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Proton–proton chain

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Comparing the mass of the final helium-4 atom with the masses of the four protons reveals that 0.7 percent of the mass of the original protons has been lost. This mass has been converted into energy, in the form of kinetic energy of produced particles, gamma rays, and neutrinos released during each
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This process, mediated by the strong nuclear force rather than the weak force, is extremely fast by comparison to the first step. It is estimated that, under the conditions in the Sun's core, each newly created deuterium nucleus exists for only about one second before it is converted into helium-3.
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0.02 percent. Since half the neutrinos produced in branches II and III are produced in the first step (synthesis of a deuteron), only about 8.35 percent of neutrinos come from the later steps (see below), and about 91.65 percent are from deuteron synthesis. However, another solar model from around
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fusion processes at different temperatures (T). The dashed line shows the combined energy generation of the PP and CNO processes within a star. At the Sun's core temperature of 15.5 million K the PP process is dominant. The PP process and the CNO process are equal at around 20
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are the much more common result of proton–proton reactions within the star, and diprotons almost immediately decay back into two protons. Since the conversion of hydrogen to helium is slow, the complete conversion of the hydrogen initially in the
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branch. Other even rarer reactions may occur. The rate of these reactions is very low due to very small cross-sections, or because the number of reacting particles is so low that any reactions that might happen are statistically insignificant.
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of the same basic interaction, where the electron passes to the right side of the reaction as a positron. This is represented in the figure of proton–proton and electron-capture reactions in a star, available at the NDM'06 web site.
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the same time gives only 7.14 percent of neutrinos from the later steps and 92.86 percent from the synthesis of deuterium nuclei. The difference is apparently due to slightly different assumptions about the composition and
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In the Sun, each helium-3 nucleus produced in these reactions exists for only about 400 years before it is converted into helium-4. Once the helium-3 has been produced, there are four possible paths to generate
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See Figure 2. The caption is not very clear but it has been confirmed that the percentages refer to how much of each reaction takes place, or equivalently how much helium-4 is produced by each branch.
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Neutrinos do not interact significantly with matter and therefore do not heat the interior and thereby help support the Sun against gravitational collapse. Their energy is lost: the neutrinos in the
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rather than as neutrinos. The starting figures used are the ones mentioned higher in this article. The table concerns only the 99% of the power and neutrinos that come from the
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Energy released as gamma rays will interact with electrons and protons and heat the interior of the Sun. Also kinetic energy of fusion products (e.g. of the two protons and the
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Note that the energies in the second reaction above are the energies of the neutrinos that are produced by the reaction. 90 percent of the neutrinos produced in the reaction of
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The last three stages of this chain, plus the positron annihilation, contribute a total of 18.209 MeV, though much of this is lost to the neutrino.
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in the normal sense. In most nuclear reactions, a chain reaction designates a reaction that produces a product, such as neutrons given off during
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in the Sun). In this reaction, helium-3 captures a proton directly to give helium-4, with an even higher possible neutrino energy (up to
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is about 0.862 MeV, almost all of which is lost to the neutrino if the decay goes directly to the stable lithium.
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The theory that proton–proton reactions are the basic principle by which the Sun and other stars burn was advocated by
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Bellini, G.; et al. (2 February 2012). "First Evidence of pep Solar Neutrinos by Direct Detection in Borexino".
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Adelberger, Eric G.; et al. (12 April 2011). "Solar fusion cross sections. II. The pp chain and CNO cycles".
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reaction) adds energy to the plasma in the Sun. This heating keeps the core of the Sun hot and prevents it from
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for the energy released by this reaction plus the ensuing annihilation, some of which is lost to the neutrino.
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attempted to calculate the rates of various reactions in stars. Starting with two protons combining to give a
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he found what we now call Branch II of the proton–proton chain. But he did not consider the reaction of two
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Aldo Serenelli; et al. (Nov 2009). "New Solar Composition: The Problem With Solar Models Revisited".
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After it is formed, the deuteron produced in the first stage can fuse with another proton to produce the
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released by the pep reaction are far more energetic: while neutrinos produced in the first step of the
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Adelberger, E. G.; et al. (2010). "Solar fusion cross sections. II. Theppchain and CNO cycles".
