The ILC Higgs Factory Philip Burrows John Adams Institute, Oxford - - PowerPoint PPT Presentation

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The ILC Higgs Factory Philip Burrows John Adams Institute, Oxford - - PowerPoint PPT Presentation

The ILC Higgs Factory Philip Burrows John Adams Institute, Oxford University 1 Outline Introduction The Large Hadron Collider + the Higgs boson The Higgs factory The International Linear Collider (ILC) Higgs physics


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Philip Burrows

John Adams Institute, Oxford University

The ILC Higgs Factory

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Outline

  • Introduction
  • The Large Hadron Collider + the Higgs boson
  • The Higgs factory
  • The International Linear Collider (ILC)
  • Higgs physics at ILC
  • Project implementation and timeline
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Large Hadron Collider (LHC)

Largest, highest-energy particle collider

CERN, Geneva

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A Higgs boson?

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A Higgs boson?

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The 2012 discovery

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The 2012 discovery

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ATLAS status

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Monica D’Onofrio, LHCC June 4 2014

ATLAS CONF 2014 009

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It’s officially a Higgs Boson!

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Finger-printing the Higgs boson

Determine its ‘profile’:

  • Mass
  • Width
  • Spin
  • CP nature
  • Coupling to fermions
  • Coupling to gauge bosons
  • Yukawa coupling to top quark
  • Self coupling  Higgs potential
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Finger-printing the Higgs boson

Is it: the Higgs Boson of the Standard Model? another type of Higgs boson? something that looks like a Higgs boson but is actually more complicated?

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Finger-printing the Higgs boson

Is it: the Higgs Boson of the Standard Model? another type of Higgs boson? something that looks like a Higgs boson but is actually more complicated?  Measurements of the Higgs couplings to the different species of quarks, leptons and gauge bosons are the key to answering these questions

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Non-Standard Higgs couplings

Snowmass Higgs working group: Decoupling limit: If all new particles (except Higgs) are at a (high) high mass scale M deviations from SM predictions are of order mH

2 / M2

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For M = 1 TeV, deviations of couplings from SM:

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Non-Standard Higgs couplings

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For M = 1 TeV, deviations of couplings from SM: Deviations in the range 1%  10%

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Non-Standard Higgs couplings

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For M = 1 TeV, deviations of couplings from SM: Deviations in the range 1%  10%  measurements must be significantly more precise to resolve such deviations

Non-Standard Higgs couplings

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LHC projections

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LHC projections

Currently, typically LHC projected precisions on Higgs coupling measurements assume that:

  • Standard Model is correct
  • No non-Standard decay modes (total width = SM)
  • Charm and top couplings deviate from SM by

same factor

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ATLAS projections

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ATL PHYS PUB 2013 014

Luca Fiorini, LHCC Dec 2013

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CMS projections

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CMS-NOTE-2013-002 Yurii Maravin, LHCC Dec 2013

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LHC projections

Currently, typically LHC projected precisions on Higgs coupling measurements assume that:

  • Standard Model is correct
  • No non-Standard decay modes (total width = SM)
  • Charm and top couplings deviate from SM by

same factor Such assumptions are not necessary for Higgs coupling measurements at e+e- Higgs Factory …

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‘Higgs factory’

  • e+e- collider:

linear collider storage ring

  • photon-photon collider:

usually considered as add-on to linear collider

  • muon collider:

usually considered as a next step beyond a future neutrino factory

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e+e- Higgs factory

e+e- annihilations: E > 91 + 125 = 216 GeV E ~ 250 GeV E > 91 + 250 = 341 GeV E ~ 500 GeV

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e+e- colliders

  • Produce annihilations of point-like particles under

controlled conditions:

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e+e- colliders

  • Produce annihilations of point-like particles under

controlled conditions: well defined centre of mass energy: 2E

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e+e- colliders

  • Produce annihilations of point-like particles under

controlled conditions: well defined centre of mass energy: 2E complete control of event kinematics: p = 0, M = 2E

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e+e- colliders

  • Produce annihilations of point-like particles under

controlled conditions: well defined centre of mass energy: 2E complete control of event kinematics: p = 0, M = 2E polarised beam(s)

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e+e- annihilations

L or R

g

/

L or R

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e+e- colliders

  • Produce annihilations of point-like particles under

controlled conditions: well defined centre of mass energy: 2E complete control of event kinematics: p = 0, M = 2E polarised beam(s) clean experimental environment

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g

/

e+e- annihilations

E E

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g

/

e+e- annihilations

2E > 160 GeV

E E

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g

/

e+e- annihilations

2E > 182 GeV

E E

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e+e- annihilations

2E > 216 GeV

E E

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g

/

e+e- annihilations

2E > 350 GeV

E E

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g

/

e+e- annihilations

???

