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Weak hypercharge

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1553: 2899: 3154: 1859: 3166: 1884:, along the Weinberg angle. The neutral Higgs field (circled) breaks the electroweak symmetry and interacts with other particles to give them mass. Three components of the Higgs field become part of the massive 2117: 522:
with U(1) transformations by definition and therefore U(1) charges for the elements of the SU(2) doublet (for example lefthanded up and down quarks) have to be equal. This is why U(1) cannot be identified with
502: 671: 1545:). The weak hypercharge for an anti-fermion is the opposite of that of the corresponding fermion because the electric charge and the third component of the weak isospin reverse sign under 1594: 2012: 760: 1935: 404: 2784: 309: 340: 2928: 3036: 2044: 3170: 2416: 354: 2913: 420:(only terms that are overall weak-hypercharge neutral are allowed in the Lagrangian). However, one of the interactions is with the 304: 440: 428:
is nonzero, particles interact with this field all the time even in vacuum. This changes their weak hypercharge (and weak isospin
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The sum of −isospin and +charge is zero for each of the gauge bosons; consequently, all the electroweak gauge bosons have
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and most extensions, this implies that baryon number minus lepton number is also always conserved.
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of strong interactions (which is not conserved in weak interactions and is zero for leptons).
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are determined up to a twofold ambiguity by requiring cancellation of all anomalies.
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The rise of the Standard Model: A history of particle physics from 1964 to 1979
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For convenience, weak hypercharge is often represented at half-scale, so that
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Rearranging, the weak hypercharge can be explicitly defined as:
2572: 2167: 1736: 594: 1880:, of the known elementary particles, showing electric charge, 1858: 1773: 1620: 497:{\displaystyle \ Q=T_{3}+{\tfrac {1}{2}}\,Y_{\mathsf {W}}\ } 2706: 2578: 2324: 1020: 410: 2618: 2627:"Electroweak symmetry breaking in historical perspective" 1537:
where "left"- and "right"-handed here are left and right
2596:(1st ed.). Cambridge University Press. p. 14. 2439: 2132:. Since weak hypercharge is always conserved within the 507:
Mathematically, weak hypercharge appears similar to the
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Donoghue, J.F.; Golowich, E.; Holstein, B.R. (1994).
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Hence this hypothetical proton decay would conserve
