CERN now and in the future

Slides:



Advertisements
Similar presentations
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
Advertisements

ATLAS LHCb CMS ALICE LHCf TOTEM MoEDAL Circumference: 26.7km Design Energy 7TeV+7TeV ATLAS/LHC Ultimate LHC→ HL-LHC Katsuo Tokushuku (KEK)
(ATLAS) Higgs Prospects at HL-LHC. ATLAS CMS ALICE LHCb Center-of-Mass Energy ( ) 7 TeV Center-of-Mass Energy (Nominal) 14 TeV ? Center-of-Mass.
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
P5 Meeting - Jan , US LHC University M&O Personnel University with major hardware responsibility at CERN Based on > 10 years of US Zeus experience.
Diffractive DIS with E e =70GeV and E p =7TeV at the LHeC For general physics aim and sketch of machine design, see plenary talk of E. Perez … … what could.
The new Silicon detector at RunIIb Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96.
1 Hunting for the Higgs at LHC Konstantin Goulianos RU HOL FORUM October 6, 2011 The key to mass?
A. Bay Beijing October Accelerators We want to study submicroscopic structure of particles. Spatial resolution of a probe ~de Broglie wavelength.
K. Kumar, W. Marciano, Y. Li Electroweak physics at EIC - Summary of week 7 INT Workshop on Pertubative and Non-Pertubative Aspects of QCD at Collider.
LHC’s Second Run Hyunseok Lee 1. 2 ■ Discovery of the Higgs particle.
The LHC and Beyond APS Meeting Anaheim May 2, 2011 Sergio Bertolucci CERN LHC.
WLCG Collaboration Workshop, “Gotham City”, May 2012 Introduction WLCG Collaboration Workshop, “Gotham City”, May 2012 Introduction.
Future Accelerators at the High Energy Frontier
Surrounding the tracker, the calorimetry system measures with high accuracy the energy of electrons and photons as well as individual hadrons with 7500.
What is the Higgs??? Prof Nick Evans University of Southampton.
Search for a Z′ boson in the dimuon channel in p-p collisions at √s = 7TeV with CMS experiment at the Large Hadron Collider Search for a Z′ boson in the.
Collider Detector at Fermilab Sung-hyun chang High Energy Physics lab. KNU.
CERN Status and Future Plans Perugia June 6, 2011 Sergio Bertolucci CERN LHC.
1 Tunnel implementations (laser straight) Central Injector complex.
Alors, c’est fini! Et maintenant?. Machine Upgrade in Stages Push LHC performance without new hardware –luminosity →2.3x10 34 cm -2 s -1, E b =7→7.54.
LHCb: Xmas 2010 Tara Shears, On behalf of the LHCb group.
Overview of Supersymmetry and Dark Matter
Status of the LHC: Past, Present and Future 24th Rencontres de Blois May 27, 2012 Sergio Bertolucci CERN LHC.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
New Results From CMS Y.Onel University of Iowa A Topical Conference on elementary particles, astrophysics and cosmology Miami 2011, Dec 15-20, 2011 conference.
LHC-CC Validity Requirements & Tests LHC Crab Cavity Mini Workshop at CERN; 21. August Remarks on using the LHC as a test bed for R&D equipment.
The Higgs Boson Beate Heinemann, University of Liverpool  The Standard Model and Beyond  Tevatron and LHC  Tevatron Results on Higgs Searches  Future.
Glion Colloquium / June Accelerating Science and Innovation R.-D. Heuer, CERN HL-LHC, Aix-les-Bains, 1 Oct ECFA HL-LHC Experiments Workshop.
The Standard Model of the elementary particles and their interactions
Ideas for Super LHC tracking upgrades 3/11/04 Marc Weber We have been thinking and meeting to discuss SLHC tracking R&D for a while… Agenda  Introduction:
From the Standard Model to Discoveries - Physics with the CMS Experiment at the Dawn of the LHC Era Dimitri Bourilkov University of Florida CMS Collaboration.
1 Arnold Pompoš, SUSY03, Tucson, Arizona, June 5-10, 2003.
Fabiola Gianotti, 14/10/20031  s = 28 TeV upgrade L = upgrade “SLHC = Super-LHC” vs Question : do we want to consider also the energy upgrade option.
Already time to think of upgrading the machine Two options presently discussed/studied Higher luminosity ~10 35 cm -2 s -1 (SLHC) –Needs changes in.
High energy photon LHC Krzysztof Piotrzkowski Université Catholique de Louvain LHC as a high energy  and  p collider Tagging photoproduction.
Backup slides Z 0 Z 0 production Once  s > 2M Z ~ GeV ÞPair production of Z 0 Z 0 via t-channel electron exchange. e+e+ e-e- e Z0Z0 Z0Z0 Other.
The Linear Collider Roadmap IWLC2010 CERN October 18, 2010 Rolf-Dieter Heuer CERN.
Searches for Resonances in dilepton final states Searches for Resonances in dilepton final states PANIC th -14 th November 2008, Eilat, ISRAEL A.
LHC, Prague, July 2003Filip Moortgat, University of Antwerpen LHC Praha 2003 Detection of MSSM Higgs bosons using supersymmetric decay modes.
Study of Diboson Physics with the ATLAS Detector at LHC Hai-Jun Yang University of Michigan (for the ATLAS Collaboration) APS April Meeting St. Louis,
Joshua Moss (Ohio State University) on behalf of the ATLAS Collaboration ICHEP 2012, Melbourne 6 July 2012 ATLAS Electroweak measurements of W and Z properties.
An Idiot’s Guide to LHC Upgrades Bohr Lunch Seminar. 16/5/08 Terry Wyatt. University of Manchester.
CERN’s Large Hadron Collider
First collisions in LHC
LHC Status and Prospects
Large Hadron Collider (LHC)
The CERN Physics Programme
B meson studies - from commissioning to new physics effects.
contribution to the round table discussion
Introduction to CERN Activities
LHC during week 45 LHC delivered ~0.837 fb-1 in week 45
Introduction to CERN Activities
Dart-yin A. Soh Institute of Physics, Academia Sinica
Lecture 2 Live Feed – CERN Control Centre
Summary Session 3 Standard Model and Beyond
The ATLAS Experiment at the LHC
SUSY post LHC-8: what’s excluded, what’s not
Exploration and Challenges at the Large Hadron Collider
MSSM4G: MOTIVATIONS AND ALLOWED REGIONS
CEPC-SppC Accelerator CDR Copmpletion at the end of 2017
Hong-Jian He Tsinghua University
CSP Meeting CERN CERN Accelerators in th November 2010
Radiation Shield Design by UA
J. Uythoven, W. Venturini Delsolaro, CERN, Geneva
SUSY SEARCHES WITH ATLAS
What do we hope to understand?
Ronan McNulty University College Dublin
Inclusive Measurements as an mSUGRA Signal with ATLAS
LS 1 start date 12th June Schedule Extension 2012 run Extension of 2012 run approved by the DG on 3rd July 2012.
Presentation transcript:

CERN now and in the future Sergio Bertolucci CERN

LHC: status LHC run 1 ended on February 14, 2013 A fantastic concurrency of exceptional performances from the accelerators, experiments and computing LS1 is now in full swing, while data analysis is proceeding at full speed. A very busy and important period in front of us

THE LAST PHYSICS BEAM OF LHC RUN 1 (2009 - 2013)

Last 3 years

WLCG Status Record amounts of data acquired ~30 PB in 2012; CERN archive now ~100 PB Peaks of >4.6 PB/week in November Data written into Castor per week All resources fully used: ~ 2 million jobs/day Use of CPU vs pledges (plot shows Tier 2s) >100% for Tier 1 & 2 Occupation of Tier 0 will  100% during LS1

Published papers LHCb + 66 from ALICE 9 from TOTEM 9 from LHCf

The highlight of a remarkable year 2012

A new particle: no doubt that it is there… By now we can establish it with a single decay channel! e.g. H  ZZ  4l

…it prefers 0+ quantum numbers

…its mass is measured to .5%

…and the signal strength is compatible with a SM Higgs

But, despite its success… …. we know that the Standard Model is not complete because: It doesn’t solve the hierarchy problem It has no explanation for dark matter/dark energy Its mechanisms of CPV are too small to explain matter/antimatter imbalance It cannot provide a QFT of gravitation ….etc

Where we stand There is a new boson of mass ~125 GeV, with properties consistent with the SM Higgs, within the current uncertainties. More data needed to ascertain the nature of this object. So far, no indications of BSM physics from direct searches at the High E Frontier: colored SUSY particles (first generations) ruled out up to O(1 TeV), for a light LSP; “natural” SUSY probed at level of a few hundred GeV of 3rd generation spartners; exotica: heavy objects probed up to masses of 2-3 TeV; a lot of room still to be explored, 14 TeV will be essential!

BSM: we have searched.... eg. exclusions plots shown at Moriond QCD 2012....

