Related Experiment Video
Updated: Jul 11, 2026

07:46
Setting Limits on Supersymmetry Using Simplified Models
Published on: November 16, 2013
Upper Limits on the Stochastic Gravitational-Wave Background from Advanced LIGO's First Observing Run
B P Abbott1, R Abbott1, T D Abbott2
1LIGO, California Institute of Technology, Pasadena, California 91125, USA.
Physical Review Letters
|April 8, 2017
Summary
Scientists searched for a cosmic gravitational-wave background using Advanced Laser Interferometer Gravitational Wave Observatory (aLIGO) data. No signal was detected, setting new limits on the background
Area of Science:
- Astrophysics and Cosmology
- Gravitational-wave Astronomy
Background:
- Astrophysical and cosmological sources are predicted to create a stochastic gravitational-wave background.
- Recent observations suggest a higher rate and mass of coalescing binary black holes, potentially increasing the expected background loudness.
Purpose of the Study:
- To search for the isotropic stochastic gravitational-wave background using data from the first observing run of the Advanced Laser Interferometer Gravitational Wave Observatory (aLIGO).
- To constrain the energy density of gravitational waves and investigate implications for astrophysical models of binary black hole backgrounds.
Main Methods:
- Analysis of data from the Advanced Laser Interferometer Gravitational Wave Observatory's (aLIGO) first observing run.
- Performing a search for the isotropic stochastic gravitational-wave background.
- Constraining dimensionless energy density for flat and arbitrary power-law spectra.
Main Results:
- No evidence of a stochastic gravitational-wave signal was found in the analyzed data.
- The dimensionless energy density of gravitational waves is constrained to be Ω₀ < 1.7 × 10⁻⁷ (95% confidence) for a flat spectrum in the 20-86 Hz LIGO band.
- This result represents a significant improvement in sensitivity, being approximately 33 times more sensitive than previous measurements.
Conclusions:
- The first aLIGO observing run did not detect a stochastic gravitational-wave background.
- New, stringent upper limits have been placed on the gravitational-wave energy density.
- The findings provide crucial data for refining astrophysical models of compact binary coalescences.
Related Concept Videos
Schwarzschild Radius and Event Horizon
No object with a finite mass can travel faster than the speed of light in a vacuum. This fact has an interesting consequence in the domain of extremely high gravitational fields.
The minimum speed required to launch a projectile from the surface of an object to which it is gravitationally bound so that it eventually escapes the object’s gravitational field is called the escape velocity. The escape velocity is independent of the mass of the object. Merging the idea of escape velocity with the...
The minimum speed required to launch a projectile from the surface of an object to which it is gravitationally bound so that it eventually escapes the object’s gravitational field is called the escape velocity. The escape velocity is independent of the mass of the object. Merging the idea of escape velocity with the...
Detection of Black Holes
Although black holes were theoretically postulated in the 1920s, they remained outside the domain of observational astronomy until the 1970s.
Their closest cousins are neutron stars, which are composed almost entirely of neutrons packed against each other, making them extremely dense. A neutron star has the same mass as the Sun but its diameter is only a few kilometers. Therefore, the escape velocity from their surface is close to the speed of light.
Not until the 1960s, when the first neutron...
Their closest cousins are neutron stars, which are composed almost entirely of neutrons packed against each other, making them extremely dense. A neutron star has the same mass as the Sun but its diameter is only a few kilometers. Therefore, the escape velocity from their surface is close to the speed of light.
Not until the 1960s, when the first neutron...
Difference from Background: Limit of Detection
The limit of detection (LOD) is the smallest amount of analyte that can be distinguished from the background noise. The LOD value corresponds to the concentration at which the analyte signal is three times larger than the standard deviation of the blank signal. Below this value, the analyte signal cannot be differentiated from the background noise. It is calculated by dividing the calibration slope by 3 times the standard deviation of the blank signals.
The LOD indicates the presence or absence...
The LOD indicates the presence or absence...
Atomic Emission Spectroscopy: Interference
In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...
Limits of the First Law of Thermodynamics
Spontaneous processes, like a rock falling to the ground or sodium reacting with chlorine, occur without external work and often involve a decrease in the system‘s energy. However, certain endothermic processes, such as the dissolution of sodium chloride in water, occur spontaneously even though they increase the energy of the system. This limitation suggests that the First Law of Thermodynamics, which states that the total energy of a system is constant in an isolated system, cannot fully...
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...

