Transcript Document

Nuclear Science & the New Standard Model:
Neutrinos & Fundamental Symmetries in the Next Decade
The
Nuclear
next physics
decade studies
presents
ofNP
ns &
with a
historic
fundamental
opportunity
symmetries
to buildplayed
on thisan
legacy
essential
in developing
role in developing
the “new
&
Standard
confirming
Model”
the Standard Model
Fifty years
of PV in
nuclear
physics
The
Our value
role has
of our
been
contribution
broadly will be
broadly
recognized
recognized
within and
outside
beyond
the NP
field
Solar ns &
the neutrino
revolution
Michael Ramsey-Musolf, APS April, 2007
Community Input
•
Pre-Town Meetings:
Santa Fe Nov 2006 (~ 50 participants)
Caltech Dec 2006 (~ 50 participants)
•
DNP Town Meeting
Chicago Jan 2007 (~ 370 participants)
•
White paper (merging two)
Substantial work by the
organizing committee
Primary Recommendation:
New Standard Model Initiative
Scientific Questions, Achievements
& Challenges
Primary Scientific Questions
•
What are the masses of neutrinos and how have
they shaped the evolution of the universe? 0nbb
decay, q13, b decay,…
•
Why is there more matter than antimatter in the
present universe? EDM, DM, LFV, 0nbb, q13 …
•
What are the unseen forces that disappeared
from view as the universe cooled? Weak decays,
PVES, gm-2,…
Tribble report
Scientific Achievements
•
Discovery of flavor oscillations in solar neutrinos;
Solution of the solar neutrino problem; 1300+
citations
•
Discovery of flavor oscillations in reactor neutrinos;
Identification of LMA solution; over 1000 citations
•
World’s most precise measurement of (gm-2)
Possible first indications of supersymmetry; over
1000 citations
•
Most precise measurement of sin2qW off the Z0
resonance using PV Moller scattering; constrains
new physics at the TeV scale (Z’, RPV SUSY…)
Scientific Achievements
•
Definitive test of large Dm2 oscillations by
MiniBoone experiment (April 2007! )
•
Definitive determinations of strange quark
contributions to nucleon EM form factors using PV
electron-proton & electron-nucleus scattering;
confirmed theoretical estimates of hadronic effects
in electroweak radiative corrections
•
Quark-lepton universality tested to 0.05% using
superallowed nuclear b-decay, yielding most
precise value of any CKM matrix element (Vud)
2006 Bonner Prize in Nuclear Physics recognizing
work of Towner & Hardy
Scientific Achievements
•
Completion of a comprehensive set of
computations of supersymmetric effects in lowenergy electroweak observables; 2005 Dissertation
Award in Nuclear Physics to A. Kurylov
•
Reduction in the theoretical hadronic uncertainty in
extraction of Vud from neutron and nuclear b-decay
•
New theoretical breakthroughs in simulating
neutrino flavor transformation in supernovae;
modeling n flavor transformation effects
nucleosynthesis with SN’s; understanding weak
interaction effects in SN shock dynamics
Scientific Achievements
•
2007 Bonner Prize (S.J. Freedman*) and
Dissertation Award in Nuclear Physics (K.
Milknaitis) for experimental work in neutrinos
•
Four Bonner Prizes (Bowman, McDonald,
Hardy/Towner, Freedman )
•
Three Dissertation Awards (Heeger, Kurylov,
Miknaitis)
* Also weak decays
Technological Achievements & Investments
b-decay: Neutrino Mass
KATRIN, NexTex, MARE…
Total Lepton Number & Neutrino Mass Term
QuickTime™ and a
TIFF (Uncompressed) decompressor
are needed to see this picture.
Majorana
0nbb-decay
QuickTime™ and a
TIFF (LZW) decompressor
are needed to see this picture.
CUORE
EXO
GERDA
Technological Achievements & Investments
QuickTime™ and a
TIFF (Uncompressed) decompressor
are needed to see this picture.
Fundamental
Neutron Physics
Beamline at SNS
QuickTime™ and a
TIFF (Uncompressed) decompressor
are needed to see this picture.
1.4 MW , 1 GeV Hbeam on L Hg
Also new capabilities at LANSCE, NIST…
Quic kTime™ and a
TIFF ( Unc ompres s ed) dec ompr es s or
are needed to s ee this pic ture.
CEBAF 12 GeV Up-grade
QuickTime™ and a
TIFF (Uncompressed) decompressor
are needed to see this picture.
Muon storage
ring at BNL
QuickTime™ and a
TIFF (Uncompressed) decompressor
are needed to see this picture.
ISAAC,
RIBF….
Technological Achievements & Investments
DUSEL
Multi-purpose Facility
Site selection process proceeding at NSF
Challenges: What role can low energy studies play
in the LHC era ? (and beyond!)
Two frontiers in the search for new physics
Collider experiments
(pp, e+e-, etc) at higher
energies (E >> MZ)
Large Hadron Collider
Indirect searches at
lower energies (E < MZ)
but high precision
Ultra cold neutrons
CERN
High energy
physics
Particle, nuclear
& atomic physics
Scientific Opportunities
•
•
•
Major Discovery Potential:
0nbb-decay & EDM
Precision measurements
Neutrino mixing & hierarchy
Weak decays, PVES, gm-2
Electroweak probes of QCD
PVES, Hadronic PV, nN scatt…
The Origin of Matter & Energy
Electroweak symmetry
breaking: Higgs ?
WIMPy D.M.: Related
to baryogenesis?
Leptogenesis: discover
the ingredients: LN- & CPviolation in neutrinos
Weak scale
baryogenesis: test
experimentally: EDMs
Baryogenesis: When?
CPV? SUSY? Neutrinos?
“New gravity”? Lorentz
violation? Grav baryogen ?
?
Nuclear Science mission: explain
the origin, evolution,
& structure
of SM symmetry (broken)
Beyond the
SM
“KnownEnergy
Unknowns”
Cosmic
Budget
the baryonic component
0nbb-Decay: LNV? Mass Term?
Dirac
Majorana
b-decay
Long baseline
Theory Challenge:
matrix


