heavy quark masses
DESCRIPTION
Heavy Quark Masses. Outline. General Remarks on Heavy Quark Masses R-Evolution of Heavy Quark Masses Bottom Mass Determinations Charm Mass Determinations Top Quark Mass from the Tevatron What mass is determined at Tevatron?. Remarks on Quark Masses. possible. - PowerPoint PPT PresentationTRANSCRIPT
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Flavor Theory Institute, CERN , June 5, 2008
Max-Planck-Institute for PhysicsMunich
André H. Hoang
Heavy Quark Masses
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 2
Outline
• General Remarks on Heavy Quark Masses
• R-Evolution of Heavy Quark Masses
• Bottom Mass Determinations
• Charm Mass Determinations
• Top Quark Mass from the Tevatron
• What mass is determined at Tevatron?
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 3
Remarks on Quark Masses
possible
We only want to use short-distance mass scheme that do not suffer from the renormalon inherent to the pole scheme!
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 4
… the POLE MASSWhat’s wrong with it?
Pole mass based on a particular renormalization prescription:
to all orders in perturbation theory
The partonic quark on-shell limit does not exist due to confinement!
So what? The strong coupling isn’t defined by a physical definition either.
The pole mass introduces, in an artificial, way a sensitivity to the Coulomb self energy of the heavy quark.
All mass-dependent quantities in the pole scheme develop a bad high order behavior.
Yes, but the partonic on-shell limit involves IR singularities.
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 5
Perturbation theory sucks!
Math for divergent series:
Siz
e o
f p
ert
. te
rms
Perturbative series are divergent.
Fortunately it is useful physically because the series are still asymptotic.
(Bernoulli, Euler, Abel, Borel,..)
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 6
Perturbation theory sucks!
Borel transform has poles in the complex plane
IR renormalons lead to ambiguities in
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 7
Perturbation theory & OPE
Pole mass scheme:
There is NO operator with the right dimension! Do not use the pole mass!
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 8
Short-Distance Masses
short-distance mass without ambiguity
perturbation series that contains the pole mass ambiguity of
What’s the best way to define ?
• infinitely many possible schemes exist
• but only certain classes can be used for certain types of problems.
How relevant it is to find a good scheme depends on the size of the uncertainties one has anyway or is willing to accept.
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 9
Top Quark Mass SchemesDifferent types of short-distance masses for different types of processes
Top Resonance Jet/resonance mass schemes
Fleming, Mantry, Stewart, AHH
absorbes infrared contributions below R into
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 10
Top Quark Mass SchemesDifferent types of short-distance masses for different types of processes
Top Resonance Jet/resonance mass schemes
Top Threshold 1S, PS mass schemes
High Energy/Off-shell MS/MSbar schemes
Beneke
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 11
Bottom+Charm Mass Schemes and are not very large.
Only two distinct classes need to be defined in practice.
Threshold Schemes:
Kinetic mass:
1S mass:
Shape fct mass:
Bigi, Uraltsev
Neubert
o from B meson form factor sum rules
o cut-off dependent
o from pert. mass
o scale independent
o from moments of B-decay shape function
o cut-off + renormalization scale dependent
• B/D physics (inclusive decays)
• Quarkonia:
• non-relativistic sum rules
Ligeti, Manohar, AHH
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 12
Bottom+Charm Mass Schemes and are not very large.
Only two distinct classes need to be defined in practice.
MSbar Mass Scheme: • high-energy, inclusive processes
• off-shell, highly virtual b and c quarks
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 13
What impact do schemes have?
Inclusive B decays:
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 14
What impact do schemes have?
Top Threshold:
• LL + NLL + NNLL(partial) QCD
• NNLL electroweak
• NLL + NNLL(partial) finite lifetime effects
Theory Status:
ILC Prospect
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 15
Need for a precise Charm mass
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 16
Need for a precise Top mass
Fit to electroweak precision observables
2 GeV error: change in
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 17
Need for a precise Top mass
Mass of Lightest MSSM Higgs Boson
5 Higgs bosons:
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 18
R-EvolutionJain, Scimemi, Stewart, AH arXiv:0803.4214
Perturbative relations between short-distance masses for widely separated R contain large logs that cannot be summed by usual UV renormalization group running.
Golden Rule: The SAME renormalization scale MUST be used to cancel the renormalon.
There is no choice of that avoids large logs!
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 19
R-EvolutionJain, Scimemi, Stewart, AH arXiv:0803.4214
In general, any short-distance mass depends on two scales:
UV-cutoffIR-cutoff
Consider R as a continuous parameter to describe an infrared renormalization group flow.
(A) Resolves the problem of large logs for
(B) Allows to study of renormalons without using bubble chains (large-nf)
(Bigi, Uraltsev, Shifmann, Vainshtein)
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 20
R-Evolution: practical application
renormalon-free !