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the average electric charge of the particles in the
2714: 2111: 2006: 1929: 1588: 754: 665: 571:electroweak quantum field to produce the observed 496: 398: 2713:Peskin, Michael E.; Schroeder, Daniel V. (1995). 2688:Particle Physics and Introduction to Field Theory 2677: 3184: 518:In the electroweak theory SU(2) transformations 2712: 2495: 993: 990: 987: 971: 2929:Mathematical formulation of the Standard Model 2741: 2778: 2631:Annual Review of Nuclear and Particle Science 334: 604:The weak hypercharge satisfies the relation 2475:Gauge Theory of Elementary Particle Physics 2029: 527:and weak hypercharge has to be introduced. 2785: 2771: 2508:. Princeton University Press. p. 87. 341: 327: 16:Abelian charge found in electroweak theory 2744:The Mathematical Theory of Cosmic Strings 2660: 2642: 2542:"Partial-symmetries of weak interactions" 2505:Elementary Particle Physics in a Nutshell 2417:Standard Model (mathematical formulation) 2108: 1966: 1949: 1904: 530:Weak hypercharge was first introduced by 478: 1857: 1596:and relation between coupling constants 1589:{\displaystyle ~\theta _{\mathsf {W}}~,} 1551: 437:). Only a specific combination of them, 2717:An Introduction to Quantum Field Theory 2539: 2472: 2007:{\displaystyle \,Y_{\rm {W}}=Q-T_{3}~,} 3185: 2448:. Cambridge University Press. p.  1574: 755:{\displaystyle Y_{\rm {W}}=2(Q-T_{3})} 485: 390: 2766: 2721:. Addison-Wesley Publishing Company. 2624: 2540:Glashow, Sheldon L. (February 1961). 2501: 3165: 2683: 2590:; Dresden, Max, eds. (1997-11-13). 2242:separately, so also the difference 13: 2792: 2662:10.1146/annurev-nucl-102313-025537 2072: 1973: 1930:{\displaystyle \,Y_{\text{W}}=0~.} 718: 14: 3214: 2128:is a conserved quantum number in 2036:baryon number minus lepton number 504:(electric charge), is conserved. 3164: 3153: 3152: 2897: 2139: 2255: 2034:Weak hypercharge is related to 1942:Hypercharge assignments in the 399:{\displaystyle Y_{\mathsf {W}}} 357:of electroweak interactions of 3080:Causal dynamical triangulation 2502:Tully, Christopher G. (2012). 2473:Cheng, T.P.; Li, L.F. (2006). 2444:Dynamics of the Standard Model 2228:Hence neutron decay conserves 2105: 2093: 1541:, respectively (distinct from 749: 730: 1: 2919:Spontaneous symmetry breaking 2427: 546:of the U(1) component of the 537: 2566:10.1016/0029-5582(61)90469-2 1515: 1512: 1494: 1418: 1400: 1382: 1349: 1346: 1328: 1252: 1234: 1216: 1147: 1144: 1141: 1080: 1062: 1059: 968: 950: 947: 7: 2625:Quigg, Chris (2015-10-19). 2410: 682:is the electric charge (in 509:Gell-Mann–Nishijima formula 377:. It is frequently denoted 373:and the third component of 10: 3219: 2265:grand unification theories 1608:. Adapted from Lee (1981). 693:is the third component of 18: 3148: 3107: 3085:Canonical quantum gravity 3055: 3022: 2991: 2948: 2937: 2906: 2895: 2800: 2746:. CRC Press. p. 12. 