e
e
elements+ mechanism
?
1000
EFF
mW
n 
De ge ne rate
Effective bb Mass (meV)
100

Inve r te d

Nor m al
m
Ue1 = 0.866
1
Ue2 = 0.5
m
2
2
atm
s ol
2
= 70 meV
= 2000 meV
Ue3 = 0

2
0.1
2
1
?
3
4
5 6 7
2
3
4
5 6 7
10
100
Minimum Neutrino Mass (meV)
2
3
4
5 6 7
1000

u




AZ,N
d 

e
W
u
u

e˜

d


W
k
e
nM
W


2

e
10

n MUek mk e2i



e
0

e˜ 

u
AdZ  2,N  2
d


EDMs: New CPV?
f˜
Electron

˜0

f˜



Improvements
of 102 to 103
f


f˜

˜0

Neutron


˜ 0
f˜




g
p

q˜

f


q˜
q
QCD



q˜
˜
N
e


q





q˜
˜


0
g
q˜



QCD


Deuteron
g
q˜


0
n
 

Neutral
Atoms


q



QCD


Baryogenesis: EDMs & Colliders
Theory progress &
challenge: refined
computations of baryon
asymmetry & EDMs
baryogenesis
LHC reach
LEP II excl
Present de
ILC reach
dn similar
Prospective de
Precision Probes of New Symmetries
Electroweak symmetry
New Symmetries
breaking: Higgs ?
1.
2.
3.
4.
Origin of Matter
Unification & gravity
Weak scale stability 
Neutrinos
?
nm
ne
n˜ m
W
˜ 0
 m

m˜ 


e


QuickT ime™ and a
T IFF (Uncompressed) decompressor
are needed to see this picture.
QuickTime™ and a
TIFF(Uncompressed) decompressor
are needed to see this picture.
Qu ickT ime ™ a nd a
TIF F (U nco mpre sse d) de com pres sor
are nee ded to s ee th is pi cture .
Quic kTime™ and a
TIFF (Uncompres sed) dec ompressor
ar e needed to see this picture.
Beyond the SM
Qui ckT ime™ and a
T IFF (Uncompressed) decompressor
are needed to see this picture.
SM symmetry (broken)
Precision Neutrino Property Studies
Mixing, hierarchy, & CPV
Daya Bay
U e1 U e2 U e 3 


