Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements

Double charge exchange (DCE) reactions could provide experimentally driven information about nuclear matrix elements of interest in the context of neutrinoless double-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics>&l...

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Main Authors: Diana Carbone, Roberto Linares, Paulina Amador-Valenzuela, Salvatore Calabrese, Francesco Cappuzzello, Manuela Cavallaro, Suna Firat, Maria Fisichella, Alessandro Spatafora, Luis Acosta, Clementina Agodi, Ismail Boztosun, Giuseppe A. Brischetto, Daniela Calvo, Efrain R. Chávez Lomelí, Irene Ciraldo, Mauro Cutuli, Franck Delaunay, Nikit Deshmukh, Paolo Finocchiaro, Antonino Foti, Aylin Hacisalihoglu, Felice Iazzi, Laura La Fauci, Gaetano Lanzalone, Nilberto H. Medina, Djalma Mendes, José R. B. Oliveira, Athina Pakou, Luciano Pandola, Horia Petrascu, Federico Pinna, Giuseppe Russo, Onoufrios Sgouros, Selçuk O. Solakci, Vasilis Soukeras, George Souliotis, Domenico Torresi, Salvatore Tudisco, Aydin Yildirim, Vinicius A. B. Zagatto
Format: Article
Language:English
Published: MDPI AG 2021-03-01
Series:Universe
Subjects:
Online Access:https://www.mdpi.com/2218-1997/7/3/58
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language English
format Article
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author Diana Carbone
Roberto Linares
Paulina Amador-Valenzuela
Salvatore Calabrese
Francesco Cappuzzello
Manuela Cavallaro
Suna Firat
Maria Fisichella
Alessandro Spatafora
Luis Acosta
Clementina Agodi
Ismail Boztosun
Giuseppe A. Brischetto
Daniela Calvo
Efrain R. Chávez Lomelí
Irene Ciraldo
Mauro Cutuli
Franck Delaunay
Nikit Deshmukh
Paolo Finocchiaro
Antonino Foti
Aylin Hacisalihoglu
Felice Iazzi
Laura La Fauci
Gaetano Lanzalone
Nilberto H. Medina
Djalma Mendes
José R. B. Oliveira
Athina Pakou
Luciano Pandola
Horia Petrascu
Federico Pinna
Giuseppe Russo
Onoufrios Sgouros
Selçuk O. Solakci
Vasilis Soukeras
George Souliotis
Domenico Torresi
Salvatore Tudisco
Aydin Yildirim
Vinicius A. B. Zagatto
spellingShingle Diana Carbone
Roberto Linares
Paulina Amador-Valenzuela
Salvatore Calabrese
Francesco Cappuzzello
Manuela Cavallaro
Suna Firat
Maria Fisichella
Alessandro Spatafora
Luis Acosta
Clementina Agodi
Ismail Boztosun
Giuseppe A. Brischetto
Daniela Calvo
Efrain R. Chávez Lomelí
Irene Ciraldo
Mauro Cutuli
Franck Delaunay
Nikit Deshmukh
Paolo Finocchiaro
Antonino Foti
Aylin Hacisalihoglu
Felice Iazzi
Laura La Fauci
Gaetano Lanzalone
Nilberto H. Medina
Djalma Mendes
José R. B. Oliveira
Athina Pakou
Luciano Pandola
Horia Petrascu
Federico Pinna
Giuseppe Russo
Onoufrios Sgouros
Selçuk O. Solakci
Vasilis Soukeras
George Souliotis
Domenico Torresi
Salvatore Tudisco
Aydin Yildirim
Vinicius A. B. Zagatto
Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements
Universe
initial state interaction
elastic and inelastic scattering
MAGNEX magnetic spectrometer
coupled-channel calculations
optical potential
double charge exchange reactions
author_facet Diana Carbone
Roberto Linares
Paulina Amador-Valenzuela
Salvatore Calabrese
Francesco Cappuzzello
Manuela Cavallaro
Suna Firat
Maria Fisichella
Alessandro Spatafora
Luis Acosta
Clementina Agodi
Ismail Boztosun
Giuseppe A. Brischetto
Daniela Calvo
Efrain R. Chávez Lomelí
Irene Ciraldo
Mauro Cutuli
Franck Delaunay
Nikit Deshmukh
Paolo Finocchiaro
Antonino Foti
Aylin Hacisalihoglu
Felice Iazzi
Laura La Fauci
Gaetano Lanzalone
Nilberto H. Medina
Djalma Mendes
José R. B. Oliveira
Athina Pakou
Luciano Pandola
Horia Petrascu
Federico Pinna
Giuseppe Russo
Onoufrios Sgouros
Selçuk O. Solakci
Vasilis Soukeras
George Souliotis
Domenico Torresi
Salvatore Tudisco
Aydin Yildirim
Vinicius A. B. Zagatto
author_sort Diana Carbone
title Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements
title_short Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements
title_full Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements
title_fullStr Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements
title_full_unstemmed Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements
title_sort initial state interaction for the <sup>20</sup>ne + <sup>130</sup>te and <sup>18</sup>o + <sup>116</sup>sn systems at 15.3 amev from elastic and inelastic scattering measurements
publisher MDPI AG
series Universe
issn 2218-1997
