Hj. Vonbardeleben et al., DEFECT AND STRUCTURE-ANALYSIS OF N(-, P(+)- AND P-TYPE POROUS SILICONBY THE ELECTRON-PARAMAGNETIC-RESONANCE TECHNIQUE()), Journal of luminescence, 57(1-6), 1993, pp. 301-313
We have studied the defects and the structure of porous silicon layers
prepared by electrochemical dissolution from n(+)-, p(+)- and p-type
conductive substrates by electron paramagnetic resonance (EPR). As-pre
pared, vacuum-annealed, thermally oxidized and anodically oxidized lay
ers of various porosities (45-85%) have been analyzed. Under photoexci
tation at temperatures below 50 K, a high-intensity EPR spectrum is ob
served in both n(+) and p(+) layers, which we attribute to the resonan
ce of photoexcited free electrons with lifetimes in the 100s range. Th
e long lifetime favours the model of a spatial separation of photoexci
ted electrons and holes at T < 50 K. For temperatures above 50 K their
lifetimes become too short to allow EPR detection. No EPR spectrum as
sociated with the dopants (phosphorus and boron) could be detected. Th
e dominant paramagnetic defect observed under thermal equilibrium cond
itions is the P-b centre at the (111) Si/SiO2 interfaces; its concentr
ation varies strongly with annealing and oxidation in the 10(10)-10(12
)cm(-2) concentration range. Anodically oxidized layers show a differe
nt EPR spectrum, which is tentatively attributed to the simultaneous p
resence of Pb centres from (Ill)and other Si/SiO, interfaces. In addit
ion, EX centre defects are detected in high-temperature oxidized mater
ial; in anodically oxidized porous silicon E' centres, a defect studie
d previously in bulk SiO2, and attributed to positively charged oxygen
vacancies, are observed. The vacuum annealing, which increases the P-
b centre concentration, can equally lead to the formation of amorphous
/disordered inclusions, as evidenced by the detection of the g = 2.005
5 dangling bond defect. The symmetry of the P-b centre is used to veri
fy the monocrystalline character of the porous layers and to determine
the internal surfaces of porous layers. The electrochemical dissoluti
on and the thermal oxidation lead to the preferential formation of (11
1) surfaces.