The big picture inclusive searches Natural SUSY long-lived particles, https://twiki.cern.ch/twiki/bin/view/AtlasPublic/CombinedSummaryPlots Natural SUSY long-lived particles, eg. split SUSY RPV

SUSY health The experiments have already explored a very vast range of masses and parameters Though, too early to declare SUSY’s death, since there remain important parameter regions to be explored, and because Difficult or impossible to give “absolute” limits, since basically always assumptions involved limits quickly degrade or disappear when raising m(LSP) beyond several hundreds of GeV inclusive searches often assume degenerate 1st and 2nd generation squarks. Limits decrease (by several hundreds of GeV) if this is given up simplified models make strong assumptions on branching ratios, masses of intermediate states theory uncertainties (cross sections/scales/pdfs, initial state radiation)

fall-off of the lower-energy PDF, at large x Parton luminosities from http://www.hep.phy.cam.ac.uk/~wjs/plots/plots.html 2 TeV 40-50 rise because of steep fall-off of the lower-energy PDF, at large x G. Rolandi, private comm. for a fixed mass scale

LHC, the next 20 years , bunch spacing 25 ns , bunch spacing 50 ns ?, IR 4x , bunch spacing 25 ns ~20-25 fb-1 ~75-100 fb-1 ~350 fb-1 , bunch spacing 50 ns Go to design energy, nominal luminosity Injector and LHC Phase-1 upgrade to ultimate design luminosity HL-LHC Phase-2 upgrade, IR, crab cavities? √s=14 TeV, L=5x1034 cm-2 s-1, luminosity levelling √s=14 TeV, L~2x1034 cm-2 s-1, bunch spacing 25 ns √s=13~14 TeV, L~1x1034 cm-2 s-1, bunch spacing 25 ns √s=7~8 TeV, L=6x1033 cm-2 s-1, bunch spacing 50 ns LHC startup, √s = 900 GeV

The machine – LS1 Repair defective interconnects Consolidate all interconnects with new design Finish off pressure release valves (DN200) Bring all necessary equipment up to the level needed for 7TeV/beam

Then… E=6.5TeV β* = 0.5m (maybe 0.4) All other conditions as in 2012 i.e. LHC availability same, etc..

The experiments A new mode of operations: All busy in repairs, consolidations, first upgrades Massive amount of work, with a very tight schedule… …while keeping looking at the data, prepare for the next energy …and proceed to a very substantial progress in their computing models. It will need a massive recommissioning, if they want to be at the same readiness level as in 2010

The experiments, upgrades Fully engaged in the LS2 upgrades, which is particularly demanding for LHCb and ALICE Active R&D programs on the BIG upgrades in 2022 Need to use the coming run to better focus the program

Extending the reach… Weak boson scattering Higgs properties Supersymmetry searches and measurements Exotics t properties Rare decays CPV ..etc Experiments are planning a workshop in October 2013 to assess their physics reach and the implications on the detector upgrades and associated R&D

HL-LHC: the detector upgrades Both ATLAS and CMS detectors are planning important upgrades to stand the harsher running conditions at HL-LHC: pile-up, rates, radiation damage Pile-up ~ 4-5 times more pile-up then today Plan: keep detector performance for main physics objects at the same level as we have today Improved trigger system New tracking systems Improved forward detectors ….

and beyond LHC ? 25

Preliminary HE-LHC - parameters Not only luminosity: High Energy LHC Preliminary HE-LHC - parameters Very preliminary with large error bars

HE-LHC – LHC modifications 2030-33 SPS+, 1.3 TeV, 2030-33 2-GeV Booster Linac4

Thinking BIG This large tunnel would also allow e+e- and e-p collisions as well as pp collisions HE-LHC dipole design will piggy back on the high gradient quadrupole R&D needed for HL-LHC Would allow an increase in energy by factor of 2-2.5 SHE-LHC (??SSC) needs a 80km tunnel In conjunction with the high field magnets would allow a factor of (2-2.5)x(80/27) = 6-7.5 times LHC (42-52 TeV/beam)

The Particle Physics Landscape at CERN High Energy Frontier LHC Hadronic Matter deconfinement non-perturbative QCD hadron structure Low Energy heavy flavours / rare decays neutrino oscillations anti-matter Non-accelerator dark matter astroparticles Multidisciplinary climate, medicine Non-LHC Particle Physics = o(1000) physicists / o(20) experiments In the past 1.5 year Several breakthroughs ! Steady progress of other programs New mid-term and long-term projects started or in discussion

In summary 2010-2012: extraordinary years! But we are just at the beginning of a long journey. By now, experimental results are dictating the agenda of the field. We need to accelerate the reflection on next steps Interesting times in front of us!

Thank you!