The structure of the Borromean nucleus Be 9 (α+ α+ n) is addressed within a three-body
approach using the analytical transformed harmonic oscillator method. The three-body …

Photodisintegration of Be 9 through the 1/2+ state near neutron threshold and cluster dipole
resonance below giant dipole resonance was measured with quasi-monochromatic γ-ray …

Background: As a Borromean system, Be 9 is weakly bound, while its mirror partner B 9 is an
unbound system. Such weakly bound and unbound nuclei are usually accompanied with …

We calculate energy spectra, electromagnetic transition rates, longitudinal and transverse
electron scattering form factors and log ft values for beta decay in 9 Be, 9 B, within the …

At the ALADIN-LAND setup at GSI the unbound nucleus 13 Be has been produced in one-
neutron knockout reactions from a 304 MeV/nucleon relativistic beam of 14 Be ions …

We study the character of the first excited 1/2+ state of Be 9, which is observed as a low-lying
sharp peak in the cross section of Be 9 (γ, n) 2 He 4 just above the Be 8+ n threshold. Using …

Background: Weakly bound and unbound nuclei close to particle drip lines are laboratories
of new nuclear structure physics at the extremes of neutron/proton excess. The …

We assume an environment of neutrons and α-particles of given density and temperature
where nuclear syntheses into 6 He, 9 Be and 12 C are possible. We investigate the resulting …

Spectra of the Be 9 (e, e′) reaction have been measured at the Superconducting Darmstadt
Electron Linear Accelerator at an electron energy of E 0= 73 MeV and scattering angles of …

We investigate the low-temperature reaction rates for radiative capture processes of three
particles. We compare direct and sequential capture mechanisms and rates using realistic …