Title: Beyond the Terascale with muons
1Beyond the Terascale with muons
Fermilab Accelerator Physics and Technology
Seminar / Low-Emittance Muon Collider Workshop,
Fermilab, February 2006
Peter Skands Theoretical Physics Dept
Fermi National Accelerator Laboratory
2Overview
- Introduction the Standard Model
- What works
- What doesnt
- Beyond the Standard Model
- Open-minded model building
- Inspirational examples
- Collider Physics in the post-LHC era
3Below the Terascale
D. B. Leinweber, hep-lat/0004025
4The Standard Model (s.m.)
What works
- 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
5What works
data
Standard Model
. . . etc
But is that all?
6What Doesnt
- The Standard Model does face a few problems
- A few experiments
- Some mathematics
- Some cosmetics
- ? is the TeV scale inhabited?
7A Few Experiments
I have done a Terrible Thing, I have invented a
particle that cannot be detected. W. Pauli
Nobel 2002 Raymond Davis Jr., Masatoshi
Koshiba
What is giving mass to neutrinos?
8A Few Experiments
Whats causing this? (Dark Matter?)
9A Few Experiments
- The Supernova Cosmology Project
- Type Ia supernovae extragalactic standard
candles - The Supernovae are too dim!
- Universe accelerates!
? Einsteins Cosmological constant ? ? 0
Whats causing this? (Dark Energy?)
10 Muons
- Ability to control handle muons to extreme
precision may already be informing against the
Standard Model
(problematic)
Is mu is, or is mu aint?
muon storage ring (BNL)
11 Some Mathematics
- WLWL scattering
- Pertubative scattering P gt 1for s 1 TeV2
- Need something (e.g. Higgs) to unitarize theory.
(See also Bogdans talk)
12 Some Mathematics
- The Standard model isnt natural!
- The Higgs is special, its the only
(spin 0) - In QFT, the mass of a scalar gets huge
contributions from high-energy quantum
fluctuations
scalar
fluct. to top quark etc
13 Some Mathematics
- Gravity does not fit in the Standard Model!
- The graviton is special, its the only
(spin 2) - General Relativity metric gµ? describes
curvature of space-time ? a mixture of S0, S1,
and S2 fields. - In QFT, S2 is
? no sense! - Also, Gravity appears very weak compared to the
other forces ? Does that mean anything?
tensor
non-renormalizable
Gravity appears to be fundamentally incompatible
with Quantum Field Theory!
14 Some Aesthetics
- Why more matter than antimatter?
- Why 3 generations of quarks and leptons?
- Why 3 forces?
- Why 3 spatial dimensions?
- Are particles really pointlike?
- your childrens favourite questions
15Open-minded model building
- So we ask ourselves. Maybe
- More than 3 Generations of Fermions?
- More Higgs Fields? 2HDM? radion? NMSSM?
- New Exotic Particles? With new quantum numbers?
(Bogdan)
- 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?
16Open-minded model building
- So we ask ourselves. Maybe
- There could be new fundamental interaction(s)?
- New Short-range Gauge Forces? (Z / W ?
Technicolor?) - Could there be Lepton or Baryon Number Violation?
Matter
(Bogdan)
- 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),
Force
17Open-minded model building
- So we ask ourselves. Maybe
- There could be new symmetries of space-time?
- Is There a Supersymmetry (SUSY) in Nature?
(Probably most well-studied BSM possibility)
Matter
Force
Spacetime
18Open-minded model building
- So we ask ourselves. Maybe
- There could be new symmetries of space-time?
- Is There a Supersymmetry (SUSY) in Nature?
(Probably most well-studied BSM possibility)
Matter
- 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 GUTs dont work. SUSY GUTs do
- SUSY is the super in superstrings
- (Gives experimentalists something to look for)
Force
Spacetime
19Open-minded model building
- So we ask ourselves. Maybe
- There could be new symmetries of space-time?
- Is There a Supersymmetry (SUSY) in Nature?
(Probably most well-studied BSM possibility
Matter
- Known symmetries might break down?
- Is Lorentz Symmetry Violated to some Small
Extent?
Force
- There could be extra dimensions?
- How Many are There?
- What Do They Look Like? (Flat / Curved? Big /
Small?) - What Lives in Them? (All Matter / Gravity /
Exotics / Branes?)
(Randall, last week)
Spacetime
20What can we say beforehand?
- 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
Matter
Force
Spacetime
21What can we say beforehand?
- 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 ?
Matter
Force
- But!
- Best Dark Matter candidate is a
weakly-interacting particle with lt 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 ?
Spacetime
22Collider physics in the post-LHC era
- We believe TeV scale to be inhabited
- LHC powerful machine, good discovery potential.
Large backgrounds. Composite initial state.
Strong-interaction debris, QCD radiation, beam
remnants. Difficult to reach high precision.
Real life is more complicated
Textbook
23High Precision is important!
- (apologies) ILC propaganda (but also works for
MC!)
- High precision allows us to extrapolate to
fundamental scales ? GUT? Superheavy intermediate
physics?
24Collider physics in the post-LHC era
- ILC precision machine. Below 0.5 TeV.
- NB for SUSY WMAP
COBE
WMAP Wilkinson Microwave Anisotropy Probe
25Collider physics in the post-LHC era
- ILC precision machine. Below 0.5 TeV.
- WMAP killed the bulk ?
- CLIC technically challenging, but serious
alternative. - Both are ee- , 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)
26A Note on Luminosity
- Goal L1035 cm-2s-1 (acc. units)
- ? L 1000 fb-1 / yr ? 100 evts/yr for s gt 0.1 fb
- But lots of physics potential with smaller
luminosity as well ? s gt a few fb. - Physics case exists also for L1032,33,34
cm-2s-1, due to high energy. - (Large lumi still needed for precision)
27Outlook for the TeV scale and the 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!