LL Solution:
R-evolution equation
All logs are summed up properly.
Pole mass renormalon cancelled.
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 21
R-Evolution: practical application
renormalon-free !
All order Solution:
R-evolution equation
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 22
R-Evolution: practical application
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 23
R-Evolution: conceptual application
Study the pole mass renormalon without bubble chain approximation
has all the bad properties of the pole mass
Absolute convergent sum rule !
Sums to the same value for ALL short-distance masses!
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 24
R-Evolution: conceptual application
PS mass
static mass
MSR mass
Bubble chain:
Convergence of the sum rule for masses known to 3-loop order
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 25
R-Evolution: spin-off
Answer: Not quite, but we can construct a mass from it than can.
Can the MSbar mass RG-run below the mass ??
Jain, Scimemi, Stewart, AHH
arXiv:0803.4214
MSbar Scheme:
MSR Scheme:
runs with the R-evolution equationcan be used as jet/resonance or threshold mass
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Bottom Quark Mass Determinations
• Spectral Moments of Inclusive B Decays
• Sum Rules → relativistic
→ non-relativistic
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 27
Sum Rules
nonperturbative power corrections very small
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 28
Sum Rules Relativistic:
Kühn, Steinhauser, Sturm (2006) 3-loop for n=1 (update)
Boughezal, Czakon, Schutzmeier (2006) 3-loop for n=1 (update)
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Sum Rules Non-Relativistic:
NNLL RG-improved analyis (w.i.p.)
partial result: Pineda, Signer
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 30
Global Fits Experimental Data:
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 31
Global Fits Theoretical Moments:
• theory input: perturbative QCD
power corrections
• expansion scheme:
A) short-distance mass (MSbar)
B) eliminated
• mass scheme: threshold mass ( (A) kinetic, (B) 1S )
A) expansion
B) expansion
input: meson mass difference
A) Gambino, Uraltsev (2004)
B) Bauer, Ligeti, Manohar, Trott (2004)
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 32
Global FitsFit Results:
?
→ expansion scheme?
→ mass scheme ?
→ uncertainties underestimated ?
Number for kinetic mass without seem to be incompatible with sum rules.
(2007)
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Charm Quark Mass
• Spectral Moments of Inclusive B Decays
• Sum Rules → relativistic
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Charm mass from B decays
Buchmüller etal.
(based on Gambino,Uraltsev )
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 37
Charm Mass from Sum Rules
AH,Jamin, 2004
usual fixed order: fixed
RGI-A :
RGI-B :
pert. Behavior of moments: (2-loops)
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 38
Charm Mass from Sum Rules
AH,Jamin, 2004
Kühn, Steinhauser, (Sturm) (2001/2006)
Boughezal, Czakon, Schutzmeier (2006)
(2-loops fixed o.) (3-loops fixed o.)
(3-loops fixed o.)
(2-loops, accounting for countour analysis)
Contour analysis
should be done (w.i.p.)
+ updated data
+ updated data
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 39
Most recent Analysis
arXiv:0805.2999v1
Lattice results for moments of the pseudoscalar & vector
current-current correlators (“substitute for experimental data”)
• “substitute” for experimental data
• only continuum limit needs to be taken
• no further matching needed
• very small errors O(1%)
3-loop perturbative computations of the moments (fixed order method)
&
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 40
Top Quark Mass
• Tevatron Mass Measurement
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 41
Top Mass at Tevatron
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 42
Methods at TevatronTemplate Method
Dynamics Method
• dominated by the top invariant mass distribution
• systematics partly unclear
• effects of radiative corrections ? (LO-MC !)
• kinematics involves yet unresolved conceptual problems to proof a factorization theorem
(top quarks are slow, low p_T)
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 43
Top Production at the ILC
t
t-
W
W
b
b-
jetjetjet
jet
ILC: • No beam remnant : all soft radiation can be assigned to top or anti-top
→ jet algorithm
→ hemisphere prescription
• Avoids : Underying Events & Inititial State Radiation
• Event-shape: complete event characterized/controlled by a few IR-safe variables
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 44
Large- Method at the LHC
p pt
t-
W
W
b
b-
jetjetjet
jet
LHC:
Tevatron: no large p_T events !
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Flavor Theory Institute, CERN , June 5, 2008André H. Hoang - 45
What is the MC-mass at Tevatron?Strictly speaking at this time it is a model parameter like the quark mass in a potential model for mesons. Top is treated like a physical T-meson with color charge. Nowhere is an on-shell condition implemented.
Facts: The Tevatron method(s) are dominated by the reconstructed top invariant mass spectrum & Peak of invariant mass distr. is close to top mass.
Tevatron measures very likely a resonance-like mass, but it is not known which one OR at which value for R exactly due to unknown higher order corrections.
R-RGE
(ex) (R) (NNLL R-RGE)
To make more definite statements one needs to make a connection between MC and field theory.