Hadronic Weak Interactions · Hadronic weak interactions at low energies-Quarks confined in...
Transcript of Hadronic Weak Interactions · Hadronic weak interactions at low energies-Quarks confined in...
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Hadronic Weak Interactions
Matthias R. Schindler
Fundamental Neutron Physics Summer School 2015
Some slides courtesy of N. Fomin
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Weak interactions
- One of “fundamental” interactions- Component of Standard Model- SU(2)×U(1) gauge theory- Quarks and leptons interact via weak interaction- Mediated by W, Z exchange
See lectures by S. Gardner
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Typology of weak interactions
- Leptonic: only leptons, no quarksExample:
µ+ → e+ + νe + νµ
- Semileptonic: some leptons, some quarksExample:
K 0 → π+ + e− + νe
- Hadronic: no leptons, only quarksExample:
K 0 → π+ + π−
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Strangeness-changing hadronic weak interactions
K 0 → π+ + π−
- Simple quark model
K 0 = ds, π+ = ud , π− = ud
- Strangeness-changing decay- Mediated by W exchange
Ignore from now on
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Strangeness-conserving hadronic weak interactions
At low energies current-current form
L∆S=0weak =
G√2
cos2 θCJ0,†W J0
W︸ ︷︷ ︸∆I=0,2
+ sin2 θCJ1,†W J1
W︸ ︷︷ ︸∆I=1
+J†Z JZ
- Isospin structure ∆I = 0,1,2- ∆I = 1 dominated by neutral current JZ (sin2 θC ∼ 0.05)- NC JZ not observed in flavor-changing hadronic decays
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Hadronic weak interactions
Well understood in terms of SM degrees of freedom
So what is the problem?
- Free quarks not observed→ Hadrons (N, π, . . . )- Range of weak interactions ≈ 1/MW ∼ 0.002 fm- 0.002 fm� rnucleon
- Quarks confined into hadrons by strong interactions (QCD)
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Strong interactions
Quantum chromodynamics- SU(3) gauge theory- Quarks as matter fields- Interaction mediated by gluons
LQCD =6∑
f =1
qf (i /D −mf )qf −12
Tr (GµνGµν)
with covariant derivative Dµqf ≡ (∂µ + igAµ) qf ,
Looks simple enough?
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Strong interactions
- QCD coupling increases for lower energies
0
0.1
0.2
0.3
1 10 102
µ GeV
α s(µ)
adapted from Particle Data Group
- Perturbation theory in αS not useful at low energies- Non-perturbative regime of QCD- Construct effective interaction on hadronic level
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Example: Nucleon structure
Desy
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Hadronic weak interactions at low energies
- Quarks confined in hadrons by strong interactions- Size ∼ (fm)
- Quarks interact weakly- Range ∼ 0.002 fm
Interplay of weak and nonperturbative strong interactions
- Construct PV interaction between hadrons (Here: NN)- Use to calculate observables in hadronic systems- Relate to underlying SM
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Why should I care?
- Weak neutral current in hadron sector- Probe of strong interactions
- Weak interactions short-ranged- Sensitive to quark-quark correlations inside nucleon- No need for high-energy probe- “Inside-out probe”
- Isospin dependence of interaction strengths?→ ∆I = 1/2 puzzle (strangeness-changing )?
