A. Guglielmetti
University of Milan
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Featured researches published by A. Guglielmetti.
Physical Review Letters | 1999
R. Bonetti; C. Broggini; L. Campajola; P. Corvisiero; A. D'Alessandro; M. Dessalvi; A. D'Onofrio; A. Fubini; G. Gervino; L. Gialanella; U. Greife; A. Guglielmetti; C. Gustavino; G. Imbriani; M. Junker; P. Prati; V. Roca; C. Rolfs; M. Romano; F. Schuemann; F. Strieder; F. Terrasi; H. P. Trautvetter; S. Zavatarelli
We give the LUNA results on the cross section measurement of a key reaction of the proton-proton chain strongly affecting the calculated neutrino luminosity from the Sun: He3+He3-->He4+2p. Due to the cosmic ray suppression provided by the Gran Sasso underground laboratory it has been possible to measure the cross section down to the lower edge of the solar Gamow peak, i.e. as low as 16.5 keV centre of mass energy. The data clearly show the cross section increase due to the electron screening effect but they do not exhibit any evidence for a narrow resonance suggested to explain the observed solar neutrino flux.
European Physical Journal A | 2004
F. Raiola; P. Migliardi; G. Gyürky; M. Aliotta; A. Formicola; R. Bonetti; C. Broggini; L. Campajola; P. Corvisiero; H. Costantini; J. Cruz; A. D'Onofrio; Zs. Fülöp; G. Gervino; L. Gialanella; A. Guglielmetti; G. Imbriani; C. Gustavino; A.P. Jesus; M. Junker; R.W. Kavanagh; P.G. Prada Moroni; A. Ordine; J.V. Pinto; P. Prati; V. Roca; J.P. Ribeiro; Detlef Rogalla; C. Rolfs; M. Romano
Abstract:The recent observation of a large electron screening effect in the d(d, p)t reaction using a deuterated Ta target has been confirmed using somewhat different experimental approaches: Ue = 309±12 eV for the electron screening potential energy. The high Ue value arises from the environment of the deuterons in the Ta matrix, but a quantitative explanation is missing.
European Physical Journal A | 2005
G. Imbriani; H. Costantini; A. Formicola; A. Vomiero; C. Angulo; D. Bemmerer; R. Bonetti; C. Broggini; F. Confortola; P. Corvisiero; J. Cruz; Pierre Descouvemont; Zs. Fülöp; G. Gervino; A. Guglielmetti; C. Gustavino; Gy. Gyürky; A.P. Jesus; M. Junker; J. N. Klug; A. Lemut; R. Menegazzo; P. Prati; V. Roca; C. Rolfs; M. Romano; C. Rossi-Alvarez; F. Schümann; D. Schürmann; E. Somorjai
Abstract.The astrophysical S(E) factor of 14N(p,γ)15O has been measured for effective center-of-mass energies between Eeff = 119 and 367 keV at the LUNA facility using TiN solid targets and Ge detectors. The data are in good agreement with previous and recent work at overlapping energies. R-matrix analysis reveals that due to the complex level structure of 15O the extrapolated S(0) value is model dependent and calls for additional experimental efforts to reduce the present uncertainty in S(0) to a level of a few percent as required by astrophysical calculations.
Physics Letters B | 2006
A. Lemut; D. Bemmerer; F. Confortola; R. Bonetti; C. Broggini; P. Corvisiero; H. Costantini; J. Cruz; A. Formicola; Zs. Fülöp; G. Gervino; A. Guglielmetti; C. Gustavino; G. Gyürky; G. Imbriani; A.P. Jesus; M. Junker; B. Limata; R. Menegazzo; P. Prati; V. Roca; Detlef Rogalla; C. Rolfs; M. Romano; C. Rossi Alvarez; F. Schümann; E. Somorjai; O. Straniero; F. Strieder; F. Terrasi
Abstract In stars with temperatures above 20 × 10 6 K , hydrogen burning is dominated by the CNO cycle. Its rate is determined by the slowest process, the 14N(p, γ)15O reaction. Deep underground in Italys Gran Sasso laboratory, at the LUNA 400 kV accelerator, the cross section of this reaction has been measured at energies much lower than ever achieved before. Using a windowless gas target and a 4π BGO summing detector, direct cross section data has been obtained down to 70 keV, reaching a value of 0.24 picobarn. The Gamow peak has been covered by experimental data for several scenarios of stable and explosive hydrogen burning. In addition, the strength of the 259 keV resonance has been remeasured. The thermonuclear reaction rate has been calculated for temperatures 90 – 300 × 10 6 K , for the first time with negligible impact from extrapolations.
Physical Review Letters | 2006
D. Bemmerer; F. Confortola; H. Costantini; A. Formicola; Gy. Gyürky; R. Bonetti; C. Broggini; P. Corvisiero; Z. Elekes; Zs. Fülöp; G. Gervino; A. Guglielmetti; C. Gustavino; G. Imbriani; M. Junker; M. Laubenstein; A. Lemut; B. Limata; V. Lozza; M. Marta; R. Menegazzo; P. Prati; V. Roca; C. Rolfs; C. Rossi Alvarez; E. Somorjai; O. Straniero; F. Strieder; F. Terrasi; H. P. Trautvetter
The nuclear physics input from the 3He(alpha,gamma)7Be cross section is a major uncertainty in the fluxes of 7Be and 8B neutrinos from the Sun predicted by solar models and in the 7Li abundance obtained in big-bang nucleosynthesis calculations. The present work reports on a new precision experiment using the activation technique at energies directly relevant to big-bang nucleosynthesis. Previously such low energies had been reached experimentally only by the prompt-gamma technique and with inferior precision. Using a windowless gas target, high beam intensity, and low background gamma-counting facilities, the 3He(alpha,gamma)7Be cross section has been determined at 127, 148, and 169 keV center-of-mass energy with a total uncertainty of 4%. The sources of systematic uncertainty are discussed in detail. The present data can be used in big-bang nucleosynthesis calculations and to constrain the extrapolation of the 3He(alpha,gamma)7Be astrophysical S factor to solar energies.