1659: 1152: 878: 784: 776: 769: 3090:Superfluid vacuum theory 2702:– via Archive.org. 2602:10.1017/cbo9780511471094 2263:is a prediction of many 2030:Baryon and lepton number 1873:, and weak hypercharge, 542:Weak hypercharge is the 426:vacuum expectation value 424:. Since the Higgs field 19:Not to be confused with 2872:Quantum electrodynamics 2862:Electroweak interaction 2742:Anderson, M.R. (2003). 2479:Oxford University Press 2019:which is equal to just 697:(the SU(2) component). 599:quantum electrodynamics 406:and corresponds to the 315:Flavour complementarity 112:Related quantum numbers 2850:Quantum chromodynamics 2113: 2008: 1950:Alternative half-scale 1931: 1889: 1609: 1590: 756: 667: 498: 400: 2966:Cosmological constant 2514:10.1515/9781400839353 2114: 2009: 1932: 1861: 1591: 1555: 757: 668: 499: 401: 3075:Loop quantum gravity 3014:Theory of everything 3009:Grand Unified Theory 2983:Neutrino oscillation 2830:Quantum field theory 2045: 1963: 1901: 1562: 709: 613: 593:gauge boson and the 441: 381: 3042:Split supersymmetry 3004:Kaluza–Klein theory 2877:Fermi's interaction 2653:2015ARNPS..65...25Q 2558:1961NucPh..22..579G 560:and its associated 3203:Electroweak theory 3070:Superstring theory 2840:Strong interaction 2684:Lee, T.D. (1981). 2109: 2091: 2058: 2004: 1927: 1890: 1610: 1586: 1547:charge conjugation 752: 663: 645: 494: 476: 396: 3180: 3179: 3103: 3102: 2978:Strong CP problem 2956:Hierarchy problem 2728:978-0-201-50397-5 2611:978-0-521-57082-4 2580:Hoddeson, Lillian 2523:978-1-4008-3935-3 2385: 2384: 2357:  └→   2090: 2057: 2023:isospin multiplet 2000: 1923: 1912: 1856: 1855: 1582: 1567: 1535: 1534: 684:elementary charge 659: 654: 644: 493: 475: 446: 351: 350: 3210: 3168: 3167: 3156: 3155: 2946: 2945: 2901: 2900: 2882:Weak hypercharge 2867:Weak interaction 2808:Particle physics 2787: 2780: 2773: 2764: 2763: 2758: 2757: 2739: 2733: 2732: 2720: 2710: 2704: 2703: 2691: 2681: 2675: 2674: 2664: 2646: 2622: 2616: 2615: 2588:Riordan, Michael 2576: 2570: 2569: 2537: 2528: 2527: 2499: 2493: 2492: 2470: 2464: 2463: 2447: 2437: 2398: 2397: 2393: 2381: 2380: 2378: 2377: 2370: 2369: 2342: 2341: 2339: 2338: 2331: 2330: 2316: 2314: 2313: 2306: 2305: 2291: 2290: 2289: 2282: 2281: 2272: 2271: 2251: 2250: 2246: 2241: 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3211: 3209: 3208: 3207: 3193:Nuclear physics 3183: 3182: 3181: 3176: 3144: 3099: 3057:Quantum gravity 3051: 3018: 2987: 2940: 2933: 2924:Higgs mechanism 2902: 2898: 2893: 2796: 2791: 2761: 2754: 2740: 2736: 2729: 2711: 2707: 2700: 2682: 2678: 2623: 2619: 2612: 2577: 2573: 2546:Nuclear Physics 2538: 2531: 2524: 2500: 2496: 2489: 2471: 2467: 2460: 2438: 2434: 2430: 2413: 2395: 2391: 2390: 2376: 2374: 2373: 2372: 2368: 2366: 2365: 2364: 2362: 2360: 2337: 2335: 2334: 2333: 2329: 2327: 2326: 2325: 2323: 2322: 2312: 2310: 2309: 2308: 2304: 2302: 2301: 2300: 2298: 2288: 2286: 2285: 2284: 2280: 2278: 2277: 2276: 2275: 2258: 