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in the 1920s. At the time, the temperature of the Sun was considered to be too low to overcome the
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This reaction is predicted theoretically, but it has never been observed due to its rarity (about
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of the protons through the repulsive barrier allows for fusion at a lower temperature than the
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of this reaction experimentally because it is so low but it can be calculated from theory.
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but 2.2 percent of this energy (0.59 MeV) is lost to the neutrinos that are produced. The
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This is the rate-limiting reaction and is extremely slow due to it being initiated by the
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nuclei (Branch I) which we now know to be important. This was part of the body of work in
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The following table calculates the amount of energy lost to neutrinos and the amount of "
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chains carry away 2.0%, 4.0%, and 28.3% of the energy in those reactions, respectively.
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chain is not a major source of energy in the Sun, but it was very important in the
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of the individual reactions. The total energy yield of one whole chain is
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Although sometimes called the "proton–proton chain reaction", it is not a
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Burbidge, E.; Burbidge, G.; Fowler, William; Hoyle, F. (1 October 1957).
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can also be produced by the rare pep (proton–electron–proton) reaction (
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releasing 26.73 MeV of energy, some of which is lost to the neutrinos.
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One of the fusion reactions by which stars convert hydrogen to helium
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About 99% of the energy output of the sun comes from the various
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waits 9 billion years before it successfully fuses with another
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In the Sun, the frequency ratio of the pep reaction versus the
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under its own weight as it would if the sun were to cool down.
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chain proceeds at slow rate, resulting in a low production of
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This time and the two other times above come from: Byrne, J.
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Int'l Conference on Neutrino and Dark Matter, 7 Sept 2006,
2640:: 42, 59, (1971), The Proton type-nuclear fission reaction. 2455:, the pep reaction produces sharp-energy-line neutrinos of 711:, helium-4 is produced by fusing two helium-3 nuclei; the 770:. According to one model of the sun, 83.3 percent of the 486:(which is the same as the PEP reaction, see below) has a 119:) of the protons is high enough to overcome their mutual 228:
The first step in all the branches is the fusion of two
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because it generates very high energy neutrinos (up to
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In general, proton–proton fusion can occur only if the
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Proton–proton and electron-capture reactions in a star
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It has not been possible to measure the 3034: 2976: 2893: 2809: 2778:, Dover Publications, Mineola, NY, 2011, 2690: 2529: 2840:Calculated from model AGSS09 in Table 3. 2746:(2nd ed.). Chichester: John Wiley. 2282: 2126: 794:branches is produced via branch I while 60: 3392: 2852:An Introduction to Stellar Astrophysics 2501: 2470:reactions can be seen as two different 1412:, while the remaining 10 percent carry 3007:Claus E. Rolfs and William S. Rodney, 2941: 2909: 2907: 2905: 44:of the relative energy output (ε) of 7: 2867:"Synthesis of the Elements in Stars" 2704: 2702: 2045:The mass–energy relationship gives 73:, also commonly referred to as the 25: 2798:The Astrophysical Journal Letters 2128:Luminosity production in the sun 810:There is also the extremely rare 3467: 3455: 3443: 3431: 3419: 3407: 3395: 3098: 2443:reaction is 1:400. However, the 2451:reaction range in energy up to 3053:10.1103/PhysRevLett.108.051302 374:from the environment into two 80:, is one of two known sets of 1: 2742:Phillips, Anthony C. (1999). 3105:Proton-proton chain reaction 2828:10.1088/0004-637X/705/2/L123 2776:Neutrons, Nuclei, and Matter 2665:"Energy Production in Stars" 2651:Introductory Nuclear Physics 130:-producing events are rare. 2914:Iliadis, Christian (2015). 2709:Iliadis, Christian (2007). 2303: 1909: 1463: 1031: 844: 798:produces 16.68 percent and 563: 386: 256: 170:. After the development of 3511: 2663:Hans Bethe (Mar 1, 1939). 1023: 29: 2987:10.1103/RevModPhys.83.195 2965:Reviews of Modern Physics 2895:10.1103/RevModPhys.29.547 2874:Reviews of Modern Physics 2571:"The Proton–Proton Chain" 2548:10.1103/RevModPhys.83.195 2518:Reviews of Modern Physics 2118:electromagnetic radiation 818:The overall reaction is: 174:, it was discovered that 3490:Nuclear fusion reactions 2917:Nuclear physics of stars 2711:Nuclear Physics of Stars 790:produced by the various 216:for which Bethe won the 3185:Double electron capture 3023:Physical Review Letters 3009:Cauldrons in the Cosmos 2713:. Weinheim: Wiley-VCH. 2472:Feynman representations 2463:collaboration in 2012. 1458:Proton–proton III chain 224:The proton–proton chain 214:stellar nucleosynthesis 121:electrostatic repulsion 2692:10.1103/PhysRev.55.434 2653:, Wiley, 1987, p. 537. 2288: 1876:solar neutrino problem 1459: 1021: 1020:Proton–proton II chain 218:Nobel Prize in Physics 66: 58: 18:Proton-proton reaction 2286: 1457: 1019: 158:History of the theory 64: 40: 3107:at Wikimedia Commons 2744:The Physics of Stars 2609:. pp. 119–121. 