- Can contribute to T violating observables
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Parity-violating NN interactions
- Parity-violating component in NN interaction- Suppressed by GF m2
π/g2πNN ∼ 10−7
- Isolate in pseudoscalar observables (~σ · ~p)- Longitudinal asymmetries- Angular asymmetries- Spin rotation- γ circular polarization- Anapole moment
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PV in complex nuclei
Enhancements in heavy nuclei- Large parity conserving matrix amplitudes- Close level spacings between states with opposite parity
〈+|VPV |−〉E+ − E−
- Up to 10% effect (~n 139La)- Many-body problem→ Difficult to interpret
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PV in few-nucleon systems
- No enhancements
O(10−7) effects
- High-intensity sources (neutrons, photons, . . . )- Control over systematics- Understand in terms of NN interactions
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NPDGamma
γθ
- Radiative capture of polarized neutrons on protons- Angular asymmetry Aγ
1Γ
dΓ
d cos θ= 1 + Aγ cos θ
- Correlation between neutron spin and photon momentum- Measured at SNS
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NPDGamma data taking completed in June 2014
Spin octet
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• In principle, experiment can be done with just one detector, reversing the neutron spin:
• Add opposite detector at same angle
(eliminates some systematic errors):
Asymmetry Extraction
↓↑
↓↑
+
−=
YYYYAraw
⎟⎟
⎠
⎞
⎜⎜
⎝
⎛
+
−+
+
−=
↓↓
↓↓
↑↑
↑↑
ij
ij
ji
jiraw YY
YYYYYY
A21
ii
j
θ
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~n 3He→ p 3H
- Charge-exchange reaction- Correlation between neutron spin and proton momentum
10 Gauss solenoid
RF spin Flipper
3He target / ion chamber
FnPB cold neutron guide
3He Beam Monitor
FNPB n3He detector (“the Cave”)
Super-mirror polarizer
Aim: extract parameters characterizing hadronic PV interactions
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Early ideas about NN interaction
NN potential- Finite range- Massive particle exchange- Yukawa: M ∼ 100 MeV
Long-range (r & 1.5 fm): One-pion exchange
- Intermediate distance (0.7 fm . r . 1.5 fm): two-pionexchange?
- Short-distance (r . 0.7 fm): ?
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NN potentials: basics
Symmetry constraints on possible form of NN potential- Galilei invariance- C,P,T- Isospin
V =∑
ViOi
- Operators Oi : 1, ~S · ~S, S12, ~L · ~S, (~L · ~S)2
- Coefficients Vi(r , ~p 2, ~L 2): undetermined
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A note on potentials
Potentials are not observable
- Matrix element〈f |V |i〉
- Unitary transformation:
〈f | → 〈f |U†, |i〉 → U|i〉
- Matrix element unchanged if
V → UVU†
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Models
Phenomenological models- Make ansatz for Vi
- Long range: one-pion exchange- ≈ 40− 50 parameters- Fit to NN scattering data- Interpretation?- Connection to QCD?
One-boson-exchange models- Long range: one-pion exchange- Intermediate and short range: σ, 2π, ρ, ω, . . .- Mi < 1 GeV- Connection to QCD?
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PV potential
Meson-exchange models- Single-meson exchange (π±, ρ, ω) between two nucleons
with one strong and one weak vertex
π±, ρ, ω
- Barton’s theorem: no π0 exchange- Weak interaction encoded in PV meson-nucleon couplings
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DDH model
- Hadronic weak interaction observable through flavor-changing decays, but
�SM: flavor-changing neutral currents GIM suppressed, unobservableݓ to see the hadronic neutral current, must study ΔS=0 ⇒�ݓ interactions
- NN, nuclear systems the only accessible possibilities
�must use PNC to filter out the effects of strong, E&M interactionsݓ�often modeled as a series of one-boson exchangesݓ
strong vertex⇔
π±, ρ, ω
Motivation Old Paradigm New Direction Summary S-P Amplitudes Meson-Exchange Model PV M–N Couplings Current Status
Predictions for /P Meson-Nucleon Couplings
⇥107 DDH Range Best DZ FCDH KMh1
� 0.0⇤+11.4 4.6 1.1 2.7 0.2h0
⇥ -30.8⇤+11.4 -11.4 -8.4 -3.8 -3.7h1
⇥ -0.4⇤+00.0 -0.2 0.4 -0.4 -0.1h2
⇥ -11.0⇤+-7.6 -9.5 -6.8 -6.8 -3.3h0
⇤ -10.3⇤+05.7 -1.9 -3.8 -4.9 -6.2h1
⇤ -1.9⇤+-0.8 -1.1 -2.3 -2.3 -1.0h⌅1⇥ 0.0 -2.2
M
B B’
M
B B’
B B’
M
(b) Quark Model
(c) Sum Rule
(a) Factorization
Calculations by DDH, DZ, FCDH are based on quark models, KM used thechiral soliton modelh⌅1⇥ term is usually ignored, so leaving 6 /P couplings to be checked by exps.
