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Standard Model
Tout ce qui nous entoure est constitué de particules de matière divisées en deux familles : les quarks et les leptons. Chaque groupe compte six particules qui se regroupent en paires ou « générations ». Les particules les plus légères et plus stables appa (Image: CERN)
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Member States of CERN
Map of CERN's Member states (Image: CERN)
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Distribution of All CERN Users by Location of Institute on 24 January 2018
Distribution of All CERN Users by Location of Institute on 24 January 2018 (Image: CERN)
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Distribution of all CERN Users by Nationality on 24 January 2018
Distribution of all CERN Users by Nationality on 24 January 2018 (Image: CERN)
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Distribution of all CERN Users by Location of Institutes on 5 July 2017
Distribution of all CERN Users by Location of Institutes on 5 July 2017 (Image: CERN)
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Distribution of all CERN Users by Nationality on 5 July 2017
Distribution of all CERN Users by Nationality on 5 July 2017 (Image: CERN)
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Representation of a doubly heavy-quark baryon
LHCb experiment observed a new particle with two heavy quarks: Ξcc++ (Image: CERN)
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Representation of a doubly heavy-quark baryon
LHCb experiment observed a new particle with two heavy quarks: Ξcc++ (Image: CERN)
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Enhanced production of multi-strange hadrons in high-multiplicity proton-proton collisions in ALICE experiment
Production élevée de hadrons multi-étranges dans des collisions proton-proton de haute multiplicité mesurées avec l’expérience ALICE. (Image: CERN)
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Enhanced production of multi-strange hadrons in high-multiplicity proton-proton collisions in ALICE experiment
Production élevée de hadrons multi-étranges dans des collisions proton-proton de haute multiplicité mesurées avec l’expérience ALICE. (Image: CERN)
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Magnetic monopoles and dipoles
Conventional bar magnets are also called ‘magnetic dipoles’ because they have two magnetic poles. In theory, “magnetic monopoles” could exist that act like an isolated “magnetic charge”, i.e. either a “North” or a “South” magnetic pole. (Image: CERN)
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Magnetic monopoles and dipoles
Conventional bar magnets are also called ‘magnetic dipoles’ because they have two magnetic poles. In theory, “magnetic monopoles” could exist that act like an isolated “magnetic charge”, i.e. either a “North” or a “South” magnetic pole. (Image: CERN)
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Reduced coupling strength scale factors measured from combined ATLAS and CMS
Reduced coupling strength scale factors measured from combined ATLAS and CMS data for weak bosons and fermions plotted as a function of their mass. A significant deviation would be a potential indicator of New Physics. (Image: CERN)
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LHCb experiment reports observation of exotic pentaquark particles
Illustration of the possible layout of the quarks in a pentaquark particle such as those discovered at LHCb. (Image: CERN)
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LHCb experiment reports observation of exotic pentaquark particles
Illustration of the possible layout of the quarks in a pentaquark particle such as those discovered at LHCb. (Image: CERN)
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Experimental limits from ATLAS on Standard Model Higgs production.
Experimental limits from ATLAS on Standard Model Higgs production in the mass range 110-600 GeV. The solid curve reflects the observed experimental limits for the production of a Higgs of each possible mass value (horizontal axis).The dashed curve shows t (Image: CERN)
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Plot showing ATLAS limits on Standard Model Higgs production in the mass range 110-150 GeV
The combined upper limit on the Standard Model Higgs boson production cross section divided by the Standard Model expectation as a function of mH is indicated by the solid line. (Image: CERN)
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CLOUD
(Image: CERN)
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Overall view of the TOTEM experiment
(Image: CERN)
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Computer generated image of the ATLAS inner detector
(Image: CERN)
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Computer generated image of the ATLAS inner detector
(Image: CERN)
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Schematic drawing of CLIC
(Image: CERN)
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The COMPASS experiment
Artistic view of the 60 m long Common Muon and Proton Apparatus for Structure and Spectroscopy (COMPASS) experiment. COMPASS is used to study the internal structure of hadrons (composite particles interacting via the strong force) by looking at a property (Image: CERN)
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ALICE A Large Ion Collider Experiment at CERN LHC : global layout
from left to right: Pierluigi Bellutti (ITC); Andrea Zanotti President of ITC; Luciano Bosisio (Trieste University); Mario Zen,Director of ITC ; Maurizio Boscardin (ITC); Jean-Robert Lutz, ITS-SSD Project leader (IPHC Strasbourg). (Image: CERN)
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A computer-generated image of the LHCb detector
