2 research outputs found

    The 6^{6}H states studied in the d(8He,α)d(^8\text{He},\alpha) reaction and evidence of extremely correlated character of the 5^{5}H ground state

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    The extremely neutron-rich system 6^{6}H was studied in the direct 2H(8He,4He)6^2\text{H}(^8\text{He},{^4\text{He}})^{6}H transfer reaction with a 26 AAMeV secondary 8^{8}He beam. The measured missing mass spectrum shows a resonant state in 6^{6}H at 6.8(3)6.8(3) MeV relative to the 3^3H+3n3n threshold. There is also some evidence of a resonant state at 4.5(3)4.5(3) MeV which is a realistic candidate for the 6^{6}H ground state (g.s.). The population cross section of the presumably pp-wave states in the energy range from 4 to 8 MeV is dσ/dΩc.m.190d\sigma/d\Omega_{\text{c.m.}} \sim 190μ\mub/sr in the angular range 5<θc.m.<165^{\circ}<\theta_{\text{c.m.}}<16^{\circ}. The obtained missing mass spectrum is free of the 6^{6}H events below 3.5 MeV (dσ/dΩc.m.3d\sigma/d\Omega_{\text{c.m.}} \lesssim 3μ\mub/sr in the angular range 5<θc.m.<205^{\circ}<\theta_{\text{c.m.}}<20^{\circ}), which indicates that the value of 4.5 MeV is the lower limit of the possible 6^{6}H g.s. location. The obtained results confirm that the decay mechanism of the 7^{7}H g.s. (located at 2.2 MeV above the 3^{3}H+4n4n threshold) is the ``true'' (or simultaneous) 4n4n emission. The resonance energy profiles and the momentum distributions of the sequential 6^{6}H \,\rightarrow \, ^5H(g.s.)+n\, \rightarrow \, ^3H+3n3n decay fragments were analyzed by the theoretically-updated direct four-body-decay and sequential-emission mechanisms. The measured momentum distributions of the 3^{3}H fragments in the 6^{6}H rest frame indicate a very strong ``dineutron-type'' correlations in the 5^{5}H ground state decay

    A new Time-of-flight detector for the R 3 B setup

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    © 2022, The Author(s).We present the design, prototype developments and test results of the new time-of-flight detector (ToFD) which is part of the R3B experimental setup at GSI and FAIR, Darmstadt, Germany. The ToFD detector is able to detect heavy-ion residues of all charges at relativistic energies with a relative energy precision σΔE/ ΔE of up to 1% and a time precision of up to 14 ps (sigma). Together with an elaborate particle-tracking system, the full identification of relativistic ions from hydrogen up to uranium in mass and nuclear charge is possible.11Nsciescopu
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