QCD sum rule calculations of h1� give 3⇥10�7 (HHK 98, formerly 2⇥10�8)
and 3.4⇥10�7 (Lobov 02)Lattice QCD calculations of h1
� (should be similar to g� but with a shorterrange) are proposed (e.g. Beane and Savage: matching PQQCD toPQChPT)
Cheng-Pang Liu Parity Violation in Few-Nucleon Systems
Haxton
- 6 (7) PV meson-nucleon couplings (π±, ρ, ω)1
- Estimate weak couplings (quark models, symmetries)⇒ ranges and “best values/guesses”
1Desplanques, Donoghue, Holstein (1980)24 / 44
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DDH potential
VDDH =ih1πgAM√
2Fπ
(~τ1 × ~τ2
2
)z
(~σ1 + ~σ2) ·[~p1 − ~p2
2M,wπ(r)
]− gρ
(h0ρ ~τ1 · ~τ2 + h1
ρ
(~τ1 + ~τ2
2
)z
+ h2ρ
3τ z1 τ
z2 − ~τ1 · ~τ2
2√
6
)×(
(~σ1 − ~σ2) ·{~p1 − ~p2
2M,wρ(r)
}+ · · ·
)+ · · ·
with- gM : strong (PC) meson-nucleon couplings- hi
M : weak (PV) meson-nucleon couplings
- wM(r) =exp(−mM r)
4πr
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Complications
- Connection to QCD?- Error estimates?- Consistency between different parts of calculations?
- Wave functions- Operators- External currents (e.m., weak)- PC and PV potentials (couplings, particle content,. . . )- 3N, 4N,. . . forces?
- “mesons” = “real” mesons? (1/Mρ ≈ 0.3 fm)
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Experimental constraints
-2 0 2 4 6 8 10 12 14f - 0.12 h 1 - 0.18 h 1
-5
0
5
10
15
20
25
30
-(h0+0.7h0 )
pp
p
133Cs
19F
205Tl
18F18F19F
pα
pp❊
DDH
best value
-2 0 2 4 6 8 10 12 14f - 0.12 h 1 - 0.18 h 1
-5
0
5
10
15
20
25
30-(h0+0.7h0 )
pp
p
133Cs
19F
205Tl
18F
-2 0 2 4 6 8 10 12 14f - 0.12 h 1 - 0.18 h 1
-5
0
5
10
15
20
25
30
-(h0+0.7h0 )
pp
p
133Cs
19F
205Tl
18F
Haxton, Holstein (2013)
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Re-analysis of pp scattering at 221 MeV- Use consistent strong couplings in PC and PV parts
!
-2 0 2 4 6 8 10 12 14
f - 0.12 h1- 0.18 h
1
-5
0
5
10
15
20
25
30
-(h0+0.7h0)
pp
p
133Cs
19F
205Tl
18F
18F19F
p!
pp
DDH
best value
-2 0 2 4 6 8 10 12 14
f - 0.12 h1- 0.18 h
1
-5
0
5
10
15
20
25
30-(h0+0.7h0)
pp
p
133Cs
19F
205Tl
18F
-2 0 2 4 6 8 10 12 14
f - 0.12 h1- 0.18 h
1
-5
0
5
10
15
20
25
30
-(h0+0.7h0)
pp
p
133Cs
19F
205Tl
18F
!
!80 !60 !40 !20
!40
!35
!30
!25
!20
0.7h!pp-h"pp (!107)
h!
pp+
0.7
h"
pp (!
10
7)
Haxton, Holstein (2013)
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Effective theories
Potential energy difference- High school:
∆U = mgh
- When does it fail? By how much?
- College:
∆U = −GMm(
1rf− 1
ri
)= −GM
Rm(
RR + h
− 1)
= mGMR2 h
RR + h
where ri = R, rf = R + h
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Effective theories
Potential energy difference- High school:
∆U = mgh
- When does it fail? By how much?- College:
∆U = −GMm(
1rf− 1
ri
)= −GM
Rm(
RR + h
− 1)
= mGMR2 h
RR + h
where ri = R, rf = R + h
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Effective theories
∆U = mgh(
1− hR
+h2
R2 + · · ·)
- mgh: lowest-order approximation- Valid for h� R (separation of scales)- Systematically improvable
Example of effective theory
Further examples:- Multipole expansion for confined charge distribution- Fermi theory of weak interactions2
- . . .
2Cow-cow scattering example: Gripaios [arXiv:1506.05039]31 / 44
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Effective field theories
- Low-energy theory for NN interactions- Effective degrees of freedom: nucleons, pion,. . .- Symmetry constraints
So what’s new?
