Dean Karlen University of Victoria & TRIUMF APS NW Section Meeting 2005 Victoria, Canada.
-
date post
21-Dec-2015 -
Category
Documents
-
view
217 -
download
2
Transcript of Dean Karlen University of Victoria & TRIUMF APS NW Section Meeting 2005 Victoria, Canada.
Dean KarlenUniversity of Victoria & TRIUMF
APS NW Section Meeting 2005Victoria, Canada
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 22
The International Linear ColliderThe International Linear Collider Next in the line of eNext in the line of e++ee-- colliders at the high colliders at the high
energy frontier of particle physicsenergy frontier of particle physics
SLAC/SLC
CERN/LEP
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 33
year
1980 1990 2000 2010 2020 2030
Cen
tre-
of-m
ass
ener
gy (
GeV
)
100
1000PETRAPEPTRISTANSLCLEP - ILEP - IIILCILC - II
eeee colliders at the frontier colliders at the frontier
Z0 threshold
W+W threshold
tt thresholdHZ0 threshold?
dark matter threshold?
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 44
Why Linear?Why Linear?
Centre-of-mass Energy (GeV)
0 100 200 300 400 500 600
Circ
umfe
renc
e /
Leng
th (
km)
0
10
20
30
40
50
60
$
circular colliders
linear colliders
2ER
EL
A circular 500 GeVmachine would be170 km around andconsume 45 GW
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 55
““High Energy” Particle PhysicsHigh Energy” Particle Physics
Increasing the collision energy allows for new Increasing the collision energy allows for new fundamental processes to be observed and fundamental processes to be observed and probes matter and space at smaller distance probes matter and space at smaller distance scalesscales
The two main HEP tools in the past 3 decades: The two main HEP tools in the past 3 decades: proton colliders and electron collidersproton colliders and electron colliders protons are more easily accelerated to high energies protons are more easily accelerated to high energies
because they radiate less synchrotron radiation in a because they radiate less synchrotron radiation in a circular acceleratorcircular accelerator
electron interactions are more easily studied because electron interactions are more easily studied because the initial state is simplerthe initial state is simpler
both tools have been essential to advance our both tools have been essential to advance our knowledge of fundamental physics:knowledge of fundamental physics:
discoveries of new phenomenadiscoveries of new phenomena testing models that account for these phenomenatesting models that account for these phenomena
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 66
Interplay of proton and electron Interplay of proton and electron colliderscolliders
proton collidersproton colliders electron colliderselectron colliders1980’s: SppS• discovery of the Z0, W, W
1990’s: LEP/SLC• detailed investigation of Z0, W, W production• indirect influence of top quark – definitive prediction of its mass• indirect influence of Higgs boson – mass estimated
2010’s: ILC• detailed study of the Higgs• detailed study of dark matter
2000’s: LHC• discovery of the Higgs boson?• discovery of the dark matter particle?
1990’s: Tevatron• discovery of the top quark
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 77
Linear Collider Physics: ILinear Collider Physics: I The electromagnetic and weak forces are now The electromagnetic and weak forces are now
known to arise from a unifying symmetry in natureknown to arise from a unifying symmetry in nature This was most precisely demonstrated by the LEP/SLC This was most precisely demonstrated by the LEP/SLC
experimentsexperiments
The symmetry between the electromagnetic and The symmetry between the electromagnetic and weak forces is broken (weak bosons are heavy)weak forces is broken (weak bosons are heavy) The Higgs model is an ad hoc component of the Standard The Higgs model is an ad hoc component of the Standard
Model that describes why the symmetry is brokenModel that describes why the symmetry is broken
it seems to work for low energy processes but falls it seems to work for low energy processes but falls apart at high energiesapart at high energies
the model predicts that a new particle exists (the the model predicts that a new particle exists (the Higgs boson) with definite propertiesHiggs boson) with definite properties
the ILC will be able to make a large variety of precision the ILC will be able to make a large variety of precision measurements that will provide critical data to measurements that will provide critical data to understand the real nature of electroweak symmetry understand the real nature of electroweak symmetry breakingbreaking
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 88
The golden processesThe golden processes At LEP, the golden processes for studying At LEP, the golden processes for studying
the electroweak sector were:the electroweak sector were:
At the ILC, the golden processes for At the ILC, the golden processes for studying the Higgs sector are:studying the Higgs sector are:
LEP beam energies were not sufficiently high LEP beam energies were not sufficiently high enough for these process to occurenough for these process to occur
0Zee WWee
HZee 0
Hee
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 99
Higgs production at a LCHiggs production at a LC
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1010
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1111
Linear Collider Physics: IILinear Collider Physics: II
From astrophysical observations, it appears From astrophysical observations, it appears that ~25% of the Universe is “Dark Matter”that ~25% of the Universe is “Dark Matter” neutral, stable, cold (massive), non-baryonicneutral, stable, cold (massive), non-baryonic new physics – a new (conserved) quantum number?new physics – a new (conserved) quantum number? production and detection of dark matter particles at production and detection of dark matter particles at
future colliders would be very exciting!future colliders would be very exciting!
