Presentation is loading. Please wait.

Presentation is loading. Please wait.

Electroweak bosons  .

Published byAugust Brown Modified over 5 years ago

Similar presentations

Presentation on theme: "Electroweak bosons  ."— Presentation transcript:

1 Electroweak bosons

2 The accelerator complex

3 W  e + ν pneutrino pelectron θneutrino θelectron UA1 proton
anti-proton Beam pipe θelectron pelectron Transverse plane

4 (p x sin θ) neutrino (p x sin θ) electron neutrino θneutrino θelectron

5 W  τ + ν 3 charged hadrons from τ (+ “missing” momentum)

6 The first Z0 boson observed
Electron Electron CERN SppS, UA1 experiment, 30 April 1983

7 Z0 discovery paper Phys.Lett. B126 (1983) UA1 collaboration

8 The Large Electron-Positron Collider
27 km circumference Electron against positron Centre-of-mass energy GeV

9 The Z0 resonance

10 Number of neutrinos Measure total width from lineshape Predict hadronic cross-section for different numbers of neutrinos

11 e+e-  Z0  Hadrons

Download ppt "Electroweak bosons  ."

Similar presentations

UT, Enschede, 11/11/'97Research & Education Program, Bob van Eijk1 presented by Bob van Eijk BAC Meeting University of Twente 11 November 1997 Research.

UT, Enschede, 11/11/'97Research & Education Program, Bob van Eijk1 presented by Bob van Eijk BAC Meeting University of Twente 11 November 1997 Research.
First results from the ATLAS experiment at the LHC

First results from the ATLAS experiment at the LHC
ATLAS Experiment at CERN. Why Build ATLAS? Before the LHC there was LEP (large electron positron collider) the experiments at LEP had observed the W and.

ATLAS Experiment at CERN. Why Build ATLAS? Before the LHC there was LEP (large electron positron collider) the experiments at LEP had observed the W and.
Experimental Observation Of Lepton Pairs Of Invariant Mass Around 95 GeV/c² At The CERN SPS Collider 不変質量 95 GeV/c² 近傍のレプトン対の実験的観測 Contents 1. Introduction.

Experimental Observation Of Lepton Pairs Of Invariant Mass Around 95 GeV/c² At The CERN SPS Collider 不変質量 95 GeV/c² 近傍のレプトン対の実験的観測 Contents 1. Introduction.
Section IX Electroweak Unification. 221 Electroweak Unification  Weak Charged Current interactions explained by W  exchange.  W bosons are charged,

Section IX Electroweak Unification. 221 Electroweak Unification  Weak Charged Current interactions explained by W  exchange.  W bosons are charged,
Is B s 0 production by neutrino interactions interesting? Presented at the Super-B factory workshop as an alternative approach Nickolas Solomey 21 April.

Is B s 0 production by neutrino interactions interesting? Presented at the Super-B factory workshop as an alternative approach Nickolas Solomey 21 April.
A Study of Anomalous Production of Z-bosons with High Transverse Momentum at the Tevatron. Alexander Paramonov The University of Chicago For the CDF Collaboration.

A Study of Anomalous Production of Z-bosons with High Transverse Momentum at the Tevatron. Alexander Paramonov The University of Chicago For the CDF Collaboration.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.

Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Detector  Basically the NOvA detector. Planes of plastic tubes filled with liquid scintillator. Fully active: Good for electron identification Total mass:

Detector  Basically the NOvA detector. Planes of plastic tubes filled with liquid scintillator. Fully active: Good for electron identification Total mass:
2-Oct-06University of Bologna1 The Future of Particle Physics The Case for Building another Huge Particle Accelerator Barry Barish CALTECH 2-Oct-06.

2-Oct-06University of Bologna1 The Future of Particle Physics The Case for Building another Huge Particle Accelerator Barry Barish CALTECH 2-Oct-06.
Positron. Pair Production  Photons above twice the electron rest mass energy can create a electron positron pair. Minimum = 0.012 ÅMinimum = 0.012 Å.

Positron. Pair Production  Photons above twice the electron rest mass energy can create a electron positron pair. Minimum = ÅMinimum = Å.
Elementary particles atom Hadrons Leptons Baryons Mesons Nucleons

Elementary particles atom Hadrons Leptons Baryons Mesons Nucleons
Single boson production at LEP Guillaume Leibenguth On behalf of the LEP experiments Institut de physique nucléaire Université catholique de Louvain DIS’04,

Single boson production at LEP Guillaume Leibenguth On behalf of the LEP experiments Institut de physique nucléaire Université catholique de Louvain DIS’04,
1 Some predictions and experiment prospects of the heavy ion physics at LHC C. Kobdaj, Y. Yan and K. Khosonthongkee School of Physics, Institute of Science.

1 Some predictions and experiment prospects of the heavy ion physics at LHC C. Kobdaj, Y. Yan and K. Khosonthongkee School of Physics, Institute of Science.
P780.02 Spring 2003 L12Richard Kass The properties of the Z 0 For about ten years the Z 0 was studied in great detail at two accelerator complexes: LEP.

P Spring 2003 L12Richard Kass The properties of the Z 0 For about ten years the Z 0 was studied in great detail at two accelerator complexes: LEP.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.

W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
What are we made of ? Neutrinos Building a Particle Collider The ring is 27km round and on average 100m underground CERN – LEP, LHC.

What are we made of ? Neutrinos Building a Particle Collider The ring is 27km round and on average 100m underground CERN – LEP, LHC.
Introduction of Nuclear Physics. How can we probe the structure in the smaller scale? Discovery of nuclear structure Development of nuclear physics –Nuclear.

Introduction of Nuclear Physics. How can we probe the structure in the smaller scale? Discovery of nuclear structure Development of nuclear physics –Nuclear.
“Experimental Observation of Isolated Large Transverse Energy Electrons with Associated Missing Energy at = 540 GeV” Okamura Yusuke Shibata lab. G. Arnison.

“Experimental Observation of Isolated Large Transverse Energy Electrons with Associated Missing Energy at = 540 GeV” Okamura Yusuke Shibata lab. G. Arnison.
Atomic theory explains what the world is and how it’s held together. The Atom.

Atomic theory explains what the world is and how it’s held together. The Atom.

Similar presentations

Ads by Google