We report on optical investigations of a near-infrared luminescence ba
nd in hexagonal GaN with a single zero-phonon line (ZPL) at 1.1934 eV.
It is attributed to the spin-forbidden internal d-d transition (1)E(D
)-(3)A(2)(F) of a defect with a d(2) electronic configuration. This as
signment is based on the observed Zeeman splittings, which agree with
the ground and excited states being threefold and twofold degenerate,
respectively. This interpretation is supported by the observed small f
ull width at half maximum (FWHM) of the ZPL, the weak phonon sideband,
and the weak temperature dependence of the luminescence band. With in
creasing temperature, the ZPL shifts towards lower energies but mainta
ins its FWHM of about 200 mu eV up to 60 K. The observed luminescence
lifetime of 65 mu s indicates a strong mixing of the (1)E(D) with the
T-3(2)(F) multiplet at slightly higher energies by spin-orbit interact
ion. Photoluminescence excitation spectra show intracenter absorption
into the higher excited T-3(1) states at 1.62 and 2.8 eV in n-type sam
ples, proving the defect to be in the luminescent charge state in n-ty
pe material. Thus, we propose Ti2+ as the luminescence center responsi
ble for the 1.19-eV transition. Implications for the band offset betwe
en GaN and GaAs are discussed.