References quoted in the ENSDF dataset: 4NN ADOPTED LEVELS
75 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 85, 942 (1952)
K.H.Sun, F.A.Pecjak, A.J.Allen
The Tetraneutron
NUCLEAR REACTIONS 103Rh, 209Bi(n, 4n), E ∼ 18 MeV; measured reaction products. 4NN; deduced tetraneutron yield upper limit.
Phys.Letters 4, 350 (1963)
P.E.Argan, A.Piazzoli
Some Possible Consequences of the Existence of the States H4 and H5
NUCLEAR STRUCTURE 4H, 5H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90505-5
Phys.Lett. 5, 292 (1963)
J.P.Schiffer, R.Vandenbosch
Search for a Particle-Stable Tetra Neutron
doi: 10.1016/S0375-9601(63)96134-6
Phys.Lett. 9, 184 (1964)
V.I.Goldansky
The Occurrence of He8 Casts Doubts on the Stability of H5, H4 and Tetraneutron
doi: 10.1016/0031-9163(64)90136-2
At.Energ. 17, 687 (1964)
N.A.Vlasov, L.N.Samoilov
Heavy hydrogen and neutron isotopes
NUCLEAR REACTIONS 3H(d, n), E=6.3, 10.9, 19 MeV; analyzed available data. 4He; deduced energy levels, level scheme, neutron polarization.
RADIOACTIVITY 5H(β-), (2n) [from 7Li(γ, 2p), (p, 3p), E not given]; analyzed available data; deduced production σ ratios, lack of 5H boud states.
NUCLEAR STRUCTURE 4NN, 4He; analyzed available data; calculated binding energies, the existence of a bound tetraneutron conditions; deduced lack of tetraneutron bound states.
doi: 10.1007/BF01650846
Phys.Rev.Lett. 12, 128 (1964); Erratum Phys. Rev. Lett. 12, 497 (1964)
F.von Hippel, P.P.Divakaran
Analysis of the Experimental Evidence for the Existence of a 4H State with T = 2
NUCLEAR REACTIONS 4He(γ, π+), E not given; analyzed available data. 3,4H; deduced theoretical internal energy spectrum in the n-T system, in the absence of an experimental Q(n, T) spectrum, it is difficult to conclude whether or not there is a 4H state present in the products of reaction.
doi: 10.1103/PhysRevLett.12.128
Phys.Rev. 137, B345 (1965)
S.Cierjacks, G.Markus, W.Michaelis, W.Ponitz
Further Evidence for the Nonexistence of Particle-Stable Tetraneutrons
NUCLEAR STRUCTURE 4n; measured not abstracted; deduced nuclear properties.
Phys.Lett. 19, 335 (1965)
L.Gilly, M.Jean, R.Meunier, M.Spighel, J.P.Stroot, P.Duteil
Double Charge Exchange with Negative Pions Search for Tetraneutron
doi: 10.1016/0031-9163(65)91012-7
Phys.Rev.Lett. 15, 165 (1965)
Y.C.Tang, B.F.Bayman
Nonexistence of the Tetraneutron
doi: 10.1103/PhysRevLett.15.165
Nucl.Phys. B2, 181 (1967)
P.Grassberger, W.Sandhas
Systematical treatment of the non-relativistic n-particle scattering problem
doi: 10.1016/0550-3213(67)90017-X
Phys.Letters 25B, 536 (1967)
L.Kaufman, B.W.Gauld, V.Perez-Mendez, J.M.Sperinde, S.H.Williams
π- - Helium Inelastic Interactions at 140 MeV
NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90137-2
Yadern.Fiz. 7, 28(1968); Soviet J.Nucl.Phys. 7, 20(1968)
Y.A.Batusov, S.A.Bunyatov, V.M.Sidorov, V.A.Yarba
Production of He8 in π- -Meson Capture by Carbon, Nitrogen, and Oxygen Nuclei
NUCLEAR REACTIONS 12C, 14N, 16O(π-, X), E=80 MeV; measured 16 π- capture events; deduced σ. 4n, 8He deduced mass.
Phys.Rev. 175, 1358 (1968)
L.Kaufman, V.Perez-Mendez, J.Sperinde
π- - 4He Inelastic and Capture Reactions Leading to Excited and Multineutron Final States
Nucl.Phys. A109, 1 (1968)
W.E.Meyerhof, T.A.Tombrello
Energy Levels of Light Nuclei A = 4
doi: 10.1016/0375-9474(68)90556-3
Nucl.Phys. A143, 304 (1970)
D.R.Thompson
Study of the d + d System using the Method of Resonating-Group Structure
doi: 10.1016/0375-9474(70)90565-8
Nucl.Phys. A206, 1 (1973)
S.Fiarman, W.E.Meyerhof
Energy Levels of Light Nuclei A = 4
NUCLEAR STRUCTURE 4H, 4He, 4Li; compiled levels, reaction Q-values, J, π, T.
doi: 10.1016/0375-9474(73)90605-2
Yad.Fiz. 26, 249 (1977); Sov.J.Nucl.Phys. 26, 129 (1977)
Y.A.Batusov, L.Vizireva, V.B.Kovacheva, P.Cuer, J.P.Massue, F.Mirsalikhova, V.M.Sidorov, K.M.Chernev
Search for Neutron Nuclei in Absorption of π- Mesons in Emulsion Loaded with 7Li
NUCLEAR REACTIONS 7Li(π-, α), (π-,3He), E=0 MeV; measured σ for production of neutron nuclei 3n, 4n.