U  U m1 U m 2 U m 3 


U1 U 2 U 3 
1
0
0   cosq13
0 ei CP sin q13   cosq12 sin q12 0 1 0
0

 


 
i / 2
 0 cosq 23 sin q23   
0
1
0
0
  sin q12 cosq12 0  0 e

  i CP

 
i / 2ib

cosq13   0
0
1 0 0 e
0 sin q 23 cosq 23  e sin q13 0

•
proton
s





nSNS Long baseline
site oscillation studies:
CPV?
Normal or Inverted ?
Mini Boone
SNS Hall
Precision Neutrino Property Studies
High energy solar ns
Solar Neutrinos
DM +
EWB
Ice Cube
EM vs. n luminosity: MNSP
KamLAND
Borexino
unitarity?
Solar model?
SNO+
LENS
Weak decays & new physics
SUSYCorrelations
models
Vud

u c t Vcd

 Vtd
d  u e n e
s  u e n e
b  u e n e
nm
ne
n˜ m

˜
 m




m˜ 
˜ 0

ne



d
SUSY
CKM, (g-2)m,
MW, Mpt
pe pMn
M
dW 1 a m˜ L q˜L A n 
E e En
e
Ee

e
u˜

O
 ~ 0.001
 OSM
0
u

W

Vus Vub  d
 
Vcs Vcb  s 
 
Vts Vtb  b
˜



 
n˜ e
e
SUSY
Non
(V-A)
x probes
(V-A) of
Similarly
unique
Vud from
neutron
interactions:
me/E
new
physics in muon
and
decay:
LANSCE,
pion decay
SNS, NIST
TRIUMF &RIA?
PSI
SNS, NIST, LANSCE,
Weak Mixing in the Standard Model
Parity-violating electron scattering
SLAC Moller
JLab Future
Z0 pole tension
Scale-dependence of Weak Mixing
Probing SUSY with PV Electron Scattering
RPV:
No SUSY DM
Majorana n s
12 GeV
 QWP, SUSY / QWP, SM
SUSY Loops
QuickTime™ and a
TIFF (LZW) decompressor
are needed to see this picture.
E158
 QWe, SUSY / QWe, SM
6 GeV
gm-2
Muon Anomalous Magnetic Moment
m

QED
m
Z
Weak
Future goal

Had
VP
Had
LbL
SM Loops
QuickTime™ and a
TIFF (LZW) decompressor
are needed to see this picture.
SUSY Loops
Quic kTime™ and a
TIFF ( LZW) dec ompres sor
are needed to s ee this pic ture.
New Standard Model Initiative
A Road Map
• A robust neutrino program: DUSEL (+ exp) &
immediate 0nbb
• An EDM program: nEDM (SNS), atomic, 2H R&D
• Precision Electroweak: PVES, b-decay, gm-2
• Supernova simulation & observation
• Cross-disciplinary research support: q13 , DM, CLV
• Theory: focus on problems & junior theorists
Resources & Benefits
Equivalent to a major new initiative:
•
•
•
“New Standard Model Initiative” (NSMI)
~ $750m over 10+ years (~$185m non DUSEL)
One major new facility (DUSEL)
Targeted program at other facilities
Benefits to NP:
• Make NP a major player in era of historic
discovery potential; we can help write
the textbook on the new SM
• Builds on substantial achievements since 2002 LRP
& development of strong groups
• Attractive to junior scientists
• Economy of resources & synergy with other NP
facilities
Resources
Project Funding for Neutrinos and Fundamental Symmetries
Non DUSEL: $184m
Total: $748m
DUSEL Const: $250m
1 ton 0nbb