One possible explanation arises in a model of One possible explanation arises in a model of particle physics known as “supersymmetry”particle physics known as “supersymmetry” in this model, all particles have supersymmetric in this model, all particles have supersymmetric
partners (sparticles) – the lightest would be stablepartners (sparticles) – the lightest would be stable
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1212
Dark Matter at the ILC?Dark Matter at the ILC?
There are strong hints that the dark matter There are strong hints that the dark matter could be produced at the ILCcould be produced at the ILC Supersymmetric models generally favour sparticle Supersymmetric models generally favour sparticle
masses below ~ 1 TeVmasses below ~ 1 TeV The dark matter density is consistent with a The dark matter density is consistent with a
neutral particle having “weak” strength couplingsneutral particle having “weak” strength couplings The LHC has the best chance to discover the The LHC has the best chance to discover the
supersymmetric particlessupersymmetric particles the signature: a large amount of energy is taken the signature: a large amount of energy is taken
away by invisible particlesaway by invisible particles challenging study at LHC: initial state is not well challenging study at LHC: initial state is not well
known, final state involves at least two DM known, final state involves at least two DM particlesparticles
The ILC offers the ability to study them in The ILC offers the ability to study them in detaildetail
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1313
Consensus in the HEP communityConsensus in the HEP community
Given the broad range of fundamental Given the broad range of fundamental physics questions that it addresses, the physics questions that it addresses, the HEP community sees the ILC to be the HEP community sees the ILC to be the next step that is needed to advance the next step that is needed to advance the fieldfield over 2700 particle physicists have signed a over 2700 particle physicists have signed a
document supporting the physics potential of document supporting the physics potential of the ILCthe ILC
the US DOE places the ILC as the top priority the US DOE places the ILC as the top priority for mid-term new facilities for mid-term new facilities
committees for future accelerators in Asia and committees for future accelerators in Asia and Europe also put the ILC as their first priorityEurope also put the ILC as their first priority
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1414
Building the ILCBuilding the ILC
Over the past decade, significant effort has Over the past decade, significant effort has gone into the necessary R&D to design a gone into the necessary R&D to design a linear collider to reach the required linear collider to reach the required specifications:specifications:
Energy: 500 GeV – 1000 GeVEnergy: 500 GeV – 1000 GeV requires RF cavities with a large accelerating requires RF cavities with a large accelerating
gradient (>30 MeV/m)gradient (>30 MeV/m)
Luminosity (density of collisions): > 10Luminosity (density of collisions): > 103434 cm cmss
requires large numbers of electrons (> 10requires large numbers of electrons (> 101010) ) packed into very small bunches (< 500 x 5 nmpacked into very small bunches (< 500 x 5 nm22) ) brought into collision at high rate (> 10brought into collision at high rate (> 1044 s s))
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1515
Building the ILCBuilding the ILC
Two complete designs were prepared that Two complete designs were prepared that met these requirementsmet these requirements the key feature distinguishing them was the the key feature distinguishing them was the
nature of the RF accelerating cavities:nature of the RF accelerating cavities: US + Japan – high frequency, room US + Japan – high frequency, room
temperaturetemperature Germany – lower frequency, superconductingGermany – lower frequency, superconducting
international technical review found both suitableinternational technical review found both suitable
In 2004, an international committee charged In 2004, an international committee charged with selecting one accelerating technology with selecting one accelerating technology chose the superconducting optionchose the superconducting option the world’s labs now work toward a single designthe world’s labs now work toward a single design
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1616
Superconducting accelerator cavitiesSuperconducting accelerator cavities
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1717
Possible Tunnel LayoutPossible Tunnel Layout
Need a 30 km tunnel to reach energy goalNeed a 30 km tunnel to reach energy goal
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1818
Damping ring R&DDamping ring R&D
ATF facility in Japan hasATF facility in Japan hasdemonstrated necessarydemonstrated necessaryreduction in emittancereduction in emittance
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 1919
Linear collider detector conceptsLinear collider detector concepts
