standard model of particle physics...schöning/rodejohann 4 standard model of particle physics ss...
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Schöning/Rodejohann 1 Standard Model of Particle Physics SS 2013
Lecture:
Standard Model of Particle Physics
Heidelberg SS 2013
Flavour Physics I + II
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Schöning/Rodejohann 2 Standard Model of Particle Physics SS 2013
ContentsPART I
Determination of the CKM Matrix
CP Violation in Kaon system
CP violation in the B-system
PART II
Search for Flavor Violating Neutral Currents (Lepton Flavor Violation)
Search for Lepton/Baryon Number Violation
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Schöning/Rodejohann 3 Standard Model of Particle Physics SS 2013
CKM Matrix
Definition:
Experimental values:
no theory prediction!
(Particle Data Group 2012)
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Schöning/Rodejohann 4 Standard Model of Particle Physics SS 2013
CKM MatrixStandard Parameterisation (Euler Angles):
Unitary matrix has N x N parameters: 3 families → 9 parameters2 x N -1 trivial phases: → 5 phasesN x (N-1) / 2 rotation angles → 3 anglesN x N - N x (N-1)/ 2 - (2 x N -1) = N x (N-3)/2 +1 → 1 CPV phase
need 3 families for generating CP-violation!
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Schöning/Rodejohann 5 Standard Model of Particle Physics SS 2013
CKM MatrixStandard Parameterisation (Euler Angles):
Experimental values:
no theory prediction!
(Particle Data Group 2012)
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Schöning/Rodejohann 6 Standard Model of Particle Physics SS 2013
CKM MatrixWolfenstein Parameterisation:
note that definition with η and ρ depends on phase convention, η and ρ does not
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Schöning/Rodejohann 7 Standard Model of Particle Physics SS 2013
CKM MatrixWolfenstein Parameterisation:
Experimental values: no theory prediction!
note that definition with η and ρ depends on phase convention, η and ρ does not
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Schöning/Rodejohann 8 Standard Model of Particle Physics SS 2013
Experimental Determination of CKM Matrix Elements
Vus
:
K- → μ- ν
π- → μ- ν
s → u
d → u=
s μ-
u νform-factor
theory uncertainties due to Kaon/Pion formfactors mostly cancel
Tau decay:
Kaon decay:
Vus
:
ν
τ-
s
u
s
u
s
u
τ → ν K Xform-factor
→ fK /f
π = 1.189 ± 0.007
|Vus
| = 0.2252 ± 0.0009.
|Vus
| = 0.2208 ± 0.0039 LEP, Barbar, Belle combined:
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Schöning/Rodejohann 9 Standard Model of Particle Physics SS 2013
D0 - DecaysV
cd:
D0 → K- lν
D0 → π- lν
c → s
c → d=
l-
ν
D-meson decay:u
c
|Vcd
| = 0.229 ± 0.006 ± 0.024
s d
u
,
from CLEOcarXiv 0906.2983
CLEOc + Belle combined:
Also hadronic decays analysed:
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Schöning/Rodejohann 10 Standard Model of Particle Physics SS 2013
Neutrino Scattering
d
ν
Vcd
: from neutrino (antineutrino) scattering
μ-
u
d
ν μ-
c
Vcd
d
μ+
W
WW+
ν
two muons
one muons
|Vcd
| = 0.230 ± 0.011.
from CDHS, CCFR, CHARM II
and CHORUS experiments:
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Schöning/Rodejohann 11 Standard Model of Particle Physics SS 2013
Vcs
:s μ-
c ν
from DS decays
s
|Vcs
| = 1.006 ± 0.023
DS - Decays
DS → lν
l-
ν
u
c s d
u
,D0 → K- lν
combined CLEOc, Belle, Babar:
Vcs
: from D0 decays
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Schöning/Rodejohann 12 Standard Model of Particle Physics SS 2013
B and Top Decays
inclusive and exclusive B decays
Determination of Vub
and Vcb
from B-decays
Vub
: B → Xu lν
Vcb
:
|Vub
| = (4.15 ± 0.49) × 10−3
|Vcb
| = (40.9 ± 1.1) × 10−3 .