Nucl.Phys. A341, 414 (1980)
J.J.Bevelacqua
Theoretical Estimates of the Trineutron and Tetraneutron Finding Energies
NUCLEAR STRUCTURE 3n, 4n; calculated binding energies. Translationally invariant, symmetrized oscillator basis.
doi: 10.1016/0375-9474(80)90374-7
Nucl.Phys. A350, 149 (1980)
F.W.N.De Boer, J.J.Van Ruyven, A.W.B.Kalshoven, H.Verheul, R.Vis, E.Sugarbaker, C.Fields, C.S.Zaidins
The Tetraneutron Revisited
NUCLEAR REACTIONS 130Te(3He, 4n), E=44, 130 MeV; deduced upper limit for process.
RADIOACTIVITY 132Te [from 130Te(4n, 2n)]; measured Eγ, Iγ, Eβ, Iβ. Ge(Li) detector, chemical separations, enriched, natural targets.
doi: 10.1016/0375-9474(80)90393-0
Phys.Lett. 102B, 381 (1981)
R.I.Jibuti, R.Ya.Kezerashvili, K.I.Sigua
Investigation of π-(π+) + 4He → π+(π-) + 4n(4p) Reactions
NUCLEAR REACTIONS 4He(π-, π+), E=140, 176 MeV; calculated σ(θ, E(π+)); 4He(π+, π-), E=0.1-1.75 GeV; calculated σ(E); deduced final state interaction effects. Four-body model, hyperspherical basis.
doi: 10.1016/0370-2693(81)91236-3
Yad.Fiz. 34, 661 (1981)
G.P.P.Kamuntavichyus
Lower Limits on the Bound State Energies of Atomic Nuclei
NUCLEAR STRUCTURE 3,4,5n, 3,4,5H, 3,4,5He, 4,5Li, 4,5Be, 5B; calculated binding energy lower limit. Realistic potentials.
LA-8768-PR, p.29 (1981)
V.Perez-Mendez, A.Stetz
Pion-Induced Double Charge Exchange on Helium Isotopes
NUCLEAR REACTIONS 3,4He(π-, π+), E=140, 200, 295 MeV; measured σ(θ, E(π)) vs three, four-neutron missing mass.
Phys.Lett. 144B, 333 (1984)
J.E.Ungar, R.D.McKeown, D.F.Geesaman, R.J.Holt, J.R.Specht, K.E.Stephenson, B.Zeidman, C.L.Morris
Search for the Tetraneutron by the Double-Charge-Exchange of Negative Pions
NUCLEAR REACTIONS 12C, 4He(π-, π+), E=165 MeV; measured σ(θ) vs pion momentum; deduced bound tetraneutron production σ upper limit.
doi: 10.1016/0370-2693(84)91272-3
Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1936 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 64 (1986)
A.V.Belozerov, K.Borcha, Z.Dlouty, A.M.Kalinin, Nguen Khoai Tyau, Yu.E.Penionzhkevich
Determination of Nucleon Stability and Investigation of Quasi-Stationary States for Multi-Neutron Nuclei 3n, 4n, 4H, 5H, 6H
NUCLEAR REACTIONS 7Li(11B, 14O), (11B, 15O), 9Be(11B, 14O), (11B, 15O), (11B, 16O), E=88 MeV; measured product spectra. 3,4n, 4,5,6H deduced unbound levels, T1/2, Γ.
Pisma Zh.Eksp.Teor.Fiz. 44, 498 (1986); JETP Lett.(USSR) 44, 641 (1986)
A.V.Belozerov, K.Borcha, Z.Dlouhy, A.M.Kalinin, Nguyen Hoai Tyau, Yu.E.Penionzhkevich
Search for 3n and 4n in the Reactions 7Li + 11B
NUCLEAR REACTIONS 7Li(11B, 14O), (11B, 15O), E=88 MeV; measured σ(E(14O)), σ(E(15O)), σ(ejecticle θ, E); deduced residual production σ limits. Magnetic analyzer.
Yad.Fiz. 44, 842 (1986); Sov.J.Nucl.Phys. 44, 542 (1986)
R.Ya.Kezerashvili
Does a Tetraneutron Exist ( Question )
NUCLEAR REACTIONS 4He(π-, π+), E at 165 MeV/c; calculated σ(Eπ+, θπ+); deduced no evidence for tetraneutron.