E E

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e+e- colliders

Wyatt

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e+e- colliders

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e+e- colliders

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e+e- colliders

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e+e- colliders

L ~ 1034 (250 GeV)  20,000 H / year

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e+e- colliders

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e+e- colliders

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European particle physics strategy 2013

There is a strong scientific case for an electron-positron collider, complementary to the LHC, that can study the properties of the Higgs boson and other particles with unprecedented precision and whose energy can be upgraded.

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European particle physics strategy 2013

There is a strong scientific case for an electron-positron collider, complementary to the LHC, that can study the properties of the Higgs boson and other particles with unprecedented precision and whose energy can be upgraded. The Technical Design Report of the International Linear Collider (ILC) has been completed, with large European

  • participation. The initiative from the Japanese particle

physics community to host the ILC in Japan is most welcome, and European groups are eager to participate.

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European particle physics strategy 2013

There is a strong scientific case for an electron-positron collider, complementary to the LHC, that can study the properties of the Higgs boson and other particles with unprecedented precision and whose energy can be upgraded. The Technical Design Report of the International Linear Collider (ILC) has been completed, with large European

  • participation. The initiative from the Japanese particle

physics community to host the ILC in Japan is most welcome, and European groups are eager to participate. Europe looks forward to a proposal from Japan to discuss a possible participation.

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Snowmass executive summary 2013

Compelling science motivates continuing this program with experiments at lepton colliders. Experiments at such colliders can reach sub-percent precision in Higgs boson properties in a unique, model-independent way, enabling discovery of percent-level deviations from the Standard Model predicted in many theories.

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Snowmass executive summary 2013

Compelling science motivates continuing this program with experiments at lepton colliders. Experiments at such colliders can reach sub-percent precision in Higgs boson properties in a unique, model-independent way, enabling discovery of percent-level deviations from the Standard Model predicted in many theories. They can improve the precision of our knowledge of the W, Z, and top quark well enough to allow the discovery of predicted new-physics

  • effects. They search for new particles in a manner

complementing new particle searches at the LHC.

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Snowmass executive summary 2013

Compelling science motivates continuing this program with experiments at lepton colliders. Experiments at such colliders can reach sub-percent precision in Higgs boson properties in a unique, model-independent way, enabling discovery of percent-level deviations from the Standard Model predicted in many theories. They can improve the precision of our knowledge of the W, Z, and top quark well enough to allow the discovery of predicted new-physics

  • effects. They search for new particles in a manner

complementing new particle searches at the LHC. A global effort has completed the technical design of the International Linear Collider (ILC) accelerator and detectors that will provide these capabilities in the latter part of the next decade. The Japanese particle physics community has declared this facility as its first priority for new initiatives.

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e+e- Higgs Factory

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ILC Higgs Factory Roadmap

250 GeV: Mass, Spin, CP nature Absolute meas. of HZZ BRs Higgs  qq, ll, VV 350 GeV: Top threshold: mass, width, anomalous couplings … (more stats on Higgs BRs) 500 GeV: HWW coupling  total width  absolute couplings Higgs self coupling Top Yukawa coupling  1000 GeV: as motivated by physics

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Higgs mass measurement

Recoil mass:

  • independent of

Higgs decay Discovery mode for ‘H’ decay to weakly-interacting particles (Fujii)

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Higgs spin determination

Rise of cross-section near threshold

(TESLA TDR)

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Higgs branching ratios determination (1)

(ILC TDR)

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Higgs branching ratios determination (2)

(Fujii / ILC TDR)

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Higgs branching ratios determination

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Higgs self-coupling determination

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Higgs top-coupling determination

(Price, Roloff)

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Baseline: 250 fb-1 @ 250 GeV 3 years 500 fb-1 @ 500 GeV 3 years 1000 fb-1 @ 1000 GeV 3 years

ILC roadmap

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Baseline: 250 fb-1 @ 250 GeV 3 years 500 fb-1 @ 500 GeV 3 years 1000 fb-1 @ 1000 GeV 3 years Followed by luminosity upgrade: ‘HL-ILC’: +900 fb-1 @ 250 GeV +3 years +1100 fb-1 @ 500 GeV +3 years +1500 fb-1 @ 1000 GeV +3 years

ILC roadmap

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ILC baseline precisions

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Higgs coupling map

(Fujii)

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ILC baseline + HL-ILC precisions

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Model-independent couplings extraction

33 input measurements 11-parameter fit

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Model-independent couplings

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Model-independent couplings

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Comparison with LHC

LHC does not project making model-independent Higgs coupling measurements LHC projections assume the Standard Model and estimate precision relative to SM couplings, also assuming charm follows top

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Model-dependent couplings extraction

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Comparison with LHC

LHC does not project making model-independent Higgs coupling measurements LHC projections assume the Standard Model and estimate precision relative to SM couplings, also assuming charm follows top For purpose of comparison, can follow same model- dependent procedure for ILC …

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Model-dependent couplings extraction

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Model-dependent couplings extraction

~10 x LHC sensitivity

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For M = 1 TeV, deviations of couplings from SM: Deviations in the range 1%  10%  measurements must be significantly more precise to resolve such deviations

Non-Standard Higgs couplings

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Specific beyond-SM examples

2HDM/MSSM

Zivkovic et al

Simulated ILC measurements

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The accelerator

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Large Electron Positron collider (RIP)

0.1 TeV beams

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Large Electron Positron collider (RIP)

0.1 TeV beams Synch rad  18 MW

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Super Large Electron Positron collider?

