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T. S. Suzuki

Publications and source records attributed to T. S. Suzuki.

2 recordsLinked to original sources

Molecular Dynamics Simulation of Vacancy Cluster Formation in β- and α-$Si_3N_4$

Molecular dynamics simulation is used to study vacancy cluster formation in $β$- and $α$-$Si_3N_4$ with varying vacancy contents (0 - 25.6 at%). Vacancies are randomly created in supercells, which were subsequently heat-treated for 114 nanoseconds. The results show that both $β$ and $α$ can tolerate vacancies up to 12.8 at% and form clusters, confirming previous experimental data indicating 8 at% vacancy in $α$-$Si_3N_4$. However, 25.6 at% vacancy in $β$ results in complete amorphization, while the same amount in $α$ results in a transformation of a semi-amorphous $α$ phase to a defective $β$ phase, leading to the removal of the clusters in newly formed $β$. This clearly explains why cluster vacancies are not experimentally observed in $β$, considering that $β$-$Si_3N_4$ ceramics are produced from $α$. Furthermore, the lattice parameters of both modifications increase with increasing vacancy content, revealing the cause of different lattice constants that were previously reported for $α$-$Si_3N_4$.

cond-mat.mtrl-sci↗

Non-resonant direct p- and d-wave neutron capture by 12C

Discrete gamma-rays from the neutron capture state of 13C to its low-lying bound states have been measured using pulsed neutrons at En = 550 keV. The partial capture cross sections have been determined to be 1.7+/-0.5, 24.2+/-1.0, 2.0+/-0.4 and 1.0+/-0.4 microb for the ground (1/2-), first (1/2+), second (3/2-) and third (5/2+) excited states, respectively. From a comparison with theoretical predictions based on the non-resonant direct radiative capture mechanism, we could determine the spectroscopic factor for the 1/2+ state to be 0.80 +/- 0.04, free from neutron-nucleus interaction ambiguities in the continuum. In addition we have detected the contribution of the non-resonant d-wave capture component in the partial cross sections for transitions leading to the 1/2- and 3/2- states. While the s-wave capture dominates at En < 100 keV, the d-wave component turns out to be very important at higher energies. From the present investigation the 12C(n,gamma)13C reaction rate is obtained for temperatures in the range 10E+7 - 10E+10 K.

nucl-th↗