A. M. Mukhamedzhanov
Texas A&M University
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Reports on Progress in Physics | 2014
R. E. Tribble; C. A. Bertulani; M. La Cognata; A. M. Mukhamedzhanov; C. Spitaleri
In this review, we discuss the present status of three indirect techniques that are used to determine reaction rates for stellar burning processes, asymptotic normalization coefficients, the Trojan Horse method and Coulomb dissociation. A comprehensive review of the theory behind each of these techniques is presented. This is followed by an overview of the experiments that have been carried out using these indirect approaches.
Physical Review C | 1999
Carl A. Gagliardi; R. E. Tribble; A. Azhari; H. L. Clark; Y.-W. Lui; A. M. Mukhamedzhanov; A. Sattarov; L. Trache; V. Burjan; J. Cejpek; V. Kroha; S. Piskor; J. Vincour
The {sup 16}O({sup 3}He,d){sup 17}F reaction has been used to determine asymptotic normalization coefficients for transitions to the ground and first excited states of {sup 17}F. The coefficients provide the normalization for the tails of the overlap functions for {sup 17}F{r_arrow}{sup 16}O+p and allow us to calculate the {ital S} factors for {sup 16}O(p,{gamma}){sup 17}F at astrophysical energies. The calculated {ital S} factors are compared to measurements and found to be in very good agreement. This provides a test of this indirect method to determine astrophysical direct capture rates using transfer reactions. In addition, our results yield S(0) for capture to the ground and first excited states in {sup 17}F, without the uncertainty associated with extrapolation from higher energies. {copyright} {ital 1999} {ital The American Physical Society}
Physics of Atomic Nuclei | 2011
C. Spitaleri; A. M. Mukhamedzhanov; L. D. Blokhintsev; M. La Cognata; R. G. Pizzone; A. Tumino
The study of energy production and nucleosynthesis in stars requires an increasingly precise knowledge of the nuclear reaction rates at the energies of interest. To overcome the experimental difficulties arising from the small cross sections at those energies and from the presence of the electron screening, the Trojan Horse Method has been introduced. The method provides a valid alternative path to measure unscreened low-energy cross sections of reactions between charged particles, and to retrieve information on the electron screening potential when ultra-low energy direct measurements are available.
The Astrophysical Journal | 2010
M. La Cognata; C. Spitaleri; A. M. Mukhamedzhanov; A. Banu; S. Cherubini; A. Coc; V. Crucillà; V. Z. Goldberg; M. Gulino; B. F. Irgaziev; G. G. Kiss; L. Lamia; J. Mrazek; R. G. Pizzone; S. M. R. Puglia; G. G. Rapisarda; S. Romano; M. L. Sergi; G. Tabacaru; L. Trache; R. E. Tribble; W. H. Trzaska; A. Tumino
The 18O(p, ?)15N reaction is of primary importance to pin down the uncertainties, due to nuclear physics input, affecting present-day models of asymptotic giant branch stars. Its reaction rate can modify both fluorine nucleosynthesis inside such stars and oxygen and nitrogen isotopic ratios, which allow one to constrain the proposed astrophysical scenarios. Thus, an indirect measurement of the low-energy region of the 18O(p, ?)15N reaction has been performed to access, for the first time, the range of relevance for astrophysical application. In particular, a full, high-accuracy spectroscopic study of the 20 and 90 keV resonances has been performed and the strengths deduced to evaluate the reaction rate and the consequences for astrophysics.
Physical Review C | 1999
C. A. Gagliardi; R. E. Tribble; A. Azhari; H. L. Clark; Y.-W. Lui; A. M. Mukhamedzhanov; A. Sattarov; L. Trache; V. Burjan; J. Cejpek; V. Kroha; S. Piskor; J. Vincour
The {sup 16}O({sup 3}He,d){sup 17}F reaction has been used to determine asymptotic normalization coefficients for transitions to the ground and first excited states of {sup 17}F. The coefficients provide the normalization for the tails of the overlap functions for {sup 17}F{r_arrow}{sup 16}O+p and allow us to calculate the {ital S} factors for {sup 16}O(p,{gamma}){sup 17}F at astrophysical energies. The calculated {ital S} factors are compared to measurements and found to be in very good agreement. This provides a test of this indirect method to determine astrophysical direct capture rates using transfer reactions. In addition, our results yield S(0) for capture to the ground and first excited states in {sup 17}F, without the uncertainty associated with extrapolation from higher energies. {copyright} {ital 1999} {ital The American Physical Society}
The Astrophysical Journal | 2014
A. Tumino; R. Spartá; C. Spitaleri; A. M. Mukhamedzhanov; S. Typel; R. G. Pizzone; E. Tognelli; S. Degl'Innocenti; V. Burjan; V. Kroha; Z. Hons; M. La Cognata; L. Lamia; J. Mrazek; S. Piskor; P. G. Prada Moroni; G. G. Rapisarda; S. Romano; M. L. Sergi
The cross sections of the 2H(d,p)3H and 2H(d,n)3He reactions have been measured via the Trojan Horse method applied to the quasi-free 2H(3He,p 3H)1H and 2H(3He,n 3He)1H processes at 18 MeV off the proton in 3He. For the first time, the bare nucleus S(E) factors have been determined from 1.5 MeV, across the relevant region for standard Big Bang nucleosynthesis, down to the thermal energies of deuterium burning in the pre-main-sequence (PMS) phase of stellar evolution, as well as of future fusion reactors. Both the energy dependence and the absolute value of the S(E) factors deviate by more than 15% from the available direct data and existing fitting curves, with substantial variations in the electron screening by more than 50%. As a consequence, the reaction rates for astrophysics experience relevant changes, with a maximum increase of up to 20% at the temperatures of the PMS phase. From a recent primordial abundance sensitivity study, it turns out that the 2H(d,n)3He reaction is quite influential on 7Li, and the present change in the reaction rate leads to a decrease in its abundance by up to 10%. The present reaction rates have also been included in an updated version of the FRANEC evolutionary code to analyze their influence on the central deuterium abundance in PMS stars with different masses. The largest variation of about 10%-15% pertains to young stars (≤1 Myr) with masses ≥1 M ☉.
