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CP violation Lecture 2. N. Tuning. s. b. b. s. Matter Dominates !. Recap:. CP-violation (or flavour physics) is about charged current interactions. Interesting because: Standard Model: in the heart of quark interactions

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cp violation lecture 2

CP violationLecture 2

N. Tuning

Niels Tuning (1)

recap

s

b

b

s

Matter Dominates !

Recap:
  • CP-violation (or flavour physics) is about charged current interactions
  • Interesting because:
    • Standard Model: in the heart of quark interactions
    • Cosmology: related to matter – anti-matter asymetry
    • Beyond Standard Model: measurements are sensitive to new particles

Niels Tuning (3)

slide4

Recap

uI

u

W

W

d,s,b

dI

  • Diagonalize Yukawa matrix Yij
    • Mass terms
    • Quarks rotate
    • Off diagonal terms in charged current couplings

Niels Tuning (4)

ok we ve got the ckm matrix now what
Ok…. We’ve got the CKM matrix, now what?

It’s unitary

“probabilities add up to 1”:

d’=0.97 d + 0.22 s + 0.003 b (0.972+0.222+0.0032=1)

How many free parameters?

How many real/complex?

How do we normally visualize these parameters?

Niels Tuning (5)

quark field re phasing
Quark field re-phasing

Under a quark phase transformation:

and a simultaneous rephasing of the CKM matrix:

or

In other words:

Niels Tuning (6)

quark field re phasing1

2 generations:

No CP violation in SM!

This is the reason Kobayashi and Maskawa first suggested a 3rd family of fermions!

Quark field re-phasing

Under a quark phase transformation:

and a simultaneous rephasing of the CKM matrix:

or

the charged current

is left invariant.

Degrees of freedom in VCKM in 3 N generations

Number of real parameters: 9+ N2

Number of imaginary parameters: 9 + N2

Number of constraints (VV† = 1): -9- N2

Number of relative quark phases: -5- (2N-1)

-----------------------

Total degrees of freedom: 4(N-1)2

Number of Euler angles: 3N (N-1) / 2

Number of CP phases: 1 (N-1) (N-2) / 2

Niels Tuning (7)

timeline
Timeline:
  • Timeline:
    • Sep 1972: Kobayashi & Maskawa predict 3 generations
    • Nov 1974: Richter, Ting discover J/ψ: fill 2nd generation
    • July 1977: Ledermann discovers Υ: discovery of 3rd generation

Niels Tuning (9)

quark field re phasing2

2 generations:

No CP violation in SM!

This is the reason Kobayashi and Maskawa first suggested a 3rd family of fermions!

Quark field re-phasing

Under a quark phase transformation:

and a simultaneous rephasing of the CKM matrix:

or

the charged current

is left invariant.

Degrees of freedom in VCKM in 3 N generations

Number of real parameters: 9+ N2

Number of imaginary parameters: 9 + N2

Number of constraints (VV† = 1): -9- N2

Number of relative quark phases: -5- (2N-1)

-----------------------

Total degrees of freedom: 4(N-1)2

Number of Euler angles: 3N (N-1) / 2

Number of CP phases: 1 (N-1) (N-2) / 2

Niels Tuning (10)

cabibbos theory successfully correlated many decay rates
Cabibbos theory successfully correlated many decay rates

Cabibbos theory successfully correlated many decay rates by counting the number of cosqc and sinqc terms in their decay diagram

Niels Tuning (11)

cabibbos theory successfully correlated many decay rates1
Cabibbos theory successfully correlated many decay rates

There was however one major exception which Cabibbo could not describe: K0 m+m-

Observed rate much lower than expected from Cabibbos ratecorrelations (expected rate  g8sin2qccos2qc)

s

d

cosqc

sinqc

u

W

W

nm

m-

m+

Niels Tuning (12)

the cabibbo gim mechanism
The Cabibbo-GIM mechanism

Solution to K0 decay problem in 1970 by Glashow, Iliopoulos and Maiani  postulate existence of 4th quark

Two ‘up-type’ quarks decay into rotated ‘down-type’ states

Appealing symmetry between generations

u

c

W+

W+

d’=cos(qc)d+sin(qc)s

s’=-sin(qc)d+cos(qc)s

Niels Tuning (13)

the cabibbo gim mechanism1
The Cabibbo-GIM mechanism

How does it solve the K0 m+m- problem?

Second decay amplitude added that is almost identical to original one, but has relative minus sign Almost fully destructive interference

Cancellation not perfect because u, c mass different

s

d

s

d

-sinqc

cosqc

cosqc

+sinqc

c

u

nm

nm

m-

m+

m-

m+

Niels Tuning (14)

from 2 to 3 generations
From 2 to 3 generations

2 generations: d’=0.97 d + 0.22 s (θc=13o)

3 generations: d’=0.97 d + 0.22 s + 0.003 b

NB: probabilities have to add up to 1: 0.972+0.222+0.0032=1

 “Unitarity” !