0.2 TeV beams?

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Super Large Electron Positron collider?

0.2 TeV beams? Synch rad  300 MW

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Super Large Electron Positron collider?

0.2 TeV beams? Synch rad  300 MW

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Linear Colliders for electrons + positrons

Stanford Linear Accelerator Center (California)

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main linac bunch compressor damping ring source pre-accelerator collimation final focus IP extraction & dump KeV few GeV few GeV few GeV 250-500 GeV

Designing a Linear Collider

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International Linear Collider (ILC)

31 km

  • c. 250 GeV / beam
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Beam parameters

ILC (500) Electrons/bunch 0.75 10**10 Bunches/train 2820 Train repetition rate 5 Hz Bunch separation 308 ns Train length 868 us Horizontal IP beam size 655 nm Vertical IP beam size 6 nm Longitudinal IP beam size 300 um Luminosity 2 10**34

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ILC Detectors

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ILC project status

  • 2005-12 ILC run by Global Design Effort (Barish)
  • C. 500 accelerator scientists worldwide involved
  • A Reference Design Report (RDR) was completed in 2007

including a first cost estimate

  • 2008-12 engineering design phase

major focus on risk minimisation + cost reduction

  • Technical Design document released end 2012

revised cost estimate + project implementation plan

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Technical Volumes

Reference Design Report ILC Technical Progress Report (“interim report”) TDR Part I: R&D TDR Part II: Baseline Reference Report Technical Design Report

~250 pages Deliverable 2 ~300 pages Deliverables 1,3 and 4

AD&I

Global Design Effort 85

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ILC project status

  • 2005-12 ILC run by Global Design Effort (Barish)
  • C. 500 accelerator scientists worldwide involved
  • A Reference Design Report (RDR) was completed in 2007

including a first cost estimate

  • 2008-12 engineering design phase

major focus on risk minimisation + cost reduction

  • Technical Design document released end 2012

revised cost estimate + project implementation plan

  • Lyn Evans assumed project leadership 2013

Japan preparing implementation of ILC at Kitakami

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ILC Plan in Japan

► Japanese HEP community proposes to host ILC

based on the “staging scenario” to the Japanese Government.

  • ILC starts as a 250GeV Higgs factory, and will evolve

to a 500GeV machine.

  • Technical extendability to 1TeV is to be preserved.

Yamauchi

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ILC Plan in Japan

► Japanese HEP community proposes to host ILC

based on the “staging scenario” to the Japanese Government.

  • ILC starts as a 250GeV Higgs factory, and will evolve

to a 500GeV machine.

  • Technical extendability to 1TeV is to be preserved.

Yamauchi

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Developments in Japan

Yamamoto, HEPAP, 11/3/13

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ILC in Japan?

meeting of Lyn Evans and Prime Minister Abe, March 27, 2013

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Developments in Japan

Yamamoto, HEPAP, 11/3/13

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PPAP recommendation

‘It is essential that the UK engages with the Higgs Factory initiative and positions itself to play a leading role should the facility go ahead.’

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Extra material follows

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Model-independent couplings

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Key challenges

  • Energy:

sustain high gradients > 30 MeV/m

  • Luminosity:
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Niobium Accelerating Cavities

TM010 mode

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Niobium Accelerating Cavities

  • c. 20,000 needed
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Niobium Accelerating Cavities

  • c. 20,000 needed
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Niobium Accelerating Cavities

Courtesy: R. Geng

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European X-FEL at DESY

3.4km

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Key challenges

  • Energy:

sustain high gradients > 30 MeV/m

  • Luminosity:

goal is > 10**34 / cm**2/ s

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ILC Cost Estimate (February 2007)

  • shared value = 4.87 Billion ILC Value Units
  • site-dependent value = 1.78 Billion ILC Value Units
  • total value = 6.65 Billion ILC Value Units

(shared + site-dependent)

  • labour = 22 million person-hours = 13,000 person-

years (assuming 1700 person-hours per person-year)

1 ILC Value Unit = 1 US Dollar (2007) = 0.83 Euros = 117 Yen

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500 1,000 1,500 2,000 2,500 3,000 3,500 4,000 4,500 Main Linac DR RTML e+ Source BDS Common Exp Hall e- Source VALUE - $M

ILC value breakdown

Conventional Facilities Components

Main Cost Driver