Introduction Agnieszka Zalewska Epiphany Conference on Neutrinos and

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Introduction Agnieszka Zalewska Epiphany Conference on Neutrinos and Dark Matter, 6. 01. 2006 Epiphany

Introduction Agnieszka Zalewska Epiphany Conference on Neutrinos and Dark Matter, 6. 01. 2006 Epiphany Conference on Neutrinos and Dark Matter as compared to 2000 Epiphany Conference on Neutrinos in Physics and Astrophysics A. Zalewska, Epiphany 2006 1

Neutrino sources from hep-ex/0211035 Experiments study solar, reactor, atmospheric , accelerator and UHE astrophysical

Neutrino sources from hep-ex/0211035 Experiments study solar, reactor, atmospheric , accelerator and UHE astrophysical neutrinos A. Zalewska, Epiphany 2006 2

At the time of Epiphany 2000 Ø The main conference highlight was the evidence

At the time of Epiphany 2000 Ø The main conference highlight was the evidence for oscillations of atmospheric neutrinos in Super. Kamiokande Ø „Solar puzzle” was not yet resolved: SNO was at startup of data taking Ø Accelerator experiments: K 2 K had collected data for less than one year, Minos and Mini. BOONE were under construction, CNGS experiments were before a formal approval Ø Reactor experiments: CHOOZ analysis was well advanced, Kam. LAND was under construction Ø Astrophysical HE neutrinos: experiments under construction A. Zalewska, Epiphany 2006 Ø Many interesting theoretical ideas 3

Between 2000 and 2006 Ø Solid experimental evidence for neutrino oscillations coming from the

Between 2000 and 2006 Ø Solid experimental evidence for neutrino oscillations coming from the Super. Kamiokande, K 2 K, SNO and Kam. LAND experiments (J. Zalipska on K 2 K) 50 kton H 2 O Super. Kamiokande A. Zalewska, Epiphany 2006 1 ktona D 2 O SNO 1 ktona, scyntylatora Kam. LAND 4

Ø Kam. LAND: Testing the Model with L/E Behavior • Rate + Shape: Oscillations

Ø Kam. LAND: Testing the Model with L/E Behavior • Rate + Shape: Oscillations at 99. 999995% C. L. Kam. LAND, PRL 94, 2005 J. Klein, EPS HEP 2005 A. Zalewska, Epiphany 2006 5

Three neutrino mixing Oscillation parameters: 3 mixing angles, 2 differences of mass squared, 1

Three neutrino mixing Oscillation parameters: 3 mixing angles, 2 differences of mass squared, 1 phase If neutrino is a Majorana particle, additional phases Atmospheric neutrinos CP phase 2 solar neutrinos connects solar and atmospheric regions If d 0, p, 2 p. . . then CP is violated for leptons (like for quarks), q 13 is very important for a measurement of d A. Zalewska, Epiphany 2006 6

Oscillation parameters The most probable values: q 23 = 450 (maximal mixing), q 12

Oscillation parameters The most probable values: q 23 = 450 (maximal mixing), q 12 = 330 (large), q 13 < 100 (small), Dm 223 2. 5 x 10 -3 e. V 2, Dm 212 8 x 10 -5 e. V 2, | Dm 213 |=| Dm 223 - Dm 212| Why this scheme of mixing angles is so much different from the scheme for quark mixing? A. Zalewska, Epiphany 2006 7

Between 2000 and 2006 Ø MINOS started data taking at the beginning of 2005

Between 2000 and 2006 Ø MINOS started data taking at the beginning of 2005 (first results from the beam are discussed these days at the collaboration meeting in Oxford) (D. Kiełczewska) Ø Mini. BOONE has been running since 2002 - first results should be presented during the first half of 2006 Ø OPERA will start data taking in 2006 (R. Zimmermann) Ø Big LAr detector „a la Icarus” should be redesigned A. Zalewska, Epiphany 2006 8

Three oscillation regions Two oscillation regions with a very solid experimental evidence: atmospheric region

Three oscillation regions Two oscillation regions with a very solid experimental evidence: atmospheric region solar region Third region: LSND being checked by the Mini. BOONE experiment If confirmed, a 4 th neutrino is required A. Zalewska, Epiphany 2006 9

LSND effect Excess of positrons above background interpreted as anty-ne appearance due to oscillations

LSND effect Excess of positrons above background interpreted as anty-ne appearance due to oscillations A. Zalewska, Epiphany 2006 10

Ø Mini. Boo. NE – checking the LSND effect è 8 Ge. V protons

Ø Mini. Boo. NE – checking the LSND effect è 8 Ge. V protons from the Fermilab booster neutrino beam of energy about 1 Ge. V è detector at a distance of 500 m from the target è 1021 p. o. t. to confirm/exclude the LSND effect Results expected ~end of 2005 A. Zalewska, Epiphany 2006 11

If Mini. BOONE confirms LSND. . . revolution ! = 2. 5 x 10

If Mini. BOONE confirms LSND. . . revolution ! = 2. 5 x 10 -3 e. V 2 = 8 x 10 -5 e. V 2 A. Zalewska, Epiphany 2006 12

The ICARUSexperiment 4 th December 2004 Existing T 600 detector – 600 t of

The ICARUSexperiment 4 th December 2004 Existing T 600 detector – 600 t of LAr 20 m 40 m T 600 detector – installation in Gran Sasso T 3000 – by cloning 300 t modules – canceled in 2005 A. Zalewska, Epiphany 2006 Bigger monolithic detector – worshop in March 2006 13

T 600 – data quality – from 2001 tests Hadronic interaction (2. 5 Me.

T 600 – data quality – from 2001 tests Hadronic interaction (2. 5 Me. V) EM shower e+ e- pair (24 Me. V) e 1 (9 Me. V) Muon bundle „Electronic bubble chamber” Collection view Richness of a single event A. Zalewska, Epiphany 2006 14 7 publications based on this data

ICARUS experiment Original plan for the detector upgrade: four modules, each of 300 tons

ICARUS experiment Original plan for the detector upgrade: four modules, each of 300 tons of LAr, to be constructed in the years 2005 -2007 4 th December 2004 Responsibility of the Polish groups: production of anode wires (about 55000 in total) for TPC chambers of the future A. Zalewska, Epiphany 2006 15 modules

At the time of Epiphany 2006 Ø Neutrino oscillations: Oscillation experiments enter a period

At the time of Epiphany 2006 Ø Neutrino oscillations: Oscillation experiments enter a period of precise measurements – intense sources of neutrinos and huge detectors are needed as well as good theoretical tools to answer the following questions: Is q 23 really maximal? How small is q 13? Mass hierarchy – normal or inverted? Is CP violated for neutrinos? - talks by D. Kiełczewska, D. Motta, K. Long, A. Blondel, S. Katsanevas, J. Sobczyk, M. Rolinec A. Zalewska, Epiphany 2006 16

High intensity sources of neutrinos Conventional beams of v. high intensity (D. Kiełczewska) New

High intensity sources of neutrinos Conventional beams of v. high intensity (D. Kiełczewska) New type of accelerator: neutrinos from decays of accelerated muons (K. Long, A. Blondel) b beams recent idea A. Zalewska, Epiphany 2006 New type of accelerator: neutrinos (antineutrinos) from accelerated 18 Ne (6 He) (S. Katsanevas) 17

Neutrino mass hierarchy Two important questions: Normal hierarchy (above) or inverted hierarchy (w. r.

Neutrino mass hierarchy Two important questions: Normal hierarchy (above) or inverted hierarchy (w. r. t. Dm 2 atm) How far from zero the whole picture is? A. Zalewska, Epiphany 2006 18

At the time of Epiphany 2006 Ø Neutrino mass: Direct measurement based on the

At the time of Epiphany 2006 Ø Neutrino mass: Direct measurement based on the electron spectrum from the Tritium b decay in the KATRIN experiment (J. Bonn) A. Zalewska, Epiphany 2006 19

At the time of Epiphany 2006 Ø Is neutrino a Majorana or a Dirac

At the time of Epiphany 2006 Ø Is neutrino a Majorana or a Dirac particle? Searches for neutrinoless double beta decays – many experiments proposed – observation of such a decay would be a great discovery - talks by K. Zuber, M. Wójcik, A. Bobyk A. Zalewska, Epiphany 2006 20

At the time of Epiphany 2006 Ø Dark Matter searches One should remember that

At the time of Epiphany 2006 Ø Dark Matter searches One should remember that only 15 years ago neutrinos were serious candidates for Dark Matter, nowadays WIMPs (Weakly Interacting Massive Particles) are in fashion - talks by Ch. Sander, B. Baret, M. Sapiński, A. Szelc Dark Energy 73% Ø High level theory by B. F. L. Ward A. Zalewska, Epiphany 2006 Ordinary Matter 4% (of this only about 10% luminous) Dark Matter 23% Neutrinos 0. 1 -2% 21

At the time of Epiphany 2006 Ø Increasing synergy between particle physics and astrophysics

At the time of Epiphany 2006 Ø Increasing synergy between particle physics and astrophysics and intense discussions about the future initiatives in both fields Will be reflected by many talks but especially by S. Katsanevas, J. Engelen, Ch. Spiering and S. Pokorski A. Zalewska, Epiphany 2006 22