期刊文献+

Optical behavior of self-assembled high-density Ge nanoislands embedded in SiO_2

Optical behavior of self-assembled high-density Ge nanoislands embedded in SiO_2
原文传递
导出
摘要 The radio frequency magnetron sputtering method is used to prepare well-dispersed pyramidal-shaped Ge nanoislands embedded in amorphous SiO2 sublayers of various thicknesses. The estimated size and number density of Ge nanoislands in SiO2 sublayer thicknesses beyond 30 nm are approximately 15 nm and 1011 cm-2, respectively. Atomic force microscopy (AFM) reveals root mean square (RMS) roughness sensitivity as the SiO2 sublayer thickness varies from 30 to 40 nm. The formation of nanoislands with high aspect ratios is attributed to the higher rate of surface reactions between Ge adatoms and nucleated Ge islands than reactions associated with SiO2 and Ge. The Ge nanoisland polyorientation on SiO2 (50-nm thickness) is revealed by X-ray diffraction (XRD) patterns. Photoluminescence (PL) peaks of 2.9 and 1.65 eV observed at room temperature (RT) are attributed to the radiative recombination of electrons and holes from the Ge nanoislands/SiO2 and Si02/Si interfaces, respectively. The mean island sizes are determined by fitting the experimental Raman profile to two models, namely, the phonon confinement model and the size distribution combined with phonon confinement model. The latter model yields the best fit to the experimental data. We confirm that SiO2 matrix thickness variations play a significant role in the formation of Ge nanoislands mediated via the minimization of interfacial and strain energies. OCIS codes: 250.5230, 170.5660. The radio frequency magnetron sputtering method is used to prepare well-dispersed pyramidal-shaped Ge nanoislands embedded in amorphous SiO2 sublayers of various thicknesses. The estimated size and number density of Ge nanoislands in SiO2 sublayer thicknesses beyond 30 nm are approximately 15 nm and 1011 cm-2, respectively. Atomic force microscopy (AFM) reveals root mean square (RMS) roughness sensitivity as the SiO2 sublayer thickness varies from 30 to 40 nm. The formation of nanoislands with high aspect ratios is attributed to the higher rate of surface reactions between Ge adatoms and nucleated Ge islands than reactions associated with SiO2 and Ge. The Ge nanoisland polyorientation on SiO2 (50-nm thickness) is revealed by X-ray diffraction (XRD) patterns. Photoluminescence (PL) peaks of 2.9 and 1.65 eV observed at room temperature (RT) are attributed to the radiative recombination of electrons and holes from the Ge nanoislands/SiO2 and Si02/Si interfaces, respectively. The mean island sizes are determined by fitting the experimental Raman profile to two models, namely, the phonon confinement model and the size distribution combined with phonon confinement model. The latter model yields the best fit to the experimental data. We confirm that SiO2 matrix thickness variations play a significant role in the formation of Ge nanoislands mediated via the minimization of interfacial and strain energies. OCIS codes: 250.5230, 170.5660.
出处 《Chinese Optics Letters》 SCIE EI CAS CSCD 2013年第11期91-95,共5页 中国光学快报(英文版)
基金 supported by visiting researcher grants provided by the MoHE(Nos.Q.J090000.21A4.00D20 and Q.J130000.2526.02H94)
关键词 Ge SIO HIGH
  • 相关文献

参考文献26

  • 1Z. Dong, W. Wang, B. Huang, X. Zhang, N. Guan, and H. Chen, Chin. Opt. Lett. 9, 082301 (2011).
  • 2P. Cappelletti, Microelectron. Reliab. 38, 185 (1998).
  • 3C. L. Heng and T. G. Finstad, Phys. E 26, 386 (2005).
  • 4P. Schnittenhelm, M. Gall, J. Brunner, J. F. Nutzel, and G. Abstreiter, Appl. Phys. Lett. 67, 1292 (1995).
  • 5S. A. Chaparro, Y. Zhang, and J. Drucker, App[. Phys. Lett. 76, 3534 (2000).
  • 6A. A. Shklyaev, M. Shibata, and M. Ichikawa, Phys. Rev. B 62, 1540 (2000).
  • 7A. I. Nikiforov, V. V. Ulyanov, O. P. Pchelyakov, S. A. Teys, and A. K. Gutakovsky, Mat. Sci. Semicon. Proc. 8, 47 (2005).
  • 8R. P. U. Karunasiri, R. Bruinsma, and J. Rudnick, Phys. Rev. Lett. 62, 788 (1989).
  • 9J. L. Liu, J. Wan, Z. M. Jiang, A. Khitun, and K. L. Wang, J. Appl. Phys 92, 6804 (2002).
  • 10A. R. Samavati, Z. Othaman, S. K. Ghoshal, M. R. Dousti, and R. J. Amjad, Chin. Phys. Lett. 29, 118101 (2012).

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部