Related Experiment Video
Updated: Dec 25, 2025

07:46
Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
8.9K
A multi-dimensional search for new heavy resonances decaying to boosted , , or boson pairs in the dijet final
A M Sirunyan1, A Tumasyan1, W Adam2
11Yerevan Physics Institute, Yerevan, Armenia.
Summary
This study searched for new massive resonances in all-jet final states using CMS data. No new resonances were found, setting the best limits to date in the dijet final state.
Area of Science:
- High Energy Physics
- Particle Physics
- Collider Physics
Background:
- Searches for new physics beyond the Standard Model are crucial.
- Resonances decaying to W, Z, or Higgs boson pairs are predicted by various theories.
- Previous searches have limitations in sensitivity and mass reach.
Purpose of the Study:
- To search for new massive resonances decaying into W, Z, or Higgs boson pairs.
- To improve sensitivity in the all-jet final state using a novel analysis method.
- To set exclusion limits on new resonances in specific theoretical models.
Main Methods:
- Analysis of proton-proton collision data at 13 TeV center-of-mass energy.
- Utilized an integrated luminosity of 77.3 fb⁻¹ from the CMS experiment.
- Employed a novel three-dimensional maximum likelihood fit of jet masses and dijet invariant mass for signal extraction.
Main Results:
- No significant excess was observed above the Standard Model background.
- Exclusion limits were set on spin-1 W' and Z' resonances up to 3.5 and 3.8 TeV, respectively.
- Upper limits on cross sections were established for bulk graviton resonances between 1.2 and 5.2 TeV.
Conclusions:
- The study achieved improved sensitivity of up to 30% compared to previous methods.
- The obtained limits are the most stringent to date for resonances in the dijet final state.
- The results constrain new physics models, including heavy vector triplet and bulk graviton models.
Related Concept Videos
¹³C NMR: ¹H–¹³C Decoupling
1.6K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.6K
Detection of Black Holes
2.5K
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...
2.5K
Double Resonance Techniques: Overview
618
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
618
Tandem Mass Spectrometry
2.1K
Tandem mass spectrometry is a technique that uses multiple mass analyzers in series to obtain a higher selectivity and reduce chemical noise during analyte detection. Instruments with multiple analyzers separated by an interaction cell enable secondary fragmentation and selected study of the fragment ions.Secondary fragmentations occur in the interaction cell and can be induced by various factors. Fragmentation induced by collision with inert gases, such as N2, Ar, He, etc., is called...
2.1K
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)
1.5K
When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
1.5K
Carbon-13 (¹³C) NMR: Overview
7.4K
Carbon-13 is a naturally occurring NMR-active isotope of carbon with a low natural abundance of 1.1%. In contrast, carbon-12 is the most abundant isotope of carbon with zero nuclear spin. Therefore, it is NMR inactive. The gyromagnetic ratio of carbon-13 is smaller than that of protons. As a result, carbon-13 resonance is about 6000 times weaker than proton resonance. For a given magnetic field strength, the resonance frequency of carbon-13 is about one-fourth of the resonance frequency for...
7.4K

