Big Bang Nucleosynthesis大爆炸核合成
![]() The modeling of the early universe by the standard big bang model gives a scenario that involves twelve nuclear interactions that led to the present cosmic abundances of elements outside the stars. The vast majority of the mass of ordinary matter in the universe is hydrogen and helium, remaining from the early stages of the universe. The illustration above gives nominal abundances of the current constituents. These abundances are model dependent and subject to revision. 标准大爆炸模型对早期宇宙的建模提供了一个涉及十二种核相互作用的场景,这些相互作用导致了现在宇宙中元素(除恒星外)的丰度。宇宙中普通物质的绝大多数质量仍来自宇宙早期阶段的氢和氦。上图给出了当前构成物的名义丰度。这些丰度取决于模型,并可能被修订。
Beryllium-7 is an isotope that is produced in this process, but is not a part of the cosmic abundances because it is radioactive with half-life 53.28 days, decaying to 7Li. Neutrons are not part of the background elements because free neutrons decay with half-life 10.3 minutes. The other constituent of the reactions is tritium, 3H, which has a half-life of 12.32 years. 铍-7是一种在此过程中产生的同位素,但它不属于宇宙丰度成分,因为它具有53.28天的半衰期,会衰变成锂-7。中子不属于背景元素,因为自由中子的半衰期为10.3分钟。反应的另一个组成部分是氚,即3H,其半衰期为12.32年。
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Index References Carroll & Ostlie Ch 29 索引参考Carroll & Ostlie第29章 | ||
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Hydrogen-Helium Abundance氢-氦丰度
Hydrogen and helium account for nearly all the nuclear matter in today's universe. This is consistent with the standard or "big bang" model. The process of forming the hydrogen and helium and other trace constituents is often called "big bang nucleosynthesis". Schramm's figures for relative abundances indicate that helium is about 25% by mass and hydrogen about 73% with all other elements constituting less than 2%. Carroll & Ostlie give 23 to 24% helium. There is a window of uncertainty, but it is clear that hydrogen and helium make up 98% plus of the ordinary matter in the universe. This high percentage of helium argues strongly for the big bang model, since other models gave very small percentages of helium. Since there is no known process which significantly changes this H/He ratio, it is taken to be the ratio which existed at the time when the deuteron became stable in the expansion of the universe. This ratio is significant as a test of cosmological models since it will be affected by the time period from the time when the temperature dropped below that necessary to produce neutrons from protons to the time when the deuteron became stable, halting the decay of the free neutrons. 氢和氦几乎构成了今天宇宙中所有的核物质。这与标准或“大爆炸”模型是一致的。形成氢、氦和其他痕量成分的过程通常被称为“大爆炸核合成”。Schramm的相对丰度数据表明,氦约占质量的25%,氢约占73%,其他所有元素加起来不到2%。Carroll和Ostlie给出的氦比例是23%到24%。存在一定的不确定性范围,但可以明确的是,氢和氦构成了宇宙中普通物质的98%以上。这种高比例的氦强烈支持大爆炸模型,因为其他模型给出的氦比例非常小。由于目前没有已知的过程能显著改变这个H/He比例,因此认为这个比例是在宇宙膨胀过程中氘变得稳定的时刻存在的比例。这个比例对于检验宇宙学模型具有重要意义,因为它会受到从温度下降到足以从质子中产生中子的时刻到氘变得稳定的时刻之间的时期的影响。
![]() Basically , the hydrogen-helium abundance helps us to model the expansion rate of the early universe. If it had been faster, there would be more neutrons and more helium. If it had been slower, more of the free neutrons would have decayed before the deuterium stability point and there would be less helium. 基本上,氢和氦的丰度帮助我们建模早期宇宙的膨胀速率。如果膨胀得更快,就会有更多中子和更多氦。如果膨胀得更慢,自由中子会在氘稳定点之前更多地衰变,从而导致氦更少。
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Index References Trefil Schramm Big Bang ... Harwit Ch 12 Carroll & Ostlie Ch 29 索引 参考文献 Trefil Schramm 大爆炸 ... Harwit 第12章 Carroll & Ostlie 第29章 | |||
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Hydrogen-Helium Calculations氢-氦计算
The critical temperatures determining the hydrogen-helium abundance can be calculated with the assumption that they are driven by the internal energy of the expanding universe. 决定氢-氦丰度的临界温度可以假定是由膨胀宇宙的内能驱动而计算得出的。
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Index Reference Trefil 索引参考 Trefil | ||
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