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Synchrotron x-ray thermal diffuse scattering probes for phonons in Si/SiGe/Si trilayer nanomembranes

  • Kyle M. McElhinny (a1), Gokul Gopalakrishnan (a1), Donald E. Savage (a1), David A. Czaplewski (a2), Max G. Lagally (a1), Martin V. Holt (a2) and Paul G. Evans (a1)...

Abstract

Nanostructures offer the opportunity to control the vibrational properties of via the scattering of phonons due to boundaries and mass disorder as well as through changes in the phonon dispersion due to spatial confinement. Advances in understanding these effects have the potential to lead to thermoelectrics with an improved figure of merit by lowering the thermal conductivity and to provide insight into electron-phonon scattering rates in nanoelectronics. Characterizing the phonon population in nanomaterials has been challenging because of their small volume and because optical techniques probe only a small fraction of reciprocal space. Recent developments in x-ray scattering now allow the phonon population to be evaluated across all of reciprocal space in samples with volumes as small as several cubic micrometers. We apply this approach, synchrotron x-ray thermal diffuse scattering (TDS), to probe the population of phonons within a Si/SiGe/Si trilayer nanomembrane. The distributions of scattered intensity from Si/SiGe/Si trilayer nanomembranes and Si nanomembranes with uniform composition are qualitatively similar, with features arising from the elastic anisotropy of the diamond structure. The TDS signal for the Si/SiGe/Si nanomembrane, however, has higher intensity than the Si membrane of the same total thickness by approximately 3.75%. Possible origins of the enhancement in scattering from SiGe in comparison with Si include the larger atomic scattering factor of Ge atoms within the SiGe layer or reduced phonon frequencies due to alloying.

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*Corresponding author. E-mail: pgevans@wisc.edu

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[1] Bannov, N., Mitin, V., and Stroscio, M., Phys. Status Solidi B 183, 131 (1994).
[2] Cuffe, J., Chávez, E., Shchepetov, A., Chapuis, P.-O., El Boudouti, E. H., Alzina, F., Kehoe, T., Gomis-Bresco, J., Dudek, D., Pennec, Y., Djafari-Rouhani, B., Prunnila, M., Ahopelto, J., and Sotomayor Torres, C. M., Nano Lett. 12, 3569 (2012).
[3] Balandin, A. and Wang, K. L., Phys. Rev. B 58, 1544 (1998).
[4] Balandin, A. A., Nanosci, J.. Nanotechnol. 5, 1015 (2005).
[5] Hori, T., Shiga, T., and Shiomi, J., J. Appl. Phys. 113, 203514 (2013).
[6] Garg, J., Bonini, N., Kozinsky, B., and Marzari, N., Phys. Rev. Lett. 106, 045901 (2011).
[7] Lamb, H., Proc. R. Soc. Lond. Ser. A 93, 114 (1917).
[8] Als-Nielsen, J. and McMorrow, D., Elements of Modern X-Ray Physics, 2nd ed (Wiley, Hoboken, 2011).
[9] Holt, M., Wu, Z., Hong, H., Zschack, P., Jemian, P., Tischler, J., Chen, H., and Chiang, T.-C., Phys. Rev. Lett. 83, 3317 (1999).
[10] Gopalakrishnan, G., Czaplewski, D. A., McElhinny, K. M., Holt, M. V., Silva-Martínez, J. C., and Evans, P. G., Appl. Phys. Lett. 102, 033113 (2013).
[11] McElhinny, K. M., Gopalakrishnan, G., Savage, D. E., Silva-Martínez, J. C., Lagally, M. G., Holt, M. V., and Evans, P. G., J. Phys. Appl. Phys. 48, 015306 (2015).
[12] Gopalakrishnan, G., Holt, M. V., McElhinny, K. M., Spalenka, J. W., Czaplewski, D. A., Schülli, T. U., and Evans, P. G., Phys. Rev. Lett. 110, 205503 (2013).
[13] Trigo, M., Chen, J., Vishwanath, V. H., Sheu, Y. M., Graber, T., Henning, R., and Reis, D. A., Phys. Rev. B 82, 235205 (2010).
[14] Trigo, M., Fuchs, M., Chen, J., Jiang, M. P., Cammarata, M., Fahy, S., Fritz, D. M., Gaffney, K., Ghimire, S., Higginbotham, A., Johnson, S. L., Kozina, M. E., Larsson, J., Lemke, H., Lindenberg, A. M., Ndabashimiye, G., Quirin, F., Sokolowski-Tinten, K., Uher, C., Wang, G., Wark, J. S., Zhu, D., and Reis, D. A., Nat. Phys. 9, 790 (2013).

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