astroparticles in the lhc era

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ASTROPARTICLES IN THE LHC ERA Antonio Masiero Univ. of Padova and INFN, Padova NO - VE 2008, Venice, April 15- 18, 2008

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NO - VE 2008, Venice, April 15-18, 2008. ASTROPARTICLES IN THE LHC ERA. Antonio Masiero Univ. of Padova and INFN, Padova. LHC and “LOW-ENERGY” NEW PHYSICS. LHC discovers NP : difficult, if not impossible, to “reconstruct” the fundamental theory lying behind those signals of NP; - PowerPoint PPT Presentation

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Page 1: ASTROPARTICLES IN THE LHC ERA

ASTROPARTICLES IN THE LHC ERA

Antonio MasieroUniv. of Padova

andINFN, Padova

NO - VE 2008, Venice, April 15-18, 2008

Page 2: ASTROPARTICLES IN THE LHC ERA

LHC and “LOW-ENERGY” NEW PHYSICS

• LHC discovers NP: difficult, if not impossible, to “reconstruct” the fundamental theory lying behind those signals of NP;

• LHC does not see any signal of NP: still a NP related to the stabilization of the elw. scale may be present, but with particles whose masses are in the multi-TeV range.

Page 3: ASTROPARTICLES IN THE LHC ERA

FCNC, CP ≠, (g-2), ()0 m n …

LINKED TO COSMOLOGICAL EVOLUTION

Possible interplay with dynamical DE

NEWPHYSICS AT

THE ELW SCALE

DM - FLAVOR

for DISCOVERY

and/or FUND. TH.

RECONSTRUCTION

A MAJOR LEAP AHEAD IS NEEDED

LFV

NEUTRINO PHYSICSLEPTOGENESIS

TEVATRON I L C

Page 4: ASTROPARTICLES IN THE LHC ERA

WHY TO GO BEYOND THE SM

“OBSERVATIONAL” REASONS

•HIGH ENERGY PHYSICS

(but AFB……)

•FCNC, CPNO (but evidence >3σ for NP in b - s transitions,,,)

•HIGH PRECISION LOW-EN.

NO (but (g-2) …)

•NEUTRINO PHYSICS YE m 0, 0

•COSMO - PARTICLE PHYSICS

YE (DM, ∆B cosm, INFLAT., DE)

Z bbNO

NO

NO

YES

YES

THEORETICAL REASONS•INTRINSIC INCONSISTENCY OF SM AS QFT

(spont. broken gauge theory without anomalies)

•NO ANSWER TO QUESTIONS THAT “WE” CONSIDER “FUNDAMENTAL” QUESTIONS TO BE ANSWERED BY “FUNDAMENTAL” THEORY

(hierarchy, unification, flavor)

NO

YESStrong CP violation?

Page 5: ASTROPARTICLES IN THE LHC ERA
Page 6: ASTROPARTICLES IN THE LHC ERA

ON THE COMPLEMENTARITY OFDM and LFV SEARCHES to DIRECT

LHC SEARCHES FOR NP

• Twofold meaning of such complementarity:

i) synergy in “reconstructing” the “fundamental theory” staying behind the signatures of NP;

ii) coverage of complementary areas of the NP parameter space ( ex.: multi-TeV SUSY physics)

Page 7: ASTROPARTICLES IN THE LHC ERA

MICRO MACROPARTICLE PHYSICS COSMOLOGY

GWS STANDARD MODEL HOT BIG BANG STANDARD MODEL

HAPPY MARRIAGE Ex: NUCLEOSYNTHESIS

BUT ALSO POINTS OF FRICTION

-COSMIC MATTER-ANTIMATTER ASYMMETRY

-INFLATION

- DARK MATTER + DARK ENERGY

“OBSERVATIONAL” EVIDENCE FOR NEW PHYSICS BEYOND

THE (PARTICLE PHYSICS) STANDARD MODEL

Page 8: ASTROPARTICLES IN THE LHC ERA

Present “Observational” Evidence for New Physics

• NEUTRINO MASSES

• DARK MATTER

• MATTER-ANTIMATTER ASYMMETRY

• INFLATION

Page 9: ASTROPARTICLES IN THE LHC ERA

SM FAILS TO GIVE RISE TO A SUITABLE COSMIC MATTER-ANTIMATTER ASYMMETRY

• SM DOES NOT SATISFY AT LEAST TWO OF THE THREE SACHAROV’S NECESSARY CONDITIONS FOR A DYNAMICAL BARYOGENESIS:

• NOT ENOUGH CP VIOLATION IN THE SM NEED FOR NEW SOURCES OF CPV IN ADDITION TO THE PHASE PRESENT IN THE CKM MIXING MATRIX

• FOR MHIGGS > 80 GeV THE ELW. PHASE TRANSITION OF THE SM IS A SMOOTH CROSSOVER

NEED NEW PHYSICS BEYOND SM. IN PARTICULAR, FASCINATING POSSIBILITY: THE ENTIRE MATTER IN THE UNIVERSE ORIGINATES FROM THE SAME MECHANISM RESPONSIBLE FOR THE EXTREME SMALLNESS OF NEUTRINO MASSES

Page 10: ASTROPARTICLES IN THE LHC ERA

MATTER-ANTIMATTER ASYMMETRY NEUTRINO MASSES CONNECTION: BARYOGENESIS THROUGH

LEPTOGENESIS

• Key-ingredient of the SEE-SAW mechanism for neutrino masses: large Majorana mass for the RIGHT-HANDED neutrino

• In the early Universe the heavy RH neutrino decays with Lepton Number violatiion; if these decays are accompanied by a new source of CP violation in the leptonic sector, then

it is possible to create a lepton-antilepton asymmetry at the moment RH neutrinos decay. Since SM interactions preserve Baryon and Lepton numbers at all orders in perturbation theory, but violate them at the quantum level, such LEPTON ASYMMETRY can be converted by these purely quantum effects into a BARYON-ANTIBARYON ASYMMETRY ( Fukugita-Yanagida mechanism for leptogenesis )

Page 11: ASTROPARTICLES IN THE LHC ERA

1 2l R R R RL f h fL Me Lh

202

2 20

†1( o

8g3 ) lij jL i

G

m AM

f fM

m

Non-diagonality of the slepton mass matrix in the basis of diagonal lepton mass matrix depends on the unitary matrix U which diagonalizes (f+ f)

~

SUSY SEESAW: Flavor universal SUSY breaking and yet large lepton flavor violation

Borzumati, A. M. 1986 (after discussions with W. Marciano and A. Sanda)

see Isidori’s talk at this meeting

Page 12: ASTROPARTICLES IN THE LHC ERA

µ e+ in SUSYGUT: past and future

Calibbi, Faccia, A. M., Vempati

Page 13: ASTROPARTICLES IN THE LHC ERA

INFLATION

SEVERE COSMOGICAL PROBLEMS

COMMON SOLUTION FOR THESE PROBLEMSVERY FAST (EXPONENTIAL) EXPANSION IN THE UNIV.

V()

TRUE VACUUM

VACUUM ENERGY

dominated by vacuum en.

NO WAY TO GET AN “INFLATIONARY SCALAR POTENTIAL” IN THE STANDARD MODEL

CAUSALITY(isotropy of CMBR)

FLATNESS( close to 1 today)

AGE OF THE UNIV. PRIMORDIAL MONOPOLES

Page 14: ASTROPARTICLES IN THE LHC ERA

NO ROOM IN THE PARTICLE

PHYSICS STANDARD MODEL FOR

INFLATION

V=2 2 + 4 no inflation

Need to extend the SM scalar potential

Ex: GUT’s, SUSY GUT’s,…

ENERGY SCALE OF “INFLATIONARY PHYSICS”:LIKELY TO BE » Mw

DIFFICULT BUT NOT IMPOSSIBLE TO OBTAIN ELECTROWEAK INFLATION IN SM EXTENSIONS

But for one solution requiring a non-trivial gymnastics

See Giudice’s talk at this meeting

Page 15: ASTROPARTICLES IN THE LHC ERA

The Energy Scale from the“Observational” New Physics

neutrino masses

dark matter

baryogenesis

inflation

NO NEED FOR THE NP SCALE TO BE CLOSE TO THE ELW. SCALE

The Energy Scale from the “Theoretical” New Physics

Stabilization of the electroweak symmetry breaking at MW calls for an ULTRAVIOLET COMPLETION of the SM already

at the TeV scale +

CORRECT GRAND UNIFICATION “CALLS” FOR NEW PARTICLES AT THE ELW. SCALE

Page 16: ASTROPARTICLES IN THE LHC ERA

Mandatory to look for P - DECAY

Page 17: ASTROPARTICLES IN THE LHC ERA

On the Energetic Budget of the Universe

Courtesy of H. Murayama

Page 18: ASTROPARTICLES IN THE LHC ERA

WMAP3 + small scale CMB exps (BOOMERang, ACBAR, CBI ans VSA)