Phys.Rev.Lett. 57, 3152 (1986)
E.R.Kinney, J.L.Matthews, P.A.M.Gram, D.W.MacArthur, E.Piasetzky, G.A.Rebka, Jr., D.A.Roberts
Inclusive Pion Double Charge Exchange in 4He
NUCLEAR REACTIONS 4He(π+, π-), (π-, π+), E=120, 150, 180, 240, 270 MeV; measured σ(E(π), θ(π)); deduced reaction mechanism. Liquid helium target, double focusing spectrometer.
doi: 10.1103/PhysRevLett.57.3152
JINR-E7-87-140 (1987)
A.V.Belozyorov, C.Borcea, Z.Dlouhy, A.M.Kalinin, Nguyen Hoai Chau, Yu.E.Penionzhkevich
Search for the Tri- and Tetraneutron in Reactions Induced by 11B and 9Be Ions on 7Li and 9Be
NUCLEAR REACTIONS 7Li(9Be, 12N), 9Be(9Be, 14O), E=107 MeV; 7Li(11B, 14O), (11B, 15O), E=88 MeV; measured σ(E(12N)), σ(E(14O)), σ(E(15O)); deduced trineutron, tetraneutron production σ uper limit. Magnetic spectrograph, ionization chamber.
Rev.Roum.Phys. 32, 497 (1987)
C.Borcea, A.V.Belozyorov, Z.Dlouhy, A.M.Kalinin, Nguyen Hoai Chau, Yu.E.Penionzhkevich
Experimental Study of Multineutron Systems and Heavy Isotopes of H and He
NUCLEAR REACTIONS 7Li(11B, 15O), (11B, 14O), (11B, 14N), (11B, 13C), (11B, 12C), (11B, 11C), (11B, 10C), E(cm)=34.2 MeV; 7Li(9Be, 12N), E(cm)=46.81 MeV; 9Be(11B, 16O), (11B, 15O), (11B, 14O), (11B, 13N), E(cm)=39.6 MeV; 9Be(14C, 14O), E(cm)=61.83 MeV; 9Be(14C, 16O), E(cm)=60.26 MeV; measured energy spectra, σ(θ). 3n, 4n, 5H deduced unbound states. 6H deduced excitation energy. 5,6,7,8,9He deduced levels, Γ. Magnetic spectrograph. Phase space calculations.
Nucl.Phys. A477, 131 (1988)
A.V.Belozyorov, C.Borcea, Z.Dlouhy, A.M.Kalinin, Nguyen Hoai Chau, Yu.E.Penionzhkevich
Search for the Tri- and Tetra-Neutron in Reactions Induced by 11B and 9Be Ions on 7Li
NUCLEAR REACTIONS 7Li(11B, 14O), E=48-71 MeV; 7Li(11B, 15O), E=52-76 MeV; 7Li(9Be, 12N), E=58-85 MeV; 9Be(9Be, 14O), E=72-90 MeV; measured σ(E(14O)), σ(E(15O)), σ(E(12N)); deduced 3n, 4n production σ upper limit. Phase space analysis.
doi: 10.1016/0375-9474(88)90365-X
Ukr.Fiz.Zh. 33, 176 (1988)
E.V.Inopin, Yu.V.Kirichenko
On Possibility of Existence of Multineutrons
NUCLEAR STRUCTURE 4n; calculated total energy; deduced no tetraneutron stable state. Variational principle.
Phys.Rev. C40, 2390 (1989)
T.P.Gorringe, S.Ahmad, D.S.Armstrong, R.A.Burnham, M.D.Hasinoff, A.J.Larabee, C.E.Waltham, G.Azuelos, J.A.Macdonald, J.-M.Poutissou, M.Blecher, D.H.Wright, P.Depommier, R.Poutissou, E.T.H.Clifford
Search for the Tetraneutron using the Reaction 4He(π-, π+)4n
NUCLEAR REACTIONS 4He(π-, π+), E=80 MeV; measured pion momentum spectra; deduced tetraneutron production σ upper limit.
Yad.Fiz. 50, 347 (1989)
A.M.Gorbatov, P.V.Komarov, Yu.N.Krylov, A.V.Bursak, V.L.Skopich, P.Yu.Nikishov, E.A.Kolganova
Multineutron Systems in Hyperspherical Basis
NUCLEAR STRUCTURE 3,4,6,8n; calculated bound state nonexistence. Hyperspherical basis.
Yad.Fiz. 50, 19 (1989)
I.F.Gutich, A.V.Nesterov, I.P.Okhrimenko
Study of Tetraneutron Continuum States
NUCLEAR STRUCTURE 4n; calculated continuum levels; deduced kinematical barrier resonance, parameters. Hyperspherical method.
