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This paper examines nucleosynthesis in a low-mass neutron star crust that loses mass due to accretion in a close binary system and, reaching a hydrodynamically unstable configuration explodes. The r-process proceeds mainly in the inner…

High Energy Astrophysical Phenomena · Physics 2024-09-10 A. Yu. Ignatovskiy , I. V. Panov , A. V. Yudin

We examine the nucleosynthesis products that are produced in the outflow from rapidly accreting disks. We find that the type of element synthesis varies dramatically with the degree of neutrino trapping in the disk and therefore the…

Astrophysics · Physics 2009-11-13 R. Surman , G. C. McLaughlin , W. R. Hix

The evolution of the electro-weak phase transition, including reheating due to the release of latent heat in shock waves, is calculated for various values of as yet unknown parameters of electro-weak theory such as latent heat and bubble…

Astrophysics · Physics 2010-11-01 Andrew F. Heckler

We use network calculations of r-process nucleosynthesis to explore the origin of the peak in the solar r-process abundance distribution near nuclear mass number A = 160. The peak is due to a subtle interplay of nuclear deformation and beta…

Astrophysics · Physics 2016-08-30 R. Surman , J. Engel , J. R. Bennett , B. S. Meyer

Because of their neutron-richness and association with supernovae, post-explosion protoneutron star winds are thought to be a likely astrophysical site for rapid neutron capture nucleosynthesis (the r-process). However, the most recent…

Astrophysics · Physics 2009-11-07 Todd A. Thompson

The nucleosynthesis of elements beyond iron is dominated by neutron captures in the s and r processes. However, 32 stable, proton-rich isotopes cannot be formed during those processes, because they are shielded from the s-process flow and…

