Related Experiment Video
Updated: Apr 22, 2026

09:10
Fabrication and Testing of Microfluidic Optomechanical Oscillators
Published on: May 29, 2014
11.7K
Single molecule as a local acoustic detector for mechanical oscillators
Yuxi Tian1, Pedro Navarro1, Michel Orrit1
1MoNOS, Huygens-Kamerlingh Onnes Laboratory, Universiteit Leiden, 2300 RA Leiden, Netherlands.
Physical Review Letters
|October 11, 2014
Summary
A single molecule acts as a highly sensitive nanomicrophone for acoustic strain detection. This optical method enables precise monitoring of nanomechanical oscillators, paving the way for advanced control systems.
Area of Science:
- Nanotechnology
- Acoustics
- Molecular Physics
Background:
- Single molecules offer potential for nanoscale sensing due to their small size and high sensitivity.
- Acoustic strain detection is crucial for understanding and manipulating nanoscale mechanical systems.
Purpose of the Study:
- To demonstrate a single molecule as a nanomicrophone for acoustic strain detection.
- To characterize the sensitivity and vibration amplitude of the molecular sensor.
- To establish a foundation for optical detection and feedback control of nanomechanical oscillators.
Main Methods:
- Utilizing a single dibenzoterrylene molecule embedded in an anthracene crystal.
- Attaching the crystal to an oscillating tuning fork to generate acoustic strain.
- Monitoring the fluorescence intensity of the single molecule to detect strain.
Main Results:
- Successfully demonstrated a single molecule's capability to detect acoustic strain.
- Characterized the vibration amplitude of the tuning fork through molecular fluorescence.
- Quantified the detection sensitivity of the nanomicrophone.
Conclusions:
- A single molecule can function as a sensitive nanomicrophone.
- Optical monitoring of molecular fluorescence provides a viable method for nanomechanical sensing.
- This technique is a critical first step towards optical detection and feedback control of nanomechanical systems.
Related Concept Videos
Oscillations In An LC Circuit
2.6K
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
2.6K
Damped Oscillations
6.2K
In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Although friction and other non-conservative...
6.2K
Forced Oscillations
6.3K
When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
6.3K
Oscillations about an Equilibrium Position
5.7K
Stability is an important concept in oscillation. If an equilibrium point is stable, a slight disturbance of an object that is initially at the stable equilibrium point will cause the object to oscillate around that point. For an unstable equilibrium point, if the object is disturbed slightly, it will not return to the equilibrium point. There are three conditions for equilibrium points—stable, unstable, and half-stable. A half-stable equilibrium point is also unstable, but is named so...
5.7K