2248: 2244: 2243: 2239: 2232: 2220: 2217: 2216: 2215: 2212: 2209: 2207: 2206: 2205: 2204: 2199: 2197: 2196: 2195: 2191: 2189: 2188: 2187: 2186: 2180: 2178: 2177: 2176: 2172: 2170: 2169: 2168: 2166: 2160: 2158: 2157: 2156: 2152: 2150: 2149: 2148: 2146: 2145: 2142: 2081: 2071: 2070: 2066: 2048: 2046: 2043: 2042: 2032: 1992: 1988: 1972: 1971: 1967: 1964: 1961: 1960: 1952: 1909: 1905: 1902: 1899: 1898: 1881: 1879: 1874: 1872: 1867: 1862:The pattern of 1844: 1841: 1838: 1837: 1835: 1823: 1821: 1820: 1819: 1815: 1813: 1812: 1811: 1809: 1808: 1786: 1784: 1783: 1782: 1778: 1776: 1775: 1774: 1772: 1771: 1749: 1747: 1746: 1745: 1741: 1739: 1738: 1737: 1735: 1734: 1712: 1710: 1709: 1708: 1704: 1702: 1701: 1700: 1698: 1697: 1678: 1676: 1675: 1674: 1670: 1668: 1667: 1666: 1664: 1663: 1655: 1650: 1649: 1647: 1643: 1638: 1637: 1635: 1629: 1628: 1626: 1616: 1573: 1572: 1568: 1563: 1560: 1559: 1526: 1523: 1520: 1519: 1517: 1505: 1502: 1499: 1498: 1496: 1489: 1486: 1485: 1484: 1480: 1478: 1477: 1476: 1475: 1470: 1467: 1466: 1465: 1461: 1459: 1458: 1457: 1456: 1451: 1448: 1447: 1446: 1442: 1440: 1439: 1438: 1437: 1429: 1426: 1423: 1422: 1420: 1411: 1408: 1405: 1404: 1402: 1393: 1390: 1387: 1386: 1384: 1360: 1357: 1354: 1353: 1351: 1339: 1336: 1333: 1332: 1330: 1323: 1320: 1319: 1318: 1314: 1312: 1311: 1310: 1309: 1304: 1301: 1300: 1299: 1295: 1293: 1292: 1291: 1290: 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2858: 2857: 2852: 2847: 2837: 2832: 2827: 2826: 2825: 2820: 2815: 2804: 2802: 2798: 2797: 2794:Standard Model 2790: 2789: 2782: 2775: 2767: 2760: 2759: 2752: 2734: 2727: 2705: 2699:978-3718600335 2698: 2676: 2617: 2610: 2571: 2552:(4): 579–588. 2529: 2522: 2494: 2487: 2465: 2458: 2431: 2429: 2426: 2425: 2424: 2419: 2412: 2409: 2387: 2386: 2383: 2382: 2375: 2367: 2358: 2355: 2353: 2351: 2349: 2346: 2345: 2343: 2336: 2328: 2320: 2317: 2311: 2303: 2296: 2293: 2287: 2279: 2257: 2254: 2252:is conserved. 2226: 2225: 2218: 2208: 2198: 2190: 2179: 2171: 2159: 2151: 2141: 2138: 2134:Standard Model 2120: 2119: 2107: 2104: 2101: 2098: 2095: 2089: 2086: 2080: 2074: 2069: 2065: 2062: 2056: 2053: 2031: 2028: 2017: 2016: 2015: 2014: 2003: 1995: 1991: 1987: 1984: 1981: 1975: 1970: 1951: 1948: 1944:Standard Model 1940: 1939: 1938: 1937: 1926: 1920: 1917: 1908: 1886:W and Z bosons 1877: 1870: 1854: 1853: 1850: 1832: 1829: 1822: 1814: 1806: 1802: 1801: 1798: 1795: 1792: 1785: 1777: 1769: 1765: 1764: 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355:Standard Model 349: 348: 346: 345: 338: 331: 323: 320: 319: 318: 317: 312: 307: 299: 298: 297:Flavour mixing 294: 293: 292: 291: 290: 289: 275: 266: 262: 251: 243: 234: 233: 232: 228: 215: 177: 176: 172: 171: 170: 169: 160: 151: 148: 135: 126: 114: 113: 109: 108: 107: 106: 96: 87: 78: 69: 66: 50: 49: 42: 41: 15: 9: 6: 4: 3: 2: 3215: 3204: 3201: 3199: 3196: 3194: 3191: 3190: 3188: 3173: 3172: 3163: 3161: 3160: 3151: 3150: 