Related Experiment Video
Updated: Jun 5, 2025

Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
CaloQVAE: Simulating high-energy particle-calorimeter interactions using hybrid quantum-classical generative models
Sehmimul Hoque1,2, Hao Jia3, Abhishek Abhishek4,5
1Perimeter Institute for Theoretical Physics, Waterloo, ON N2L 2Y5 Canada.
Abstract:
The Large Hadron Collider's high luminosity era presents major computational challenges in the analysis of collision events. Large amounts of Monte Carlo (MC) simulation will be required to constrain the statistical uncertainties of the simulated datasets below these of the experimental data. Modelling of high-energy particles propagating through the calorimeter section of the detector is the most computationally intensive MC simulation task. We introduce a technique combining recent advancements in generative models and quantum annealing for fast and efficient simulation of high-energy particle-calorimeter interactions.
Related Concept Videos
The Quantum-Mechanical Model of an Atom
Maxwell-Boltzmann Distribution: Problem Solving
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
Equilibrium Conditions for a Particle
To understand the concept of equilibrium, let us first consider the forces acting on an object. When different forces act on an object, they can...
Interaction of EM Radiation with Matter: Spectroscopy
Fermi Level Dynamics
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electromagnetic Waves in Matter
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the...