2490:Triple-alpha process 823:4 H + 2 e → He + 2 ν 240:, converting into a 3329:Photodisintegration 3250:Proton–proton chain 3220:Spontaneous fission 3200:Isomeric transition 3195:Internal conversion 3045:2012PhRvL.108e1302B 2886:1957RvMP...29..547B 2820:2009ApJ...705L.123S 2683:1939PhRv...55..434B 2607:John Wiley and Sons 2540:2011RvMP...83..195A 2129: 1408:carry an energy of 512:in the core of the 84:reactions by which 71:proton–proton chain 2850:LeBlanc, Francis. 2649:Kenneth S. Krane, 2289: 2127: 1460: 1022: 737:with pre-existing 506:weak nuclear force 67: 59: 3383: 3382: 3379: 3378: 3210:Positron emission 3180:Double beta decay 3142:Nuclear processes 3103:Media related to 2927:978-3-527-33649-4 2466:Both the pep and 2435: 2434: 2276: 2275: 2041: 2040: 1852: 1851: 1357: 1356: 959: 958: 678: 677: 482: 481: 378:. Including this 358: 357: 250:electron neutrino 172:quantum mechanics 16:(Redirected from 3502: 3472: 3471: 3470: 3460: 3459: 3458: 3448: 3447: 3446: 3436: 3435: 3424: 3423: 3422: 3412: 3411: 3410: 3400: 3399: 3391: 3340: 3240:Deuterium fusion 3205:Neutron emission 3190:Electron capture 3135: 3128: 3121: 3112: 3102: 3086: 3079: 3073: 3072: 3038: 3018: 3012: 3005: 2999: 2998: 2980: 2960: 2954: 2953: 2947: 2939: 2911: 2900: 2899: 2897: 2871: 2862: 2856: 2855: 2847: 2841: 2839: 2813: 2804:(2): L123–L127. 2793: 2787: 2772: 2766: 2765: 2739: 2733: 2732: 2706: 2697: 2696: 2694: 2660: 2654: 2647: 2641: 2627: 2621: 2620: 2596: 2590: 2589: 2587: 2586: 2577:. 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1238: 1235: 1234: 1233: 1229: 1227: 1226: 1225: 1223: 1222: 1212: 1210: 1209: 1208: 1204: 1201: 1200: 1199: 1197: 1186: 1184: 1183: 1182: 1178: 1176: 1175: 1174: 1172: 1161: 1159: 1158: 1157: 1153: 1150: 1149: 1148: 1146: 1139: 1127: 1125: 1124: 1123: 1119: 1117: 1116: 1115: 1113: 1112: 1102: 1100: 1099: 1098: 1094: 1091: 1090: 1089: 1087: 1076: 1074: 1073: 1072: 1068: 1065: 1064: 1063: 1061: 1050: 1048: 1047: 1046: 1042: 1039: 1038: 1037: 1035: 1028: 1026:Lithium burning 1014: 1009: 1000: 998: 997: 996: 992: 990: 989: 988: 987: 983: 979: 972: 968: 965:26.732 MeV 964: 954:12.859 MeV 953: 942: 940: 939: 938: 934: 931: 930: 929: 927: 915: 913: 912: 911: 907: 904: 903: 902: 900: 889: 887: 886: 885: 881: 878: 877: 876: 874: 863: 861: 860: 859: 855: 852: 851: 850: 848: 841: 836: 826: 822: 811: 799: 795: 791: 785: 783: 782: 781: 777: 775: 774: 773: 771: 763: 751: 749: 748: 747: 743: 741: 740: 739: 738: 733: 731: 730: 729: 725: 723: 722: 721: 720: 716: 712: 708: 702: 700: 699: 698: 694: 692: 691: 690: 688: 672: 660: 658: 657: 656: 652: 650: 649: 648: 646: 645: 634: 632: 631: 630: 626: 623: 622: 621: 619: 608: 606: 605: 604: 600: 597: 596: 595: 593: 582: 580: 579: 578: 574: 571: 570: 569: 567: 554: 552: 551: 550: 546: 544: 543: 542: 540: 476: 464: 461: 460: 459: 455: 453: 452: 451: 449: 448: 438: 436: 435: 434: 430: 427: 426: 425: 423: 417: 415: 414: 413: 409: 407: 406: 405: 403: 352: 340: 337: 336: 335: 331: 329: 328: 327: 325: 324: 314: 312: 311: 310: 306: 304: 303: 302: 300: 290: 288: 287: 286: 282: 279: 278: 277: 275: 238:beta plus decay 226: 207: 205: 204: 203: 202: 168:Coulomb barrier 160: 137:core of the Sun 75: 35: 28: 23: 22: 15: 12: 11: 5: 3508: 3506: 3498: 3497: 3492: 3482: 3481: 3477: 3476: 3464: 3452: 