European Physical Journal A | 2005
D. Bemmerer; F. Confortola; A. Lemut; R. Bonetti; C. Broggini; P. Corvisiero; H. Costantini; J. Cruz; A. Formicola; Zs. Fülöp; G. Gervino; A. Guglielmetti; C. Gustavino; Gy. Gyürky; G. Imbriani; A.P. Jesus; M. Junker; B. Limata; R. Menegazzo; P. Prati; V. Roca; Detlef Rogalla; C. Rolfs; M. Romano; C. Rossi Alvarez; F. Schümann; E. Somorjai; O. Straniero; F. Strieder; F. Terrasi
Abstract.The LUNA (Laboratory Underground for Nuclear Astrophysics) facility has been designed to study nuclear reactions of astrophysical interest. It is located deep underground in the Gran Sasso National Laboratory, Italy. Two electrostatic accelerators, with 50 and 400 kV maximum voltage, in combination with solid and gas target setups allowed to measure the total cross-sections of the radiative-capture reactions ^2H2H(p, γ)^3He3Heand ^14N14N(p, γ)^15O15Owithin their relevant Gamow peaks. We report on the gamma background in the Gran Sasso laboratory measured by germanium and bismuth germanate detectors, with and without an incident proton beam. A method to localize the sources of beam-induced background using the Doppler shift of emitted gamma rays is presented. The feasibility of radiative-capture studies at energies of astrophysical interest is discussed for several experimental scenarios.
Nuclear Physics | 2001
M. Aliotta; E. Somorjai; P. Corvisiero; M. Romano; G. Imbriani; Z. S. Fulop; A. D'Onofrio; A. Guglielmetti; H. P. Trautvetter; F. Raiola; O. Straniero; G. Gervino; S. Zavatarelli; G. Gyürky; A. Ordine; C. Broggini; A. Formicola; L. Campajola; C. Rolfs; P.G. Prada Moroni; F. Strieder; M. Junker; P. Prati; Detlef Rogalla; F. Terrasi; Frank O. Schumann; L. Gialanella; R. Bonetti; V. Roca; C. Gustavino
The cross section of the reactions 3He(d, p)4He and d(3He, p)4He has been measured at the center-of-mass energies E=5 to 60 keV and 10 to 40 keV, respectively. The experiments were performed to determine the magnitude of the electron screening effect leading to the respective electron-screening potential energy Ue=219±7 and 109±9 eV, which are both significantly higher than the respective values from atomic physics models, Ue=120 and 65 eV.
European Physical Journal A | 2009
A. Caciolli; L. Agostino; D. Bemmerer; R. Bonetti; C. Broggini; F. Confortola; P. Corvisiero; H. Costantini; Z. Elekes; A. Formicola; Zs. Fülöp; G. Gervino; A. Guglielmetti; C. Gustavino; Gy. Gyürky; G. Imbriani; M. Junker; M. Laubenstein; A. Lemut; B. Limata; M. Marta; C. Mazzocchi; R. Menegazzo; P. Prati; V. Roca; C. Rolfs; C. Rossi Alvarez; E. Somorjai; O. Straniero; F. Strieder
Ultra-sensitive in-beam
Physics Letters B | 2000
H. Costantini; A. Formicola; M. Junker; R. Bonetti; C. Broggini; L. Campajola; P. Corvisiero; A. D'Onofrio; A. Fubini; G. Gervino; L. Gialanella; U. Greife; A. Guglielmetti; C. Gustavino; G. Imbriani; A. Ordine; P. G. Prada Moroni; P. Prati; Vincent Roca; Detlef Rogalla; C. Rolfs; M. Romano; Frank O. Schumann; O. Straniero; F. Strieder; F. Terrasi; H. P. Trautvetter; S. Zavatarelli
\gamma
The Astrophysical Journal | 2013
O. Straniero; G. Imbriani; F. Strieder; D. Bemmerer; C. Broggini; A. Caciolli; P. Corvisiero; Herve Costantini; S. Cristallo; A. DiLeva; A. Formicola; Z. Elekes; Zs. Fülöp; G. Gervino; A. Guglielmetti; C. Gustavino; G. Gyürky; M. Junker; A. Lemut; B. Limata; M. Marta; C. Mazzocchi; R. Menegazzo; Luciano Piersanti; P. Prati; V. Roca; C. Rolfs; C. Rossi Alvarez; E. Somorjai; F. Terrasi
-ray spectroscopy studies for nuclear astrophysics are performed at the LUNA (Laboratory for Underground Nuclear Astrophysics) 400 kV accelerator, deep underground in Italy’s Gran Sasso laboratory. By virtue of a specially constructed passive shield, the laboratory