+ Large-Scale Structures (SDSS,2dFCRS)

+ SuperNova ( HST/GOODS, SNLS)

CONSISTENT WITH BARYON DENSITY

DETERMINATION FROM BIG BANG NUCLEOSYNTHESIS

Page 19: ASTROPARTICLES IN THE LHC ERA

DM: the most impressive evidence at the “quantitative” and “qualitative” levels of

New Physics beyond SM

• QUANTITATIVE: Taking into account the latest WMAP data which in combination with LSS data provide stringent bounds on DM and B EVIDENCE FOR NON-BARYONIC DM AT MORE THAN 10 STANDARD DEVIATIONS!! THE SM DOES NOT PROVIDE ANY CANDIDATE FOR SUCH NON-BARYONIC DM

• QUALITATIVE: it is NOT enough to provide a mass to neutrinos to obtain a valid DM candidate; LSS formation requires DM to be COLD NEW PARTICLES NOT INCLUDED IN THE SPECTRUM OF THE FUNDAMENTAL BUILDING BLOCKS OF THE SM !

Page 20: ASTROPARTICLES IN THE LHC ERA

THE RISE AND FALL OF NEUTRINOS AS DARK MATTER

• Massive neutrinos: only candidates in the SM to account for DM. From here the “prejudice” of neutrinos of a few eV to correctly account for DM

• Neutrinos decouple at ~1 MeV ; being their mass<<decoupling temperature, neutrinos remain relativistic for a long time. Being very fast, they smooth out any possible growth of density fluctuation forbidding the formation of proto-structures.

• The “weight” of neutrinos in the DM budget is severely limited by the observations disfavoring scenarios where first superlarge structures arise and then galaxies originate from their fragmentation

Page 21: ASTROPARTICLES IN THE LHC ERA
Page 22: ASTROPARTICLES IN THE LHC ERA

WIMPS (Weakly Interacting Massive Particles)

#~# m

# exp(-m/T)# does not change any more

Tdecoupl. typically ~ m /20

depends on particle physics (annih.) and “cosmological” quantities (H, T0, …

h2_ ~ 10-3

<(annih.) V > TeV2

~ 2 / M2 From T0 MPlanck

h2 in the range 10-2 -10-1 to be cosmologically interesting (for DM)

m ~ 102 - 103 GeV (weak interaction) h2 ~ 10-2 -10-1 !!!

THERMAL RELICS (WIMP in thermodyn.equilibrium with the

plasma until Tdecoupl)

Page 23: ASTROPARTICLES IN THE LHC ERA

STABLE ELW. SCALE WIMPs from PARTICLE PHYSICS

1) ENLARGEMENT OF THE SM

SUSY EXTRA DIM. LITTLE HIGGS. (x, ) (x, ji) SM part + new part

Anticomm. New bosonic to cancel 2

Coord. Coord. at 1-Loop2) SELECTION RULE

DISCRETE SYMM.

STABLE NEW PART.

R-PARITY LSP KK-PARITY LKP T-PARITY LTP

Neutralino spin 1/2 spin1 spin0

3) FIND REGION (S) PARAM. SPACE WHERE THE “L” NEW PART. IS NEUTRAL + ΩL h2 OK

* But abandoning gaugino-masss unif. Possible to have mLSP down to 7 GeV

mLSP

~100 - 200

GeV *

mLKP

~600 - 800

GeV

mLTP

~400 - 800

GeV

Bottino, Donato, Fornengo, Scopel

Page 24: ASTROPARTICLES IN THE LHC ERA

D. kAZAKOV

Page 25: ASTROPARTICLES IN THE LHC ERA

FROM THE MSSM TO THE CMSSM ( constrained MSSM)

PROLIFERATION OF PARAMETRS IN THE SOFT BREAKING SECTOR OF THE MSSM:

OVERALL NUMBER OF PARAM. IN THE MSSM IS

1 2 4

CMSSM

Page 26: ASTROPARTICLES IN THE LHC ERA

WHICH SUSY

HIDDEN SECTOR SUSY BREAKING AT

SCALE F

OBSERVABLE SECTOR

SM + superpartnersMSSM : minimal content

of superfields

ME

SS

EN

GE

RSF = MW MPl

GRAVITY

Mgravitino ~ F/MPl ~

(102 -103) GeV

GAUGE INTERACTIONS

F = (105 - 106) GeV

Mgravitino ~ F/MPl ~

(102 - 103) eV

Page 27: ASTROPARTICLES IN THE LHC ERA

GRAVITINO LSP?