3147: 3141: 3138: 3136: 3133: 3131: 3128: 3126: 3123: 3121: 3118: 3116: 3113: 3112: 3110: 3106: 3096: 3093: 3091: 3088: 3086: 3083: 3081: 3078: 3076: 3073: 3071: 3068: 3066: 3065:String theory 3063: 3062: 3060: 3058: 3054: 3048: 3045: 3043: 3040: 3038: 3035: 3033: 3030: 3029: 3027: 3025: 3024:Supersymmetry 3021: 3015: 3012: 3010: 3007: 3005: 3002: 3000: 2997: 2996: 2994: 2990: 2984: 2981: 2979: 2976: 2972: 2969: 2968: 2967: 2964: 2962: 2959: 2957: 2954: 2953: 2951: 2947: 2944: 2942: 2936: 2930: 2927: 2925: 2922: 2920: 2917: 2915: 2912: 2911: 2909: 2905: 2888: 2885: 2883: 2880: 2878: 2875: 2873: 2870: 2868: 2865: 2864: 2863: 2860: 2856: 2853: 2851: 2848: 2846: 2843: 2842: 2841: 2838: 2836: 2833: 2831: 2828: 2824: 2821: 2819: 2816: 2814: 2811: 2810: 2809: 2806: 2805: 2803: 2799: 2795: 2788: 2783: 2781: 2776: 2774: 2769: 2768: 2765: 2755: 2753:0-7503-0160-0 2749: 2745: 2738: 2730: 2724: 2719: 2718: 2709: 2701: 2695: 2690: 2689: 2680: 2672: 2668: 2663: 2658: 2654: 2650: 2645: 2640: 2636: 2632: 2628: 2621: 2613: 2607: 2603: 2599: 2595: 2594: 2589: 2585: 2584:Brown, Laurie 2581: 2575: 2567: 2563: 2559: 2555: 2551: 2547: 2543: 2536: 2534: 2525: 2519: 2515: 2511: 2507: 2506: 2498: 2490: 2488:0-19-851961-3 2484: 2480: 2476: 2469: 2461: 2459:0-521-47652-6 2455: 2451: 2446: 2445: 2436: 2432: 2423: 2420: 2418: 2415: 2414: 2408: 2406: 2405:baryon number 2402: 2401:lepton number 2379: 2359: 2356: 2354: 2352: 2350: 2348: 2347: 2344: 2340: 2321: 2318: 2315: 2297: 2294: 2274: 2273: 2270: 2269: 2268: 2266: 2262: 2253: 2238: 2237:lepton number 2231: 2230:baryon number 2183: 2163: 2144: 2143: 2140:Neutron decay 2137: 2135: 2131: 2127: 2126: 2102: 2099: 2096: 2087: 2084: 2078: 2067: 2063: 2060: 2054: 2051: 2041: 2040: 2039: 2037: 2027: 2025: 2024: 2001: 1993: 1989: 1985: 1982: 1979: 1968: 1959: 1958: 1957: 1956: 1955: 1947: 1945: 1924: 1918: 1915: 1906: 1897: 1896: 1895: 1894: 1893: 1887: 1865: 1860: 1851: 1833: 1830: 1826: 1807: 1804: 1803: 1799: 1796: 1793: 1789: 1770: 1767: 1766: 1762: 1759: 1756: 1752: 1733: 1730: 1729: 1725: 1722: 1719: 1715: 1696: 1695: 1691: 1688: 1685: 1681: 1662: 1658: 1645: 1633: 1624: 1622: 1619: 1614: 1613: 1607: 1603: 1599: 1583: 1569: 1558: 1554: 1550: 1548: 1544: 1540: 1436: 1380: 1376: 1372: 1369: 1368: 1270: 1213: 1193: 1173: 1155: 1151: 1083: 1056: 1036: 1016: 998: 997: 983:May not exist 943: 922: 901: 881: 877: 862: 853: 848: 842: 837: 835: 821: 812: 807: 801: 796: 794: 793: 790: 787: 782: 779: 774: 768: 744: 740: 736: 733: 727: 724: 713: 705: 704: 703: 702: 701: 698: 696: 685: 660: 648: 641: 638: 632: 627: 623: 619: 616: 609: 608: 607: 606: 605: 602: 600: 596: 590: 563: 562:quantum field 550:gauge group, 549: 545: 535: 533: 528: 521: 516: 514: 510: 505: 480: 472: 469: 463: 458: 454: 450: 447: 432: 427: 423: 419: 414: 412: 409: 385: 376: 372: 369:relating the 368: 364: 360: 356: 344: 339: 337: 332: 330: 325: 324: 322: 321: 316: 