Vtd:
Vts:
Both difficult to determine from top decays
with high precision → instead use trick
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Schöning/Rodejohann 13 Standard Model of Particle Physics SS 2013
B and BS oscillations
W-
W+
b
d
t t
d
b
b
s
t t
s
b
testing Vtd
testing Vts
B0 – B0 oscillations
BS – B
S oscillations
W W
b
dt
td
b
W-
W+
W W
b
st
ts
btesting V
ts
testing Vtd
|Vtd | = (8.4 ± 0.6) × 10−3 , |V
ts | = (42.9 ± 2.6) × 10−3
by measuring time dependence of oscillations:
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Schöning/Rodejohann 14 Standard Model of Particle Physics SS 2013
ResultFitting the four free parameters to the experimental results yields (global fit):
Representation using the Wolfenstein parameterisation (only 4 parameters!)
As η≠ 0 (ñ≠ 0) the CKM matrix violates CP-invariance!
However, CP-violation is too small to explain observed matter-antimatter asymmetryin universe
∣V 12∣≈∣V 21∣≈λ
∣V 23∣≈∣V 32∣≈λ2
∣V 13∣≈∣V 31∣≈λ3
(mystery!)
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Schöning/Rodejohann 15 Standard Model of Particle Physics SS 2013
CP Violation and the Consequences
Direct CP-Violation: different partial decay widths for particles and antiparticles
b
b
c
l-
ν
c
d
u
W-
W+
γ
b
b
c
l+
c
u
d
ν
W-
W+
γ
If CP-violated, the above final states do not occur with same rate!
CPV can explain observed baryon asymmetry in universe if in addition
baryon-number violating process exists
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Schöning/Rodejohann 16 Standard Model of Particle Physics SS 2013
CP violation in the Kaon systemfirst discovered here!
W-
W+
s
d
u,c,t u,c,t
d
s
K0 – K0 oscillations
W W
s
d
d
su,c,t
u,c,t
Transition Amplitude:
(V ud∗)2(V us)
2 f (mu) + (V cd∗)2(V cs)
2 f (mc)+ (V td∗)2(V ts)
2 f (mt)
CKM elements of anti-fermions are complex conjugated
if δ13
=0 (Vtd), then CP is conserved: ⟨K 0∣T∣K 0
⟩ = ⟨ K 0∣T∣K 0⟩
if δ13
<> 0 (Vtd), then CP is violated: ⟨K 0∣T∣K 0
⟩ ≠ ⟨ K 0∣T∣K 0⟩
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Schöning/Rodejohann 17 Standard Model of Particle Physics SS 2013
Kaon Physics(reminder)
Quark-Model: K0 = d s K0 = d sBoth states can be experimentally distinguished.
Different cross sections with matter (strong interactions):
K 0 p → K 0 p , K + n
K 0 p → K 0 p , Λπ+
Weak Interactions (oscillations):
∣K 1 ⟩ = 1
√2(∣K 0 ⟩ + ∣K 0 ⟩)
Define CP invariant (hypothetical) states:
∣K 2 ⟩ = 1
√2(∣K 0 ⟩ − ∣K 0 ⟩)
CP∣K 1 ⟩ =−∣K1 ⟩
CP∣K 2 ⟩ =+∣K 2 ⟩
Physical States:
K L0→ πππ CP= -1 ∣K L ⟩ ≈∣K 1 ⟩
K S0→ π π CP= +1 ∣K S ⟩ ≈∣K 2 ⟩
τ(K L0)=5⋅10−8 s
τ(K S0)=0.9⋅10−10 s
Δ M=M L−M S≈ O(10−12MeV ) very small mass difference!
large cross section
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Schöning/Rodejohann 18 Standard Model of Particle Physics SS 2013
K0 OscillationsKaons at rest:
∣K L(t )⟩ =∣K L(0) ⟩ e−i M Lt e−ΓL t /2
∣K S(t )⟩ =∣K S(0)⟩ e−i M S t e−ΓS t /2
oscillation decay
Hamilton operator: H=i ∂∂t → eigenvalues:
H = (M S−i2ΓS 0
0 M L−i2ΓL)
A (t ) = ⟨ K 0(t )∣K 0(0) ⟩ = 14
⟨K L(t )−K S(t )∣K L(0)+ K S(0)⟩
Oscillations:
P(t )=A∗(t ) A (t ) = 1
4(e−ΓL t + e−ΓS t − 2cos(Δ M t ) e−1/2(ΓL+ ΓS)t )
with
Δ M=M L−M S
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Schöning/Rodejohann 19 Standard Model of Particle Physics SS 2013
Kaon Oscillations and Regeneration
50% KS and K
L
100% KL
(1/2)2
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Schöning/Rodejohann 20 Standard Model of Particle Physics SS 2013
Discovery of CP Violation
BR(K L → π+π−) = 0.2⋅10−3
Question: CP violation in KL decay or in mixing?
