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Neutrino measurement with MACRO: Neutrino measurement with MACRO: neutrino oscillation, dark matter and astronomy neutrino oscillation, dark matter and astronomy studies studies Teresa Montaruli Teresa Montaruli Bari University and INFN


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Neutrino measurement with MACRO: neutrino oscillation, dark matter and astronomy studies Neutrino measurement with MACRO: neutrino oscillation, dark matter and astronomy studies

Les Houches, 21 Jan.-1 Feb. 2002 School and Workshop on Neutrino Particle Astrophysics

Teresa Montaruli

Bari University and INFN for the MACRO Collaboration

Teresa Montaruli

Bari University and INFN for the MACRO Collaboration

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Teresa Montaruli, Les Houches, 25 Jan. 2002 2

MACRO at LNGS MACRO at LNGS MACRO at LNGS

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Teresa Montaruli, Les Houches, 25 Jan. 2002 3

Outline Outline Outline

  • Min rock coverage 3150 hg/cm2
  • 600 ton liquid scintillator (600 ps), 20000 m2 streamer tubes (< 1º)

76.6×12×12 m3 Eth ~1 GeV @vertical

NIM A324(1993)

  • Neutrino detection in MACRO since 89 to Dec. 2000 (acq end)
  • Through-going upward muon results: matter effects νµ →ν

→ντ or νµ →ν →νsterile

  • Low energy topologies
  • Multiple scattering to infer Eν
  • ν astronomy results: point-like

sources and diffuse flux

  • Search for WIMPs

Clear event topologies, different energies, fully automatic analysis, no rejection of events at trigger level (efficiency, acceptance, backgrounds can be studied using atm. muons) Different technique than SuperKamiokande

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Teresa Montaruli, Les Houches, 25 Jan. 2002 4

Throughgoing Internal Down Internal Up µ stop

Throughgoing: Emedian∼50 GeV 180/yr Internal Up: Emedian∼3.5 GeV 50/yr Internal Down+Stopping µ: Emedian∼4.2 GeV 35+35/yr (expected)

ν event topologies ν ν event topologies event topologies

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Teresa Montaruli, Les Houches, 25 Jan. 2002 5

Main cut: position along

  • scint. counter from ST

track in agreement inside 70 cm with that from ToF ~200 gr/cm2 in rock absorber to reduce at 1% background from upgoing πs No scanning, fully automatic

  • 1.25 < 1/β < -0.75

Upward throughgoing µ analysis Upward throughgoing µ analysis

T.o.F. technique:

1/β distribution (full detector)

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Teresa Montaruli, Les Houches, 25 Jan. 2002 6

The backgrounds The backgrounds

Incorrect β: showering events, multiple µs; large β: µ decay

MACRO Coll., Astr. Phys 9 (1998)

First study

  • f physical

background to ν underground measurement Photonuclear interactions atmospheric µ ↓ produce upgoing soft particles Important for shallow detectors (Baksan, IMB while SK and Soudan2 have vetos) 243 upgoing particles between 12.2 ·106 µs ↓ ~10-4 π/µ ↓

~1% in throughgoing µs↑ ~5% in stopping µs

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Teresa Montaruli, Les Houches, 25 Jan. 2002 7

Event 23 Dec 1994

Total n. of events 863 Backgrounds Incorrect β 22.5 Soft upgoing π 14.2 Internal ν interactions 17 Measured 809 Expected 1122 ± 17% (Bartol flux 14% checked on atmospheric µ data, cross sections (GRV94) 9%, µ energy Loss 5% (Lohmann et al.) R = 0.72 ± 0.026stat±0.043sys± 0.12theor

Mar 89-Nov 91 (1.4y) Dec 92-Jun 93 (0.4y) Apr 94-Dec 2000 (5.5y) 26 µ↑ µ↑ 55 µ↑ µ↑ 782 µ↑ µ↑ 1/6 lower detector Lower detector Complete detector

  • Phys. Lett. B357 (1995) 481
  • Phys. Lett. B434 (1998) 451
  • Phys. Lett. B517(2001) 59

Results for Upward throughgoing µs Results for Upward throughgoing µs

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Teresa Montaruli, Les Houches, 25 Jan. 2002 8

µ↑ µ↑ flux angular distribution µ↑ µ↑ flux angular distribution

∆m2 = 0.0025eV2

χ2 test on the angular distribution (10 bins) with prediction

normalized to data: χ2/dof=25.9/9 for no-oscillations P = 0.2% χ2/dof=9.6/9 for νµ→ντ (∆m2 = 0.0024 eV2 sin22θ=1) P = 37%

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Teresa Montaruli, Les Houches, 25 Jan. 2002 9

νµ→ν →ντ oscillations in upward throughgoing µ νµ→ν →ντ oscillations in upward throughgoing µ

Peak probabilities: 37% shape 66% shape × normalization

∆m2 = 0.0024 eV2 sin22θ=1

Reduction factors for νµ→ντ MACRO threshold ~1 GeV more sensitive to vertical deficit than SK (average threshold ~6 GeV)

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Teresa Montaruli, Les Houches, 25 Jan. 2002 10

Angular distribution for selected sample Angular distribution for selected sample

3 box events (redundant time measurement ⇒ low background+better time resolution) same shape of full sample χ2/dof=9.4/7 for no-oscillations P = 22.8% χ2/dof=3.7/7 for νµ→ντ (∆m2 = 0.0025 eV2 sin22θ=1) P = 81.5%

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Teresa Montaruli, Les Houches, 25 Jan. 2002 11

Azimuth distribution for selected sample Azimuth distribution for selected sample

Full detector sample

Oscillations do not affect azimuth angular distribution χ2/dof=2.8/11 normalizing prediction to data