- Connection to QCD through symmetries- Only relevant degrees of freedom, not more- Expansion in ratio of scales Q/Λ < 1: Power counting
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Power counting
Perturbation theory in QED- Coupling α� 1- Expand observables in α- Calculate order by order (Feynman graphs, etc)
Perturbation theory in EFT- Possibly strong coupling C ⇒ PT in C not possible- Identify ratio of scales
- Typical low-energy (long-distance) scale E- Underlying high-energy (short-distance) scale Λ
- Expand observables in ratio E/Λ
- Calculate order by order (Feynman graphs, etc)
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Advantages
- Model independent- Unified framework
- PC and PV potentials- External currents- 2N, 3N, 4N, . . .
- Systematically improvable- Theoretical error estimates
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Pionless EFT- At very low energy: pion-exchange not resolved:
1~q 2 + m2
π
≈ 1m2π
(1−
~q 2
m2π
+ · · ·)
- EFT with only nucleons as degrees of freedom: EFT(6π)- Contact interactions- Order by number of derivatives- Lowest-order parity-conserving Lagrangian (partial-wave
basis)
L =N†(i∂0 +~∇2
2M)N − 1
8C(1S0)
0 (NT τ2τaσ2N)†(NT τ2τaσ2N)
− 18C(3S1)
0 (NT τ2σ2σiN)†(NT τ2σ2σiN) + . . . ,
- Connect C(1S0)0 , C(3S1)
0 , etc to effective range expansion
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Parity violation in EFT(6π)
- Parity determined by orbital angular momentum L : (−1)L3
- Simplest parity-violating interaction: L→ L± 1- Leading order: S − P wave transitions
P S
- Spin, isospin: 5 different combinations
3Danilov (1965, ’71); Zhu et al. (2005); Phillips, MRS, Springer (2009); Girlanda (2008)36 / 44
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Lowest-order parity-violating LagrangianPartial wave basis4
LPV =−[C(3S1−1P1)
(NTσ2 ~στ2N
)†·(
NTσ2τ2i↔∇N
)+ C(1S0−3P0)
(∆I=0)
(NTσ2τ2~τN
)†(NTσ2 ~σ · i
↔∇τ2~τN
)+ C(1S0−3P0)
(∆I=1) ε3ab(
NTσ2τ2τaN)†(
NTσ2 ~σ ·↔∇τ2τ
bN)
+ C(1S0−3P0)(∆I=2) Iab
(NTσ2τ2τ
aN)†(
NTσ2 ~σ · i↔∇τ2τ
bN)
+ C(3S1−3P1) εijk(
NTσ2σiτ2N
)†(NTσ2σ
kτ2τ3↔∇
jN)]
+ h.c.
- Need 5 experimental results to determine LECs
4Phillips, MRS, Springer (2009)37 / 44
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Example: ~np → dγ
γθ
5
1Γ
dΓ
d cos θ= 1 + Aγ cos θ
Aγ =43
√2π
M32
κ1(1− γa1S0
) g(3S1−3P1)
5Savage (2001); MRS, Springer (2009)38 / 44
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Chiral EFT for NN interaction
- Degrees of freedom: nucleons and pions- Energy scales: E ≈ mπ < Λ ≈ 1 GeV- Symmetries: Galilei, C, (P), T, chiral (non-trivial)- Lowest-order PC potential:
V LOPC = − g2
A4F 2
(~σ1 · ~q)(~σ2 · ~q)
~q 2 + m2π
(~τ1 · ~τ2) + CS + CT (~σ1 · ~σ2)
- one-pion exchange- Contact terms (short-distance operators)- Low-energy constants CS,CT
- Systematic corrections possible- Higher powers of q = pf − pi- Two-pion exchange- . . .
