G. Neyens

Nuclear magnetic and quadrupole moments for nuclear structure research on exotic nuclei

Some errors were found in this review after it was published. Page 642, line 1: gSchmidt(πd3/2)=0.083 Page 642, paragraph 2.1.3, line 7 and line 12: gSchmidt = -1.913 should read μSchmidt = -1.913 Page 663, expression (4.7) should read: Figure 13 was incorrectly labelled. The correct figure is given below. Figure 13. (a) Zeeman splitting of the nuclear m-quantum levels due to interaction of the nuclear dipole moment (μ = gIμN) with a static magnetic field B. In a classical picture this can be seen as a precession of the spin I around B with a Larmor frequency νL. (b) Non-equidistant quadrupole splitting of the nuclear m-quantum levels due to interaction of the nuclear spectroscopic quadrupole moment Qs with an EFG Vzz. Page 673, expression (5.8) should read:

Nuclear Charge Radius of 12 Be

The nuclear charge radius of (12)Be was precisely determined using the technique of collinear laser spectroscopy on the 2s(1/2)→2p(1/2,3/2) transition in the Be(+) ion. The mean square charge radius increases from (10)Be to (12)Be by δ(10,12)=0.69(5) fm(2) compared to δ(10,11)=0.49(5) fm(2) for the one-neutron halo isotope ^{11}Be. Calculations in the fermionic molecular dynamics approach show a strong sensitivity of the charge radius to the structure of ^{12}Be. The experimental charge radius is consistent with a breakdown of the N=8 shell closure.

Precision measurement of 11Li moments: influence of halo neutrons on the 9Li core.

The electric quadrupole moment and the magnetic moment of the 11Li halo nucleus have been measured with more than an order of magnitude higher precision than before, |Q| = 33.3(5) mb and mu = +3.6712(3)muN, revealing a 8.8(1.5)% increase of the quadrupole moment relative to that of 9Li. This result is compared to various models that aim at describing the halo properties. In the shell model an increased quadrupole moment points to a significant occupation of the 1d orbits, whereas in a simple halo picture this can be explained by relating the quadrupole moments of the proton distribution to the charge radii. Advanced models so far fail to reproduce simultaneously the trends observed in the radii and quadrupole moments of the lithium isotopes.

Nuclear spins, magnetic moments, and quadrupole moments of Cu isotopes from N = 28 to N = 46: Probes for core polarization effects

Measurements of the ground-state nuclear spins and magnetic and quadrupole moments of the copper isotopes from

Quadrupole-moments of high-spin isomers studied by level mixing spectroscopy (lems)

^{61}\mathrm{Cu}

Use of a Continuous Wave Laser and Pockels Cell for Sensitive High-Resolution Collinear Resonance Ionization Spectroscopy.

up to

g-factor measurements of μs isomeric states in neutron-rich nuclei around 68Ni produced in projectile-fragmentation reactions

^{75}\mathrm{Cu}

Nuclear Charge Radius of 12Be

are reported. The experiments were performed at the CERN online isotope mass separator (ISOLDE) facility, using the technique of collinear laser spectroscopy. The trend in the magnetic moments between the

Development of the CRIS (Collinear Resonant Ionisation Spectroscopy) beam line

N=28

Extension of the level mixing resonance (LMR) method to study the alignment and the quadrupole moment of light exotic projectile fragments

and