Instrumentation and Methods for Astrophysics · Physics 2016-01-13 R. Reifarth , S. Altstadt , K. Göbel , T. Heftrich , M. Heil , A. Koloczek , C. Langer , R. Plag , M. Pohl , K. Sonnabend , M. Weigand , T. Adachi , F. Aksouh , J. Al-Khalili , M. AlGarawi , S. AlGhamdi , G. Alkhazov , N. Alkhomashi , H. Alvarez-Pol , R. Alvarez-Rodriguez , V. Andreev , B. Andrei , L. Atar , T. Aumann , V. Avdeichikov , C. Bacri , S. Bagchi , C. Barbieri , S. Beceiro , C. Beck , C. Beinrucker , G. Belier , D. Bemmerer , M. Bendel , J. Benlliure , G. Benzoni , R. Berjillos , D. Bertini , C. Bertulani , S. Bishop , N. Blasi , T. Bloch , Y. Blumenfeld , A. Bonaccorso , K. Boretzky , A. Botvina , A. Boudard , P. Boutachkov , I. Boztosun , A. Bracco , S. Brambilla , J. Briz Monago , M. Caamano , C. Caesar , F. Camera , E. Casarejos , W. Catford , J. Cederkall , B. Cederwall , M. Chartier , A. Chatillon , M. Cherciu , L. Chulkov , P. Coleman-Smith , D. Cortina-Gil , F. Crespi , R. Crespo , J. Cresswell , M. Csatlós , F. Déchery , B. Davids , T. Davinson , V. Derya , P. Detistov , P. Diaz Fernandez , D. DiJulio , S. Dmitry , D. Doré , J. Duenas , E. Dupont , P. Egelhof , I. Egorova , Z. Elekes , J. Enders , J. Endres , S. Ershov , O. Ershova , B. Fernandez-Dominguez , A. Fetisov , E. Fiori , A. Fomichev , M. Fonseca , L. Fraile , M. Freer , J. Friese , M. G. Borge , D. Galaviz Redondo , S. Gannon , U. Garg , I. Gasparic , L. Gasques , B. Gastineau , H. Geissel , R. Gernhäuser , T. Ghosh , M. Gilbert , J. Glorius , P. Golubev , A. Gorshkov , A. Gourishetty , L. Grigorenko , J. Gulyas , M. Haiduc , F. Hammache , M. Harakeh , M. Hass , M. Heine , A. Hennig , A. Henriques , R. Herzberg , M. Holl , A. Ignatov , A. Ignatyuk , S. Ilieva , M. Ivanov , N. Iwasa , B. Jakobsson , H. Johansson , B. Jonson , P. Joshi , A. Junghans , B. Jurado , G. Körner , N. Kalantar , R. Kanungo , A. Kelic-Heil , K. Kezzar , E. Khan , A. Khanzadeev , O. Kiselev , M. Kogimtzis , D. Körper , S. Kräckmann , T. Kröll , R. Krücken , A. Krasznahorkay , J. Kratz , D. Kresan , T. Krings , A. Krumbholz , S. Krupko , R. Kulessa , S. Kumar , N. Kurz , E. Kuzmin , M. Labiche , K. Langanke , I. Lazarus , T. Le Bleis , C. Lederer , A. Lemasson , R. Lemmon , V. Liberati , Y. Litvinov , B. Löher , J. Lopez Herraiz , G. Münzenberg , J. Machado , E. Maev , K. Mahata , D. Mancusi , J. Marganiec , M. Martinez Perez , V. Marusov , D. Mengoni , B. Million , V. Morcelle , O. Moreno , A. Movsesyan , E. Nacher , M. Najafi , T. Nakamura , F. Naqvi , E. Nikolski , T. Nilsson , C. Nociforo , P. Nolan , B. Novatsky , G. Nyman , A. Ornelas , R. Palit , S. Pandit , V. Panin , C. Paradela , V. Parkar , S. Paschalis , P. Pawłowski , A. Perea , J. Pereira , C. Petrache , M. Petri , S. Pickstone , N. Pietralla , S. Pietri , Y. Pivovarov , P. Potlog , A. Prokofiev , G. Rastrepina , T. Rauscher , G. Ribeiro , M. Ricciardi , A. Richter , C. Rigollet , K. Riisager , A. Rios , C. Ritter , T. Rodríguez Frutos , J. Rodriguez Vignote , M. Röder , C. Romig , D. Rossi , P. Roussel-Chomaz , P. Rout , S. Roy , P. Söderström , M. Saha Sarkar , S. Sakuta , M. Salsac , J. Sampson , J. Sanchez del Rio Saez , J. Sanchez Rosado , S. Sanjari , P. Sarriguren , A. Sauerwein , D. Savran , C. Scheidenberger , H. Scheit , S. Schmidt , C. Schmitt , L. Schnorrenberger , P. Schrock , R. Schwengner , D. Seddon , B. Sherrill , A. Shrivastava , S. Sidorchuk , J. Silva , H. Simon , E. Simpson , P. Singh , D. Slobodan , D. Sohler , M. Spieker , D. Stach , E. Stan , M. Stanoiu , S. Stepantsov , P. Stevenson , F. Strieder , L. Stuhl , T. Suda , K. Sümmerer , B. Streicher , J. Taieb , M. Takechi , I. Tanihata , J. Taylor , O. Tengblad , G. Ter-Akopian , S. Terashima , P. Teubig , R. Thies , M. Thoennessen , T. Thomas , J. Thornhill , G. Thungstrom , J. Timar , Y. Togano , U. Tomohiro , T. Tornyi , J. Tostevin , C. Townsley , W. Trautmann , T. Trivedi , S. Typel , E. Uberseder , J. Udias , T. Uesaka , L. Uvarov , Z. Vajta , P. Velho , V. Vikhrov , M. Volknandt , V. Volkov , P. von Neumann-Cosel , M. von Schmid , A. Wagner , F. Wamers , H. Weick , D. Wells , L. Westerberg , O. Wieland , M. Wiescher , C. Wimmer , K. Wimmer , J. S. Winfield , M. Winkel , P. Woods , R. Wyss , D. Yakorev , M. Yavor , J. Zamora Cardona , I. Zartova , T. Zerguerras , I. Zgura , A. Zhdanov , M. Zhukov , M. Zieblinski , A. Zilges , K. Zuber