Unlike most of the detectors on the LHC, which use barrel detectors, the LHCb detector will use walls of sub-detectors to study the particles produced in the 14 TeV proton-proton collisions. LHCb will investigate Naure's preference for matter over antimat (Image: CERN)
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Layout of the ALICE detector
The ALICE experiment will study the collisions of beams of lead nuclei in an attempt to produce a new state of matter known as 'quark-gluon plasma'. The barrel of the detector will be housed in the solenoid that once contained the L3 experiment. Outside o (Image: CERN)
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Layout of the ALICE detector
This computer-simulated view of the ALICE detector shows the framework that will be used to hold the detector in place. Located within the huge solenoid used for the previous L3 experiment at LEP, the new LHC experiment will observe the collisions of lead (Image: CERN)
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ALICE detector layout
This computer-simulation of the ALICE detector layout shows the collision point inside the tracking systems and barrel detector. The ALICE experiment at the LHC at CERN will sit inside the huge solenoid that once housed the L3 experiment until the LEP acc (Image: CERN)
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Virtual reality image of ATLAS with cavern walls visible
(Image: CERN)
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Diagram of the CNGS neutrino beam
Les protons, accéléré dans SPS au CERN, seront projetés sur une cible en graphite, produisant des pions et des kaons. Ces particules, passeront dans un tube où elles se désintègreront en neutrinos du muon. (Image: CERN)
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Diagram of CNGS neutrinos travelling through the Earth
Les protons, accéléré dans SPS au CERN, seront projetés sur une cible en graphite, produisant des particules qui seront désintégrées en neutrinos. Ces neutrinos voyageront à travers la Terre, vers le détecteur de Gran Sasso, Italie. (Image: CERN)
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Diagram of CNGS production complex
Les protons, accéléré dans SPS au CERN, seront projetés sur une cible en graphite, produisant des pions et des kaons. Ces particules, à la durée de vie courte, passeront dans un tube où elles se désintègreront en neutrinos du muon. (Image: CERN)
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Diagram of an LHC dipole magnet
Schéma montrant la coupe transversale d'un aimant dipôle du LHC avec la masse froide et la chambre sous vide. (Image: CERN)
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High energy cosmic rays striking atoms at the top of the atmosphere give the rise to showers of particles striking the Earth's surface
(Image: CERN)
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Computer-generated diagram of an LHC dipole
Cette image générée par ordinateur montre certains composants essentiels d'un dipôle du LHC. Le vide doit être maintenu dans les conduits des faisceaux, pour éviter des collisions non désirées entre le faisceau et d’autres particules. (Image: CERN)
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Comparative description of the electrons accelerating in a TV set and in the LEP
Version in French : CERN-DI-9808008 (Image: CERN)
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The forces in Nature
Version en anglais : CERN-DI-9808005 (Image: CERN)
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Layout of LHCb
Schema du detecteur LHC-B, une experience proposee pour le LHC. (Image: CERN)
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Layout of CMS
Schema du detecteur CMS, une experience proposee pour le LHC. Vue eclatee montrant quatre couches exterieures de detecteurs de muon, les calorimetres centraux et le systeme de trajectographie centrale. (Image: CERN)
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Layout of ATLAS
Schema du detecteur ATLAS, une experience proposee pour le LHC. A noter la taille des personnes autour du detecteur. (Image: CERN)
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Computer graphic of LHC in the tunnel
Cette image générée par ordinateur, montre le futur accélérateur de particules, le LHC, dans le tunnel construit pour l’accélérateur LEP (fermé en 2000). La deuxième image, est un schéma d’une coupe d’un aimant dipôle du LHC. (Image: CERN)
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Computer graphic of LHC in the tunnel
Cette image générée par ordinateur, montre le futur accélérateur de particules, le LHC, dans le tunnel construit pour l’accélérateur LEP (fermé en 2000). La deuxième image, est un schéma d’une coupe d’un aimant dipôle du LHC. (Image: CERN)
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Standard Model: constituents of matter
Schema expliquant les constituents de la matiere. (Image: CERN)
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From a grain of salt to quarks
Du grain de sel aux quarks. L'interieur d'un grain de sel. (Image: CERN)
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History of the Universe
Ce tableau montre les differents stades de l'evolution de l'Univers, du Big Bang a nos jours. (Image: CERN)
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Precision measurement of the Z0 line shape
Mesure de precision de la forme de la resonance Z0 prouvant que la matiere est constituee de trois familles de quarks and leptons (Image: CERN)
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ID: OPEN-PHO-CHART-2015-001-1

Tout ce qui nous entoure est constitué de particules de matière divisées en deux familles : les quarks et les leptons. Chaque groupe compte six particules qui se regroupent en paires ou « générations ». Les particules les plus légères et plus stables appa

2015-03-19

Conditions of Use © 2015 CERN

Dominguez, Daniel: CERN

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