seeking new physics with rare kaon decays 50 10...new physics not found at lhc precision...
TRANSCRIPT
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Seeking New Physics with Rare Kaon Decays(with a little help from a friend)
"Excellent!" [Watson] cried.
Douglas Bryman
University of British Columbia
"Elementary," said [Holmes].
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Standard Model : A great story …
but not likely the whole story…
Standard Model : A great story …
but not likely the whole story…
• Cosmological issues: inflation, dark matter,
dark energy, matter anti-matter asymmetry…
• Theoretical issues: gravity, neutrino mass,
11/9/2010 BNL 90-50-10 Celebration 2
• Theoretical issues: gravity, neutrino mass,
flavor problem, hierarchy problem,
divergences .…
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Tevatron LHC; TeV Energy Scale→
New Physics
3
COSMOLOGICAL
EVOLUTION, BBN
NEUTRINO PHYSICSLEPTOGENESIS?
Rare Decays and CP violation
Symmetry Violation
High Mass High Mass
Scales?Scales?
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The Flavor Puzzle
u c t
d s b
e µ τ
νe νµ ντ
Quarks Leptons
• Fermion weak states � mass states
11/9/2010 BNL 90-50-10 Celebration 4
• Fermion weak states � mass states• Quark, lepton flavors not conserved• Three flavors �CP violation, …BAU,…
Unexplained observations (no theory of flavor):
• Huge mass differences between and within the generations• Universality of interactions• Symmetry, relationship between lepton and quark sectors• Tiny neutrino mass
BNL Nobel Prize discoveries (2 neutrinos, J, CPV) are all closely related to the flavor puzzle.
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Light Particle Rare Decay Experiments
Exotic
SearchesNew physics if seen;
SM effects are
negligible.
e LFVµ γ→
State of the art: single event sensitivity, 10-12
<4.7 10-12
<7.8 10-13
<1.2 10-11
Big BNL Impact
0 , LFVLK e K eµ πµ→ →
0
"Axions"
T-violation
K f
K
π
π µ ν
+ +
− +
→
→v
N e N LFVµ − −→
Probe new physics at the 1-1000 TeV Scales!
5
BSM Physics
New physics if
deviations from well-
calculated SM
predictions occur.
Lepton Universa lity ( )
( )
K e
K
π νπ µ ν
+ + +
+ + +
→→
10-8: 6200 events
10-10: 3events
10-4: 4x105 events
0 T-violationLK π µ ν− +→
0
0 0 violation
L
L
K
K
K CP
µ µ
π νν
π νν
+ −
+ +
→
→
→
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Selected Rare Kaon Decay Experiments
c.1980s-2000s
0
0 0
Search for T-violation in
Search for
Measurements of and ,
R. Adair .
S. Wojckiki, R. Cousins, W. Molzon, J. Ritchie
...
Search for
Measurem
.
ent
L
L L
et al
K
K e
K K ee
et a
e
l
K
πµν
µ
µµ
π µ+ +
→
→
→ →
→
s of (V ) , ,...K K
BNL AGS
0 0 0
0 03 3
0 0
Measurement of '/ in
Measurements of , ( ),
Searches for ,...
B. Winstein,... Blucher, Nguyen . (Fermilab)
H. Wahl, ... A. Ceccucci . (CERN
L
L e us
L
K
K ll K V K
K e
et al
et al
µ
ε ε π π
π
π µ
→
→
→
)
CERN, Fermilab
KEK
11/9/2010 BNL 90-50-10 Celebration 6
Measurement 3 us 4
0
s of (V ) , ,...
Measurement of
Measurements
M. Zeller .
A. J. S. Smith, T. Kycia, L. Littenberg
of ,
, D.B;
,
( ),
( ),..
.
e e
et al
K K
K
K K
K SD K DE
π νν
π γγ π µµ
µνγ π π γ
+ +
+ + + +
+ + +
→
→ →
→ →
S. Kettell, S. Sugimoto, .et al
0 0
0
Search for , ...