Niels Tuning (15)

from 2 to 3 generations1
From 2 to 3 generations
  • 2 generations: d’=0.97 d + 0.22 s (θc=13o)
  • 3 generations: d’=0.97 d + 0.22 s + 0.003 b
  • Parameterization used by Particle Data Group (3 Euler angles, 1 phase):
possible forms of 3 generation mixing matrix
Possible forms of 3 generation mixing matrix
  • ‘General’ 4-parameter form (Particle Data Group) with three rotations q12,q13,q23 and one complex phase d13
    • c12 = cos(q12), s12 = sin(q12) etc…
  • Another form (Kobayashi & Maskawa’s original)
    • Different but equivalent
  • Physics is independent of choice of parameterization!
    • But for any choice there will be complex-valued elements

Niels Tuning (17)

possible forms of 3 generation mixing matrix1
Possible forms of 3 generation mixing matrix

 Different parametrizations! It’s about phase differences!

KM

Re-phasing V:

PDG

3 parameters: θ, τ, σ

1 phase: φ

Niels Tuning (18)

how do you measure those numbers
How do you measure those numbers?
  • Magnitudes are typically determined from ratio of decay rates
  • Example 1 – Measurement of Vud
    • Compare decay rates of neutrondecay and muon decay
    • Ratio proportional to Vud2
    • |Vud| = 0.97425 ± 0.00022
    • Vud of order 1

Niels Tuning (19)

how do you measure those numbers1
How do you measure those numbers?
  • Example 2 – Measurement of Vus
    • Compare decay rates of semileptonic K- decay and muon decay
    • Ratio proportional to Vus2
    • |Vus| = 0.2252 ± 0.0009
    • Vus sin(qc)
how do you measure those numbers2
How do you measure those numbers?
  • Example 3 – Measurement of Vcb
    • Compare decay rates of B0 D*-l+n and muon decay
    • Ratio proportional to Vcb2
    • |Vcb| = 0.0406 ± 0.0013
    • Vcb is of order sin(qc)2 [= 0.0484]
how do you measure those numbers3
How do you measure those numbers?
  • Example 4 – Measurement of Vub
    • Compare decay rates of B0 D*-l+n and B0 p-l+n
    • Ratio proportional to (Vub/Vcb)2
    • |Vub/Vcb| = 0.090 ± 0.025
    • Vub is of order sin(qc)3 [= 0.01]
how do you measure those numbers4
How do you measure those numbers?
  • Example 5 – Measurement of Vcd
    • Measure charm in DIS with neutrinos
    • Rate proportional to Vcd2
    • |Vcd| = 0.230 ± 0.011
    • Vcb is of order sin(qc)[= 0.23]
how do you measure those numbers5
How do you measure those numbers?
  • Example 6 – Measurement of Vtb
    • Very recent measurement: March ’09!
    • Single top production at Tevatron
    • CDF+D0: |Vtb| = 0.88 ± 0.07
how do you measure those numbers6

Vts

Vts

Vts

 = 1.210 +0.047 from lattice QCD

-0.035

Vts

How do you measure those numbers?
  • Example 7 – Measurement of Vtd, Vts
    • Cannot be measured from top-decay…
    • Indirect from loop diagram
    • Vts: recent measurement: March ’06
    • |Vtd| = 0.0084 ± 0.0006
    • |Vts| = 0.0387 ± 0.0021

Ratio of frequencies for B0 and Bs

Vts ~ 2

Vtd ~3 Δms ~ (1/λ2)Δmd ~ 25 Δmd

what do we know about the ckm matrix
What do we know about the CKM matrix?
  • Magnitudes of elements have been measured over time
    • Result of a large number of measurements and calculations

Magnitude of elements shown only, no information of phase

Niels Tuning (26)

what do we know about the ckm matrix1
What do we know about the CKM matrix?

Magnitudes of elements have been measured over time

Result of a large number of measurements and calculations

Magnitude of elements shown only, no information of phase

Niels Tuning (27)

approximately diagonal form

d

s

b

u

c

t

Approximately diagonal form
  • Values are strongly ranked:
    • Transition within generation favored
    • Transition from 1st to 2nd generation suppressed by cos(qc)
    • Transition from 2nd to 3rd generation suppressed bu cos2(qc)
    • Transition from 1st to 3rd generation suppressed by cos3(qc)

CKM magnitudes

Why the ranking?We don’t know (yet)!

