MétaCan
Menu
Retour à la cohorte
Enregistrement W2005752816 · doi:10.1063/1.3141922

αβγ, Hoyle, and the history of nucleosynthesis

2009· article· en· W2005752816 sur OpenAlex
David Arnett, George Wallerstein

Pourquoi ce travail est dans la base

Une base qui oublie comment elle a trouvé un travail ne peut pas être vérifiée. Voici les voies qui ont admis celui-ci.

aboutLe titre ou le résumé porte un signal canadien du lexique géographique.
no affAucune affiliation canadienne : ce travail est invisible pour une base fondée sur la seule affiliation.
Aucune affiliation canadienne. Une base fondée sur la seule affiliation (le devis habituel) n'aurait jamais vu ce travail. C'est l'un des travaux qui justifient l'inversion de la base.

Notice bibliographique

RevuePhysics Today · 2009
Typearticle
Langueen
DomainePhysics and Astronomy
ThématiqueAstronomical and nuclear sciences
Établissements canadiensnon disponible
Organismes subventionnairesnon disponible
Mots-clésNucleosynthesisPhysicsBig Bang nucleosynthesisCosmologyAstrophysicsSupernovaStellar nucleosynthesisAstronomy

Résumé

récupéré en direct d'OpenAlex

We wish to clarify the first part of Michael Turner’s Reference Frame (Physics Today, December 2008, page 8), which dealt with the early history of nucleosynthesis. Turner states that “[George] Gamow’s Big Bang model spurred Fred Hoyle to think more creatively about the stellar nucleosynthesis to keep his steady-state model competitive and in 1957, with Geoffrey Burbidge, Margaret Burbidge, and William Fowler, he worked out the correct theory of how the bulk of the elements were made in stars.” That timing is wrong: Nucleosyn thesis (1946) came before cosmology (1948). The correct story adds weight to Turner’s theme of the positive influence of a wrong paper.The Alpher, Bethe, and Gamow (αβγ) paper was wrong about nucleosynthesis but embedded it in what we believe to be the correct cosmological framework. A second wrong idea, the steady-state cosmology, was enormously influential because it gave definite predictions for observers to aim for and so was a key step along the way to developing precision cosmology. The steady-state theory was motivated by the success of the theory of stellar nucleosynthesis, which preceded it. Stellar nucleosynthesis was mostly worked out by Hoyle in two papers 1 1. F. Hoyle, Mon. Not. R. Astron. Soc. 106, 343 (1946); F. Hoyle, Astrophys. J. Suppl. 1, 121 (1954). https://doi.org/10.1086/190005 in which he identified the processes that synthesized the elements from carbon to nickel and identified supernovae as the sites. The rarer elements beyond nickel (actually beyond zinc, the heaviest species produced in the quasi-equilibrium of the iron peak) were produced in neutron-capture processes both rapid and slow. The synthesis of many of the rare heavy elements was first understood by Alastair Cameron, who explained the presence of the unstable element technetium in evolved stars. His papers on the s-process 2 2. See, for example, A. G.W. Cameron, Astrophys. J. 121, 144 (1955). https://doi.org/10.1086/145970 came out before the 1957 reviews by Hoyle and company and by Cameron. 3 3. See E. M. Burbidge, G. R. Burbidge, W. A. Fowler, F. Hoyle, Rev. Mod. Phys. 29, 547 (1957); https://doi.org/10.1103/RevModPhys.29.547 A. G. W. Cameron, Stellar Evolution, Nuclear Astrophysics, and Nucleogenesis, (CRL-41) Atomic Energy of Canada Ltd (1957). Although some isotopes of the light elements lithium, beryllium, and boron might be made in stars (or cosmic-ray spallation), the origins of helium-4 are not so straightforward. Stars do produce 4He, but observational estimates of the yield are less than about 0.08 by mass, much less than the cosmological yield of 0.24, requiring a more prolific source for 4He production, such as the Big Bang. Cosmological nucleosynthesis was coming into disfavor in the late 1940s. Enrico Fermi and Anthony Turkevich realized that only hydrogen-1, hydrogen-2, 3He, and 4He could be made in significant amounts. (See reference 44. See figure 20 in R. A. Alpher, R. C. Herman, Rev. Mod. Phys. 22, 153 (1950). https://doi.org/10.1103/RevModPhys.22.153 ; we now know 3He is rapidly destroyed also, but 7Li may be produced.) Unlike the stellar case, there were no “seed” heavy nuclei to capture neutrons, which made the cosmological neutron capture theory irrelevant. It was natural that the success of stellar nucleosynthesis started Hoyle questioning the necessity for a Big Bang cosmology, which was failing as a general theory of nucleosynthesis. The steady-state theory was formulated in 1948. 5 5. H. Bondi, T. Gold, Mon. Not. R. Astron. Soc. 108, 252 (1948) F. Hoyle, Mon. Not. R. Astron. Soc. 108, 372 (1948); F. Hoyle, Mon. Not. R. Astron. Soc. 109, 365 (1949). Probably one of its attractions is the generalization to time of the Copernican notion that we are not in a special place in space. One thing the theory did was to make the spectacular prediction that on average the universe did not change, a testable idea.With the deep-field images from the Hubble Space Telescope , 6 6. See http://hubblesite.org/newscenter/archive/releases/cosmology/2006/44. astronomers can see back to a redshift corresponding to 7% of the age of the universe in the Big Bang cosmology. That the fainter and more distant images look different from the nearer ones is a striking indication that we live in an evolutionary cosmology. Even incorrect theories may be helpful, if they are well posed and can be falsified. Both αβγ and the steady state were important steps along the way to precision cosmology. REFERENCESSection:ChooseTop of pageREFERENCES <<1. F. Hoyle, Mon. Not. R. Astron. Soc. 106, 343 (1946); Google ScholarCrossref, ISI F. Hoyle, Astrophys. J. Suppl. 1, 121 (1954). https://doi.org/10.1086/190005 , , Google ScholarCrossref2. See, for example, A. G.W. Cameron, Astrophys. J. 121, 144 (1955). https://doi.org/10.1086/145970 , Google ScholarCrossref, ISI3. See E. M. Burbidge, G. R. Burbidge, W. A. Fowler, F. Hoyle, Rev. Mod. Phys. 29, 547 (1957); https://doi.org/10.1103/RevModPhys.29.547 , Google ScholarCrossref, ISI A. G. W. Cameron, Stellar Evolution, Nuclear Astrophysics, and Nucleogenesis, (CRL-41) Atomic Energy of Canada Ltd (1957). , Google Scholar4. See figure 20 in R. A. Alpher, R. C. Herman, Rev. Mod. Phys. 22, 153 (1950). https://doi.org/10.1103/RevModPhys.22.153 , Google ScholarCrossref, ISI5. H. Bondi, T. Gold, Mon. Not. R. Astron. Soc. 108, 252 (1948) Google ScholarCrossref, ISI F. Hoyle, Mon. Not. R. Astron. Soc. 108, 372 (1948); , Google ScholarCrossref, ISI F. Hoyle, Mon. Not. R. Astron. Soc. 109, 365 (1949). , Google ScholarCrossref, ISI6. See http://hubblesite.org/newscenter/archive/releases/cosmology/2006/44. Google Scholar© 2009 American Institute of Physics.