We follow the chemical evolution of the Galaxy for elements from Ba to Eu, using an evolutionary model suitable to reproduce a large set of Galactic (local and non local) and extragalactic constraints. Input stellar yields for neutron-rich…

Astrophysics · Physics 2009-10-31 C. Travaglio , D. Galli , R. Gallino , M. Busso , F. Ferrini , O. Straniero

We study the neutrino-driven wind from the proto-neutron star by the general relativistic hydrodynamical simulations. We examine the properties of the neutrino-driven wind to explore the possibility of the r-process nucleosynthesis. The…

Astrophysics · Physics 2015-06-24 K. Sumiyoshi , H. Suzuki , K. Otsuki , M. Terasawa , S. Yamada

During the merger of a black hole and a neutron star, baryonic mass can become unbound from the system. Because the ejected material is extremely neutron-rich, the r-process rapidly synthesizes heavy nuclides as the material expands and…

We present a new nucleosynthesis process, that we denote nu p-process, which occurs in supernovae (and possibly gamma-ray bursts) when strong neutrino fluxes create proton-rich ejecta. In this process, antineutrino absorptions in the…

We reanalyze $r$-process nucleosynthesis in the neutron-rich ejecta from a prompt supernova explosion of a low-mass (11 M$_\odot$) progenitor. A pompt explosion is not yet ruled out as a possibility for low-mass supernova progenitors.…

Astrophysics · Physics 2009-11-06 K. Sumiyoshi , M. Terasawa , G. J. Mathews , T. Kajino , S. Yamada , H. Suzuki

The neutrino driven wind during a core collapse supernova is an attractive site for r-process nucleosynthesis. The electron fraction $Y_e$ in the wind depends on observable neutrino energies and luminosities. The mean antineutrino energy is…

Astrophysics · Physics 2009-11-07 C. J. Horowitz

Although initially thought to be promising for production of the r-process nuclei, standard models of neutrino-heated winds from proto-neutron stars (PNSs) do not reach the requisite neutron-to-seed ratio for production of the lanthanides…

High Energy Astrophysical Phenomena · Physics 2019-11-05 Todd A. Thompson , Asif ud-Doula

A cosmological model with a time-varying mass of electrons seems a promising solution for the so-called Hubble tension. We examine the big bang nucleosynthesis (BBN) constraints on the time-varying electron mass model, because a larger…

Cosmology and Nongalactic Astrophysics · Physics 2023-05-01 Osamu Seto , Yo Toda

There has been significant progress in the understanding of the r-process over the last ten years. The conditions required for this process have been examined in terms of the parameters for adiabatic expansion from high temperature and…

Astrophysics · Physics 2009-11-07 Yong-Zhong Qian

We outline a partial historical summary of the steps through which the nucleosynthesis phenomena induced by {\it slow} neutron captures (the {\it s-process}) were clarified, a scientific achievement in which Franz K\"appeler played a major…

Nuclear Theory · Physics 2023-05-03 Maurizio M. Busso , Sara Palmerini

We analyze data from several studies of metal-poor stars in the Milky Way, focusing on both strong (Eu) and weak (Sr) $r$-process elements. Because these elements were injected in an explosion, we calculate the mass swept up when the blast…

High Energy Astrophysical Phenomena · Physics 2018-09-12 Phillip Macias , Enrico Ramirez-Ruiz

We present a review of the possible sources for r-process nuclei. It is known that there is as yet no self-consistent mechanism to provide abundant neutrons for a robust r-process in the neutrino-driven winds from nascent neutron stars. We…

Astrophysics · Physics 2010-11-11 Y. -Z. Qian , G. J. Wasserburg

For r-process nucleosynthesis the beta decay rates of very neutron-rich nuclei are important ingredients. We consider the region around the neutron number N=82 and calculate the half-lives and rates for a number of nuclei. Forms for beta…

Astrophysics · Physics 2008-12-01 Kamales Kar , Soumya Chakravarti