Christensen at al. (1964)
(Nobel Prize Cronin and Fitch 1980)
very small CP-violating effects in Kaon system
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Schöning/Rodejohann 21 Standard Model of Particle Physics SS 2013
How to measure CP violation?
Need to measure all CKM matrix elements:
CKM: V td = A λ3(1−ρ−iη) (Wolfenstein parameterisation)
Example top decay: t → d W (e.g. LHC, difficult!)
B(t → dW ) ∝ ∣V td2∣= A2 λ6 [(1−ρ)2+ η2] but complex phase not visible!
Complex phase can only be measured in interference processes:
Three possibilities: direct CP Violation
CP violation in mixing
interference between decays with and without mixing
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Schöning/Rodejohann 22 Standard Model of Particle Physics SS 2013
CP transformationConsider CP violating (weak) process i → f:
i f i fCP∣ai ⟩ = e+ iϕi ∣ai ⟩
CP∣a f ⟩ = e+ iϕf ∣a f ⟩
transition amplitudes:A f = ⟨af∣O∣ai ⟩ A f = ⟨ a f∣O∣ai⟩
it follows if A f = e+ i(ϕf−ϕi) A f[O ,CP]=0
weak weak
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Schöning/Rodejohann 23 Standard Model of Particle Physics SS 2013
CP transformationConsider CP violating (weak) process i → f:
i f i fCP∣ai ⟩ = e+ iϕi ∣ai ⟩
CP∣a f ⟩ = e+ iϕf ∣a f ⟩
transition amplitudes:A f = ⟨af∣O∣ai ⟩ A f = ⟨ a f∣O∣ai⟩
it follows if A f = e+ i(ϕf−ϕi) A f[O ,CP]=0
If quarks involved, there is an additional QCD phase shift:
i f i fs s
weak weak
weakweakQCD QCD
A f =∣n∣ e+i(θ+ϕi) A f =∣n∣ e+ i(θ−ϕi)
strong interaction (strong phase shift θ) is CP invariant!
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Schöning/Rodejohann 24 Standard Model of Particle Physics SS 2013
I. Direct CP violationDefinition
i f
∣A f /A f∣≠1
not possible with single process as |exp(ix)|=1 (see previous page)
Superposition of two processes:
s1
s2
like a classical double slit experiment
A f =∣n1∣ e+ i(θ1−ϕ1) + ∣n2∣ e
+ i(θ2−ϕ2)
A f =∣n1∣ e+ i(θ1+ ϕ1) + ∣n2∣ e
+ i(θ2+ ϕ2)
∣A f /A f∣≠1
∣A f /A f∣≠1 if ϕ1≠ϕ2 and θ1≠θ2
∣A f2∣= n1
2+ n2
2+ 2∣n1∣∣n2∣ cos((θ1−θ2)+ (ϕ1−ϕ2))
∣A f2∣= n1
2+ n2
2+ 2∣n1∣∣n2∣ cos((θ1−θ2)−(ϕ1−ϕ2))
i f
s1
s2
--
-
-
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Schöning/Rodejohann 25 Standard Model of Particle Physics SS 2013
I. Direct CP violationDefinition
i f
∣A f /A f∣≠1
not possible with single process as |exp(ix)|=1 (see previous page)
Superposition of two processes:
s
s
like a classical double slit experiment
A f =∣n1∣ e+ i(θ1−ϕ1) + ∣n2∣ e
+ i(θ2−ϕ2)
A f =∣n1∣ e+ i(θ1+ ϕ1) + ∣n2∣ e
+ i(θ2+ ϕ2)
∣A f /A f∣≠1
∣A f /A f∣≠1 if ϕ1≠ϕ2 and θ1≠θ2
Can be measured in decays of charged and neutral particles!
