuclear spin 1418: 1359: 1355: 1313: 1303: 1297: 1279: 1056: 1052: 1049: 1036: 1001: 968: 956: 951:-factor and 946: 725: 641: 531: 528: 515: 382: 368: 230: 226: 212: 208: 197: 150: 98: 73: 71: 53:unit is the 28: 24: 18: 4089:. NIST 2022 4067:. NIST 2022 4028:. NIST 2022 4006:. NIST 2022 997:consequence 200:integration 99:Consider a 4142:Categories 3753:1507.03640 3675:PostScript 3581:Note that 3526:2209.13084 3441:References 3378:property) 2747:precession 1716:(NMR) and 4120:(4): 65. 3944:CRC Press 3801:μ 3778:119303031 3559:123962197 3374:(another 3304:π 3296:γ 3255:γ 3223:ϕ 3219:⁡ 3204:ϕ 3200:⁡ 3175:ϕ 3171:⁡ 3147:× 3122:ϕ 3118:⁡ 3030:ϕ 3026:⁡ 3002:π 2993:ω 2945:ϕ 2919:ϕ 2915:⁡ 2857:⁡ 2842:⁡ 2622:^ 2579:^ 2558:π 2502:× 2390:± 2354:π 2316:× 2183:π 2176:γ 2148:frequency 1900:285.3508 1801:π 1781:γ 1752:γ 1681:μ 1672:equal to 1639:π 1625:γ 1553:μ 1521:ℏ 1508:μ 1438:γ 1256:≠ 1235:ψ 1210:ν 1207:μ 1196:ν 1193:μ 1189:σ 1156:μ 1135:μ 1131:∂ 1114:μ 1089:μ 1085:∂ 924:− 915:⋅ 881:− 871:π 856:γ 828:− 819:⋅ 810:− 801:⋅ 777:× 750:− 735:γ 681:− 623:α 592:⋯ 582:π 574:α 555:− 495:ℏ 483:μ 415:− 398:γ 284:π 274:π 245:μ 220:, charge 118:γ 74:different 3837:(citing 3551:36867820 3490:or see: 3456:(1993). 3405:See also 3388:and the 2127:electron 2125:, or an 2045:108.291 2032:−53.190 1999:251.815 1988:−36.264 1975:−27.116 1956:10.7084 1953:67.2828 1940:103.962 1912:−203.789 1816:(MHz⋅T) 1741:Nucleus 1373:⁠− 67:kilogram 3992:. 2022. 3974:. 2022. 3835:. 2014. 3758:Bibcode 3594:< 0 3531:Bibcode 3425:-factor 3350:) to a 2226:⁠ 2209:⁠ 2144:precess 2142:, will 2123:nucleus 2099:−11.776 2090:−73.995 2078:16.767 2070:11.319 2067:71.118 2048:17.235 2035:−8.465 2024:11.103 2021:69.763 2013:11.262 2010:70.761 2002:40.078 1991:−5.772 1978:−4.316 1964:19.331 1943:16.546 1924:−32.434 1903:45.415 1887:41.065 1860:267.515 1852:H (in H 1827:267.522 1722:precess 1611:-factor 1606:is the 1573:is the 1420:Protons 1388:⁠ 1353:in the 1351:⁠ 1339:⁠ 1335:⁠ 1323:⁠ 1317:is the 1295:⁠ 1283:⁠ 1047:⁠ 1033:⁠ 1016:⁠ 1004:⁠ 993:-factor 974:-factor 888:024.951 635:is the 522:is the 378:-factor 216:, mass 206:, area 104:charged 81:-factor 63:coulomb 39:to its 35:of its 21:physics 4158:Ratios 4093:9 July 4071:9 July 4032:19 May 4010:19 May 3950:  3921:  3888:  3859:  3839:CODATA 3776:  3704:  3662:  3557:  3549:  3466:  3421:LandĂ© 3323:q.e.d. 3315:  3262:  2936:where 2811:  2727:  2081:2.669 2059:1.382 2056:8.681 1967:3.077 1890:6.536 1869:42.576 1839:42.577 1577:, and 1544:where 1526:  1280:Here, 1262:  1246:  986:spinor 615:where 600:  513:where 346:  151:where 83:. The 55:radian 23:, the 4051:(PDF) 3774:S2CID 3748:arXiv 3555:S2CID 3521:arXiv 3376:gyric 3360:ÎłÏÏÎżÏ‚ 3356:Greek 3352:gyric 2292:is 2234:tesla 2230:hertz 2155:hertz 2146:at a 753:1.760 684:2.002 59:tesla 33:ratio 4095:2024 4073:2024 4034:2021 4012:2021 3990:NIST 3972:NIST 3948:ISBN 3919:ISBN 3886:ISBN 3857:ISBN 3833:NIST 3702:ISBN 3660:ISBN 3637:NIST 3619:NIST 3583:NIST 3577:NIST 3547:PMID 3464:ISBN 2232:per 2101:7338 1931:(28) 1919:(18) 1876:(17) 1864:(11) 1862:3194 1846:(18) 1834:(11) 1301:and 892:4242 371:spin 65:per 4122:doi 3915:960 3766:doi 3539:doi 3517:130 3383:= 2 3216:sin 3197:sin 3168:sin 3115:sin 3023:sin 2912:sin 2103:(3) 2094:(2) 2092:401 2086:Xe 2075:Zn 2064:Cu 2053:Fe 2029:Si 2018:Al 2007:Na 1937:Li 1929:033 1926:100 1914:460 1908:He 1871:385 1856:O) 1844:461 1841:478 1829:187 761:630 757:859 696:361 692:304 688:319 644:= 2 231:mvr 19:In 4144:: 4116:. 