Related Experiment Video
Updated: Jul 3, 2026

09:10
Fabrication and Testing of Microfluidic Optomechanical Oscillators
Published on: May 29, 2014
A self-sustaining ultrahigh-frequency nanoelectromechanical oscillator.
X L Feng1, C J White, A Hajimiri
1Kavli Nanoscience Institute, MC 114-36, California Institute of Technology, Pasadena, California 91125, USA.
Nature Nanotechnology
|July 26, 2008
Summary
Researchers developed a self-sustaining nanoelectromechanical oscillator. This device generates continuous ultrahigh-frequency signals from a DC power source, enabling advanced sensing applications.
Area of Science:
- Nanoscience and Nanotechnology
- Electrical Engineering
- Mechanical Engineering
Background:
- Nanoelectromechanical systems (NEMS) offer superior performance for sensing applications.
- Current NEMS sensors are passive, requiring external excitation for resonance.
- Achieving high sensitivity in displacement, mass, force, and charge detection is a key goal.
Purpose of the Study:
- To demonstrate an autonomous and self-sustaining NEMS oscillator.
- To generate continuous ultrahigh-frequency signals using a steady DC power source.
- To explore practical sensing applications and nanomechanical control.
Main Methods:
- Integration of a 428 MHz NEMS resonator within a tunable electrical feedback network.
- Development of a system for active and stable self-oscillation.
- Utilizing a steady direct current (DC) source for power.
Main Results:
- Successful demonstration of an autonomous, self-sustaining NEMS oscillator.
- Generation of continuous ultrahigh-frequency signals.
- Exhibited excellent frequency stability, linewidth narrowing, and low phase noise.
Conclusions:
- The developed NEMS oscillator provides a novel approach for ultrahigh-frequency signal generation.
- This technology offers a simplified method for various practical sensing applications.
- Opens new avenues for nanomechanical frequency control, timing, and synchronization.
Related Concept Videos
Generating Electromagnetic Radiations
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in the...
Oscillations In An LC Circuit
An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
Design Example: Underdamped Parallel RLC Circuit
Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
Starting with a fixed...
MOSFET: Enhancement Mode
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
Standing Waves in a Cavity
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:

