Notes
Outline
Status and Perspective of the (new) Physics ay Gran Sasso National Laboratory and in the other European Underground Facilities
Snowmass Workshop
 A. Bettini July 3 2001
The mission
The energy region beyond the reach of present end future accelerators can be explored searching for naturally happening phenomena. But they are extremely rare
Extreme energy frontier = the frontier of background and disturbance reduction
The Gran Sasso Laboratory
1400 m rock overburden
Flat cross-section
Low n fluence from rock (CaCO3)
Cosmic µ flux attenuation = 10–6 (1 /m2 h)
Underground area 18 000 m2
Accelerator laboratory standard facilities on the surface
Operational budget 25 Glit/yr
Preparing the next phase
Mixing
Neutrino masses
Status of neutrino oscillations
Bi-maximal mixing
LUNA & LUNA2
GALLEX & GNO
GNO. Expected seasonal effects
Winter (W) - Summer (S) event rate in (SNU), after geometric effect removal
GNO is not in real time.
Winter: long nights. Summer: short nights
a means to look for day-night effects (mainly from pp))
Fogli e co.
Method may define parameters in the LOW solution, but larger sensitive masses are necessary.
Very expensive today. 100 t of Ga = 250 M$
Neutrinos from the atmosphere. MACRO
Next steps. How can Gran Sasso contribute?
Detect direct oscillation signals @ Dm2 (atmospheric)
Prove if oscillation is between nm and nt or else
detect t appearance
Improve knowledge of mixing parameters and Dm2
CNGS project
OPERA
ICARUS
Atmospheric neutrinos
MONOLITH proposal
Detect direct oscillation signals @ dm2 ( “solar”)
Improve knowledge of mixing parameters and  dm2
Choose solar solution
GNO
BOREXINO
LENS proposal
Measure relevant cross-sections and screening effect
LUNA2
Nature of neutrinos: Majorana or Dirac
Measure sign of Dm2
Measure absolute values of the masses
Neutrino-less double beta decay
HM, GENIUS-TF, GENINO, GENIUS
MIBETA, CUORICINO, CUORE
CP violation not at reach for a while.
Doubly suppressed. dm2 /Dm2 and |Ue3|2 are both small!
CNGS
CERN to Gran Sasso Neutrino Project
The experiments at LNGS
ICARUS
OPERA
MONOLITH proposal
Ue3
BOREXINO
Rates
BOREXINO. Day-night effects
Day-night, yearly averaged, asymmetry (in %) normalised to SSM due to e-neutrino regeneration in the Earth (mainly at Be energy)
Fogli and co.
LENS Proposal
To complete the solar neutrino program, we need
sensitivity to the low energy (pp) neutrinos in real time
flavour sensitivity
source sensitivity (pp. 7Be,8B)
The masses of Majorana e-neutrinos
The nature of neutrinos
Neutrinos have only one “charge”: lepton number
If total lepton number is not conserved, then e-neutrino and anti e-neutrino (etc.) may be the same particle: Majorana neutrino
Supernova neutrinos
neutrinisation
(r-process)
LVD
Cosmology particle physics interplay
An example
Dark Matter Searches
DAMA
CRESST
Ge detectors. Heidelberg
Life can be even harder
Underground laboratories
LMS
LSC
Status of double beta searches
Boulby
Gamma background
Concluding remarks