Authors | S.D. Bardashevska1, I.M. Budzulyak1 , S.I. Budzulyak2 , B.I. Rachiy1 , L.S. Yablon1 , O.V. Morushko1 |
Affiliations |
1Vasyl Stefanyk Precarpathian National University, 57, Shevchenko St., 76018 Ivano-Frankivsk, Ukraine 2V.E. Lashkaryov Institute of Semiconductor Physics NAS of Ukraine, 45, Nauki Prosp., 02000 Kyiv, Ukraine |
Е-mail | yablon_lyubov@ukr.net |
Issue | Volume 11, Year 2019, Number 5 |
Dates | Received 20 February 2019; revised manuscript received 21 October 2019; published online 25 October 2019 |
Citation | S.D. Bardashevska, I.M. Budzulyak, S.I. Budzulyak, et al., J. Nano- Electron. Phys. 11 No 5, 05043 (2019) |
DOI | https://doi.org/10.21272/jnep.11(5).05043 |
PACS Number(s) | 78.67.Hc, 79.60.Jv, 73.22.– f |
Keywords | Quantum dots (3) , ZnSe (11) , Nanoporous carbon (3) , Photoluminescence spectra. |
Annotation |
The ZnSe quantum dots in a matrix of nanoporous carbon are synthesized in the work. For this purpose, nanoporous carbon was synthesized with the required pore size distribution. From the received photoluminescence spectra, it was found that the peak near the band edge in the excitation spectrum can be assigned to the highest transfer efficiency of photogenerated carriers at the correlated sub-band states (about 34 meV below the conduction band of ZnSe) to the deep centre states. |
List of References |