• GAUGE MEDIATED SUSY BREAKING

(GMSB) : LSP likely to be the GRAVITINO ( it can be so light that it is more a warm DM than a cold DM candidate )

Although we cannot directly detect thegravitino, there could be interesting signatures from the next to the LSP ( NLSP) : for instance the s-tau could decay into tau and gravitino,Possibly with a very long life time, even of the order of days or months

Page 28: ASTROPARTICLES IN THE LHC ERA

SWIMPS (Super Weakly Interacting Massive Particles)

• - LSP Gravitino in SUSY

• - First excitation of the graviton in UED …

They inherit the appropriate relic density through the decay of a more massive thermal species that has earlier decoupled from the thermal bath

DIFFERENT FROM THE THERMAL HISTORY OF WIMPS

Page 29: ASTROPARTICLES IN THE LHC ERA

ELLIS, OLIVE,SANTOSO,SPANOS

Page 30: ASTROPARTICLES IN THE LHC ERA
Page 31: ASTROPARTICLES IN THE LHC ERA

THE “WHY NOW” PROBLEM

Page 32: ASTROPARTICLES IN THE LHC ERA

DM DEDO THEY “KNOW” EACH OTHER?

DIRECT INTERACTION (quintessence) WITH DARK MATTER DANGER:

Very LIGHTm ~ H0

-1 ~ 10-33 eVThreat of violation of the equivalence principle, constancy of the fundamental “constants”, …CARROLL

INFLUENCE OF ON THE NATURE AND THE ABUNDANCE OF CDM

Modifications of the standard picture of WIMPs FREEZE - OUT

CDM CANDIDATES

CATENA, FORNENGO, A.M., PIETRONI, ROSATI, SCHELKE

SCALAR-TENSOR THEORIES OF GRAVITY, KINATION, RS II EXTRA DIM.

Page 33: ASTROPARTICLES IN THE LHC ERA

SCHELKE, CATENA, FORNENGO, A.M., PIETRONI

Page 34: ASTROPARTICLES IN THE LHC ERA

NEUTRALINO RELIC ABUNDANCE IN GR AND S-T THEORIES OF GRAVITY

Page 35: ASTROPARTICLES IN THE LHC ERA

CONSTRAINTS ON THE ENHANCEMENT OF THE UNIV.EXPANSION RATE FROM THE LIMITS ON THE

ANTIPROTON ABUNDANCE

SCFMP

Page 36: ASTROPARTICLES IN THE LHC ERA

SEARCHING FOR WIMPs

WIMPS HYPOTHESIS

DM made of particles with mass 10Gev - 1Tev

ELW scale

With WEAK INTERACT.

LHC, ILC may PRODUCE WIMPS

WIMPS escape the detector MISSING ENERGY

SIGNATURE

FROM “KNOWN” COSM. ABUNDANCE OF WIMPs PREDICTION FOR WIMP PRODUCTION AT COLLIDERS WITHOUT SPECYFING THE PART. PHYSICS MODEL OF WIMPs

BIRKEDAL, MATCHEV, PERELSTEIN , FENG,SU, TAKAYAMA

Page 37: ASTROPARTICLES IN THE LHC ERA
Page 38: ASTROPARTICLES IN THE LHC ERA

Model Independent Annual Modulation ResultModel Independent Annual Modulation Result

experimental single-hit residuals rate vs time and energy DAMA/NaI (7 years) + DAMA/LIBRA (4 years) Total exposure: 300555 kgday = 0.82 tonyr

2-5 keV

2-6 keV

A=(0.0215±0.0026) cpd/kg/keV

2/dof = 51.9/66 8.3 C.L.

2-4 keV

The data favor the presence of a modulated behavior with proper features at The data favor the presence of a modulated behavior with proper features at 8.28.2 C.L. C.L.

A=(0.0176±0.0020) cpd/kg/keV

2/dof = 39.6/66 8.8 C.L.

A=(0.0129±0.0016) cpd/kg/keV

2/dof = 54.3/66 8.2 C.L.

