towards precision lepton flavour physics. some reflections… have brought us many clues for a...
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Towards precision lepton flavour physics
Some reflections…
have brought us many clues for a deeper understandingin the SM and continue to do so:
They were the key to the weak interactions
• first "almost" invisible carriers of energy
• first realization of an “almost” Weyl fermion: only one helicity state!
• first state with only a chiral gauge charge
We got the SM but not quite a deeper understanding
chiral gauge theories are finely tunned and extremely hard to get as effective theories:
• anomaly cancellation
• complex vacuum structure that we naively describe with one boring scalar (hierarchy problem) problem and many free parameters to parametrize our ignorance (flavour puzzle)
It seemed that could not tell us anything about the vacuum because they could not feel it but they do…again in a extremely weak way
The “other” helicity states
• non-decoupling physics (scales at or below v): at least three new fundamental s=1/2 fields with no charge
m= Weyl no new scale M=0 L conserved Majorana new scale M 0 L violated
These could be furthermore coupled to a hidden sector: gauge interactions, more fermions, scalars… only linked to the visible sector through neutrino masses
• decoupling L-violating physics: >> v
• mixture: decoupling and not decoupling
+…
Weinberg
If M>> v the see-saw solution
New scale solution M v, =O(:
m ~ v2/M decoupling effect
No new scale solution M ~ v:
m ~2 v Yukawa smallness
( if e m ~ O(1 eV) )
why are masses so small ?
what value of M is more natural ?
M << v is natural because of L symmetryM>>v is not hierarchy problem:
Casas, Espinosa, Hidalgo
Whether the new physics is associated to just a high scale or there is a hidden sector around the corner, its (strongest) link to the visible world is the mass matrix:
• Generically non-unitary PMNS matrix• Flavour structure in neutral currents • Mixing O(v/M) ~O(mv)
and not just a typical CKM… (|Ufi|,|Ufj|,|Ufk|)
Maximal mixing in the 23 sector seems to imply redundancy: symmetry ?
The fundamental questions:
• what are the “other” helicity states: Weyl, Majorana or decoupling physics
• what are the scales and dynamics involved in the interactions of these new fields? Is it a decoupling scale >>v or is there a hidden sector at low scales
• is there a L number conserved ?
• are relevant in cosmology and in the genesis of baryons ?
The answers will provide a new perspective into the flavour puzzle and the hierarchy problem
Einstein’s dream Photomultiplier
Solving the Flavour Puzzle
Our safest bet is to measure precisely the light mass matrix:
• overconstrain the PMNS matrix to see that it is not the whole story…
• test symmetries: CP, CPT, maximal mixing…to give us a clueon the new interactions
Standard 3scenario
The observables:
Masses Angles CP-phases
m12
< m22, m3
2
The unknowns…
Hierarchy 0
m21, m2
3
Precise oscillations
0
Cosmologysign(cos
The knowns…
|m223|, m2
12
Precise oscillations
More precision and overconstraining the known parameters will also be important:
• to resolve correlations with the unknown ones
• search for new physics or symmetries: test of unitarity of the PMNS, establish maximal mixing
The challenge…
Measure small oscillation probabilities or measure large ones with high accuracy
There are only two mass splittings: |m223| >> m2
12
Tunning E/L ~ m2
ij we can enhance different terms even inthe same channel
ee e e 1 1
1 1
sign(
sign(cos2 1 1
Sensitivity to unknows at E/L ~|m223| in matter
vac/matter small parameters
Golden Silver
Sensitivity to knowns at E/L ~|m223|
small parameters
ee e e m
1 1
sin22 1 1
m 1 1
sin22 1 1
Sensitivity at E/L ~m212
ee e
sign(
sign(cos 1 1
ee e m
sin22 1
m 1
sin22 1
Correlations and degeneracies
At fixed EL:
P(eas1
P(eas2
Generically two solutions: trueand intrinsic degeneracy Burguet-Castell, Gavela, Gomez-Cadenas,P.H.,Mena
Including the discrete ambiguities eight-fold
P(cos 2eas1
P(cos 2eas2
Barger,Marfatia, WhisnantMinakata, Nunokawa
rue Fake
wrong octant
• Position of depend strongly on the E,L and channel
• Fake do not depend on E and L
• are the ones that increase the error on • In vacuum all are CP violating or all CP conserving: fake
wrong sign
Terrestrial precision oscillation experiments
Ultimate reactors E/L ~|m223| ?
L(km) sin22DChooz 1.1 ~ 0.03
UR 1.7 ~ 0.017
• No sensitivity to the other unknowns• No dependence on • If large, great synergies with superbeams to resolve degeneracies Minakata, et al Anderson et al
90%CL
< 1% syst
Reactors at E/L ~m212
SK-Gd can reach a sensitivity to m212 2.8% (3CL
Choubey,Petcov
The sensitivity to sin2 can reach 2% (1CL) in a reactor experiment tuned to the oscillation maximum
SADO Minakata, Nunokawa, Teves, Zukanovich Funchal
L=(50-70)km [8 x 10-5 eV2/m212]
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4% syst.