Nucl.Phys. A541, 1 (1992)
D.R.Tilley, H.R.Weller, G.M.Hale
Energy Levels of Light Nuclei A = 4
COMPILATION 4H, 4He, 4Li; compiled, evaluated structure data.
doi: 10.1016/0375-9474(92)90635-W
J.Phys.(London) G23, 1619 (1997)
S.A.Sofianos, S.A.Rakityansky, G.P.Vermaak
Subthreshold Resonances in Few-Neutron Systems
NUCLEAR STRUCTURE 3,4n; calculated subthreshold resonant states; deduced potential sensitivity. Jost function.
doi: 10.1088/0954-3899/23/11/010
Phys.Rev. C65, 044006 (2002)
F.M.Marques, M.Labiche, N.A.Orr, J.C.Angelique, L.Axelsson, B.Benoit, U.C.Bergmann, M.J.G.Borge, W.N.Catford, S.P.G.Chappell, N.M.Clarke, G.Costa, N.Curtis, A.D'Arrigo, E.de Goes Brennand, F.de Oliveira Santos, O.Dorvaux, G.Fazio, M.Freer, B.R.Fulton, G.Giardina, S.Grevy, D.Guillemaud-Mueller, F.Hanappe, B.Heusch, B.Jonson, C.Le Brun, S.Leenhardt, M.Lewitowicz, M.J.Lopez, K.Markenroth, A.C.Mueller, T.Nilsson, A.Ninane, G.Nyman, I.Piqueras, K.Riisager, M.G.Saint Laurent, F.Sarazin, S.M.Singer, O.Sorlin, L.Stuttge
Detection of Neutron Clusters
NUCLEAR REACTIONS C(14Be, nX), E=35 MeV/nucleon; C(11Li, nX), E=30 MeV/nucleon; C(15B, X), E=48 MeV/nucleon; measured En, (charged particle)n-, nn-coin, angular distributions; deduced possible neutron cluster formation.
doi: 10.1103/PhysRevC.65.044006
Phys.Rev. C 68, 034303 (2003)
K.Arai
Resonance states of 5H and 5Be in a microscopic three-cluster model
NUCLEAR STRUCTURE 5H, 5,6He, 4,5Li, 5,6Be; calculated resonance energies, J, π, widths. 4n calculated energy eigenvalues; deduced no resonance states. Microscopic three-cluster model.
doi: 10.1103/PhysRevC.68.034303
J.Phys.(London) G29, 2431 (2003)
C.A.Bertulani, V.Zelevinsky
Is the tetraneutron a bound dineutron-dineutron molecule?
NUCLEAR STRUCTURE 4n; calculated dinuetron-dineutron molecular potential; deduced no bound state.
doi: 10.1088/0954-3899/29/10/309
Phys.Rev.Lett. 90, 252501 (2003)
S.C.Pieper
Can Modern Nuclear Hamiltonians Tolerate a Bound Tetraneutron ?
NUCLEAR STRUCTURE 2,4,6,8n, 2,3,4,5H, 4,5,6He, 6Li; calculated binding energies. Various nuclear Hamiltonians compared.
doi: 10.1103/PhysRevLett.90.252501
J.Phys.(London) G29, L9 (2003)
N.K.Timofeyuk
Do multineutrons exist?
NUCLEAR STRUCTURE 4,6,8,10n; calculated hyperradial potentials, deduced no bound or resonance states. 4H, 4He; calculated binding energies.
doi: 10.1088/0954-3899/29/2/102
Nucl.Phys. A722, 55c (2003)
R.Wolski, S.I.Sidorchuk, G.M.Ter-Akopian, A.S.Fomichev, A.M.Rodin, S.V.Stepantsov, W.Mittig, P.Roussel-Chomaz, H.Savajols, N.Alamanos, F.Auger, V.Lapoux, R.Raabe, Yu.M.Tchuvil'sky, K.Rusek
Elastic scattering of 8He on 4He and 4n system
NUCLEAR REACTIONS 4He(8He, 8He), E=26 MeV/nucleon; measured σ(θ). 2H(8He, 6Li), E=96 MeV; calculated σ(θ), excitation energy distribution.
doi: 10.1016/S0375-9474(03)01335-6
Eur.Phys.J. A 19, 187 (2004)
L.V.Grigorenko, N.K.Timofeyuk, M.V.Zhukov
Broad states beyond the neutron drip line Examples of 5H and 4n
NUCLEAR STRUCTURE 5H; calculated levels, J, π, widths. 4n, 5H; calculated continuum response, related features. Model with source approach.
doi: 10.1140/epja/i2003-10124-1
Phys.Rev. C 69, 027601 (2004)
B.M.Sherrill, C.A.Bertulani
Proton-tetraneutron elastic scattering
NUCLEAR REACTIONS 4n(p, p), E=14 MeV; calculated σ(θ), backscattered proton spectra. Implications for previous experiment discussed.
doi: 10.1103/PhysRevC.69.027601
Nucl.Phys. A738, 431 (2004)
R.Wolski, P.Roussel-Chomaz, S.I.Sidorchuk, G.M.Ter-Akopian
Search for extremely neutron rich systems
NUCLEAR REACTIONS C(6He, X), E=240 MeV/nucleon; 2H(t, p), E not given; 2H(8He, 4n), E not given; analyzed data. 4n, 4,5H deduced resonance features.
doi: 10.1016/j.nuclphysa.2004.04.080
Nucl.Phys. A752, 279c (2005)
Y.Blumenfeld
Reactions near the neutron drip-line
NUCLEAR REACTIONS 1H(6He, 6He), (6He, 6He'), E=15 MeV/nucleon; measured σ(q); deduced halo effect. 1H(6He, α), E=25 MeV/nucleon; measured σ(θ). 2H(8He, 6Li), E=15 MeV/nucleon; measured excitation energy spectrum; deduced possible resonance structure. 1H(22O, 22O'), E=46.6 MeV/nucleon; measured σ(E, θ).