publishDate 2021-03-01
description Double charge exchange (DCE) reactions could provide experimentally driven information about nuclear matrix elements of interest in the context of neutrinoless double-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> decay. To achieve this goal, a detailed description of the reaction mechanism is mandatory. This requires the full characterization of the initial and final-state interactions, which are poorly known for many of the projectile-target systems involved in future DCE studies. Among these, we intend to study the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>20</mn></msup></semantics></math></inline-formula>Ne + <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>130</mn></msup></semantics></math></inline-formula>Te and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>18</mn></msup></semantics></math></inline-formula>O + <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>116</mn></msup></semantics></math></inline-formula>Sn systems at 15.3 AMeV, which are particularly relevant due to their connection with the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>130</mn></msup></semantics></math></inline-formula>Te<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mo>→</mo><mn>130</mn></msup></semantics></math></inline-formula>Xe and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>116</mn></msup></semantics></math></inline-formula>Cd<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mo>→</mo><mn>116</mn></msup></semantics></math></inline-formula>Sn double-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> decays. We measure the elastic and inelastic scattering cross-section angular distributions and compare them with theoretical calculations performed in the optical model, one-step distorted wave Born approximation, and coupled-channel approaches using the São Paulo double-folding optical potential. A good description of the experimental data in the whole explored range of transferred momenta is obtained provided that couplings with the 2<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mrow></mrow><mn>1</mn><mo>+</mo></msubsup></semantics></math></inline-formula> states of the projectile and target are explicitly included within the coupled-channel approach. These results are relevant also in the analysis of other quasi-elastic reaction channels in these systems, in which the same couplings should be included.
topic initial state interaction
elastic and inelastic scattering
MAGNEX magnetic spectrometer
coupled-channel calculations
optical potential
double charge exchange reactions
url https://www.mdpi.com/2218-1997/7/3/58
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spelling doaj-880aa33e24bc4d63912e234b566d39212021-03-06T00:03:14ZengMDPI AGUniverse2218-19972021-03-017585810.3390/universe7030058Initial State Interaction for the <sup>20</sup>Ne + <sup>130</sup>Te and <sup>18</sup>O + <sup>116</sup>Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering MeasurementsDiana Carbone0Roberto Linares1Paulina Amador-Valenzuela2Salvatore Calabrese3Francesco Cappuzzello4Manuela Cavallaro5Suna Firat6Maria Fisichella7Alessandro Spatafora8Luis Acosta9Clementina Agodi10Ismail Boztosun11Giuseppe A. Brischetto12Daniela Calvo13Efrain R. Chávez Lomelí14Irene Ciraldo15Mauro Cutuli16Franck Delaunay17Nikit Deshmukh18Paolo Finocchiaro19Antonino Foti20Aylin Hacisalihoglu21Felice Iazzi22Laura La Fauci23Gaetano Lanzalone24Nilberto H. Medina25Djalma Mendes26José R. B. Oliveira27Athina Pakou28Luciano Pandola29Horia Petrascu30Federico Pinna31Giuseppe Russo32Onoufrios Sgouros33Selçuk O. Solakci34Vasilis Soukeras35George Souliotis36Domenico Torresi37Salvatore Tudisco38Aydin Yildirim39Vinicius A. B. Zagatto40Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyInstituto de Física, Universidade Federal Fluminense, Niterói 24210-340, BrazilDepartamento de Aceleradores y Estudio de Materiales, Instituto Nacional de Investigaciones Nucleares, Ocoyoacac 52750, MexicoIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyDepartment of Physics, Akdeniz University, Antalya 07058, TurkeyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyInstituto de Fisica, Universidad Nacional Autónoma de México, Mexico City 04510, MexicoIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyDepartment of Physics, Akdeniz University, Antalya 