3440: 3428: 3416: 3404: 3381: 3380: 3377: 3376: 3374: 3373: 3371:(n-p) reaction 3367: 3365: 3361: 3360: 3358: 3357: 3355:Proton capture 3352: 3346: 3344: 3337: 3336: 3331: 3325: 3323: 3317: 3316: 3314: 3313: 3308: 3303: 3295: 3287: 3282: 3277: 3272: 3267: 3262: 3257: 3252: 3247: 3242: 3236: 3234: 3226: 3225: 3223: 3222: 3217: 3212: 3207: 3202: 3197: 3192: 3187: 3182: 3177: 3172: 3167: 3162: 3156: 3154: 3146: 3145: 3140: 3138: 3137: 3130: 3123: 3115: 3109: 3108: 3094: 3093:External links 3091: 3088: 3087: 3074: 3013: 3000: 2955: 2926: 2901: 2880:(4): 547–650. 2857: 2842: 2788: 2767: 2752: 2734: 2719: 2698: 2677:(5): 434–456. 2655: 2642: 2622: 2615: 2591: 2562: 2500: 2499: 2497: 2494: 2493: 2492: 2487: 2480: 2477: 2437: 2436: 2433: 2432: 2424: 2416: 2408: 2405: 2398: 2389: 2382: 2379: 2372: 2363: 2356: 2353: 2346: 2338: 2331: 2328: 2321: 2312: 2280: 2277: 2274: 2273: 2270: 2267: 2264: 2262: 2259: 2255: 2254: 2248: 2242: 2239: 2236: 2230: 2226: 2225: 2219: 2216: 2213: 2207: 2201: 2197: 2196: 2190: 2187: 2184: 2178: 2172: 2168: 2167: 2160: 2153: 2146: 2139: 2138:He-4 produced 2134: 2080: 2071: 2060:26.73 MeV 2054: 2053:Energy release 2051: 2043: 2042: 2039: 2038: 2030: 2022: 2014: 2011: 2004: 1996: 1989: 1986: 1979: 1970: 1963: 1960: 1953: 1944: 1937: 1934: 1927: 1918: 1891: 1884: 1880:14.06 MeV 1854: 1853: 1850: 1849: 1843: 1834: 1826: 1823: 1820: 1817: 1810: 1801: 1793: 1792: 1790: 1782: 1774: 1767: 1764: 1757: 1749: 1742: 1739: 1732: 1723: 1716: 1713: 1710: 1707: 1700: 1691: 1683: 1682: 1676: 1668: 1661: 1658: 1651: 1642: 1635: 1632: 1625: 1616: 1609: 1606: 1599: 1590: 1582: 1581: 1576: 1573: 1570: 1567: 1559: 1551: 1543: 1540: 1533: 1524: 1517: 1514: 1507: 1498: 1491: 1488: 1481: 1472: 1451: 1444: 1436: 1425: 1414:0.383 MeV 1410:0.861 MeV 1403: 1395: 1385: 1377: 1359: 1358: 1355: 1354: 1352:17.35 MeV 1349: 1346: 1343: 1340: 1333: 1324: 1316: 1313: 1306: 1297: 1290: 1287: 1280: 1271: 1263: 1262: 1260:0.383 MeV 1257: 1254: 1251:0.861 MeV 1248: 1245: 1236: 1228: 1220: 1217: 1211: 1202: 1195: 1192: 1185: 1177: 1170: 1167: 1160: 1151: 1143: 1142: 1137: 1134: 1126: 1118: 1110: 1107: 1101: 1092: 1085: 1082: 1075: 1066: 1059: 1056: 1049: 1040: 1013: 1006: 999: 991: 961: 960: 957: 956: 951: 948: 941: 932: 924: 921: 914: 905: 898: 895: 888: 879: 872: 869: 862: 853: 840: 833: 829: 828: 824: 784: 776: 750: 742: 732: 724: 719:branches fuse 701: 693: 680: 679: 676: 675: 673:5.493 MeV 670: 667: 659: 651: 643: 640: 633: 624: 617: 614: 607: 598: 591: 588: 581: 572: 553: 545: 508:. The average 484: 483: 480: 479: 477:1.442 MeV 474: 471: 462: 454: 446: 443: 437: 428: 416: 408: 400: 397: 394: 360: 359: 356: 355: 350: 347: 338: 330: 322: 319: 313: 305: 298: 295: 289: 280: 273: 270: 267: 264: 244:by emitting a 225: 222: 206: 197:nucleus and a 159: 156: 144:chain reaction 113:kinetic energy 100:, whereas the 82:nuclear fusion 26: 24: 14: 13: 10: 9: 6: 4: 3: 2: 3507: 3496: 3493: 3491: 3488: 3487: 3485: 3475: 3465: 3463: 3453: 3451: 3441: 3439: 3434: 3429: 3427: 3417: 3415: 3405: 3403: 3398: 3393: 3389: 3372: 3369: 3368: 3366: 3362: 3356: 3353: 3351: 3348: 3347: 3345: 3341: 3335: 3332: 3330: 3327: 3326: 3324: 3318: 3312: 3309: 3307: 3304: 3302: 3300: 3296: 3294: 3292: 