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We present calculations of neutron thermal cross sections, Westcott factors, resonance integrals, Maxwellian-averaged cross sections and astrophysical reaction rates for 843 ENDF materials using data from the major evaluated nuclear…

Solar and Stellar Astrophysics · Physics 2013-09-13 B. Pritychenko , S. F. Mughabghab

The LIT approach is tested for the calculation of astrophysical S-factors. As an example the S-factor of the reaction 2H(p,gamma)3He is considered. It is discussed that a sufficiently high density of LIT states at low energies is necessary…

Nuclear Theory · Physics 2016-12-15 Sergio Deflorian , Victor D. Efros , Winfried Leidemann

Measuring neutron star radii with spectroscopic and timing techniques relies on the combination of multiple observables to break the degeneracies between the mass and radius introduced by general relativistic effects. Here, we explore a…

High Energy Astrophysical Phenomena · Physics 2015-10-21 Feryal Ozel , Dimitrios Psaltis

We implement the Bayesian inference to retrieve energy spectra of all neutrinos from a galactic core-collapse supernova (CCSN). To achieve high statistics and full sensitivity to all flavours of neutrinos, we adopt a combination of several…

High Energy Physics - Phenomenology · Physics 2023-09-26 Xu-Run Huang , Chuan-Le Sun , Lie-Wen Chen , Jun Gao

Many real world problems exhibit patterns that have periodic behavior. For example, in astrophysics, periodic variable stars play a pivotal role in understanding our universe. An important step when analyzing data from such processes is the…

Machine Learning · Computer Science 2012-08-20 Yuyang Wang , Roni Khardon , Pavlos Protopapas

Effective energy windows (Gamow windows) of astrophysical reaction rates for (p,gamma), (p,n), (p,alpha), (alpha,gamma), (alpha,n), (alpha,p), (n,gamma), (n,p), and (n,alpha) on targets with 10<=Z<=83 from proton- to neutron-dripline are…

Solar and Stellar Astrophysics · Physics 2015-03-13 T. Rauscher

The relevant energy ranges for stellar nuclear reactions are introduced. Low-energy compound and direct reactions are discussed. Stellar modifications of the cross sections are presented. Implications for experiments are outlined.

High Energy Astrophysical Phenomena · Physics 2015-05-19 T. Rauscher

Calculations that demonstrate the influence of three key nuclear reaction rates on the evolution of Asymptotic Giant Branch stars have been carried out. We study the case of a star with an initial mass of 2Msun and a metallicity of Z=0.01,…

Astrophysics · Physics 2009-11-13 F. Herwig , Sam M. Austin , John C. Lattanzio

The description of stellar interior remains as a big challenge for the nuclear astrophysics community. The consolidated knowledge is restricted to density regions around the saturation of hadronic matter $\rho _{0} = 2.8\times 10^{14} {\rm\…

A generalized method to calculate the excitation-energy dependent parity ratio in the nuclear level density is presented, using the assumption of Poisson distributed independent quasi particles combined with BCS occupation numbers. It is…

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

Stars are gravitationally stabilized fusion reactors changing their chemical composition while transforming light atomic nuclei into heavy ones. The atomic nuclei are supposed to be in thermal equilibrium with the ambient plasma. The…

Classical Analysis and ODEs · Mathematics 2016-09-06 William J. Anderson , Hans J. Haubold , Arak Mathai Mathai

The usual procedure for estimating the significance of a peak in a power spectrum is to calculate the probability of obtaining that value or a larger value by chance (known as the "p-value"), on the assumption that the time series contains…

High Energy Astrophysical Phenomena · Physics 2009-11-13 P. A. Sturrock , J. D. Scargle

With recent advances in neutron star observations, major progress has been made in determining the pressure of neutron star matter at high density. This pressure is constrained by the neutron star deformability, determined from…

These notes aim at presenting an overview of Bayesian statistics, the underlying concepts and application methodology that will be useful to astronomers seeking to analyse and interpret a wide variety of data about the Universe. The level…

Cosmology and Nongalactic Astrophysics · Physics 2017-01-09 Roberto Trotta

The theoretical predictions of big bang nucleosynthesis (BBN) are dominated by uncertainties in the input nuclear reaction cross sections. In this paper, we examine the impact on BBN of the recent compilation of nuclear data and…

Astrophysics · Physics 2009-09-15 Richard H. Cyburt , Brian D. Fields , Keith A. Olive

The structure of the Borromean nucleus $^9$Be ($\alpha+\alpha+n$) is addressed within a three-body approach using the analytical transformed harmonic oscillator method. The three-body formalism provides an accurate description of the…

Nuclear Theory · Physics 2016-04-26 J. Casal , M. Rodríguez-Gallardo , J. M. Arias , I. J. Thompson

The $^{12}\mathrm{C}(\alpha,\gamma)^{16}\mathrm{O}$ reaction governs the carbon-to-oxygen ratio set during helium burning, shaping white-dwarf structure and Type~Ia supernova yields. At the astrophysical energy $E \approx 300~\mathrm{keV}$,…

High Energy Astrophysical Phenomena · Physics 2025-11-18 A. M. Mukhamedzhanov

The usual procedure for estimating the significance of a peak in a power spectrum is to calculate the probability of obtaining that value or a larger value by chance, on the assumption that the time series contains only noise (e.g. that the…

Astrophysics · Physics 2008-09-03 P. A. Sturrock

The $p$ process nucleosynthesis is responsible for the synthesis of 35 neutron-deficient nuclei from $^{35}$Se to $^{196}$Hg. An important input that can affect the modeling of this process is the nuclear level density at the relevant…

Nuclear Theory · Physics 2024-02-20 A. Chalil , C. Ducoin , O. Stézowski , N. Millard-Pinard , J. Dudouet , Y. Demane , M. Chamseddine