4112:. 3988:. 3970:. 3917:. 3884:. 3880:. 3831:. 3772:. 3764:. 3756:. 3744:24 3742:. 3716:^ 3700:. 3696:. 3635:. 3617:. 3575:. 3553:. 3545:. 3537:. 3529:. 3515:. 3511:. 3392:. 3385:πf 3358:: 2686:: 2240:. 1996:F 1972:N 1961:N 1917:78 1874:43 1832:08 1371:= 1358:⊕ 1057:ΌΜ 898:85 884:28 785:11 781:10 771:53 765:23 706:27 700:18 526:. 389:: 229:= 213:πr 211:= 91:. 51:SI 4130:. 4124:: 4118:6 4097:. 4075:. 4036:. 4014:. 3956:. 3894:. 3865:. 3829:" 3817:h 3813:/ 3806:N 3780:. 3768:: 3760:: 3750:: 3735:ÎŒ 3733:ψ 3729:s 3726:g 3677:) 3673:( 3639:. 3621:. 3592:Îł 3587:Îł 3579:. 3561:. 3541:: 3533:: 3523:: 3423:g 3381:ω 3318:. 3312:B 3301:2 3291:= 3288:f 3265:. 3259:B 3252:= 3247:J 3242:B 3238:m 3231:= 3212:J 3194:B 3190:m 3183:= 3164:J 3156:| 3151:B 3143:m 3138:| 3130:= 3111:J 3103:| 3099:T 3095:| 3087:= 3083:| 3074:t 3069:d 3056:J 3050:d 3040:| 3019:J 3014:1 3009:= 3006:f 2999:2 2996:= 2968:J 2924:, 2909:J 2886:J 2860:t 2854:d 2846:J 2839:d 2814:. 2807:B 2785:. 2781:m 2759:J 2730:. 2723:T 2719:= 2713:t 2710:d 2704:J 2700:d 2673:T 2650:J 2618:d 2594:, 2589:m 2585:= 2575:d 2566:2 2562:r 2555:I 2552:= 2548:d 2541:m 2536:q 2514:. 2510:) 2506:B 2498:d 2494:( 2488:m 2483:q 2479:= 2474:T 2451:. 2446:B 2423:d 2399:m 2394:q 2379:p 2362:2 2358:r 2351:I 2348:= 2345:m 2325:. 2320:B 2312:m 2308:= 2303:T 2279:B 2257:m 2238:Îł 2222:π 2220:2 2217:/ 2213:Îł 2192:. 2189:B 2180:2 2171:= 2168:f 2151:f 2135:B 2041:P 1984:O 1949:C 1896:H 1883:H 1854:2 1822:H 1804:) 1798:2 1795:( 1791:/ 1785:n 1756:n 1730:Îł 1697:h 1693:/ 1686:N 1660:, 1649:n 1644:g 1636:2 1629:n 1609:g 1591:n 1586:g 1558:N 1529:, 1513:N 1496:n 1491:g 1487:= 1481:n 1476:g 1465:p 1461:m 1457:2 1452:e 1447:= 1442:n 1413:Îł 1409:Îł 1405:Îł 1385:3 1382:/ 1379:2 1375:+ 1369:g 1360:D 1356:D 1348:2 1345:/ 1342:3 1332:2 1329:/ 1326:1 1314:A 1304:F 1298:σ 1292:2 1289:/ 1286:1 1265:. 1259:2 1253:g 1249:, 1243:0 1239:= 1230:] 1223:2 1219:m 1215:+ 1203:F 1180:4 1175:e 1169:g 1166:+ 1162:) 1152:A 1147:e 1143:i 1140:+ 1126:( 1120:) 1110:A 1105:e 1101:i 1098:+ 1095:u 1080:( 1074:[ 1053:F 1050:σ 1044:4 1041:/ 1037:e 1029:g 1013:2 1010:/ 1007:1 991:g 972:g 953:Îł 949:g 933:. 927:1 920:T 911:z 908:H 905:M 901:) 895:( 877:= 868:2 861:e 831:1 824:T 813:1 806:s 797:d 794:a 791:r 774:) 768:( 746:= 740:e 712:. 709:) 703:( 678:= 672:e 667:g 652:g 642:g 603:, 596:) 589:+ 579:2 569:+ 566:1 562:( 558:2 552:= 546:e 541:g 519:B 516:ÎŒ 501:, 488:B 476:e 471:g 464:= 460:| 453:e 448:g 443:| 432:e 427:m 423:2 418:e 409:= 403:e 386:e 383:g 376:g 349:. 343:L 337:m 334:2 330:q 325:= 322:r 319:v 316:m 309:m 306:2 302:q 297:= 292:2 288:r 277:r 271:2 266:v 263:q 257:= 254:A 251:I 248:= 227:L 222:q 218:m 209:A 204:r 182:m 160:q 133:m 130:2 126:q 121:= 85:g 79:g 46:Îł

Index

physics
ratio
magnetic moment
angular momentum
Îł
SI
radian
tesla
coulomb
kilogram
g-factor
dimensionless
nonconductive
charged
integration
spin
g-factor
Bohr magneton
fine-structure constant
anomalous magnetic dipole moment
electron magnetic moment
Precision tests of QED
g-factor
Schrödinger equation
Klein–Gordon equation
spinor
g-factor
consequence
Dirac equation
Klein–Gordon equation

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