Related Experiment Video
Updated: Jul 18, 2026

09:10
Fabrication and Testing of Microfluidic Optomechanical Oscillators
Published on: May 29, 2014
Direct limits on the oscillation frequency
V M Abazov1, B Abbott, M Abolins
1Joint Institute for Nuclear Research, Dubna, Russia.
Physical Review Letters
|August 16, 2006
Summary
Researchers measured the B(s)(0) oscillation frequency using D0 experiment data. The study provides a precise measurement, with a most probable value of 19 ps(-1) for the B(s)(0) oscillation frequency.
Area of Science:
- Particle Physics
- High Energy Physics
- Quantum Mechanics
Background:
- The B(s)(0) meson is a type of subatomic particle composed of a bottom antiquark and a strange quark.
- Understanding B(s)(0) meson oscillations is crucial for testing the Standard Model of particle physics.
Purpose of the Study:
- To measure the oscillation frequency of the B(s)(0) meson.
- To provide a precise, direct measurement of the B(s)(0) oscillation frequency using a large dataset.
Main Methods:
- Analysis of approximately 1 fb(-1) of integrated luminosity data from semileptonic B(s)(0) decays.
- Utilized the amplitude method and a likelihood scan to determine the oscillation frequency.
- Data collected by the D0 experiment at the Fermilab Tevatron Collider between 2002 and 2006.
Main Results:
- A lower limit on the B(s)(0) oscillation frequency was set at 14.8 ps(-1) (95% C.L.) using the amplitude method.
- At delta m(s) = 19 ps(-1), the amplitude deviated by 2.5 (1.6) standard deviations from the A=0 hypothesis, yielding a two-sided C.L. of 1% (10%).
- A likelihood scan yielded a most probable value of 19 ps(-1) and a 90% C.L. range of 17 < delta m(s) < 21 ps(-1).
Conclusions:
- This study presents the first direct, two-sided measurement of the B(s)(0) oscillation frequency by a single experiment.
- The results provide a significant constraint on the B(s)(0) oscillation frequency, with implications for new physics searches.
- The probability of observing a similar likelihood minimum for delta m(s) > 22 ps(-1) is (5.0 +/- 0.3)%.
Related Concept Videos
Damped Oscillations
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...
Forced Oscillations
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.
Concept of Resonance and its Characteristics
If a driven oscillator needs to resonate at a specific frequency, then very light damping is required. An example of light damping includes playing piano strings and many other musical instruments. Conversely, to achieve small-amplitude oscillations as in a car's suspension system, heavy damping is required. Heavy damping reduces the amplitude, but the tradeoff is that the system responds at more frequencies. Speed bumps and gravel roads prove that even a car's suspension system is not immune...
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...
Limits with Oscillating Discontinuities
An oscillating discontinuity is a type of discontinuity in which a function’s values fluctuate infinitely often as the input approaches a particular point. Unlike jump discontinuities, where the function suddenly shifts between two values, or infinite discontinuities, where the function diverges without bound, an oscillating discontinuity arises from rapid back-and-forth variation. Because the function never stabilizes toward a single value, no finite limit exists at that point.One of the most...

