Hyperfine splitting and isotope shift in the atomic D2D_2 line of 22,23^{22,23}Na and the quadrupole moment of 22^{22}Na

The hyperfine structure of the $D_2$ optical line in $^{22}$Na and $^{23}$Na has been investigated using high resolution laser spectroscopy of a well-collimated atomic beam. The hyperfine splitting constants $A$ and $B$ for the excited $3p$ $^2P_{3/2}$ level for both investigated sodium isotopes have been obtained. They are as follows: $A(22) = 7.31(4)$ MHz, $B(22) = 4.71(28)$ MHz, $A(23) = 18.572(24)$ MHz, $B(23) = 2.723(55)$ MHz. With this data, using the high precision MCHF calculations for the electric field gradient at the nucleus, the electric quadrupole moment of $^{22}$Na has been deduced: $Q_s(22) = + 0.185(11)$ b. The sign of $Q_s(22)$, determined for the first time, indicates a prolate nuclear deformation. A precise value of the isotope shift $^{22,23}$Na in the $D_2$ line has also been obtained

Pulse-height defect in single-crystal CVD diamond detectors

International audienceThe pulse-height versus deposited energy response of a single-crystal chemical vapor deposition (scCVD) diamond detector was measured for ions of Ti, Cu, Nb, Ag, Xe, Au, and of fission fragments of$^{252}$ Cf at different energies. For the fission fragments, data were also measured at different electric field strengths of the detector. Heavy ions have a significant pulse-height defect in CVD diamond material, which increases with increasing energy of the ions. It also depends on the electrical field strength applied at the detector. The measured pulse-height defects were explained in the framework of recombination models. Calibration methods known from silicon detectors were modified and applied. A comparison with data for the pulse-height defect in silicon detectors was performed