example: δL =Γ(K L→ l+ νlπ
−)− Γ(K L→ l− νlπ
+)
Γ(K L→ l+ νlπ− ) + Γ(K L→ l− νlπ
+ )
∣A f2∣= n1
2+ n2
2+ 2∣n1∣∣n2∣ cos((θ1−θ2)+ (ϕ1−ϕ2))
∣A f2∣= n1
2+ n2
2+ 2∣n1∣∣n2∣ cos((θ1−θ2)−(ϕ1−ϕ2))
δL = (3.32±0.06)×10−3
(experiment)
Note: total decay width is not affect by CP violation (would violate CPT)
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Schöning/Rodejohann 26 Standard Model of Particle Physics SS 2013
Example KL Decays
l+
ν
d
s u
π-
W+
K0
∣K L ⟩ ≈ 1
√2(∣K 0 ⟩ + ∣K 0 ⟩)
l+
ν
d
s u
π-W-
K0
different weak and QCD phases!
t
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Schöning/Rodejohann 27 Standard Model of Particle Physics SS 2013
Direct CP Violation in Charged Meson Decay
b s
ρ0B-
W-
B− →K − ρ0
u
u
uK-
V*ub
Vus
bs
ρ0
B-
W-
u
u
u
K- V*tb
Vts
different weak and QCD phases!huge asymetry!
t
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Schöning/Rodejohann 28 Standard Model of Particle Physics SS 2013
II. CP violation in mixing oscillations of neutral mesons measure time dependent decay width
Aosc =d Γ/dt (M 0
→ l + X ) − d Γ/dt (M 0→ l− X )
d Γ/dt (M 0→ l + X ) + d Γ/dt (M 0→ l− X )
time dependent charge asymmetryδC=Aosc
K 0− K 0 oscillations
K → l± νlπ∓
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Schöning/Rodejohann 29 Standard Model of Particle Physics SS 2013
III. Interference Decay + Mixing
B0 f
B0
interference between decay withoutmixing and decay with mixing
oscillation
AΓ =Γ(B0
(t )→ f ) − Γ(B0(t )→ f )
Γ(B0(t )→ f ) + Γ(B0(t )→ f )
neutral final state
Note, in Kaon system all three kinds of CP violating effects were discovered!
It took about 40 years of measurements and theory to fully understand this subject!
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Schöning/Rodejohann 30 Standard Model of Particle Physics SS 2013
Quantitative Description of KL state
∣K L ⟩ = 1
√2+ 2∣ϵ2∣(∣(1+ ϵ)K 0 ⟩ + ∣(1−ϵ) K 0 ⟩)
assume that KL is not a pure K
1 state:
ε describes CP odd admixture
∣K L ⟩ = 1
√1+∣ϵ2∣(∣K 1 ⟩ + ∣ϵK 2 ⟩)
∣K S ⟩ = 1
√1+∣ϵ2∣(∣ϵK 1 ⟩ + ∣K 2 ⟩)
pure CP eigenstates
mixing causes oscillations which aretime dependent affects in contrast todirect CP violation
Decompose into mixing and direct CP violation effect
η± =⟨π
+π
−∣T∣K L⟩
⟨π + π−∣T∣K S⟩= ϵ + ϵ ´ ϵ ´ =
⟨π+π
−∣T∣K 1⟩
⟨π + π−∣T∣K 2⟩
mixing direct
with
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Schöning/Rodejohann 31 Standard Model of Particle Physics SS 2013
KS and K
L Interference
Experimental Result:
η± = (2.333±0.010)⋅10−3
η± ≈ ϵ
CP violation mainly due to mixing!
What about ε´ ?
δC=Aosc
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Schöning/Rodejohann 32 Standard Model of Particle Physics SS 2013
KS and K
L Interference
Experimental Result:
η± = (2.333±0.010)⋅10−3
η± ≈ ϵ
CP violation mainly due to mixing! consistent with type II CP violation
result of
What about ε´ ?
δC=Aosc
time dependent charge asymmetry
K 0− K 0 oscillations
δC=2ℜ(ϵ) = (3.33±0.14)⋅10−3
K → l± νlπ∓
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Schöning/Rodejohann 33 Standard Model of Particle Physics SS 2013
Direct CP Violation in K → ππ DecaysWhat about ε´ ?
Idea: mixing effects are in the K
0 - anti-K
0 system
direct CP violation is decay specific look into different decays!
