Rise-time distribution spectra of a polycrystalline chemical vapor deposited diamond detector were directly measured from alpha-particle induced pulse shapes over a temperature range of 240-280 K. Pulses due to hole-dominated charge transport showed a strong delayed component due to thermal detrapping of charge from a shallow level, with a mean rise time that decreased strongly with increasing temperature. The activation energy of this shallow hole trap was directly measured using an Arrhenius plot, with a value of 0.31± 0.03 eV. No priming or pre-irradiation of the device was required in order to observe thermal detrapping, indicating that the concentration of shallow hole traps in this sample is relatively high. In contrast, no delayed component was observed from electron transport, indicating that only deep electron-trapping levels are active. © 2006 American Institute of Physics. ͓DOI: 10.1063/1.2162673͔ Polycrystalline diamond grown by chemical vapor deposition ͑CVD͒ has been studied extensively for use as charged particle detectors operating under harsh radiation and thermal environments. This is due to diamond's unique mechanical and electrical properties, which include a wide band gap ͑ϳ5.5 eV͒, high electron and hole mobilities ͑1800 and 1200 cm 2 V −1 s −1 , respectively͒, high resistivity ͑Ͼ10 11 ⍀ cm͒, and very low device dark currents. 1,2 Unfortunately, the presence of defects and polycrystalline grain boundaries leads to significant charge trapping and recombination, resulting in reduced charge drift lengths and degraded detector performance. Various authors have tentatively identified trapping states in CVD diamond, although there is no clear picture of the role of particular levels, or bands of states, in affecting charge transport performance. However, it is accepted that CVD diamond contains both deep levels, responsible for short carrier lifetimes, and one or more shallow levels that are partially ionized at room temperature. Several techniques have been used to study the defect states in diamond; for example, Glesener 3 measured a boronrelated level with an activation energy of 0.29 eV in borondoped diamond using photoinduced current transient spectroscopy ͑PICTS͒. A wide range of deeper levels has been reported, including Gonon et al. 4 and Hearne et al., 5 who reported activation energies of 1.86 and 1.1 eV, respectively, measured using thermally stimulated current technique ͑TSC͒. Bruzzi et al.6 reported a variety of defect levels in electronic-grade polycrystalline CVD diamond, with activation energies in the range 0.3-1.5 eV, observed using both TSC and PICTS. Alpha particle response measurements are a powerful technique to separate the charge transport and carrier lifetimes of electrons and holes. Marinelli et al. 7 used an analysis of alpha-particle pulse shapes as a function of temperature to deduce a "shallow" hole trap with an activation energy of 0.35 eV. In this letter, we report a new measurement of shallow trap states in CVD diamond, calculated from direct observation of the ...