N. Sasao .
Search for
T. Inagaki .
Search for T-violation in
J. Imazato .
L
L
K ee
et al
K e
et al
K
et al
π
µ
πµν
→
→
→
KlOE Frascati
P. Franzini .et al
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AGS Rare K ExperimentsAGS Rare K Experiments
K π νν+ +→
Lepton Flavor Violation
0 0 LK π νν→
0 12
11
( ) 4.7 10
( ) 1.3 10
LB K e x
B K e x
µ
π µ
−
+ + −
→ <
→ <
Flavor-changing neutral current
}AGS{
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90% CL7 E787/E949
100
1000
1210−
Future?
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BNL/AGS Rare Kaon Decay Experiments 1980s-2000s
0 5.3 124.8
D. Ambrose et al. PRL 20, 4309 (1998).
Measurement of 8.7 10
!L
K ee R x Rarest particle decay observed+ −−→ =
11/9/2010 BNL 90-50-10 Celebration 8
03
A. Sher et al Phys.Rev.Lett.91:261802,2003
70000 : R( ) (5.13 .02 0.09 0.04 )%
2.3 ; !
e stat ys norm
us
K e K
V higher solved the unitarity problem
π ν
σ
+ +→ = ± ± ±
→7
S. R. Blatt et al. PRD 27 1056 (1983)
3
limit
Observed 2x10 decays:
Stringent on new source of T Viola o
K
ti n
µ+r
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New Physics found at LHC
New particles with unknown
flavor- and CP-violating couplingsNew Physics NOT found at LHC
Precision flavor-physics experiments
needed to help sort out the flavor- and
CP-violating couplings of the NP.
Precision flavor-physics experiments
needed -> sensitive to NP at mass
scales beyond the reach of the LHC
(through virtual effects).
Rare Decays in the LHC Era
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0 0
Quark Gen. Processes to Study NP
1 -e Conversion,
3 , other rare de s
2
ca
,
yLK K
e
b s
π νν π ν
π
γ
ν
µ ν+ +→ →
→
→
These reactions have special status
because of their small SM uncertainties
and large NP reach.
Thanks to Jack Ritchie
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K πνν→ FCNC!
..the curious incident of the dog in the
night-time...
"The dog did nothing in the night-time."
"That was the curious incident,"
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"That was the curious incident,"
remarked Sherlock Holmes.
Sherlock Holmes in "Silver Blaze"
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K ππππ
u c t
d s b
2/3
1/3
Flavor-changing neutral currents (e.g. s d)
are absent in the Standard Model:
→
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K ππππ
u c t
d s b
2/3
1/3
d s b1/3
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• A single effective operator
• Dominated by top quark (charm significant,
µ
L L L µ L(s γ d )(ν γ ν )
in the Standard ModelK π νν+ +→The decays are the most precisely calculated FCNC decays.K πνν→
υ χτ
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• Dominated by top quark (charm significant, but controlled)
• Hadronic matrix element shared with Ke3
• Uncertainty from CKM elements (will improve)
• Remains clean in New Physics models
(unlike many other observables)
Brod and Gorbahn, PRD 78, 034006(2008)
-11SMB ( ) = (8.5 ± 0.7) x 10K π νν+ +→
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Summary of SM Theory Uncertainties
CKM parameter uncertainties
dominate the error budget today.
With foreseeable
improvements, expect
total SM theory error ≤6%.A. Kronfeld (FNAL)
K π νν+ +→
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U. Haisch, arXiv:0707.3098
Unmatched by any other
FCNC process (K or B).
A. Kronfeld (FNAL)
30% deviation from the SM
would be a 5σ signal of NP
0 0SM theory error for mode exceeds that for .LK Kπ νν π νν+ +→ →
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SM
±5% at 1.7x BSM
Minimal Flavor Violation (a highly pessimistic hypothesis)
The MFV hypothesis
assumes that all flavor- and
CP-violating effects in New
Physics are governed by
the SM Yukawa couplings
(CKM mixing and phase).
Bobeth et al, Nucl Phys B726, 252(2005)
±5% measurement of
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MFV allowed
68% and 95% allowed regions for
NP, based on B → Xsγ and B → Xsl+l
C = C – CSM,
where C characterizes the
Z-penguin in b→s
±5% measurement of
B( ) will provide
strong constraints on New Physics
within MFV, or demonstrate
failure of the MFV hypothesis.
