Abstract:We investigate how strong a hypothetical 1 S 0 bound state of two neutrons would affect different observables in the neutron-deuteron reactions. To that aim we extend our momentum space scheme of solving threenucleon Faddeev equations to incorporate in addition to the deuteron also the 1 S 0 dineutron bound state.We discuss effects induced by dineutron on the angular distribution of the neutron-deuteron elastic scattering and cross sections of the deuteron breakup. A comparison to the available data for neutro… Show more
“…It is possible to extend the proposed scheme on searches for heavier neutral nuclei ( 3 n, 4 n) exploiting the π − absorption at rest on 4 He and, in further perspective, on lithium isotopes.…”
Section: Discussionmentioning
confidence: 99%
“…Three-nucleon forces cannot account for these discrepancies. Increasing the binding of the (standard) nn potential partly improves the situation but the results are inconclusive yet [4]. (iv) An interesting hint for the stronger than commonly accepted nn binding comes from lattice QCD calculations [8].…”
Section: Neutral Nuclei-hints From Theory?mentioning
confidence: 99%
“…They differ also in the detection of a multi-neutron bound state. The strategy of the first experiment [12] is to produce a highly (charge) depleted system in the double pion exchange reaction (DPE) on helium: 4 He(π − , π + ) 4 n and looking for possible structures in the spectrum of the recoiling pion. The second experiment [13] tries to produce bound tetra-neutrons by breaking up neutron reach, loosely bound 14 Be nuclei in the Coulomb field and subsequently detecting neutral particles in a liquid organic scintillator.…”
Section: Experimental Searches For Bound Multi-neutronsmentioning
confidence: 99%
“…As all these arguments give only limited confidence (see e.g. [4]), the nonexistence of bound di-neutrons is still an open question.…”
An experiment is proposed aiming at the unambiguous detection of mass A = 2 neutral particles via elastic scattering and neutron exchange reactions on protons in a plastic scintillating fibre detector. Dineutrons would be produced in ordinary π − absorption at rest on 3 He together with tagging protons. The basic advantages of the proposed process are the strict collinearity and opposite, and constant momenta of hypothetical di-neutrons and recoiling particles in the LAB reference frame. Moreover, the detection cross sections ( 2 n + p → p + 2 n; 2 n + p → d + n) are calculable with three-nucleon codes based on 1 a nn dependent nn interactions.
“…It is possible to extend the proposed scheme on searches for heavier neutral nuclei ( 3 n, 4 n) exploiting the π − absorption at rest on 4 He and, in further perspective, on lithium isotopes.…”
Section: Discussionmentioning
confidence: 99%
“…Three-nucleon forces cannot account for these discrepancies. Increasing the binding of the (standard) nn potential partly improves the situation but the results are inconclusive yet [4]. (iv) An interesting hint for the stronger than commonly accepted nn binding comes from lattice QCD calculations [8].…”
Section: Neutral Nuclei-hints From Theory?mentioning
confidence: 99%
“…They differ also in the detection of a multi-neutron bound state. The strategy of the first experiment [12] is to produce a highly (charge) depleted system in the double pion exchange reaction (DPE) on helium: 4 He(π − , π + ) 4 n and looking for possible structures in the spectrum of the recoiling pion. The second experiment [13] tries to produce bound tetra-neutrons by breaking up neutron reach, loosely bound 14 Be nuclei in the Coulomb field and subsequently detecting neutral particles in a liquid organic scintillator.…”
Section: Experimental Searches For Bound Multi-neutronsmentioning
confidence: 99%
“…As all these arguments give only limited confidence (see e.g. [4]), the nonexistence of bound di-neutrons is still an open question.…”
An experiment is proposed aiming at the unambiguous detection of mass A = 2 neutral particles via elastic scattering and neutron exchange reactions on protons in a plastic scintillating fibre detector. Dineutrons would be produced in ordinary π − absorption at rest on 3 He together with tagging protons. The basic advantages of the proposed process are the strict collinearity and opposite, and constant momenta of hypothetical di-neutrons and recoiling particles in the LAB reference frame. Moreover, the detection cross sections ( 2 n + p → p + 2 n; 2 n + p → d + n) are calculable with three-nucleon codes based on 1 a nn dependent nn interactions.
“…The large stability of the QFS cross sections to the underlying dynamics, implies that the present day 1 S 0 nn interaction is probably incorrect. Modifications of the 1 S 0 nn force by multiplying its matrix elements by a factor λ lead to large changes of the nn QFS cross sections, leaving the np ones practically unchanged [10][11][12]. To remove the discrepancy found in experiment for nn QFS one needs to increase λ by about 8 %.…”
Section: The Dineutron and Its Influence On Nd Observablesmentioning
Faddeev calculations using the chiral three-nucleon force in next-to-next-to-next-to-leading-order show that this force is too weak to provide an explanation for the low-energy A y puzzle. The large discrepancy between data and theory for the neutron-neutron quasi-free-scattering cross section in low energy neutrondeuteron breakup requires a modification of the 1 S 0 neutron-neutron force. We discuss the consequences that a bound 1 S 0 state of two neutrons has on neutron-deuteron scattering observables. At higher energies we compare the solutions of the non-relativistic three-nucleon Faddeev equations with three-nucleon force included to the solutions of its Poincaré invariant version.
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