3288: 3286: 3283: 3281: 3278: 3276: 3273: 3271: 3268: 3266: 3263: 3261: 3258: 3256: 3253: 3251: 3248: 3246: 3243: 3241: 3238: 3237: 3235: 3233: 3227: 3221: 3218: 3216: 3213: 3211: 3208: 3206: 3203: 3201: 3198: 3196: 3193: 3191: 3188: 3186: 3183: 3181: 3178: 3176: 3175:Cluster decay 3173: 3171: 3168: 3166: 3163: 3161: 3158: 3157: 3155: 3153: 3147: 3143: 3136: 3131: 3129: 3124: 3122: 3117: 3116: 3113: 3106: 3101: 3097: 3096: 3092: 3084: 3078: 3075: 3070: 3066: 3062: 3058: 3054: 3050: 3046: 3042: 3037: 3032: 3029:(5): 051302. 3028: 3024: 3017: 3014: 3010: 3004: 3001: 2996: 2992: 2988: 2984: 2979: 2974: 2970: 2966: 2959: 2956: 2951: 2945: 2937: 2933: 2929: 2923: 2919: 2918: 2910: 2908: 2906: 2902: 2896: 2891: 2887: 2883: 2879: 2875: 2868: 2861: 2858: 2853: 2846: 2843: 2837: 2833: 2829: 2825: 2821: 2817: 2812: 2807: 2803: 2799: 2792: 2789: 2785: 2781: 2777: 2771: 2768: 2763: 2759: 2755: 2749: 2745: 2738: 2735: 2730: 2726: 2722: 2720:9783527406029 2716: 2712: 2705: 2703: 2699: 2693: 2688: 2684: 2680: 2676: 2672: 2671: 2666: 2659: 2656: 2652: 2646: 2643: 2639: 2635: 2631: 2626: 2623: 2618: 2616:0-470-09220-3 2612: 2608: 2604: 2603: 2595: 2592: 2581:on 2016-06-20 2580: 2576: 2572: 2566: 2563: 2557: 2553: 2549: 2545: 2541: 2537: 2532: 2527: 2523: 2519: 2512: 2510: 2508: 2506: 2502: 2495: 2491: 2488: 2486: 2483: 2482: 2478: 2476: 2473: 2464: 2462: 2457:1.44 MeV 2453:0.42 MeV 2446: 2429: 2409: 2406: 2402: 2383: 2380: 2376: 2357: 2354: 2350: 2332: 2329: 2325: 2306: 2305: 2302: 2301: 2300: 2298: 2294: 2285: 2278: 2271: 2268: 2265: 2263: 2260: 2257: 2256: 2249: 2243: 2240: 2237: 2231: 2228: 2227: 2220: 2217: 2214: 2208: 2202: 2199: 2198: 2191: 2188: 2185: 2179: 2173: 2170: 2169: 2161: 2157:of luminosity 2154: 2147: 2140: 2135: 2132: 2131: 2125: 2119: 2115: 2110: 2095: 2093: 2084: 2063: 2052: 2050: 2035: 2015: 2012: 2008: 1990: 1987: 1983: 1964: 1961: 1957: 1938: 1935: 1931: 1912: 1911: 1908: 1907: 1906: 1903:18.8 MeV 1899: 1885: 1883: 1877: 1868: 1857: 1847: 1827: 1824: 1821: 1818: 1814: 1795: 1794: 1791: 1787: 1768: 1765: 1761: 1743: 1740: 1736: 1717: 1714: 1711: 1708: 1704: 1685: 1684: 1662: 1659: 1655: 1636: 1633: 1629: 1610: 1607: 1603: 1584: 1583: 1579:1.59 MeV 1577: 1574: 1571: 1568: 1563: 1544: 1541: 1537: 1518: 1515: 1511: 1492: 1489: 1485: 1466: 1465: 1462: 1461: 1456: 1445: 1443: 1419: 1370: 1350: 1347: 1344: 1341: 1337: 1317: 1314: 1310: 1291: 1288: 1284: 1265: 1264: 1258: 1255: 1249: 1246: 1241: 1221: 1218: 1215: 1196: 1193: 1189: 1171: 1168: 1164: 1145: 1144: 1140:1.59 MeV 1138: 1135: 1130: 1111: 1108: 1105: 1086: 1083: 1079: 1060: 1057: 1053: 1034: 1033: 1030: 1029: 1027: 1018: 1007: 1005: 976: 952: 949: 945: 925: 922: 918: 899: 896: 892: 873: 870: 866: 847: 846: 843: 842: 834: 832: 821: 820: 819: 816: 808: 806: 788: 769: 760: 758: 705: 684: 671: 668: 663: 644: 641: 637: 618: 615: 611: 592: 589: 585: 566: 565: 562: 561: 560: 557: 538: 534: 530: 525: 523: 522:cross-section 519: 515: 511: 507: 502: 500: 496: 492: 490: 475: 472: 467: 447: 444: 441: 420: 401: 398: 395: 392: 389: 388: 385: 384: 383: 381: 377: 373: 369: 365: 353:0.42 MeV 351: 348: 343: 323: 320: 317: 299: 296: 293: 274: 271: 268: 265: 262: 259: 258: 255: 254: 253: 251: 247: 243: 