If you figure this out,you will win the nobelprize

l

l3

l

l2

l3

l2

l=sin(qc)=0.23

Niels Tuning (28)

intermezzo how about the leptons
Intermezzo: How about the leptons?
  • We now know that neutrinos also have flavour oscillations
  • thus there is the equivalent of a CKM matrix for them:
    • Pontecorvo-Maki-Nakagawa-Sakata matrix
  • a completely different hierarchy!

vs

Niels Tuning (29)

wolfenstein parameterization
Wolfenstein parameterization

3 real parameters: A, λ, ρ

1 imaginary parameter: η

wolfenstein parameterization1
Wolfenstein parameterization

3 real parameters: A, λ, ρ

1 imaginary parameter: η

exploit apparent ranking for a convenient parameterization
Exploit apparent ranking for a convenient parameterization
  • Given current experimental precision on CKM element values, we usually drop l4 and l5 terms as well
    • Effect of order 0.2%...
  • Deviation of ranking of 1st and 2nd generation (l vs l2) parameterized in A parameter
  • Deviation of ranking between 1st and 3rd generation, parameterized through |r-ih|
  • Complex phase parameterized in arg(r-ih)

Niels Tuning (32)

1995 what do we know about a and
~1995 What do we know about A, λ, ρ and η?
  • Fit all known Vij values to Wolfenstein parameterization and extract A, λ, ρ and η
  • Results for A and l most precise (but don’t tell us much about CPV)
    • A = 0.83, l = 0.227
  • Results for r,h are usually shown in complex plane of r-ih for easier interpretation

Niels Tuning (33)

deriving the triangle interpretation
Deriving the triangle interpretation
  • Starting point: the 9 unitarity constraints on the CKM matrix
  • Pick (arbitrarily) orthogonality condition with (i,j)=(3,1)

Niels Tuning (34)

deriving the triangle interpretation1
Deriving the triangle interpretation

Starting point: the 9 unitarity constraints on the CKM matrix

3 orthogonality relations

Pick (arbitrarily) orthogonality condition with (i,j)=(3,1)

Niels Tuning (35)

deriving the triangle interpretation2
Deriving the triangle interpretation

Starting point: the 9 unitarity constraints on the CKM matrix

Pick (arbitrarily) orthogonality condition with (i,j)=(3,1)

Niels Tuning (36)

visualizing the unitarity constraint
Visualizing the unitarity constraint
  • Sum of three complex vectors is zero  Form triangle when put head to tail

(Wolfenstein params to order l4)

Niels Tuning (37)

visualizing the unitarity constraint1
Visualizing the unitarity constraint
  • Phase of ‘base’ is zero  Aligns with ‘real’ axis,

Niels Tuning (38)

visualizing the unitarity constraint2
Visualizing the unitarity constraint
  • Divide all sides by length of base
  • Constructed a triangle with apex (r,h)

(r,h)

(0,0)

(1,0)

Niels Tuning (39)

visualizing arg v ub and arg v td in the r h plane
Visualizing arg(Vub) and arg(Vtd) in the (r,h) plane
  • We can now put this triangle in the (r,h) plane

Niels Tuning (40)

the unitarity triangle
“The” Unitarity triangle
  • We can visualize the CKM-constraints in (r,h) plane
slide42
β
  • We can correlate the angles βandγto CKM elements:
deriving the triangle interpretation3
Deriving the triangle interpretation

Another 3 orthogonality relations

Pick (arbitrarily) orthogonality condition with (i,j)=(3,1)

Niels Tuning (43)

the other unitarity triangle
The “other” Unitarity triangle
  • Two of the six unitarity triangles have equal sides in O(λ)
  • NB: angle βs introduced. But… not phase invariant definition!?

Niels Tuning (44)

the b s triangle s
The “Bs-triangle”: βs
  • Replace d by s:

Niels Tuning (45)

the ckm matrix

W-

b

gVub

u

The CKM matrix
  • Couplings of the charged current:
  • Wolfensteinparametrization:
  • Magnitude:
  • Complex phases:

Niels Tuning (47)

back to finding new measurements

g

b

Back to finding new measurements
  • Next order of business: Devise an experiment that measures arg(Vtd)b and arg(Vub)g.
    • What will such a measurement look like in the (r,h) plane?

Fictitious measurement of b consistent with CKM model

CKM phases

Niels Tuning (48)

consistency with other measurements in r h plane
Consistency with other measurements in (r,h) plane

Precise measurement ofsin(2β) agrees perfectlywith other measurementsand CKM model assumptionsThe CKM model of CP violation experimentallyconfirmed with high precision!

Niels Tuning (49)

what s going on
What’s going on??
  • ??? Edward Witten, 17 Feb 2009…
  • See “From F-Theory GUT’s to the LHC” by Heckman and Vafa (arXiv:0809.3452)