doi: 10.1016/j.nuclphysa.2005.02.146
Phys.Rev. C 72, 044608 (2005)
E.R.Kinney, J.L.Matthews, P.A.M.Gram, D.W.MacArthur, E.Piasetzky, G.A.Rebka, Jr., D.A.Roberts
Inclusive pion double charge exchange in 4He at intermediate energies
NUCLEAR REACTIONS 4He(π+, π-), E=120, 150, 180, 240, 270 MeV; 4He(π-, π+), E=180, 240 MeV; measured σ(E, θ); deduced multiple scattering effects, total σ.
doi: 10.1103/PhysRevC.72.044608
Phys.Rev. C 72, 034003 (2005)
R.Lazauskas, J.Carbonell
Is a physically observable tetraneutron resonance compatible with realistic nuclear interactions?
NUCLEAR STRUCTURE 4n; calculated resonance energies; deduced no observable state. Faddeev-Yakubovski equations, realistic interactions, complex scaling and analytical continuation in the coupling constant.
doi: 10.1103/PhysRevC.72.034003
Eur.Phys.J. A 25, Supplement 1, 311 (2005)
F.M.Marques Moreno, for the Demon-Charissa Collaborations
Multineutron clusters: Perspectives to create nuclei 100% neutron-rich
NUCLEAR REACTIONS C(14Be, nX), E not given; analyzed En, (charged particle)n-coin; deduced possible neutron cluster formation.
doi: 10.1140/epjad/i2005-06-208-8
Ukr.J.Phys. 51, 954 (2006)
I.V.Simenog, B.E.Grinyuk, Yu.M.Bidasyuk
Can tetraneutron exist from theoretical point of view?
NUCLEAR STRUCTURE 4n, 3H, 4He; calculated bound state features, pair correlation functions.
Proc.Intern.Symposium on Exotic Nuclei, Khanty-Mansiysk, Russia, 17-22 July, 2006, Yu.E.Penionzhkevich, E.A.Cherepanov, Eds. p.3 (2007); AIP Conf.Proc. 912 (2007)
S.Fortier, E.Tryggestad, E.Rich, D.Beaumel, E.Becheva, Y.Blumenfeld, F.Delaunay, A.Drouart, A.Fomichev, N.Frascaria, S.Gales, L.Gaudefroy, A.Gillibert, J.Guillot, F.Hammache, K.W.Kemper, E.Khan, V.Lapoux, V.Lima, L.Nalpas, A.Obertelli, E.C.Pollacco, F.Skaza, U.Datta Pramanik, P.Roussel-Chomaz, D.Santonocito, J.A.Scarpaci, O.Sorlin, S.V.Stepantsov, G.M.Ter Akopian, R.Wolski
Search for resonances in 4n, 7H and 9He via transfer reactions
NUCLEAR REACTIONS 2H(8He, p), (8He, α), (8He, 6Li), E=15.3 MeV/nucleon; measured charged particle energies and yields.
doi: 10.1063/1.2746575
Phys.Lett. B 644, 33 (2007)
A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber
Realistic nuclear Hamiltonian: Ab exitu approach
NUCLEAR STRUCTURE 3H, 3,4He, 6He, 6,7Li, 7,8,9,10Be, 9,10,11,12B, 10,11,12,13,14C, 12,13,14,15N, 13,14,15,16O; calculated binding energies with bare JISP16 and effective interaction generated by JISP16, ground and excitation energies. Fully-microscopic no-core shell model (NCSM).
doi: 10.1016/j.physletb.2006.10.066
Phys.Atomic Nuclei 71, 209 (2008)
Yu.A.Lashko, G.F.Filippov
Cluster structure of a low-energy resonance in tetraneutron
NUCLEAR STRUCTURE 2,3,4NN; calculated effective 2n-2n potential, eigenvalues, effective intercluster potential induced by the Rosenfeld interaction, phase shift of the elastic 2n-2n scattering in the coupled-channel approach, coefficients of the expansion of the continuum states of the 4NN system in the SU(3) basis; deduced that the tetraneutron has a good chance to exist as a compound system, where 3n+n and 2n-2n coupled cluster configurations coexist.
doi: 10.1134/S1063778808020014
Phys.Rev. C 81, 064606 (2010)
E.Yu.Nikolskii, A.A.Korsheninnikov, H.Otsu, H.Suzuki, K.Yoneda, H.Baba, K.Yamada, Y.Kondo, N.Aoi, A.S.Denikin, M.S.Golovkov, A.S.Fomichev, S.A.Krupko, M.Kurokawa, E.A.Kuzmin, I.Martel, W.Mittig, T.Motobayashi, T.Nakamura, M.Niikura, S.Nishimura, A.A.Ogloblin, P.Roussel-Chomaz, A.Sanchez-Benitez, Y.Satou, S.I.Sidorchuk, T.Suda, S.Takeuchi, K.Tanaka, G.M.Ter-Akopian, Y.Togano, M.Yamaguchi
Search for 7H in 2H+8He collisions
NUCLEAR REACTIONS 2H(8He, 3He)7H, E=42 MeV/nucleon; 2H(12Be, 3He)11Li, E=71 MeV/nucleon; measured 3He spectra; deduced missing-mass spectra of 7H. Search for 7H. Comparison with DWBA calculations.
