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Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology Seminar / Low-Emittance Muon Collider Workshop, Fermilab, February 2006

Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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Page 1: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with muons

Fermi National Accelerator Laboratory

Peter Skands

Theoretical Physics Dept

Fermilab Accelerator Physics and Technology Seminar / Low-Emittance Muon Collider Workshop, Fermilab, February 2006

Page 2: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 2

OverviewOverview

• Introduction: the Standard Model– What works– What doesn’t

• Beyond the Standard Model– Open-minded model building– Inspirational examples

• Collider Physics in the post-LHC era

Page 3: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 3

Below the TerascaleBelow the Terascale

D. B. Leinweber, hep-lat/0004025

Page 4: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 4

• Relativistic Quantum Field Theory w/ Poincare Inv.

• 45 matter particles (fermions)– 36 quarks– 9 leptons (incl. neutrinos)

• 3 Forces (gauge bosons)– Gauged U(1):

electromagnetism– Gauged SU(2): weak force– Gauged SU(3): strong force

The Standard Model (s.m.)The Standard Model (s.m.)What works …What works …

symmetry breaking

masses•1 Higgs boson (scalar)

Page 5: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 5

What worksWhat worksdatadata Standard ModelStandard Model

. . . etc. . . etc

But is that all?But is that all?

Page 6: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 6

What Doesn’tWhat Doesn’t

• The Standard Model does face a few problems:

– A few experiments …

– Some mathematics …

– Some cosmetics …

is the TeV scale inhabited?

Page 7: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 7

A Few ExperimentsA Few Experiments““I have done a Terrible Thing, I have invented I have done a Terrible Thing, I have invented a particle that cannot be detected.”a particle that cannot be detected.”

W. PauliW. Pauli

What is giving mass to neutrinos?What is giving mass to neutrinos?

Nobel 2002: Raymond Davis Jr., Masatoshi KoshibaNobel 2002: Raymond Davis Jr., Masatoshi Koshiba

Page 8: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 8

A Few ExperimentsA Few Experiments

What’s causing this? (Dark Matter?)What’s causing this? (Dark Matter?)

Page 9: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 9

A Few ExperimentsA Few Experiments

What’s causing What’s causing thisthis? (Dark Energy?)? (Dark Energy?)

The Supernova Cosmology The Supernova Cosmology Project:Project:

Type Ia supernovae = extragalactic Type Ia supernovae = extragalactic ‘standard candles’‘standard candles’

The Supernovae are The Supernovae are too dim!too dim!

Universe accelerates!Universe accelerates!

Einstein’s Cosmological Einstein’s Cosmological constant constant ΛΛ ≠ 0 ≠ 0

Page 10: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 10

+ Muons …+ Muons …

(problematic)

• Muon spin precession

• Ability to control & handle muons to extreme precision may already be informing against the Standard Model:

muon storage ring (BNL)Is mu is, or is mu ain’t? Is mu is, or is mu ain’t?

Page 11: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 11

• WLWL scattering

• Pertubative scattering P > 1for s ~ 1 TeV2 • Need something (e.g. Higgs) to unitarize theory.

+ Some Mathematics+ Some Mathematics

¾» GF s16¼

(See also Bogdan’s talk)

Page 12: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 12

• The Standard model isn’t natural! – The Higgs is special, it’s the only (spin 0)– In QFT, the mass of a scalar gets huge contributions

from high-energy quantum fluctuations

+ Some Mathematics+ Some Mathematics

fluct. to top quark etc…

scalar

–But indirectly we know

There must be a spectacular cancellation occurring for this to happen THE HIERARCHY PROBLEM

Page 13: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 13

• Gravity does not fit in the Standard Model!– The graviton is special, it’s the only (spin 2)

– General Relativity: metric gμν describes curvature of space-time a mixture of S=0, S=1, and S=2 fields.

– In QFT, S=2 is no sense!

– Also, Gravity appears very weak compared to the other forces Does that mean anything?

+ Some Mathematics+ Some Mathematics

tensor

non-renormalizable

Gravity appears to be fundamentally incompatible with Quantum Field Theory!

Page 14: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 14

• Why more matter than antimatter?• Why 3 generations of quarks and leptons?• Why 3 forces?• Why 3 spatial dimensions?• Are particles really pointlike?• + your children’s favourite questions …

+ Some Aesthetics+ Some Aesthetics

Page 15: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 15

Open-minded model Open-minded model buildingbuilding

• So: we ask ourselves. Maybe …

Ma

tterM

atter

–There could be new fundamental matter?– Is Dark Matter made of Particles? What are they like? WIMPS?

(Bogdan)

– How About Dark Energy? – More than 3 Generations of Fermions? – More Higgs Fields? 2HDM? radion? NMSSM?

– New Exotic Particles? With new quantum numbers?

– Instantons? Cosmic Strings? Monopoles? …

–‘Fundamental’ Matter Might Be Composite?– Are Quarks or Leptons Composite? (excited fermions? top?)

– Is the Higgs particle a Composite? (Technicolor? Top seesaw?)

– Is Matter Made up of Strings?

Page 16: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 16

Open-minded model Open-minded model buildingbuilding

Fo

rceF

orce

–There could be new fundamental interaction(s)?–New Short-range Gauge Forces? (Z’ / W’ ? Technicolor?)

–Could there be Lepton or Baryon Number Violation?

Ma

tter

• So: we ask ourselves. Maybe …

(Bogdan)

GG

p¡ gdx4

³R ¡ ¹ 4n + 2

aR 2+bR ¹ º R ¹ º +cR ¹ º ¾½R ¹ º ¾½

´–What is gravity, at the fundamental level?– Deviations from Einstein Gravity?