η 00 = ϵ+⟨π
0π
0∣T∣K L⟩
⟨π0π0∣T∣K S⟩= ϵ − 2ϵ´
note different sign and factor
By measuring Kaon decays into charged and neutral pions with
high precision ε´ can be measured:
ℜ(ϵ´ /ϵ) = (33±11)×10−4 (1988)
ℜ(ϵ´ /ϵ) = (16.7±2.6)×10−4 (2000)
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Schöning/Rodejohann 34 Standard Model of Particle Physics SS 2013
Summary Kaon Physics Decay K → l± νlπ
∓
direct CP violation discovered
δL =Γ(K L→ l + νlπ
−)− Γ(K L→ l− νlπ
+)
Γ(K L→ l + νlπ−)+ Γ(K L→ l− νlπ
+ )
δL = (3.32±0.06)×10−3(experiment)
Decay K →π + π− ,π 0 π 0CP violation in mixing
and CP violation in mixing
K → l± νlπ∓
∣ϵ∣= (2.228±0.011)⋅10−3
and tiny direct CP violation
ℜ(ϵ´ /ϵ) = (16.7±2.6)×10−4
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Schöning/Rodejohann 35 Standard Model of Particle Physics SS 2013
Unitarity Triangleone of six possible unitarity triangles
define angles α, β, γ
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Schöning/Rodejohann 36 Standard Model of Particle Physics SS 2013
Kaon ConstraintsRelation between CP violating ε parameter and CKM matrix elements:
S is Inami-Lim function
leads to bands (hyperbola) in η-ρ plane:
next slide
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Schöning/Rodejohann 37 Standard Model of Particle Physics SS 2013
Summary of experimental Results
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Schöning/Rodejohann 38 Standard Model of Particle Physics SS 2013
Babar Detector
PEP-C Accelerator, Stanford
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Schöning/Rodejohann 39 Standard Model of Particle Physics SS 2013
Belle DetectorKEK, Japan
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Schöning/Rodejohann 40 Standard Model of Particle Physics SS 2013
B-Oscillations at B-factories
Exploit different beam energies: E(e−)> E (e+
)
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Schöning/Rodejohann 41 Standard Model of Particle Physics SS 2013
Classification of B-decays
interfering diagrams
always two identical flavours
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Schöning/Rodejohann 42 Standard Model of Particle Physics SS 2013
sin 2β clearly non zero!
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Schöning/Rodejohann 43 Standard Model of Particle Physics SS 2013
Summary of experimental Results
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Schöning/Rodejohann 44 Standard Model of Particle Physics SS 2013
B-Mixing Formalism
slightly different convention c.t. the more historic Kaon conventions
Linear combination of low and high mass eigenstate
Oscillations:
(∣M0(t) ⟩
∣M 0(t) ⟩ ) = (M 11−iΓ1/2 M 12
M 21 M 22−iΓ2/2 )⋅ (∣M0(0)⟩
∣M 0(0)⟩ )
both have been measured for B0 and Bs
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Schöning/Rodejohann 45 Standard Model of Particle Physics SS 2013
Classification of CP ViolationI. Direct CP-violation
∣A f / A f∣≠1
II. CP-violation in mixing
∣q / p∣≠1
III. CP-violation in decay with and without mixing
ℑ(λf )=∣q A f
p A f∣≠0
CP-eigenstateasymmetry often called S
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Schöning/Rodejohann 46 Standard Model of Particle Physics SS 2013
CP Violation in B → J/ψ K
CP violating effect in B-sector is much larger than in K-sector!
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Schöning/Rodejohann 47 Standard Model of Particle Physics SS 2013
Correlation “Direct versus Mixing”
large CP violation effectsin B-meson decays
small CP violation in mixing
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Schöning/Rodejohann 48 Standard Model of Particle Physics SS 2013
Summary B-Asymmetry Parameters
I. Direct CP-violation is large
II. CP-violation in mixing is very small!
III. CP-violation in decay with and without mixing
Sensitive to new BSM physics!
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Schöning/Rodejohann 49 Standard Model of Particle Physics SS 2013
Summary of experimental Results
All measurements very consistent! No sign of non-CKM CP violation
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Schöning/Rodejohann 50 Standard Model of Particle Physics SS 2013
Summary
The CKM Matrix elements are determined from aglobal fit to precision measurements
The CKM matrix is tested to be unitary and has anon-zero CP violating phase
CP violation can be measured in particle decays if atleast two diagrams with different strong and weakphases interfere
CP violation shows up in decays and mixing (oscillations)
In Kaon system CP violation in mixing dominates
In B-system CP violation in direct decays dominates
CP violation in hadron decays explained by CKM matrix
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Schöning/Rodejohann 51 Standard Model of Particle Physics SS 2013