doi: 10.1103/PhysRevC.81.064606
Nature(London) 532, 448 (2016)
C.A.Bertulani, V.Zelevinsky
Four neutrons together momentarily
NUCLEAR STRUCTURE 4NN; analyzed available data; deduced evidence for the fleeting existence of this state, implications for neutron stars.
doi: 10.1038/nature17884
Phys.Rev. C 93, 044004 (2016)
E.Hiyama, R.Lazauskas, J.Carbonell, M.Kamimura
Possibility of generating a 4-neutron resonance with a T=3/2 isospin 3-neutron force
NUCLEAR STRUCTURE 4n; calculated narrow resonant states of tetraneutron for Jπ=0+, 2+ and 2-. 4H, 4He, 4Li; calculated energies of the lowest T=1, Jπ=2- states. 3n; calculated resonance trajectories for Jπ=3/2-, 1/2- and 1/2+ states. Complex scaling method (CSM) for resonance positions and widths. Gaussian expansion method used to solve Schrodinger equation and Lagrange-mesh technique to solve Faddeev-Yakubovsky (FY) equation. Comparison with recent experimental data from RIKEN.
doi: 10.1103/PhysRevC.93.044004
Phys.Rev.Lett. 116, 052501 (2016)
K.Kisamori, S.Shimoura, H.Miya, S.Michimasa, S.Ota, M.Assie, H.Baba, T.Baba, D.Beaumel, M.Dozono, T.Fujii, N.Fukuda, S.Go, F.Hammache, E.Ideguchi, N.Inabe, M.Itoh, D.Kameda, S.Kawase, T.Kawabata, M.Kobayashi, Y.Kondo, T.Kubo, Y.Kubota, M.Kurata-Nishimura, C.S.Lee, Y.Maeda, H.Matsubara, K.Miki, T.Nishi, S.Noji, S.Sakaguchi, H.Sakai, Y.Sasamoto, M.Sasano, H.Sato, Y.Shimizu, A.Stolz, H.Suzuki, M.Takaki, H.Takeda, S.Takeuchi, A.Tamii, L.Tang, H.Tokieda, M.Tsumura, T.Uesaka, K.Yako, Y.Yanagisawa, R.Yokoyama, K.Yoshida
Candidate Resonant Tetraneutron State Populated by the 4He(8He, 8Be) Reaction
NUCLEAR REACTIONS 4He(8He, 8Be), E=186 MeV/nucleon; measured missing-mass spectrum; deduced the tetraneutron system energy of the state with uncertainties, Q-value.
doi: 10.1103/PhysRevLett.116.052501
Phys.Rev.Lett. 117, 182502 (2016)
A.M.Shirokov, G.Papadimitriou, A.I.Mazur, I.A.Mazur, R.Roth, J.P.Vary
Prediction for a Four-Neutron Resonance
NUCLEAR REACTIONS 4He(8He, 8Be), E<30 MeV; calculated scattering phase shifts, tetraneutron ground state energy, resonance parameters. ab initio approach using the JISP16 realistic NN interaction.
doi: 10.1103/PhysRevLett.117.182502
Few-Body Systems 58, 67 (2017)
J.Carbonell, R.Lazauskas, E.Hiyama, M.Kamimura
On the Possible Existence of Four Neutron Resonances
NUCLEAR REACTIONS 3He(n, n), E=0.03-10 MeV;3He(n, x), E not given; calculated possible tetraneutron resonance trajectory for 0+ state; deduced resonance, σ, resonance energy and width vs other parameters, higher 4n resonances, tetraneutron production response function via double charge exchange; deduced parameters.
doi: 10.1007/s00601-017-1219-0
Phys.Rev.Lett. 119, 032501 (2017)
K.Fossez, J.Rotureau, N.Michel, M.Ploszajczak
Can Tetraneutron be a Narrow Resonance?
NUCLEAR STRUCTURE 4NN; analyzed available data; calculated evolution of the energy and width of the four-neutron system with the scaling of the N3LO interaction; deduced the energy of the four-neutron system compatible with the experimental value, its width must be larger than the reported upper limit, supporting the interpretation of the experimental observation as a reaction process too short to form a nucleus. Quasistationary formalism using ab initio techniques with various two-body chiral interactions.
doi: 10.1103/PhysRevLett.119.032501
Phys.Rev.Lett. 118, 232501 (2017)
S.Gandolfi, H.-W.Hammer, P.Klos, J.E.Lynn, A.Schwenk
Is a Trineutron Resonance Lower in Energy than a Tetraneutron Resonance?
