banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Room-temperature operation of a nanoelectromechanical resonator embedded in a phase-locked loop
Rent this article for


Image of FIG. 1.
FIG. 1.

(Color online) In-plane fundamental flexural resonance of a beam (upper inset) with , , and at for increasing drive amplitudes as measured by the optical reflection technique. The gap between the beam and the side gate is . The measured photodiode current was converted to a beam center displacement by using the data in the lower inset. Here, was obtained by scanning the optical spot along the structure. The center of the beam is located at and the gate at as shown by the shading.

Image of FIG. 2.
FIG. 2.

(Color online) (a) Schematic of the PLL. The NEMS resonator is modeled as a two-port electromechanical device. The following components are used: a voltage controlled oscillator (VCO), a radio frequency (rf) mixer, a low-pass filter (LPF), an amplifier, and a frequency counter. (b) PLL output frequency as a function of the VCO carrier frequency in the vicinity of . Locking is observed for . When the gain of the optical transducer-amplifier cascade is lowered by a factor of 10, frequency locking is no longer present (data in gray). The inset shows the fluctuations in while the PLL is locked to . (c) Resonance frequency shift of the NEMS resonator as thermally evaporated gold atoms are absorbed on its surface. The mass is determined from separate quartz crystal and NEMS surface area measurements. The inset shows the experimental geometry.

Image of FIG. 3.
FIG. 3.

(Color online) Results from the analysis of PLL operation. (a) vs at different loop gains . For small , . Frequency locking is observed beyond a critical gain value . For these values, is a multivalued function of . The lock range (inset) increases with increasing . (b) Frequency flow as a function of . Locking is observed for .


Generic image for table
Table I.

Experimentally determined parameters used in the simulations.


Article metrics loading...


Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Room-temperature operation of a nanoelectromechanical resonator embedded in a phase-locked loop