K π νν+ +→
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General MSSM with R-parity
E949 already
provides a
significant
constraint.
Buras et al, NP
B714,103(2005)
Fermilab proposal P996: improve the
sensitivity of B( ) by >100 !
±5% measurement
(hypothetical BSM value)
K π νν+ +→
→
New Physics models Points from a scan of
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SM
R Parity: R = (-1)2j+3B+L
with generic flavor
structure induce large
effects in .K π νν+ +→
Points from a scan of
MSSM parameters that
satisfy experimental
constraints except
B( ) K π νν+ +→
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Special Features of
Measuring
K π νν+ +→
Experimentally weak signature with background processes exceeding signal by >1010
ΙΙΙ
( )
64%
K µ ν γ+ +→0
21%
K π π+ +→
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• Determine everything possible about the K+ and π+
* π+/µ+ particle ID better than 106 (π +→ µ + → e+ )• Eliminate events with extra charged particles or photons
* π0 inefficiency < 10-6
• Suppress backgrounds well below the expected signal (S/N~10)* Predict backgrounds from data: dual independent cuts* Use “Blind analysis” techniques * Test predictions with outside-the-signal-region measurements
• Evaluate candidate events with S/N function
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“…when you have
eliminated the
impossible, whatever
remains, however
improbable, must be the
11/9/2010 BNL 90-50-10 Celebration 17
improbable, must be the
truth? ”
Sherlock Holmes in The Sign of the Four (1890)
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All
experiments
E787 E949
upgrades
HistoryK π νν+ +→
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experiments
used
stopped
kaons.
1.15 101.05
10
E787/E949 Final: 7 events observed
B( ) 1.73 10
Standard Model:
B( ) (0.85 0.07) 10
K x
K x
π νν
π νν
+ + + −−
+ + −
→ =
→ = ±
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• Fermilab (K, µ)
• J-PARC (K, µ)
Intensity Frontier: Rare K, π, µ Experiments
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• J-PARC (K, µ)
• CERN (K)• PSI and TRIUMF (π, µ)
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Intensity Frontier: Fermilab
Now and in the Future
-16
(MINOS,Miniboone,Minerva,NOVA)
Now:
Main Injector Neutrino Program
8 GeV Booster Proposals: Mu2E (10 ), g-2 (4x), ...
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-168 GeV Booster Proposals: Mu2E (10 ), g-2 (4x), ...
Tevatron Stretcher Proposal:
Future:
Project X
K π νν+ +→
2/8 GeV Linac
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Future ExperimentsK πνν→
0 0
Fermilab: (P996 and Project X)
(Project X)L
K
K
π νν
π νν
+ +→
→
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0 0
(Project X)
CERN: (NA62)
J-PARC: (KOTO, "KOTOII")
L
L
K
K
K
π νν
π νν
π νν
+ +
→
→
→
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E949 – 3nd generation 4th generation: P996 proposed at FNAL
22
ππππ ++++
ππππ ++++→→→→µµµµ ++++→→→→e ++++
Decay Sequence
µµµµ ++++
e ++++
ππππ ++++
ππππ ++++→→→→µµµµ ++++→→→→e ++++
Decay Sequence
µµµµ ++++
e ++++
Photon Veto
g
4p Photon Veto
g
500 MHz digitizers
Incremental Improvements
• 550 MeV/c K stopping
rate x5 with comparable
instantaneous rate
• Larger solid angle –
Acceptance x 10
• Finer segmentation,
improved resolutions -
Reduced backgrounds
• Overall 100 x sensitivity
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CERN NA-62 first generation
decay-in-flight experiment.
75 GeV
KOTO: 2nd try with ~same
setup as KEK ( ) 0 0 8B( ) 2.6 10L
K xπ νν −→ <
at CERN K π νν+ +→ 0 0 at J-PARC LK π νν→
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• Builds on NA-31/NA-48
• Un-separated GHz beam
• Aim: 50 events/yr at SM
• Under construction; start >2012
• Improved J-PARC Beam line
• (Eventually) higher power
• Aim: 2.8 events (S/B~1) at SM
• Under construction; start >2011
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TREK at J-PARC
Goal:
∆PT = 10-4
Search for T-violation i n K πµν→
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Fermilab Project X (ICD-2)
PKaon Production . Tvs
K + 0K
1 mA 100% d.f.