doi: 10.1103/PhysRevLett.118.232501
Prog.Theor.Exp.Phys. 2017, 073D03 (2017)
R.Lazauskas, J.Carbonell, E.Hiyama
Modeling the double charge exchange response function for a tetraneutron system
NUCLEAR REACTIONS 4He(8He, 8Be)4NN, E<8 MeV; analyzed available data; calculated σ, response functions, 4n resonance trajectory.
doi: 10.1093/ptep/ptx078
Int.J.Mod.Phys. E26, 1730003 (2017)
M.Thoennessen
2016 Update of the discoveries of nuclides
COMPILATION 4NN, 96In, 94Cd, 92Ag, 90Pd, 63Se, 67,68Kr, 178Pb, 230Am, 234Cm, 234Bk; compiled first identification (or discovery) of isotopes.
doi: 10.1142/S021830131730003X
Phys.Lett. B 782, 238 (2018)
A.Deltuva
Tetraneutron: Rigorous continuum calculation
NUCLEAR STRUCTURE 4NN; calculated energy dependence of selected 4n transition matrix elements using half-shell matrix elements of 4n transition operators.
doi: 10.1016/j.physletb.2018.05.041
Phys.Rev. C 100, 044002 (2019)
A.Deltuva, R.Lazauskas
Tetraneutron resonance in the presence of a dineutron
NUCLEAR REACTIONS 2n(2n, 2n)4n; calculated dineutron scattering phase shifts and cross sections by solving exact four-particle continuum using Faddeev-Yakubovsky (FY) and Alt, Grassberger, and Sandhas (AGS) equations, and by varying the interaction enhancement factor; deduced bound tetraneutron as a virtual 0+ state.
doi: 10.1103/PhysRevC.100.044002
Phys.Rev. C 100, 054313 (2019)
J.G.Li, N.Michel, B.S.Hu, W.Zuo, F.R.Xu
Ab initio no-core Gamow shell-model calculations of multineutron systems
NUCLEAR STRUCTURE 3,4n; calculated resonances, energies and widths using the ab-initio no-core Gamow shell model based on nuclear chiral effective field theory interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.054313
Phys.Rev.Lett. 125, 052501 (2020)
M.D.Higgins, C.H.Greene, A.Kievsky, M.Viviani
Nonresonant Density of States Enhancement at Low Energies for Three or Four Neutrons
NUCLEAR STRUCTURE 3,4NN; calculated hyperspherical potential curves, rescaled Wigner-Smith time delays, low energy enhancement of the density of states.
doi: 10.1103/PhysRevLett.125.052501
Bull.Rus.Acad.Sci.Phys. 84, 1183 (2020)
A.V.Yushkov, V.V.Dyachkov, Y.A.Zaripova
A New Approach to the Experimental Detection and Study of Multineutrons
NUCLEAR REACTIONS 4He(16O, X)4NN, E=160 MeV; 2,3H(16O, X)2NN/3NN, E=160 MeV;calculated kinematics for the detection of tetraneutrons, dineutrons and trineutrons.
doi: 10.3103/S1062873820100305
Phys.Rev. C 103, 024004 (2021)
M.D.Higgins, C.H.Greene, A.Kievsky, M.Viviani
Comprehensive study of the three- and four-neutron systems at low energies
NUCLEAR STRUCTURE 3,4n; calculated adiabatic hyperspherical potential curves for Jπ=3/2- for the 3n system and Jπ=0+ for the 4n system, phase shifts and eigenshifts using explicitly correlated Gaussian (CGHS) and the hyperspherical harmonic (HH) bases, multichannel analysis of the three-and four-neutron scattering near the scattering continuum threshold; deduced no evidence of a 4n-resonance at low energy. Discussed experimental result of possible 4n resonance by 2016Ki01 in 4He(8He, 4n8Be) reaction.
doi: 10.1103/PhysRevC.103.024004
Few-Body Systems 62, 102 (2021)
S.W.Huang, Z.H.Yang, F.M.Marques, N.L.Achouri, D.S.Ahn, T.Aumann, H.Baba, D.Beaumel, M.Bohmer, K.Boretzky, M.Caamano, S.Chen, N.Chiga, M.L.Cortes, D.Cortina, P.Doornenbal, C.A.Douma, F.Dufter, J.Feng, B.Fernandez-Dominguez, Z.Elekes, U.Forsberg, T.Fujino, N.Fukuda, I.Gasparic, Z.Ge, R.Gernhauser, J.M.Gheller, J.Gibelin, A.Gillibert, Z.Halasz, T.Harada, M.N.Harakeh, A.Hirayama, N.Inabe, T.Isobe, J.Kahlbow, N.Kalantar-Nayestanaki, D.Kim, S.Kim, S.Kiyotake, T.Kobayashi, Y.Kondo, P.Koseoglou, Y.Kubota, I.Kuti, C.Lehr, C.Lenain, P.J.Li, Y.Liu, Y.Maeda, S.Masuoka, M.Matsumoto, A.Matta, J.Mayer, H.Miki, M.Miwa, B.Monteagudo, I.Murray, T.Nakamura, A.Obertelli, N.A.Orr, H.Otsu, V.Panin, S.Park, M.Parlog, S.Paschalis, M.Potlog, S.Reichert, A.Revel, D.Rossi, A.Saito, M.Sasano, H.Sato, H.Scheit, F.Schindler, T.Shimada, Y.Shimizu, S.Shimoura, H.Simon, I.Stefan, S.Storck, L.Stuhl, H.Suzuki, D.Symochko, H.Takeda, S.Takeuchi, J.Tanaka, Y.Togano, T.Tomai, H.T.Tornqvist, E.Tronchin, J.Tscheuschner, T.Uesaka, V.Wagner, K.Wimmer, H.Yamada, B.Yang, L.Yang, Y.Yasuda, K.Yoneda, L.Zanetti, J.Zenihiro
Experimental Study of 4n by Directly Detecting the Decay Neutrons
RADIOACTIVITY 7H(t), 6He(2n) [from 1H(8He, 2p), E=150 MeV/nucleon]; measured decay products, En, In. 4NN; deduced relative-energy spectrum, neutron multiplicity distribution. The radioactive isotope beam factory (RIBF).