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Chiral expansion of nuclear forces Chiral expansion of nuclear forces
26 rubin | frühjahr 12
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Zwei-Nukleon-Kraft
Führender Beitrag
Korrektur 1. Ordnung
Korrektur 2. Ordnung
Korrektur 3. Ordnung
Drei-Nukleon-Kraft Vier-Nukleon-KraftTwo-nucleon force Three-nucleon force Four-nucleon force
LO (Q0)
NLO (Q2)
N2LO (Q3)
N3LO (Q4)
(numbers from Pudliner et al. PRL 74 (95) 4396)
E. Epelbaum
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Chiral PV NN potential
Leading order:
V LOPV = −i
gAhπ2√
2F(~σ1 + ~σ2) · ~q~q 2 + m2
π
(~τ1 × ~τ2)z
- One-pion exchange ∝ hπ6
- LO contribution to ~np → dγ
Next-to-leading order- Contact terms- TPE ∝ hπ- New γπNN contact interaction
Caveat: power counting assumes that hπ is not “small”
6Savage, Springer (1998); Kaplan et al. (1999); Zhu et al. (2005); Liu (2007); Song etal. (2011), (2012)
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Translation between different formalisms
- DDH operator structure→ EFT(6π) at low energies- Can relate DDH and EFT couplings?- Problems
- Low-energy limit of PC potentials?- Regulator dependence in potential (µP): µ2
P4πr e−µP r
- Scale dependence in EFT couplings (µ)
Relation between couplings in DDH and EFT scale-dependent
hiDDH = f (µp, µ)hi
EFT
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PV on the lattice- Standard Model degrees of freedom (quarks, gluons,. . . )- Calculating reactions not yet realistic- Determine PV couplings- PV quark operators on lattice between 3-quark operators
(proton, neutron, etc)-
hπ =(
1.099± 0.505 (stat.) +0.058−0.064 (syst.)
)× 10−7
- mπ ∼ 389 MeV, L ∼ 2.5 fm, as ∼ 0.123 fm- Connected diagrams only7
- Consistent with most model estimates, lower end of DDH“reasonable range”
(a) (b) (c)
7Wasem (2012)43 / 44
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Bibliography
B. Desplanques, J. F. Donoghue and B. R. Holstein, AnnalsPhys. 124, 449 (1980)
E. G. Adelberger and W. C. Haxton, Ann. Rev. Nucl. Part.Sci. 35, 501 (1985)
S. L. Zhu, C. M. Maekawa, B. R. Holstein,M. J. Ramsey-Musolf and U. van Kolck, Nucl. Phys. A 748,435 (2005)
M. J. Ramsey-Musolf and S. A. Page, Ann. Rev. Nucl. Part.Sci. 56, 1 (2006)
W. C. Haxton and B. R. Holstein, Prog. Part. Nucl. Phys.71, 185 (2013)
M. R. Schindler and R. P. Springer, Prog. Part. Nucl. Phys.72, 1 (2013)
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Spin rotation
- Phase accumulated after traversing a target of thickness L
ϕ = Re(n − 1)kL
- Index of refraction
n − 1 =ρµ
k2M,
ρ: target density, µ: reduced mass,M: scattering amplitude- Phase
ϕ = ρLµ
kRe(M)
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Spin rotation
- Beam in z direction with +x polarization
|x+〉 =1√2
(|+〉+ |−〉)
- Helicity states |±〉 evolve with phase factor
1√2
(e−iφ+ |+〉+ e−iφ− |−〉
)=
1√2
e−iφ+
(|+〉+ ei(φ+−φ−)|−〉
)- For φ+ 6= φ−:
φPV = φ+ − φ−- Spin rotation angle per unit length L
1ρ
dφPV
dL=µ
kRe (M+ −M−) ,
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Anapole moment
Multipole expansion of charge and current operators- P and T conserving: charge, electric quadrupole, magnetic
dipole, . . .- P and T violating: electric dipole, magnetic quadrupole, . . .- P violating, T conserving: anapole moment, . . . 8
Current matrix element
〈N(p′)|Jµ|N(p)〉 = u(p′)[γµ F1(q2) + i
σµνqν2m
F2(q2)
+1
m2 (/qqµ − q2γµ)γ5 a(q2)
+ iσµνqν
2mγ5 d(q2)
]u(p)
8Zel’dovich (1958); Flambaum et al. (1980); Haxton et al. (2002)47 / 44
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Chiral Symmetry
- QCD Lagrangian
LQCD = q(i /D −M
)q − 1
4Gµν, aGµνa
- Project onto right- and left-handed fields
LQCD = (qR i /DqR+qL i /DqL−qRMqL−qLMqR)−14Gµν, aGµνa
- ForM = 0:
L0QCD = (qR i /DqR + qL i /DqL)− 1
4Gµν, aGµνa
- Invariant under qR → URqR,qL → ULqL
SU(2)L × SU(2)R × U(1)V symmetry
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Chiral Symmetry II
Spectrum:- SU(2) multiplets
- No parity doubling
- Pions very light
Spontaneous symmetry breaking to SU(2)VPions as Goldstone bosons
Explicit symmetry breaking by mu,d 6= 0- Treat mu,d as perturbation
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