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Particle Physics Handout 5
Particle Physics Handout 5

A boost for quantum reality
A boost for quantum reality

divinity - Particle Theory Group
divinity - Particle Theory Group

Oct 6
Oct 6

The Large Hadron Collider, or LHC, is the most powerful particle
The Large Hadron Collider, or LHC, is the most powerful particle

... the magnetic field. Similar to ATLAS there is CMS (Compact Moun Solenoid). They both are general purpose detectors for the subparticles released during collisions. This detector however is contained inside a solenoid magnet that creates a magnetic field almost 100,000 times stronger than the Earth’s ...
Lecture 6
Lecture 6

Quarks, Leptons, Bosons the LHC and All That
Quarks, Leptons, Bosons the LHC and All That

Slide 1
Slide 1

... probability this will happen is proportional to the square of the charge of the target particle. Much more likely near a uranium nucleus than near a proton – by a factor of 82^2. A relatively thin shell of uranium will make most electrons produce pairs while strongly interacting particles produce on ...
Chapter 17 PowerPoint
Chapter 17 PowerPoint

... Further: hadrons interact by the strong nuclear force (e.g. protons and neutrons) Leptons do not (e.g. electrons) Bosons are virtual particles that mediate forces W+, W-, Z mediate weak nuclear force existence photons mediate electromagnetic force confirmed gluons mediate strong nuclear force gravit ...
Slide 1
Slide 1

SET 2 Option J — Particle physics J1. This question is about
SET 2 Option J — Particle physics J1. This question is about

Modern Physics
Modern Physics

Chapter 15 PowerPoint
Chapter 15 PowerPoint

... • Associated production p-+pL 0+K0 with 4 GeV/c pions in a bubble chamber. • Strangeness is a quantum number that is conserved in strong interactions but not in weak interactions. What are the forces in play in the above pictures? ...
Evolution of the Atomic Theory
Evolution of the Atomic Theory

14. Elementary Particles
14. Elementary Particles

Dilepton production
Dilepton production

... Total spectrum • We must have dilepton yield from the QGP of large enough magnitude. • M less than 1 GeV: Resonance decays from ρ,Φ,ω dominate. Difficult to see QGP signal • Continuum (not resonances) over 1.5 GeV: Hadron interactions and charm decay not important. ...
Interactions of Charged Particles with Matter (N Harding)
Interactions of Charged Particles with Matter (N Harding)

...  Electromagnetic interactions  extend over some distance  not necessary for particle to make direct collision  can transfer energy simply passing close by  atomic internal energy quantised  only certain energy values can be transferred ...
PHYSICS 357S - Problem Set #2 - January 2004
PHYSICS 357S - Problem Set #2 - January 2004

Nuclear Chemistry - sullivanchem-ap
Nuclear Chemistry - sullivanchem-ap

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Cyclotron - schoolphysics

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aspen_pb - Particle Theory

... The baryon octet ...
Overview of particle physics
Overview of particle physics

An Overview of the Field of High Energy Physics
An Overview of the Field of High Energy Physics

Any crystal that scratches glass is a diamond. Rocks must be heavy
Any crystal that scratches glass is a diamond. Rocks must be heavy

Nuclear Energy - Eastside Physics
Nuclear Energy - Eastside Physics

... comparatively few radioactive by-products are formed. However proton-proton reaction are unrealistic due to the need of extremely high temperatures and pressures. The sun functions because of the extreme density of protons at its core. Reaction of deuterium with tritium seems promising but for the c ...
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ALICE experiment

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