Récupéré en direct depuis OpenAlex et désinversé. Les résumés ne sont pas conservés dans cette base de données : les index inversés représentent 8,6 Go des 9,3 Go de texte de la base, et le serveur dispose de 13 Go libres.

Prédiction distillée sur la base complète

Imitation des enseignants

Ni prévalence calibrée, ni vérité terrain. Validation humaine à venir. Apprise à partir de 10 348 étiquettes directes de Codex et de 10 348 étiquettes directes de Gemma. Le mode candidate est l'union des têtes enseignantes seuillées; le consensus est leur intersection. Ces sorties portent le statut machine_predicted_unvalidated et ne sont ni des étiquettes humaines ni des étiquettes directes de modèles de pointe.

score de la tête « metaresearch » (Codex)0,000
score de la tête « metaresearch » (Gemma)0,000
Version: codex-gemma-dda1882f352aStatut de validation: machine_predicted_unvalidated
Catégories candidatesaucune
Catégories consensuellesaucune
DomaineSignal candidat: aucune · Signal consensuel: aucune
Devis d'étudeSignal candidat: Théorique ou conceptuel · Signal consensuel: Théorique ou conceptuel
GenreSignal candidat: Empirique · Signal consensuel: Empirique
Score de désaccord entre enseignants0,418
Score d'incertitude au seuil0,164

Scores Codex et Gemma par catégorie

CatégorieCodexGemma
Métarecherche0,0000,000
Méta-épidémiologie (sens strict)0,0000,000
Méta-épidémiologie (sens large)0,0000,000
Bibliométrie0,0000,000
Études des sciences et des technologies0,0000,000
Communication savante0,0000,000
Science ouverte0,0000,000
Intégrité de la recherche0,0000,000
Charge utile insuffisante (le modèle a refusé de juger)0,0000,000

Scores machine (provisoires)

Les deux têtes enseignantes du modèle étudiant, lues sur ce travail. Un score ordonne la base pour la relecture; il n'affirme jamais une catégorie, et le statut de validation accompagne chaque rangée tel quel.

Scores de référence d'un modèle non mature (critères de maturité non atteints, 7 itérations). Un score ordonne; il n'affirme jamais une catégorie.

Tête enseignante Opus0,007
Tête enseignante GPT0,187
Écart entre enseignants0,180 · la distance entre les deux têtes enseignantes sur ce seul travail
Statut de validationscore_only:v0-immature-baseline · tel quel depuis la passe de notation : score_only signifie que le nombre peut ordonner les travaux, et qu'aucune étiquette de catégorie n'en découle