Influence of boron on donor–acceptor pair recombination in type IIa HPHT diamonds

• Published in: Diamond and related materials Vol. 36; pp. 35 - 43
• Main Authors: Ščajev, Patrik, Trinkler, Laima, Berzina, Baiba, Ivakin, Eugeny, Jarašiūnas, Kęstutis
• Format: Journal Article
• Language: English
• Published: Amsterdam Elsevier B.V 01.06.2013; Elsevier
• Subjects: Activation energy; Boron; Condensed matter: electronic structure, electrical, magnetic, and optical properties; Delay; Density; Diamonds; Differential transmittivity; Donor–acceptor recombination; Exact sciences and technology; Excitation spectra; HPHT diamond; Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation; Other luminescence and radiative recombination; Photoluminescence; Physics; Temperature dependence; Thermoluminescence; Two photon absorption; Two photon absorption; Donor–acceptor recombination; Activation energy; HPHT diamond; Photoluminescence; Differential transmittivity; Temperature dependence; Cross section; Phonons; Excited states; Free carrier; High pressure high temperature method; Boron; Donor―acceptor recombination; Ionization; Carrier lifetime; Cross sections; Thermoluminescence
• ISSN: 0925-9635; 1879-0062
• DOI: 10.1016/j.diamond.2013.03.011

We report on the investigation of donor–acceptor pair (DAP) and free carrier recombination in HPHT IIa type diamonds and determination of boron concentration by differential transmittivity (DT) technique. Photoluminescence and photoluminescence excitation spectra were measured in 8–300K temperature range and provided a broad (~0.67eV) Gaussian DAP band which peaked at 2.2eV at low temperatures, while above 200K it sharply shifted to 2.5eV and became more intense. Thermoluminescence measurements also demonstrated a similar tendency. This peculiarity was explained by DAP recombination between the nitrogen and the boron, the latter being in the ground and the excited states at low and high temperatures, respectively. A zero phonon line position coincided with the calculated one, when using nitrogen and boron activation energies. Scanning of DT across the sample at different delay times revealed the fast (200–500ns) free carrier lifetime and the slow recovery time (of optically recharged boron to its initial state). The temperature dependence of the slow component decay time provided the boron activation energy of 360meV. Saturation of the boron-related DT signal in the samples and the determined boron ionization cross section at 1064nm (σB=3.3×10−17cm2) provided the boron density in 1014–16cm−3 range and revealed its strongly inhomogeneous distribution across the HPHT layers. The B density was found much lower than the density of nitrogen donors (~1017cm−3), which were distributed in the layers much more homogeneously. •Nitrogen to boron DAP recombination PL peaks were explained.•Fast free carrier and slow boron recharge DT components were observed.•Fast component decay rate correlated with nitrogen density.•Slow decay time temperature dependence provided activation energy of boron.•The injection dependent slow DT signal amplitude provided boron concentration.