07058, TurkeyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyINFN, Sezione di Torino, 10124 Torino, ItalyInstituto de Fisica, Universidad Nacional Autónoma de México, Mexico City 04510, MexicoIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyINFN, Sezione di Torino, 10124 Torino, ItalySchool of Sciences, Auro University, Surat 395007, IndiaIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyINFN, Sezione di Catania, 95123 Catania, ItalyInstitute of Natural Sciences, Karadeniz Teknik Universitesi, Trabzon 61080, TurkeyINFN, Sezione di Torino, 10124 Torino, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyInstituto de Fisica, Universidade de São Paulo, São Paulo 05508-060, BrazilInstituto de Física, Universidade Federal Fluminense, Niterói 24210-340, BrazilInstituto de Fisica, Universidade de São Paulo, São Paulo 05508-060, BrazilDepartment of Physics, University of Ioannina and Hellenic Institute of Nuclear Physics, 45110 Ioannina, GreeceIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyIFIN-HH, 077125 Bucarest, RomaniaINFN, Sezione di Torino, 10124 Torino, ItalyDipartimento di Fisica e Astronomia “Ettore Majorana”, Università di Catania, 95125 Catania, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyDepartment of Physics, Akdeniz University, Antalya 07058, TurkeyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyDepartment of Chemistry, University of Athens and Hellenic Institute of Nuclear Physics, 15771 Athens, GreeceIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyIstituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, 95125 Catania, ItalyDepartment of Physics, Akdeniz University, Antalya 07058, TurkeyInstituto de Física, Universidade Federal Fluminense, Niterói 24210-340, BrazilDouble charge exchange (DCE) reactions could provide experimentally driven information about nuclear matrix elements of interest in the context of neutrinoless double-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> decay. To achieve this goal, a detailed description of the reaction mechanism is mandatory. This requires the full characterization of the initial and final-state interactions, which are poorly known for many of the projectile-target systems involved in future DCE studies. Among these, we intend to study the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>20</mn></msup></semantics></math></inline-formula>Ne + <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>130</mn></msup></semantics></math></inline-formula>Te and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>18</mn></msup></semantics></math></inline-formula>O + <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>116</mn></msup></semantics></math></inline-formula>Sn systems at 15.3 AMeV, which are particularly relevant due to their connection with the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>130</mn></msup></semantics></math></inline-formula>Te<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mo>→</mo><mn>130</mn></msup></semantics></math></inline-formula>Xe and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>116</mn></msup></semantics></math></inline-formula>Cd<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mo>→</mo><mn>116</mn></msup></semantics></math></inline-formula>Sn double-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> decays. We measure the elastic and inelastic scattering cross-section angular distributions and compare them with theoretical calculations performed in the optical model, one-step distorted wave Born approximation, and coupled-channel approaches using the São Paulo double-folding optical potential. A good description of the experimental data in the whole explored range of transferred momenta is obtained provided that couplings with the 2<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mrow></mrow><mn>1</mn><mo>+</mo></msubsup></semantics></math></inline-formula> states of the projectile and target are explicitly included within the coupled-channel approach. These results are relevant also in the analysis of other quasi-elastic reaction channels in these systems, in which the same couplings should be included.https://www.mdpi.com/2218-1997/7/3/58initial state interactionelastic and inelastic scatteringMAGNEX magnetic spectrometercoupled-channel calculationsoptical potentialdouble charge exchange reactions