doi: 10.1007/s00601-021-01691-4
Eur.Phys.J. A 57, 105 (2021)
F.M.Marques, J.Carbonell
The quest for light multineutron systems
NUCLEAR REACTIONS 12C, 4He(π-, π+), E=165 MeV; 7Li(7Li, 10C), E<65 MeV; analyzed available data. 3,4NN; deduced miltineutron systems.
doi: 10.1140/epja/s10050-021-00417-8
Chin.Phys.C 45, 030003 (2021)
M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi
The AME 2020 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.
Nature(London) 606, 678 (2022)
M.Duer, T.Aumann, R.Gernhauser, V.Panin, S.Paschalis, D.M.Rossi, N.L.Achouri, D.Ahn, H.Baba, C.A.Bertulani, M.Bohmer, K.Boretzky, C.Caesar, N.Chiga, A.Corsi, D.Cortina-Gil, C.A.Douma, F.Dufter, Z.Elekes, J.Feng, B.Fernandez-Dominguez, U.Forsberg, N.Fukuda, I.Gasparic, Z.Ge, J.M.Gheller, J.Gibelin, A.Gillibert, K.I.Hahn, Z.Halasz, M.N.Harakeh, A.Hirayama, M.Holl, N.Inabe, T.Isobe, J.Kahlbow, N.Kalantar-Nayestanaki, D.Kim, S.Kim, T.Kobayashi, Y.Kondo, D.Korper, P.Koseoglou, Y.Kubota, I.Kuti, P.J.Li, C.Lehr, S.Lindberg, Y.Liu, F.M.Marques, S.Masuoka, M.Matsumoto, J.Mayer, K.Miki, B.Monteagudo, T.Nakamura, T.Nilsson, A.Obertelli, N.A.Orr, H.Otsu, S.Y.Park, M.Parlog, P.M.Potlog, S.Reichert, A.Revel, A.T.Saito, M.Sasano, H.Scheit, F.Schindler, S.Shimoura, H.Simon, L.Stuhl, H.Suzuki, D.Symochko, H.Takeda, J.Tanaka, Y.Togano, T.Tomai, H.T.Tornqvist, J.Tscheuschner, T.Uesaka, V.Wagner, H.Yamada, B.Yang, L.Yang, Z.H.Yang, M.Yasuda, K.Yoneda, L.Zanetti, J.Zenihiro, M.V.Zhukov
Observation of a correlated free four-neutron system
NUCLEAR REACTIONS 1H(8He, pα)4NN, E=156 MeV/nucleon; measured reaction products, Ep, Ip, Eα, Iα. 4NN; deduced missing mass spectra, 4NN resonance, resonance parameters. Comparison with theoretical calculations. The Radioactive Ion Beam Factory operated by the RIKEN Nishina Center and the Center for Nuclear Study, University of Tokyo, using the Superconducting Analyzer for Multi-particles from Radio Isotope Beams (SAMURAI).
doi: 10.1038/s41586-022-04827-6
Phys.Lett. B 824, 136799 (2022)
T.Faestermann, A.Bergmaier, R.Gernhauser, D.Koll, M.Mahgoub
Indications for a bound tetraneutron
NUCLEAR REACTIONS 7Li(7Li, 10C)4NN, E=46 MeV; measured reaction products. 10C; deduced energy spectra, tetraneutron binding energy.
doi: 10.1016/j.physletb.2021.136799
Phys.Rev.Lett. 130, 102501 (2023)
R.Lazauskas, E.Hiyama, J.Carbonell
Low Energy Structures in Nuclear Reactions with 4n in the Final State
NUCLEAR STRUCTURE 8He, 2,4NN; calculated strength and low energy four-neutron response functions with the AV18 nn interaction, low energy 4n response functions for the scaled nn MT13 potential; deduced the sharp low energy peak observed by studying the missing mass spectra of four neutrons as a consequence of dineutron-dineutron correlations.
doi: 10.1103/PhysRevLett.130.102501