– What is The Quantum Description Of Gravity?

– String Theory?

– Known forces might not be fundamental? – Grand Unification One Single Primeval Force?

[SU(5), SO(10), Supersymmetric Grand Unification, … ]

– ‘Stepwise unification’ ? Left-Right symmetry, flipped SU(5), …

Page 17: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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Open-minded model Open-minded model buildingbuilding

Sp

acetim

eS

pace

time

–There could be new symmetries of space-time?– Is There a Supersymmetry (SUSY) in Nature? (Probably most well-studied BSM possibility)

Ma

tterF

orce

• So: we ask ourselves. Maybe …

SUSY generators anticommute:

They relate particles of different spin:

Every SM state must have one (or more)

spin-partners!

scalar quarks and leptons, gluino,

gauginos, higgsinos

Page 18: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 18

Open-minded model Open-minded model buildingbuilding

Sp

acetim

eS

pace

time

–There could be new symmetries of space-time?– Is There a Supersymmetry (SUSY) in Nature? (Probably most well-studied BSM possibility)

Ma

tterF

orce

• So: we ask ourselves. Maybe …

Why should Nature have this weird symmetry?• SUSY is largest possible symmetry of space-time

• Stabilises the Higgs mass no hierarchy problem

• Good dark-matter candidate: lightest neutralino

• SM GUT’s don’t work. SUSY GUT’s do

• SUSY is the “super” in superstrings

• (Gives experimentalists something to look for)

Page 19: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 19

Open-minded model Open-minded model buildingbuilding

Sp

acetim

eS

pace

time

–There could be new symmetries of space-time?– Is There a Supersymmetry (SUSY) in Nature? (Probably most well-studied BSM possibility

Ma

tterF

orce

• So: we ask ourselves. Maybe …

– Known symmetries might break down?– Is Lorentz Symmetry Violated to some Small Extent?

–There could be extra dimensions?– How Many are There? – What Do They Look Like? (Flat / Curved? Big / Small?)Big / Small?)

– What Lives in Them? (All Matter / Gravity / Exotics /Exotics / Branes?)Branes?)

(Randall, last week)

Page 20: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

Beyond the Terascale with Muons 20

What can we say beforehand?What can we say beforehand?

Sp

acetim

eM

atter

Fo

rce

• A] A complete theory should:– explain the origin of mass– explain dark matter and dark energy– explain neutrino masses– unitarize WW scattering– agree with all measurements so far– address the hierarchy problem– incorporate quantum gravity

• B] A complete theory could:– involve grand unification (we have hints of it)– involve a deviation from the SM (g-2)mu – be aesthetic and natural– be simple

Page 21: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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What can we say beforehand?What can we say beforehand?

Sp

acetim

eM

atter

Fo

rce

• On one hand, we may roughly say– Simplest explanation for neutrino masses

involves no new observable physics – Quantum Gravity extremely difficult to probe

experimentally, due to smallness of hG – Dark Energy: no great ideas at the moment

• But!– Best Dark Matter candidate is a weakly-

interacting particle with <~ TeV-scale mass – WW scattering must be unitarised below the

TeV scale, probably by Higgs or similar – If Higgs is there, then hierarchy problem

means something new likely at TeV scale

Page 22: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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Collider physics in the post-Collider physics in the post-LHC eraLHC era

• We believe TeV scale to be inhabited

Textbook

Real life is more

complicated

–LHC: powerful machine, good discovery potential. Large backgrounds. Composite initial state. Strong-interaction debris, QCD radiation, beam remnants. Difficult to reach high precision.

Page 23: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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High Precision is *High Precision is *importantimportant*!*!• (apologies) ILC propaganda (but also works for MC!):

• High precision allows us to extrapolate to fundamental scales GUT? Superheavy intermediate physics?

Page 24: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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Collider physics in the post-Collider physics in the post-LHC eraLHC era

• ILC: precision machine. Below ~ 0.5 TeV.

• NB for SUSY: WMAP

COBECOBE

WMAPWMAPWilkinson Microwave Anisotropy Probe

Page 25: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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1 TeV1 TeV

??

Collider physics in the post-Collider physics in the post-LHC eraLHC era

• ILC: precision machine. Below ~ 0.5 TeV.

• WMAP killed the bulk

• CLIC: technically challenging, but serious alternative.

• Both are e+e- , muons are different.

–(E.g. intermediate SUSY Higgs factory at 500GeV?)

–Neutrino Factory

–Probe new physics differently

(talk by D. Cline)

(talk by B. Dobrescu)

Page 26: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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A Note on LuminosityA Note on Luminosity

• Goal: L=1035 cm-2s-1 (acc. units)

L ~ 1000 fb-1 / yr 100 evts/yr for σ > 0.1 fb

• But lots of physics potential with smaller luminosity as well σ > “a few” fb.

• Physics case exists also for L=1032,33,34 cm-2s-1, due to high energy.

• (Large lumi still needed for precision)

Page 27: Beyond the Terascale with muons Fermi National Accelerator Laboratory Peter Skands Theoretical Physics Dept Fermilab Accelerator Physics and Technology

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Outlook for the TeV scale and Outlook for the TeV scale and the muon colliderthe muon collider

• We believe the TeV scale to be inhabited

• The LHC is a powerful machine, but difficult to get high precision

• And high precision is important!

• If built, ILC will add immensely to our knowledge no matter what, but need higher energy if LHC indicates new physics is heavy

• Even if new physics is within ILC reach, it is likely only the top of an iceberg. Higher energies will still be needed to probe the full spectrum!