239: 235: 231: 223: 221: 219: 215: 200: 196: 192: 187: 185: 181: 180:wavefunctions 177: 173: 169: 165: 157: 155: 153: 149: 145: 140: 138: 133: 129: 124: 122: 118: 114: 109: 107: 103: 99: 95: 91: 87: 83: 79: 72: 63: 55: 51: 47: 46:proton–proton 43: 39: 33: 19: 3474:Solar System 3334:Photofission 3298: 3290: 3249: 3077: 3026: 3022: 3016: 3008: 3003: 2968: 2964: 2958: 2916: 2877: 2873: 2860: 2851: 2845: 2801: 2797: 2791: 2775: 2770: 2743: 2737: 2710: 2674: 2668: 2658: 2650: 2645: 2637: 2633: 2630:Ishfaq Ahmad 2625: 2601: 2594: 2583:. Retrieved 2579:the original 2574: 2565: 2521: 2517: 2465: 2438: 2290: 2152:energy lost 2141:Percent loss 2111: 2096: 2064: 2056: 2044: 1893: 1890:(Hep) branch 1869: 1858: 1855: 1371: 1360: 962: 830: 817: 809: 807:of the sun. 761: 685: 681: 526: 503: 488: 485: 380:annihilation 361: 227: 188: 186:prediction. 161: 141: 126:In the Sun, 125: 110: 106:solar masses 74: 70: 68: 3462:Outer space 3450:Spaceflight 3160:Alpha decay 3150:Radioactive 2971:: 195–245. 2634:The Nucleus 2166:luminosity 2145:production 805:metallicity 497:) of 1.442 152:decay chain 117:temperature 3484:Categories 3311:rp-process 3285:Si burning 3275:Ne burning 3245:Li burning 3165:Beta decay 3083:Session 14 2784:0486482383 2753:0471987972 2585:2018-07-30 2524:(1): 201. 2496:References 2229:Branch III 2162:Percentage 2136:Percent of 2092:collapsing 1865:25 MK 1431:to stable 1418:metastable 1367:25 MK 1024:See also: 980:10 MK 493:(released 376:gamma rays 368:annihilate 191:Hans Bethe 3426:Astronomy 3414:Chemistry 3322:processes 3306:p-process 3280:O burning 3270:C burning 3260:α process 3255:CNO cycle 3069:118444784 3036:1110.3230 2995:119117147 2978:1004.2318 2944:cite book 2936:908071061 2811:0909.2668 2556:119117147 2531:1004.2318 2485:CNO cycle 2445:neutrinos 2200:Branch II 2159:produced 2150:amount of 2086:from the 1896:0.3  768:CNO cycle 757:beryllium 220:in 1967. 195:deuterium 189:In 1939, 184:classical 176:tunneling 132:Diprotons 102:CNO cycle 42:Logarithm 3364:Exchange 3301:-process 3293:-process 3265:Triple-α 3061:22400925 2836:14323767 2762:40948449 2729:85897502 2479:See also 2461:Borexino 2293:deuteron 2171:Branch I 2164:of total 2148:Relative 978:. Below 973:18  755:to form 531:, light 372:electron 370:with an 364:positron 246:positron 234:deuteron 199:positron 128:deuteron 90:hydrogen 88:convert 54:Triple-α 3402:Physics 3388:Portals 3343:Capture 3230:Stellar 3041:Bibcode 2882:Bibcode 2816:Bibcode 2679:Bibcode 2536:Bibcode 2407:+  2381:→  2355:+  2330:+  2253:0.015% 2241:0.0057% 2133:Branch 2107:p–p III 2013:+  1988:+  1962:→  1936:+  1872:p–p III 1861:p–p III 1828:2  1825:→  1766:+  1741:+  1715:→  1660:+  1634:→  1608:+  1575:+  1542:+  1516:→  1490:+  1448:p–p III 1348:+  1315:→  1289:+  1256:/  1247:+  1219:+  1194:→  1169:+  1136:+  1109:+  1084:→  1058:+  950:+  926:2  923:+  897:→  871:+  800:p–p III 717:p–p III 669:+  642:+  616:→  590:+  533:isotope 473:+  422:→  396:+  349:+  272:→  266:+  248:and an 242:neutron 232:into a 230:protons 178:of the 148:fission 3495:Proton 3067:  3059:  2993:  2934:  2924:  2834:  2786:, p 8. 