Absence of modulation? No

2/dof=117.7/67 P(A=0) = 1.310-4

Absence of modulation? No

2/dof=116.1/67 P(A=0) = 1.910-4

Absence of modulation? No

2/dof=116.4/67 P(A=0) = 1.810-4

ROM2F/2008/07

Acos[(t-t0)] ; continuous lines: t0 = 152.5 d, T = 1.00 y

Page 39: ASTROPARTICLES IN THE LHC ERA

ELLIS, OLIVE, SAVAGE

Neutralino-nucleon scattering cross sections along the WMAP-allowed coannihilation strip for tanbeta=10 and coannihilation/funnel strip for tanbeta=50 using the hadronic parameters

Ellis, Olive, Sandick

LHC Sensitivity

Page 40: ASTROPARTICLES IN THE LHC ERA

SPIN - INDEPENDENT NEUTRALINO - PROTON CROSS SECTION FOR ONE OF THE SUSY PARAM. FIXED AT 10 TEV

PROFUMO, A.M., ULLIO

Page 41: ASTROPARTICLES IN THE LHC ERA
Page 42: ASTROPARTICLES IN THE LHC ERA

LFV - DM CONSTRAINTS IN MINIMAL SUPERGRAVITY

A.M., Profumo, Vempati, Yaguna

Page 43: ASTROPARTICLES IN THE LHC ERA

INDIRECT SEARCHES OF DM• WIMPs collected inside celestial bodies ( Earth, Sun):

their annihilations produce energetic neutrinos • WIMPs in the DM halo: WIMP annihilations can take place

( in particular, their rate can be enhanced with there exists a CLUMPY distribution of DM as computer simulations of the DM distribution in the galaxies seem to suggest. From the WIMP annihilation:

-- energetic neutrinos ( under-ice, under-water exps Amanda, Antares, Nemo, Antares, …)

--photons in tens of GeV range ( gamma astronomy on ground Magic, Hess, … or in space Glast…)

--antimatter: look for an excess of antimatter w.r.t. what is expected in cosmic rays ( space exps. Pamela, AMS, …)

Page 44: ASTROPARTICLES IN THE LHC ERA
Page 45: ASTROPARTICLES IN THE LHC ERA
Page 46: ASTROPARTICLES IN THE LHC ERA

Roszkowski, Ruiz,

Silk, Trotta

Page 47: ASTROPARTICLES IN THE LHC ERA

CIRELLI, STRUMIA,

TAMBURINI 2008

Page 48: ASTROPARTICLES IN THE LHC ERA

A.M., PROFUMO, ULLIO

Page 49: ASTROPARTICLES IN THE LHC ERA

A.M., PROFUMO,ULLIO

Page 50: ASTROPARTICLES IN THE LHC ERA
Page 51: ASTROPARTICLES IN THE LHC ERA

S. Katsanevas ASPERA

Page 52: ASTROPARTICLES IN THE LHC ERA

2013201120092007 2008 20182016201420122010 20172015

30 M€ (from 85)

KM3NeT

Megaton

Auger North

CTA

Grav Wave 3rd generation

> 2/3 from 100 + 50 M€

250 M€

400-800 M€

300 M€

60-100 M€

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Double Beta 1 ton

DM search 1 ton

50-200 M€

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C. SPIERING, APPEC - ASPERA ROADMAP

Page 53: ASTROPARTICLES IN THE LHC ERA

2013201120092007 2008 20182016201420122010 20172015

30 M€ (from 85)

KM3NeT

Megaton

Auger North

CTA

Grav Wave 3rd generation

> 2/3 from 100 + 50 M€

250 M€

400-800 M€

300 M€

60-100 M€

60-100 M€

Double Beta 1 ton

DM search 1 ton

50-200 M€

50-200 M€30+100+250+200+100+100+50+100 ~ 950 M€

add 300 M€ for runningexperiments, upgrades,new methods

Page 54: ASTROPARTICLES IN THE LHC ERA

FCNC, CP ≠, (g-2), ()0 m n …

LINKED TO COSMOLOGICAL EVOLUTION

Possible interplay with dynamical DE

NEWPHYSICS AT

THE ELW SCALE

DM - FLAVOR

for DISCOVERY

and/or FUND. TH.

RECONSTRUCTION

A MAJOR LEAP AHEAD IS NEEDED

LFV

NEUTRINO PHYSICSLEPTOGENESIS

TEVATRON I L C