Stat: (~1700 events/y) 0.5 kton y (SADO) ≈1.4 kton y(KL)
Superbeams Off-axis
Use the conventional (more intense) beams: p Target K, , % e
e
L(km) sin22 sign( sign(cos2
T2K-I
(2008)
295 ~0.01
0.02 - - -
810 0.003
0.02 - some -
Sensitivity to strongly depends on in both cases and
also onsign(in
T2K upgrade of K2K with a more intense beam and OA
NOupgrade of MINOS with a better detector and OA CL
Hierarchy at
Only for sin22> 0.04 and some values of
The atmospheric parameters can be measured with high precision (per cent level):
But the sensitivity to maximal mixing is not as good:=/4 sin2 2 = 1-O()
T2K-I:
Sensitivity to sin2
Minakata,Sonoyama Fernandez-Martinez et al
For 42º < 50º the error on s223 remains O(10-20%)
which is not much better than the present error!
The new era (discovery) (roughly…depends on the actual value of the parameters)
sign(
~2013 > 4º marginal 13 > 6º (0%)
13 >13º(50%)
40º-50º
deg.
T2K-I seems to be a rather optimal setup for the next generation superbeam…should start taking data in 2008
The new era (precision) (roughly…depends on the actual value of the parameters)
|m2 23| sin2 m2
12 sin2
~2013 ~1% ~2%-16% ~1% ~2%
T2K-I + reactors seem to be a rather optimal combination of setups for the next generation…
Next-to-new era
Superbeams: still room for improvement with a significant increase in power and/or detector:
JPARC: 0.75 4MW, HyperK (Megaton!) NUMI: factor 4 with new Fermilab proton driver CERN-SPL: 4MW, Megaton
Huge statistics, but systematics is critical !
T2K-II best sensitivityto but not to hierarchy
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The race for the hierarchy
: a second detector at the second oscillation maximum
Noa proposal
T2K-II:half of detector in Korea (2nd oscillation peak)
23
Ishitsuka,Kajita,Minakata,Nunokawa
Combination with atmospheric
Comes for free! Huber, Maltoni,Schwetz
T2K-II+atmospheric data
Also helps in resolving the octant: if |s232-0.5| > 0.1
The known realm…
• |m223|: Maximal mixing can be established at % level
only with a per mil sensitivity to sin22 T2K-I vs II
Fernandez-Martinez et alper mil
The purists…
At accelerators we can also do electron (anti)-neutrino beams above threshold that are pure!
• from decay:
a magnetized detector indispensable! • from radioactive ions:
beam FACT
A significant investment in accelerator infrastructure
Very well-known fluxes
Not so different starting point since the detector can be made more massive for the -beam (it does not need magnetization) CERN-Canaries
p L(km) Det. mass
FACT 200-500 3000 40KTon
-beam 60/100
130 440KTon
In both cases, there is an associated superbeam (SPL) that can be combined
CERN-Frejus
Higher -beam at longer baseline are possible and much better
• more signal because of higher cross-sections• easier to measure the energy dependence• more significant matter effects
maxe)/L GeV)
SPS 150/300km 0.6
SPS-upgrade
350/700km 1.3
LHC 2500/3000km 9.4
Burguet-Castell, et al
CERN-Canfranc ?
Comparing -beams
Hierarchy, t23
Sin22x10-3 0.04
Degeneracies at beam
Ultimate anti-degeneracy machine
FACT &40KTon iron calorimeter 2800km (Golden)eFACT & 4Ton Emulsion 730km(Silver) eSPL&Megaton Cerenkov (Bronce) 130km e
The intrinsic and the octant ambiguities are resolved (up to uncertainties) if the eand e are combined
Donini, Meloni, Migliozzi
Hierarchy and octant solved for ºº
sensitivity down to 0.3º !
Overconstraining: eee,ee,for and !
The new era (discovery) (roughly…depends on the actual value of the parameters)
sign( ~2013 > 4º marginal 13 > 6º (0%)
13 >13º(50%)
40º-50º
deg.
~202? >0.3-0.6º º large
13 > 1º- 2º(100%)
While T2K-I seems to be a rather optimal setup for the nextgeneration superbeam, the “optimal” next-to-new generation experiment is still under investigation
There are good ideas to reach the per cent sensitivity in the mass matrix in the next 10-20 years
The lepton flavour sector might turn out to be uninspiring…
Approximate oscillation probabilities O(
Cervera et al. Akhmedov et al
Extremely useful to
• optimize the observables and experiments
• understand correlations
• existence of approximately degenerate solutions: set of oscillation parameters that give the same probabilities