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Higgs boson-like particle discovery claimed at LHC

Cern scientists reporting from the Large Hadron Collider (LHC) have claimed the discovery of a new particle consistent with the Higgs boson.

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Observation of a New Particle with a Mass of 125 GeV

CMS Experiment, CERN
4 July 2012

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July 4th seminar on new CMS Higgs search results

Event display

On 4th July, at 09:00 CEST, CMS will present their latest results on the search for the Standard Model (SM) Higgs boson at the LHC.

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Blinding and unblinding analyses

 

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Communicating new CMS results for ICHEP 2012

This page is to help CMS collaborators communicate with the media, public, students, etc. It will be updated as soon new material is available.
Send comments or questions to Lucas Taylor

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CMS 2012 data already exceed 2011 sample

CMS Total Integrated Luminosity for 2011, as of June 18

LHC has delivered 6.65 fb−1 of collisions to CMS in 2012 so far

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CMS Results for the ICHEP 2012 Conference

CMS results at ICHEP 2012

*** draft *** draft *** draft ***

ICHEP agenda CMS contributions
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New CMS detectors under construction at CERN

While the LHC will play the starring role in the 2013/2014 Long Shutdown (LS1), the break will also be a chance for its experiments to upgrade their detectors.

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The search for microscopic black holes, as of March 2012

An example of a CMS event with large total transverse energy (S<sub>T</sub>=2.6 TeV) and high jet multiplicity (9 jets, denoted by light purple cones and lines).

The search for microscopic black holes at the LHC is motivated by the hierarchy problem — the huge observed difference between the strengths of the electroweak and gravitational forces.

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Measurement of the underlying event in the Drell-Yan process in proton-proton collisions at sqrt(s) = 7 TeV

The UE activity as a function of the di-muon invariant mass

A measurement of the underlying event (UE) activity in proton-proton collisions at a centre-of-mass energy of 7 TeV is performed using Drell-Yan events in a data sample corresponding to an integrated luminosity of 2.2 fb−1

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