3 Gev
3 GeV 1 mA Continuous Beam
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3 GeVK24 GeVK
1K production (<1 GeV): ~
10
Proj. X p beam intensity: ~ 300
AGSProj. X
K flux: ~ 30AGS
σσ
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• B(KL→π0νν) ~ 2.5 ×10-11
Need huge flux of K’s -> high rates
• Weak neutral particle kinematic signature
2 particles missing
• Backgrounds with π0 up to 109 times larger
• Veto inefficiency on extra particles must be ≤10-4
0 0The Challenge: LK π νν→
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• Veto inefficiency on extra particles must be ≤10-4
• Neutrons dominate the beam
– make π0 off residual gas – requires high vacuum
– halo must be very small
– hermeticity requires photon veto in the beam
• Need convincing measurement of background
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Sherlock Holmes in "The
Crooked Man"
• "You know my methods, Watson. …
And it ended by my discovering traces,
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And it ended by my discovering traces,
but very different ones from those which I
had expected.
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0 0Project X : Experiment ConceptLK π νν→
3 GeV Protons
<50 ps
a la KOPIO
28
0L
0 0 0L
0
Use TOF to work in the K c.m. system
Identify main 2-body background K
Reconstruct decays with pointing calorimeter
4 solid angle photon and charged particle vetos
π π
π γγπ
•
• →
• →
•
0 0 LK π νν→
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At Project X : 0 0LK π νν→
• High intensity allows small beam dimensions (like KOTO):
“Difficult” flat beam and vacuum vessel unnecessary
• Symmetrical beam, detector; geometric acceptance maximized
• 2-D beam kinematic constraint increases S/B
• Upstream backgrounds, backgrounds in the fiducial volume
Ideal time structure for TOF-based experiment.
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• Upstream backgrounds, backgrounds in the fiducial volume reduced
• Same micro-bunch event spoilage reduced
• Random vetos reduced due to high duty factor
• Beam veto may be unnecessary
• Neutron rates higher – could be problematic
(See 2008 Project X workshop talks by L. Littenberg, S. Kettell)
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Goals KOTO
J-PARC
Proj.X
FNAL
ProspectsK πνν→0 0LK π νν→
0 0 8
11
B( ) 2.6 10
: Sensitivity at SM 3 10
: L
K x
Future x
Now π νν −
−
→ <
Goals NA62
CERN
P996
FNAL
Proj.X
FNAL
1.15 101.05
10
: B( ) 1.73 10
(7 events)
: Sensitivity at SM (0.85 0.07) 10
Now K x
Future x
π νν+ + + −−
−
→ =
±
K π νν+ +→
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J-PARC FNAL
Events/yr ~1 “200”
S/N ~1 5-10
Precision 5%
* J-PARC plans a phase II to
reach higher sensitivity.
FNAL FNAL
Events/
yr40 200 500
S/N 5 5 5
Precision 10% 5% 3%
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Summary: Rare Kaon Decays
* Future experiments possible at : Fermilab
( ) ( )0 03
* The AGS played a major role in the study and discovery of K decays
* New experiments have ex
NA6
ceptional sensitivity to Flavor Physics:
2 , KOTO & TREK( )LCERN K JPARC K Kµπ νν π νν+ +→ → r
11/9/2010 BNL 90-50-10 Celebration 31
* Future experiments possible at :
Great potential for advancing the intensity frontier
"Ultimate" high precision experiments possible
MI+Tevatron Strecher:
Fermilab
K + →0 0 many r th o e s : Proje ct X ,
,
LK K
π νν
π νν π νν
+
+ +→ →
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“... the lowest and vilest alleys
in London do not present a
more dreadful record of sin
than does the smiling and
beautiful countryside."
11/9/2010 BNL 90-50-10 Celebration 32
Sherlock Holmes in the Copper Beeches
i.e. We really don’t know where the new physics will turn up!