Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule01:10

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule

1.5K
In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1  triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the...
1.5K
¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

1.4K
A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied...
1.4K
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

5.4K
When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
5.4K
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

1.3K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
1.3K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

1.2K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.2K
Electric Dipoles and Dipole Moment01:30

Electric Dipoles and Dipole Moment

5.6K
Consider two charges of equal magnitude but opposite signs. If they cannot be separated by an external electric field, the system is called a permanent dipole. For example, the water molecule is a dipole, making it a good solvent.
Theoretically, studying electric dipoles leads to understanding why the resultant electric forces around us are weak. Since electric forces are strong, remnant net charges are rare. Hence, the interaction between dipoles helps us understand electrical interactions in...
5.6K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

High-Energy Evolution of Power-Suppressed Amplitudes.

Physical review letters·2026
Same author

Complete Next-to-Leading Order QCD Corrections to ZZ Production in Gluon Fusion.

Physical review letters·2025
Same author

Two-Loop QED Corrections to the Scattering of Four Massive Leptons.

Physical review letters·2024
Same author

Three-Loop Gluon Scattering in QCD and the Gluon Regge Trajectory.

Physical review letters·2022
Same author

Quark and Gluon Form Factors in Four-Loop QCD.

Physical review letters·2022
Same author

Diphoton Amplitudes in Three-Loop Quantum Chromodynamics.

Physical review letters·2021

Related Experiment Video

Updated: Oct 6, 2025

Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 15, 2013

8.7K

Two-Loop Helicity Amplitudes for Diphoton Plus Jet Production in Full Color.

Bakul Agarwal1, Federico Buccioni2, Andreas von Manteuffel1

  • 1Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.

Physical Review Letters
|January 14, 2022
PubMed
Summary

We calculated quantum chromodynamics (QCD) amplitudes for two-photon and jet production at hadron colliders. This breakthrough provides crucial, precise predictions for diphoton production, simplifying complex calculations.

More Related Videos

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

8.6K
Author Spotlight: Non-Invasive Imaging of Complex Bio-Structures Using Polarization-Sensitive Two-Photon Microscopy
05:54

Author Spotlight: Non-Invasive Imaging of Complex Bio-Structures Using Polarization-Sensitive Two-Photon Microscopy

Published on: September 8, 2023

1.4K

Related Experiment Videos

Last Updated: Oct 6, 2025

Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 15, 2013

8.7K
A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

8.6K
Author Spotlight: Non-Invasive Imaging of Complex Bio-Structures Using Polarization-Sensitive Two-Photon Microscopy
05:54

Author Spotlight: Non-Invasive Imaging of Complex Bio-Structures Using Polarization-Sensitive Two-Photon Microscopy

Published on: September 8, 2023

1.4K

Area of Science:

  • High Energy Physics
  • Quantum Chromodynamics
  • Particle Physics

Background:

  • Precise predictions for particle production at hadron colliders are essential for interpreting experimental data.
  • Previous calculations for five-particle scattering processes were limited in accuracy beyond the leading-color approximation.
  • Diphoton production is a key process for probing the Standard Model and searching for new physics.

Purpose of the Study:

  • To compute the two-loop quantum chromodynamics (QCD) amplitudes for the production of two photons and a jet at hadron colliders.
  • To include full-color dependence in these calculations, going beyond the leading-color approximation.
  • To develop methodologies that simplify the calculation of multi-particle scattering processes.

Main Methods:

  • Employed perturbative quantum chromodynamics (QCD) at the two-loop level.
  • Calculated scattering amplitudes for a five-particle process (two photons and a jet).
  • Developed novel techniques to manage the complexity of radiative corrections and full-color dependence.

Main Results:

  • Presented the first-ever two-loop QCD amplitudes for a five-particle scattering process with full-color dependence.
  • Achieved calculations beyond the leading-color approximation at this perturbative order.
  • Demonstrated a significant simplification in the calculation of these complex amplitudes.

Conclusions:

  • The computed amplitudes are crucial for achieving reliable and unprecedented precision in diphoton production predictions at hadron colliders.
  • The developed methodologies offer a significant simplification and are applicable to a broader range of five-point scattering processes.
  • This work advances the precision of theoretical predictions in high-energy particle physics.