313: 311: 308: 306: 303: 302: 301: 300: 296: 295: 287: 286: 282: 274: 270: 267: 261: 257: 250: 247: 246: 242: 238: 235: 227: 223: 219: 216: 213: 209: 205: 201: 197: 193: 190: 189: 188: 184: 181: 180: 179: 178: 174: 173: 168: 164: 161: 159: 155: 152: 147: 143: 139: 136: 134: 130: 129:Lepton number 127: 125: 121: 120:Baryon number 118: 117: 116: 115: 111: 110: 104: 100: 97: 95: 91: 88: 86: 82: 79: 77: 73: 70: 65: 61: 57: 54: 53: 52: 51: 48: 44: 43: 40: 35: 32: 31: 26: 22: 3169: 3157: 3047:Supergravity 2907:Constituents 2887:Weak isospin 2881: 2845:Color charge 2835:Gauge theory 2743: 2737: 2716: 2708: 2687: 2679: 2637:(1): 25–42. 2634: 2630: 2620: 2592: 2574: 2549: 2545: 2504: 2497: 2474: 2468: 2443: 2435: 2388: 2261:Proton decay 2259: 2256:Proton decay 2227: 2123: 2121: 2033: 2020: 2018: 1953: 1941: 1891: 1864:weak isospin 1648:hypercharge 1605: 1601: 1597: 1536: 786:Right-chiral 699: 695:weak isospin 677: 603: 541: 529: 517: 506: 430: 415: 375:weak isospin 362: 352: 284: 280: 272: 268: 259: 255: 248: 240: 236: 225: 221: 217: 211: 207: 203: 199: 195: 191: 186: 175:Combinations 166: 157: 145: 141: 138:Weak isospin 132: 123: 102: 93: 84: 75: 63: 59: 3108:Experiments 2999:Technicolor 2961:Dark matter 2855:Quark model 2823:Higgs boson 2818:Gauge boson 2422:weak charge 1615:Interaction 778:Left-chiral 686:units) and 548:electroweak 513:hypercharge 422:Higgs field 310:PMNS matrix 183:Hypercharge 81:Strangeness 25:Weak charge 21:Hypercharge 3187:Categories 3115:Gran Sasso 2939:Beyond the 2914:CKM matrix 2801:Background 2644:1503.01756 2428:References 538:Definition 305:CKM matrix 210:′ + 99:Bottomness 2671:0163-8998 2100:− 1986:− 1625:Electric 1617:mediated 1570:θ 1539:chirality 1148:−2 1142:−1 1081:−1 1060:−1 969:−1 838:Electric 797:Electric 737:− 544:generator 534:in 1961. 418:conserved 3159:Category 3140:Tevatron 2992:Theories 2949:Evidence 2813:Fermions 2411:See also 2319:  + 2295:→   1636:isospin 1602:g′ 1543:helicity 879:Leptons 789:fermions 781:fermions 771:Fermion 511:for the 163:X-charge 45:Flavour 3171:Commons 3135:Super-K 2971:problem 2649:Bibcode 2554:Bibcode 1848:⁠ 1836:⁠ 1834:− 1768:Strong 1627:charge 1530:⁠ 1518:⁠ 1516:− 1509:⁠ 1497:⁠ 1495:− 1433:⁠ 1421:⁠ 1415:⁠ 1403:⁠ 1401:− 1397:⁠ 1385:⁠ 1383:− 1364:⁠ 1352:⁠ 1343:⁠ 1331:⁠ 1267:⁠ 1255:⁠ 1249:⁠ 1237:⁠ 1231:⁠ 1219:⁠ 1153:Quarks 1077:⁠ 1065:⁠ 1063:− 965:⁠ 953:⁠ 867:charge 852:isospin 826:charge 811:isospin 520:commute 353:In the 105:′ 90:Topness 56:Isospin 34:Flavour 2750:  2725:  2696:  2669:  2608:  2520:  2485:  2456:  2371:γ 2332:π 2292:  2213:ν 2122:where 1999:  1922:  1805:Higgs 1744:γ 1604:, and 1581:  1566:  1048:τ 1028:μ 973:ν 939:τ 934:ν 918:μ 913:ν 892:ν 865:hyper- 841:charge 824:hyper- 800:charge 773:family 678:where 658:  595:photon 492:  445:  416:It is 361:, the 3037:NMSSM 2639:arXiv 2038:via: 1660:Weak 1646:Weak 1634:Weak 1621:Boson 863:Weak 850:Weak 822:Weak 809:Weak 552:SU(2) 365:is a 278:= 5 ( 254:= 2 ( 220:= 2 ( 72:Charm 3032:MSSM 2748:ISBN 2723:ISBN 2694:ISBN 2667:ISSN 2606:ISBN 2518:ISBN 2483:ISBN 2454:ISBN 2403:and 2235:and 557:U(1) 523:U(1) 411:U(1) 3130:SNO 3125:LHC 3120:INO 2657:doi 2598:doi 2562:doi 2510:doi 2130:GUT 1852:+1 1689:±1 1686:±1 597:of 271:+ 2 194:= ( 144:or 62:or 23:or 3189:: 2665:. 