LDC
SiD
GLD
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2020
Linear collider detector challengesLinear collider detector challenges Compared to the LHC, the ILC environment is Compared to the LHC, the ILC environment is
much less severe, but the performance much less severe, but the performance requirements are much more demanding:requirements are much more demanding:
Vertexing: Vertexing: ipip ~ 5 ~ 5 m m 10 10 m/(p sinm/(p sin3/23/2 )) 1/5 r1/5 rbeampipebeampipe, 1/30 pixel area, 1/30 thickness c.f. LHC, 1/30 pixel area, 1/30 thickness c.f. LHC
Tracking: Tracking: (1/p(1/ptt) ~ 5 ) ~ 5 ×10×10-5-5 GeV GeV-1-1
1/10 of LHC. 1/6 material in tracking volume1/10 of LHC. 1/6 material in tracking volume
Calorimetry: Calorimetry: EE ~ 0.3 ~ 0.3 EE 1/200 granularity of calorimeter c.f. LHC1/200 granularity of calorimeter c.f. LHC
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2121
Vertex detectorVertex detector Precise Si pixel detectors near the collision Precise Si pixel detectors near the collision
point point to detect the displaced vertex of particles to detect the displaced vertex of particles
coming from the decay of a particle with a very coming from the decay of a particle with a very short lifetime (less than 10short lifetime (less than 10 s) s)
examples: charm, bottom quarks, tau examples: charm, bottom quarks, tau leptonsleptons
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2222
Tracking detectorTracking detector
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2323
Tracking challengeTracking challenge Example: Higgs recoil massExample: Higgs recoil mass
(1/pt) ~ 5 ×10-5 GeV-1
is necessary!
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2424
Tracking technologyTracking technology Two technologies considered: Si (few Two technologies considered: Si (few
precise measuring layers) or gas precise measuring layers) or gas (continuous) (continuous)
Gas tracker: Time projection chamberGas tracker: Time projection chamber to achieve resolution goal requires an advance to achieve resolution goal requires an advance
in TPC technologyin TPC technology see talk by Gabesee talk by Gabe
Rosenbaum thisRosenbaum thisafternoon (B2)afternoon (B2)
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2525
CalorimeterCalorimeter
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2626
Jet Energy Resolution RequirementsJet Energy Resolution Requirements
Goal: distinguish W and Z when they decay into Goal: distinguish W and Z when they decay into quarksquarks requires excellent jet energy resolution, requires excellent jet energy resolution, EE ~ ~
30% 30% E E , ZZeeWWee example:
E%30E%60
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2727
Calorimeter technologyCalorimeter technology
To reach resolution goal requires narrow To reach resolution goal requires narrow showers and fine segmentation: Si + W showers and fine segmentation: Si + W
Iron Tungsten
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2828
Bringing the ILC into realityBringing the ILC into reality
An international structure has been set up An international structure has been set up to complete the global design of the ILCto complete the global design of the ILC Leader of the Global Design Effort: Barry BarishLeader of the Global Design Effort: Barry Barish
ILCSC
GlobalDesignEffort
Asia Regional Team
N. American Regional Team
EuropeanRegional Team
Participating Labsand Universities
Participating Labsand Universities
Participating Labsand Universities
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 2929
ILC timescaleILC timescale 2005:2005:
GDE put togetherGDE put together Detector concept groups in formationDetector concept groups in formation
2006:2006: GDE to prepare the ILC Conceptual DesignGDE to prepare the ILC Conceptual Design Detector concept groups to prepare outlinesDetector concept groups to prepare outlines
2007/8:2007/8: GDE to complete the ILC Technical DesignGDE to complete the ILC Technical Design Detector concepts complete Conceptual DesignsDetector concepts complete Conceptual Designs
2008/9:2008/9: Site selection, government approvals, begin constructionSite selection, government approvals, begin construction Detector collaborations formDetector collaborations form
2015?:2015?: earliest start of experimental programearliest start of experimental program
May 13, 2005May 13, 2005 The International Linear Collider / Dean Karlen, UVic & TRIUMFThe International Linear Collider / Dean Karlen, UVic & TRIUMF 3030
SummarySummary The physics case for a Linear Collider is The physics case for a Linear Collider is
very compellingvery compelling
The technologies for the machine and the The technologies for the machine and the experiments are in handexperiments are in hand
The international HEP community is solidly The international HEP community is solidly behind the project and is working together behind the project and is working together to bring it to reality!to bring it to reality!
For more information see:For more information see:www.linearcollider.org www.linearcollider.cawww.linearcollider.org www.linearcollider.ca