Controlling the nonlinearity of silicon nanowire resonators using active feedback
Appl. Phys. Lett. 95, 123116 (2009); doi:10.1063/1.3232232
Published 24 September 2009
You are not logged in to this journal. Log in
We describe the use of nonlinear feedback to tune the cubic nonlinearity of a silicon nanowire resonator. We show that nonlinear feedback can be used to cancel out the native nonlinearity or even change its sign. Here, we demonstrate the usefulness of this technique by using nonlinear feedback to extend the dynamic range of a silicon nanowire parametric amplifier.
©2009 American Institute of Physics
| History: | Received 4 July 2009; accepted 31 August 2009; published 24 September 2009 |
| Permalink: |
http://link.aip.org/link/?APPLAB/95/123116/1 |
KEYWORDS and PACS
RELATED DATABASES
PUBLICATION DATA
0003-6951 (print)
1077-3118 (online)
REFERENCES (21)
For access to fully linked references, you need to log in.
For access to fully linked references, you need to Log in.
- H. W. C. Postma, I. Kozinsky, A. Husain, and M. L. Roukes, Appl. Phys. Lett. 86, 223105 (2005).
- J. S. Aldridge and A. N. Cleland, Phys. Rev. Lett. 94, 156403 (2005).
- R. Almog, S. Zaitsev, O. Shtempluck, and E. Buks, Phys. Rev. Lett. 98, 078103 (2007).
- R. Almog, S. Zaitsev, O. Shtempluck, and E. Buks, Appl. Phys. Lett. 90, 013508 (2007).
- R. Almog, S. Zaitsev, O. Shtempluck, and E. Buks, Appl. Phys. Lett. 88, 213509 (2006).
- A. Erbe, H. Krommer, A. Kraus, R. H. Blick, G. Corso, and K. Richter, Appl. Phys. Lett. 77, 3102 (2000).
- D. Rugar, R. Budakian, H. J. Mamin, and B. W. Chui,
Nature (London) 430, 329 (2004) . - Y. T. Yang, C. Callegari, X. L. Feng, K. L. Ekinci, and M. L. Roukes,
Nano Lett. 6, 583 (2006) . - S. G. Adams, F. M. Bertsch, K. A. Shaw, and N. C. MacDonald,
J. Microelectromech. Syst. 7, 172 (1998) . - I. Kozinsky, H. W. C. Postma, I. Bargatin, and M. L. Roukes, Appl. Phys. Lett. 88, 253101 (2006).
- H. Yabuno, H. Kaneko, M. Kuroda, and T. Kobayashi,
Nonlinear Dyn. 54, 137 (2008) . - D. E. Perea, E. Wijaya, J. L. Lensch-Falk, E. R. Hemesath, and L. J. Lauhon,
J. Solid State Chem. 181, 1642 (2008) . - J. M. Nichol, E. R. Hemesath, L. J. Lauhon, and R. Budakian, Appl. Phys. Lett. 93, 193110 (2008).
- D. Rugar and P. Grutter, Phys. Rev. Lett. 67, 699 (1991).
- A. H. Nayfeh and D. T. Mook, Nonlinear Oscillations, 1st ed. (Wiley, New York, 1979).
- W. H. Zhang and K. L. Turner,
Sens. Actuators, A 123, 23 (2005) . - M. V. Requa and K. L. Turner, Appl. Phys. Lett. 90, 173508 (2007).
- W. H. Zhang, R. Baskaran, and K. L. Tumer,
Sens. Actuators, A 102, 139 (2002) . - J. F. Rhoads and S. W. Shaw, ASME 2008 International Design Engineering Conferences and Computers and Information in Engineering Conference, Vol. 4, pp. 593–597, Brooklyn, New York, 3–6 August 2008.
- It is possible in principle to calculate the conversion from ac voltage amplitude Vac to
by measuring the dependence of
0 on the dc bias to determine the second derivative of the SiNW-electrode capacitance using the results from Ref. 14. The calculated value is
/Vac=0.003 22, while the fitted value is
/Vac=0.002 01. The agreement seems reasonable given that we do not know the exact capacitance of the electrode. - The lower limit of the dynamic range is set by thermal fluctuations which are below the critical amplitude, even for the native case. Also, the peak gain is predicted to be independent of the nonlinearity for small amplitudes. Thus, the amplitudes Anative and Azero for which the gain drops by 1 dB are determined, and the dynamic range increase is calculated as 20 log(Azero/Anative).







