Radiative recombination is a process which takes place when a positively charged ion captures an electron to one of its bound orbits with a simultaneous emission of a photon:
e- + A(q+) A(q-1) + photon
In the dielectronic recombination process the energy which becomes available during the capture process is carried away by the promotion of a bound electron to another bound orbit:
e- + A(q+) A(q-1)** A(q-1) + photon
In the second step of the dielectronic recombination process a photon is emitted characteristic to the doubly excited state (**) of the q-1 times ionized ion. The dielectronic recombination is a resonant process, because of the discrete energy nature of the bound electron orbits.
Both radiative and the dielectronic recombination are important capture processes which play a dominant role in determining the charge state balance of highly ionized astrophysical and laboratory plasmas.
In a recent investigation carried out with our EBIT , scandium-like and titanium-like barium ions were created, trapped, and excited. X-ray peaks arising from both radiative recombination and dielectronic recombination were studied simultaneously. In the DR process a 2p electron was promoted to the 3d orbital. One of the M-shell electrons of the recombined ion subsequently decayed radiatively to the 2p vacancy, and emitted an x-ray of energy almost twice the incident kinetic energy of the projectile electron. Comparison with theoretical estimates showed a favorable agreement with the data. The theoretical calculations were carried out by the theory group of the University of Connecticut (McLaughlin and Hahn).
The measurement of excited-state lifetimes is complementary to measuring transition wavelengths as a way of studying atomic structure. Although the lifetimes are determined by the same wavefunctions as the energy levels the measurements of the atomic decays carry different information since they are sensitive to the long-range behavior of the wavefunctions. The knowledge of the lifetimes also has important practical applications. They are critical in the density diagnostics of laboratory and astrophysical plasmas.
The principle of measuring lifetimes with an EBIT lies in the periodic fast switching of different voltages in the machine. Since the ions are created and excited with the same beam of electrons, by changing the electron beam energy one can selectively exclude certain levels from being excited. This can simply be done by setting the electron beam energy below the excitation threshold of the level to be excluded. Without further excitation the time dependence of the emitted photon signal carries the information about the lifetime of the level. After a certain period of time (determined by the lifetime of the level) the electron beam energy is set to be above the excitation threshold to repopulate the level and repeat the sequence. An alternative method for measuring lifetimes with an EBIT is to switch off the electron beam completely, take data, and turn the beam back again to re-excite the ions in the trap. While the electron beam is off, the ions remain trapped by the magnetic field. The lifetime range that can be measured with an EBIT is determined by the capabilities for the fast switching of voltages. In principle the 10 ns to 10 ms lifetime range can be addressed by this method. Since this lifetime range is only partially covered by other methods the EBIT is a unique tool for measuring the lifetime of long living metastable levels.
In a recent experiment we have measured the lifetime of a visible light emitting metastable level . The transition takes places within the ground state configuration of titanium-like ions. The measured lifetimes fall into the millisecond range.