Study of the nuclear matter distribution in neutron-rich Li isotopes

Dobrovolsky, A. V.; Alkhazov, G.; Andronenko, M. N.; Bauchet, A.; Egelhof, P.; Fritz, Steven J.; Geißel, H.; Gross, C. J.; Khanzadeev, A.; Korolev, G.A.; Kraus, G.; Lobodenko, A.; Münzenberg, G.; Mutterer, M.; Neumaier, S.; Schäfer, Th.; Scheidenberger, C.; Seliverstov, D. M.; Timofeev, N. A.; Vorobyov, A. A.; Yatsoura, V. I.

doi:10.1016/j.nuclphysa.2005.11.016

Cited by 126 publications

(97 citation statements)

References 51 publications

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“…This results in an energy signal of Z = 2.83, close to that for Li. A similar effect occurs for 6 Be during neutron removal from 7 Be. The decay energy for 6 Be is 1.4 MeV with a final state of p+p+ 4 He.…”

Section: Experiments and Comparison To Modelsmentioning

confidence: 52%

“…A similar effect occurs for 6 Be during neutron removal from 7 Be. The decay energy for 6 Be is 1.4 MeV with a final state of p+p+ 4 He. It is not possible to identify this reaction with the current experimental setup.…”

Section: Experiments and Comparison To Modelsmentioning

confidence: 52%

“…The nucleon distribution radius for unstable nuclei can be determined by several methods, including the interaction cross section (σ I ) [1,2] and the reaction cross section (σ R ) with light targets [3,4] and proton elastic scattering [5,6]. These methods have revealed new phenomena including neutron halos and neutron skins [7] in neutron-rich nuclei.…”

Section: Introductionmentioning

confidence: 99%

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Proton Radius of ¹⁴Be from Measurement of Charge-Changing Cross Sections

Terashima¹,

Tanihata²,

Kanungo³

et al. 2015

Proceedings of the Conference on Advances in Radioactive Isotope Science (ARIS2014)

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Charge-changing cross sections for 7,[9][10][11][12]14 Be have been measured at 900A MeV on a carbon target. These cross sections are discussed both in terms of a geometrical and a Glauber model. From several different analyses of the cross sections, the proton distribution radius (proton radius) of 14 Be was determined for the first time to be 2.41 ± 0.04 fm. A large difference in the proton and neutron radii is found. The charge-changing cross sections and the proton distribution radii are compared to the results of fermionic molecular dynamics (FMD) and antisymmetrized molecular dynamics (AMD) under the Glauber model.

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Section: Experiments and Comparison To Modelsmentioning

confidence: 52%

Section: Experiments and Comparison To Modelsmentioning

confidence: 52%

Section: Introductionmentioning

confidence: 99%

See 1 more Smart Citation

Proton Radius of ¹⁴Be from Measurement of Charge-Changing Cross Sections

Terashima¹,

Tanihata²,

Kanungo³

et al. 2015

Proceedings of the Conference on Advances in Radioactive Isotope Science (ARIS2014)

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“…The existing ESR (Experimental Storage Ring) at GSI, together with its internal gas-jet target, provides a unique opportunity to perform such kind of experiments on a smaller scale at the present time. We have developed a UHV-compatible (Ultra High Vacuum) detector setup mainly based on DSSDs (Double-sided Silicon-Strip Detector) for the target-like recoils [4]. With this setup we were able to successfully investigate reactions with a stored radioactive beam for the first time ever.…”

mentioning

confidence: 99%

“…By using phenomenological density distributions, and by varying their free parameters, the calculated cross section will be fitted to the experimental data. In this way, the nuclear matter radius and radial matter distribution will be extracted (see for example [4] and references therein).…”

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confidence: 99%

First EXL experiment with stored radioactive beam: Proton scattering on⁵⁶Ni

Schmid

Bagchi

Bönig

et al. 2014

EPJ Web of Conferences

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Abstract. EXL (EXotic nuclei studied in Light-ion induced reactions at the NESR storage ring) is a project within NUSTAR at FAIR. It aims at investigations of light-ion induced direct reactions in inverse kinematics with radioactive ions cooled and stored in the future NESR (New Experimental Storage Ring). The existing ESR (Experimental Storage Ring) at GSI, together with its internal gas-jet target, provides a unique opportunity to perform such kind of experiments on a smaller scale at the present time. We have developed a UHV-compatible (Ultra High Vacuum) detector setup mainly based on DSSDs (Double-sided Silicon-Strip Detector) for the target-like recoils [4]. With this setup we were able to successfully investigate reactions with a stored radioactive beam for the first time ever. As a part of the first EXL campaign we investigated the reaction 56 Ni(p,p) 56 Ni in inverse kinematics in order to measure the differential cross section for elastic proton scattering and deduce the nuclear-matter distribution and radius of 56 Ni. In the following, the experimental setup is introduced in more detail, and the current status of the ongoing analysis is discussed. a

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Ab Initio Thermodynamics Calculation of Beta Decay Rates

Parker,

Jeynes

2023

Annalen der Physik

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Study of the nuclear matter distribution in neutron-rich Li isotopes

Cited by 126 publications

References 51 publications

Proton Radius of ¹⁴Be from Measurement of Charge-Changing Cross Sections

Proton Radius of ¹⁴Be from Measurement of Charge-Changing Cross Sections

First EXL experiment with stored radioactive beam: Proton scattering on⁵⁶Ni

Ab Initio Thermodynamics Calculation of Beta Decay Rates

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Study of the nuclear matter distribution in neutron-rich Li isotopes

Cited by 126 publications

References 51 publications

Proton Radius of 14Be from Measurement of Charge-Changing Cross Sections

Proton Radius of 14Be from Measurement of Charge-Changing Cross Sections

First EXL experiment with stored radioactive beam: Proton scattering on56Ni

Ab Initio Thermodynamics Calculation of Beta Decay Rates

Contact Info

Product

Resources

About

Proton Radius of ¹⁴Be from Measurement of Charge-Changing Cross Sections

Proton Radius of ¹⁴Be from Measurement of Charge-Changing Cross Sections

First EXL experiment with stored radioactive beam: Proton scattering on⁵⁶Ni