2782:  2760:  2750:  2727:  2717:  2613:  2554:  2420:ν 2404:  2378:  2352:  2327:  2247:0.014% 2224:16.4% 2206:16.68% 2195:83.6% 2105:, and 2103:p–p II 2026:ν 2010:  1985:  1959:  1933:  1888:p–p IV 1822:  1819:  1816:  1789:  1778:ν 1763:  1738:  1712:  1709:  1706:  1672:γ 1657:  1631:  1605:  1572:  1569:  1566:  1555:γ 1539:  1513:  1487:  1450:branch 1363:p–p II 1345:  1342:  1339:  1312:  1286:  1253:  1244:  1232:ν 1191:  1166:  1133:  1122:γ 1081:  1055:  1012:branch 1010:p–p II 982:, the 947:  920:  894:  868:  839:branch 812:p–p IV 796:p–p II 713:p–p II 666:  655:γ 639:  613:  587:  537:helium 529:stable 518:proton 510:proton 495:energy 470:  458:ν 393:  346:  334:ν 263:  94:helium 48:(PP), 3438:Stars 3320:Other 3152:decay 3065:S2CID 3031:arXiv 2991:S2CID 2973:arXiv 2870:(PDF) 2832:S2CID 2806:arXiv 2552:S2CID 2526:arXiv 2272:100% 2269:97.7% 2266:2.34% 2258:total 2238:28.3% 2235:0.02% 2218:16.0% 2215:0.67% 2189:81.6% 2186:1.67% 2177:83.3% 2099:p–p I 2088:p–p I 969:p–p I 837:p–p I 709:p–p I 707:. In 491:value 366:will 86:stars 78:chain 3057:PMID 2950:link 2932:OCLC 2922:ISBN 2780:ISBN 2758:OCLC 2748:ISBN 2725:OCLC 2715:ISBN 2611:ISBN 2261:100% 1886:The 1870:The 1859:The 1446:The 1361:The 1008:The 835:The 715:and 362:The 69:The 52:and 3049:doi 3027:108 2983:doi 2890:doi 2824:doi 2802:705 2687:doi 2544:doi 2468:p–p 2449:p–p 2441:p–p 2299:): 2122:p–p 1905:). 1898:ppm 1882:). 1390:to 984:p–p 792:p–p 764:p–p 535:of 514:Sun 499:MeV 98:Sun 92:to 76:p–p 57:MK. 50:CNO 32:Pp1 3486:: 3063:. 3055:. 3047:. 3039:. 3025:. 2989:. 2981:. 2969:83 2967:. 2946:}} 2942:{{ 2930:. 2904:^ 2888:. 2878:29 2876:. 2872:. 2830:. 2822:. 2814:. 2800:. 2756:. 2723:. 2701:^ 2685:. 2675:55 2673:. 2667:. 2636:, 2632:, 2605:. 2573:. 2550:. 2542:. 2534:. 2522:83 2520:. 2504:^ 2291:A 2251:00 2233:00 2212:4% 2183:2% 2101:, 2076:He 2062:. 1975:He 1923:He 1867:. 1839:He 1806:Be 1728:Be 1595:Be 1529:Be 1503:He 1477:He 1440:Li 1429:Be 1399:Li 1381:Be 1369:. 1329:He 1318:2 1276:Li 1207:Li 1156:Be 1097:Be 1071:He 1045:He 1004:. 995:He 975:MK 910:He 884:He 858:He 780:He 746:He 728:He 697:He 629:He 559:: 549:He 539:, 445:+ 402:+ 321:+ 210:He 123:. 108:. 3390:: 3299:s 3291:r 3134:e 3127:t 3120:v 3085:. 3071:. 3051:: 3043:: 3033:: 2997:. 2985:: 2975:: 2952:) 2938:. 2898:. 2892:: 2884:: 2854:. 2838:. 2826:: 2818:: 2808:: 2764:. 2731:. 2695:. 2689:: 2681:: 2638:1 2619:. 2588:. 2558:. 2546:: 2538:: 2528:: 2425:e 2394:D 2390:1 2368:H 2364:1 2342:e 2317:H 2313:1 2245:0 2222:0 2210:0 2204:0 2193:0 2181:0 2175:0 2072:2 2031:e 2000:e 1971:2 1949:H 1945:1 1919:2 1835:2 1802:4 1783:e 1753:e 1724:4 1696:B 1692:5 1647:B 1643:5 1621:H 1617:1 1591:4 1525:4 1499:2 1473:2 1325:2 1302:H 1298:1 1272:3 1237:e 1203:3 1181:e 1152:4 1093:4 1067:2 1041:2 937:H 933:1 906:2 880:2 854:2 825:e 625:2 603:H 599:1 577:D 573:1 489:Q 463:e 433:D 429:1 412:e 399:p 391:p 339:e 309:e 297:+ 285:D 281:1 269:p 261:p 115:( 34:. 20:)

Index

Proton-proton reaction
Pp1

Logarithm
proton–proton
CNO
Triple-α

nuclear fusion
stars
hydrogen
helium
Sun
CNO cycle
solar masses
kinetic energy
temperature
electrostatic repulsion
deuteron
Diprotons
core of the Sun
chain reaction
fission
decay chain
Arthur Eddington
Coulomb barrier
quantum mechanics
tunneling
wavefunctions
classical

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