Physical Review C | 2003
L. Trache; A. Azhari; F. Carstoiu; Heather Clark; Carl A. Gagliardi; Y.-W. Lui; A. M. Mukhamedzhanov; X. Tang; N. K. Timofeyuk; R. E. Tribble
Asymptotic normalization coefficients (ANCs) for 8Li->7Li+n have been extracted from the neutron transfer reaction 13C(7Li,8Li)12C at 63 MeV. These are related to the ANCs in 8B->7Be+p using charge symmetry. We extract ANCs for 8B that are in very good agreement with those inferred from proton transfer and breakup experiments. We have also separated the contributions from the p_1/2 and p_3/2 components in the transfer. We find the astrophysical factor for the 7Be(p,gamma)8B reaction to be S_17(0)=17.6+/-1.7 eVb. This is the first time that the rate of a direct capture reaction of astrophysical interest has been determined through a measurement of the ANCs in the mirror system.
The Astrophysical Journal | 2014
R. G. Pizzone; R. Spartá; C. A. Bertulani; C. Spitaleri; M. La Cognata; J. Lalmansingh; L. Lamia; A. M. Mukhamedzhanov; A. Tumino
Nuclear reaction rates are among the most important input for understanding the primordial nucleosynthesis and therefore for a quantitative description of the early Universe. An up-to-date compilation of direct cross sections of 2 H(d,p) 3 H, 2 H(d,n) 3 He, 7 Li(p, ) 4 He and 3 He(d,p) 4 He reactions is given. These are among the most uncertain cross sections used and input for Big Bang nucleosynthesis calculations. Their measurements through the Trojan Horse Method (THM) are also reviewed and compared with direct data. The reaction rates and the corresponding recommended errors in this work were used as input for primordial nucleosynthesis calculations to evaluate their impact on the 2 H, 3;4 He and 7 Li primordial abundances, which are then compared
Journal of Physics G | 2012
L. Lamia; C. Spitaleri; V. Burjan; N. Carlin; S. Cherubini; V. Crucillà; M. Gameiro Munhoz; M. Gimenez del Santo; M. Gulino; Z. Hons; G. G. Kiss; V. Kroha; S. Kubono; M. La Cognata; C. Li; J. Mrazek; A. M. Mukhamedzhanov; R. G. Pizzone; S. M. R. Puglia; Qungang Wen; G. G. Rapisarda; C. Rolfs; S. Romano; M. L. Sergi; E. Somorjai; F. A. Souza; A. Szanto de Toledo; G. Tabacaru; A. Tumino; Y. Wakabayashi
A new measurement of the 11B(p,?0)8Be has been performed applying the Trojan horse method (THM) to the 2H(11B,?80Be)n quasi-free reaction induced at a laboratory energy of 27 MeV. The astrophysical S(E) factor has been extracted from ?600 keV down to zero energy by means of an improved data analysis technique and it has been compared with direct data available in the literature. The range investigated here overlaps with the energy region of the light element LiBeB stellar burning and with that of future aneutronic fusion power plants using the 11B+p fuel cycle. The new investigation described here confirms the preliminary results obtained in the recent TH works. The origin of the discrepancy between the direct estimate of the 11B(p,?0)8Be S(E)-factor at zero energy and that from a previous THM investigation is quantitatively corroborated. The results obtained here support, within the experimental uncertainties, the low-energy S(E)-factor extrapolation and the value of the electron screening potential deduced from direct measurements.
Physical Review Letters | 2008
M. La Cognata; C. Spitaleri; A. M. Mukhamedzhanov; B. F. Irgaziev; R. E. Tribble; A. Banu; S. Cherubini; Alain Coc; V. Crucillà; V. Z. Goldberg; M. Gulino; G. G. Kiss; L. Lamia; J. Mrazek; R. G. Pizzone; S. M. R. Puglia; G. G. Rapisarda; S. Romano; M. L. Sergi; G. Tabacaru; L. Trache; W. H. Trzaska; A. Tumino
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