2655:. 2647:. 2635:65 2633:. 2629:. 2604:. 2586:; 2582:; 2560:. 2550:22 2548:. 2544:. 2532:^ 2516:. 2481:. 2477:. 2452:. 2450:52 2407:. 2394:− 2267:. 2247:− 2203:+ 2185:+ 2165:→ 2026:. 1882:Q 1866:, 1831:0 1800:0 1797:0 1794:0 1763:0 1760:0 1757:0 1726:0 1723:0 1720:0 1692:0 1600:, 1549:. 1513:0 1474:, 1455:, 1377:, 1373:, 1347:0 1308:, 1289:, 1195:, 1175:, 1145:0 1121:, 1102:, 1038:, 1018:, 994:0 991:0 988:0 948:0 924:, 903:, 601:. 525:em 413:. 283:− 258:− 239:: 224:− 206:+ 202:+ 198:+ 185:: 165:: 156:: 140:: 131:: 122:: 101:: 92:: 83:: 74:: 58:: 36:in 2786:e 2779:t 2772:v 2756:. 2731:. 2673:. 2659:: 2651:: 2641:: 2614:. 2600:: 2568:. 2564:: 2556:: 2526:. 2512:: 2491:. 2462:. 2396:L 2392:B 2361:2 2307:e 2283:p 2249:L 2245:B 2240:L 2233:B 2219:e 2194:e 2175:p 2155:n 2125:X 2106:) 2103:L 2097:B 2094:( 2088:2 2085:5 2079:= 2073:W 2068:Y 2064:+ 2061:X 2055:2 2052:1 2002:, 1994:3 1990:T 1983:Q 1980:= 1974:W 1969:Y 1925:. 1919:0 1916:= 1911:W 1907:Y 1888:. 1878:W 1875:Y 1871:3 1868:T 1845:2 1842:/ 1839:1 1818:H 1781:g 1707:Z 1673:W 1654:W 1651:Y 1642:3 1639:T 1630:Q 1606:e 1598:g 1584:, 1575:W 1527:3 1524:/ 1521:2 1506:3 1503:/ 1500:1 1488:R 1483:b 1469:R 1464:s 1450:R 1445:d 1430:3 1427:/ 1424:1 1419:+ 1412:2 1409:/ 1406:1 1394:3 1391:/ 1388:1 1379:b 1375:s 1371:d 1361:3 1358:/ 1355:4 1350:+ 1340:3 1337:/ 1334:2 1329:+ 1322:R 1317:t 1303:R 1298:c 1284:R 1279:u 1264:3 1261:/ 1258:1 1253:+ 1246:2 1243:/ 1240:1 1235:+ 1228:3 1225:/ 1222:2 1217:+ 1205:t 1185:c 1165:u 1135:R 1130:τ 1116:R 1111:μ 1097:R 1092:e 1074:2 1071:/ 1068:1 1008:e 978:R 962:2 959:/ 956:1 951:+ 897:e 873:W 870:Y 859:3 856:T 845:Q 832:W 829:Y 818:3 815:T 804:Q 750:) 745:3 741:T 734:Q 731:( 728:2 725:= 719:W 714:Y 691:3 688:T 680:Q 661:, 653:W 649:Y 642:2 639:1 633:+ 628:3 624:T 620:= 617:Q 582:Z 569:W 565:B 554:× 486:W 481:Y 473:2 470:1 464:+ 459:3 455:T 451:= 448:Q 434:3 431:T 391:W 386:Y 342:e 335:t 328:v 288:) 285:L 281:B 276:W 273:Y 269:X 265:) 263:3 260:T 256:Q 252:W 249:Y 244:W 241:Y 231:) 229:3 226:I 222:Q 218:Y 214:) 212:T 208:B 204:C 200:S 196:B 192:Y 187:Y 167:X 158:Q 149:3 146:T 142:T 133:L 124:B 103:B 94:T 85:S 76:C 67:3 64:I 60:I 27:.

Index

Hypercharge
Weak charge
Flavour
particle physics
quantum numbers
Isospin
Charm
Strangeness
Topness
Bottomness
Baryon number
Lepton number
Weak isospin
Electric charge
X-charge
Hypercharge
Weak hypercharge
BL
CKM matrix
PMNS matrix
Flavour complementarity
v
t
e
Standard Model
particle physics
quantum number
electric charge
weak isospin
gauge symmetry

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