P = 0.99

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Teresa Montaruli, Les Houches, 25 Jan. 2002 12

Matter effects in upward throughgoing µs

When ν flavors involved in oscillations have different weak potential in matter

sterile e n e n B F weak

Y Y Y n G V ν ν ν ν

τ µ ,

2 4 2 2 2 − + − × ± =

+ for ν, - for nB = barion density

Yn,e = n, e/barion

ν

Matter effects in upward throughgoing µs

Matter effects can be important for νµ→νe,νsterile not for νµ → ντ And for Eν/∆m2 ≥103 GeV/eV2 for HE up-throughgoing µs For maximal mixing matter effect produces a reduction of oscillation effect closer to predicted with no oscillations For mixing <1 enhancement for some values of parameters (MSW)

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Teresa Montaruli, Les Houches, 25 Jan. 2002 13

Sterile or tau ν oscillations? Sterile or tau ν oscillations?

Vertical/horizontal more powerful test than χ2

  • P. Lipari & M. Lusignoli, PRD57(1998)

Pbestτ =8.4%/Pbeststerile=0.033% ⇒254 νµ→νsterile excluded at ~99% c.l.

Ratio: sensitive to deviation sign, gain in statistical significance (2bins) but some feature of angular shape could be lost MACRO bin choice through simulation (MACRO Coll. Phys. Lett. B517(2001) 59)

Max mixing sin22θ=1

Peak probability for shape 1.8% Peak probability for shape×normalization = 8%

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Teresa Montaruli, Les Houches, 25 Jan. 2002 14

Systematic errors in the ratio Systematic errors in the ratio

  • Neutrino flux sources of uncertainty:
  • P. Lipari, Nucl. Phys. Proc Supp.91(2001)

1) K/π fraction 2) Spectral index of CR E specrum

δR/R ~3%

  • Comparison of different cross

sections δR/R ~2%

  • Detector acceptance + background in

horizontal region

δR/R ~4.6%

Other uncertainties: seasonal variations dR/R ~1.3% + US atmosphere profile dR/R ≤1% MACRO upgoing µs: variation in vertical/horizontal ratio R(Nov-Apr) - R(May-Oct)≈0.19±0.17stat Seasonal effect difficult to calculate because neutrinos come from meson and muon decays and from all over the Earth

MACRO events θ

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Teresa Montaruli, Les Houches, 25 Jan. 2002 15

Internal Up events Internal Up events

Selection Criteria: 1. ToF between central/top scintillator layers 2. Vertex containment to reject up-throughgoing µs (~1% backg) DATA 161 with -1.3< 1/β <-0.7 (eff. livetime 5.58yr) Backgrounds (wrong β, secondary hits) = 7 154 Uniform deficit

  • Phys. Lett. B478 (2000) 5

∆m2=0.0025 eV2

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Teresa Montaruli, Les Houches, 25 Jan. 2002 16

Internal Down + Upward Stopping Internal Down + Upward Stopping

Selection criteria: 1. no T.o.F. 2. topological cuts: fiducial volume +bottom SC layer 3. visual scanning (real+simulated events) 4. >100 gr/cm2 in lower detector (soft πs backg. ∼5%) DATA: 272 events (5.6 yr), background 10 events 262 Uniform deficit IU and ID+UGS due to CCνµ, NC and νe (~13% IU and 10% UGS+ID)

∆m2=0.0025 eV2

Predictions: Φ = Φν ⊗ σν ⊗ ε(Εµ,θ)

25% error in MC normalization 6% difference respect to MINOS Neugen

  • Φν: Bartol ν flux with geomagnetic cutoff

checked on µ data (error ~ 14%)

  • σν = Q.E. + 1π (Lipari et al., PRL74 (1995) 4384)

+ DIS (GRV-LO-94 PDF) (error ~ 15%)

  • ε(Eµ,θzenith): detector response +acceptance

(systematic error ~ 10 %)

  • Phys. Lett. B478 (2000) 5
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Teresa Montaruli, Les Houches, 25 Jan. 2002 17

Low energy results Low energy results

DATA: 154 ± 12stat

MC: 285 ± 28sys ± 57theo MC (∆m2=0.0025 eV2): 168 ± 17sys ± 34theo

DATA: 262 ± 16stat MC: 376 ± 38sys ± 76theo MC (∆m2=0.0025 eV2): 284 ± 28sys ± 57theo Internal down + Upgoing stopping µ’s Internal Upward going µ’s

th sys stat IU

MC Data 11 . 05 . 04 . 54 .

) (

± ± ± =

th sys stat UGS ID

MC Data 14 . 07 . 04 . 70 .

) (

± ± ± =

+

  • Zenith angular distributions

constant deficit

  • RIU and RID+UGS not same

reduction deficit not due to

  • theor. overestimate of ν

flux/cross sections IU and ID+UGS have <Eν> ~ 4 GeV

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Teresa Montaruli, Les Houches, 25 Jan. 2002 18

Double Ratio Double Ratio

  • Most of the theor. err. cancel (<5%)
  • Systematic err. reduced (~6%)

Data: R = 0.59 ± 0.06stat Expected (No oscillations): R = 0.76 ± 0.04sys ± 0.04th Expected νµ ντ oscillations: R = 0.59 ± 0.04sys ± 0.03th

(max mixing and ∆m2 = 2.5 x 10-3 eV2 ) Probability to obtain double ratio so far from expected is ~2% (including non-gaussian shape of the uncertainty of the ratio) Expected reductions for ∆m2 ~1-10 ×10-3 eV2 sin22θ= θ=1 1/2 for IU 1/4 for ID+UGS (ID not reduced)

Internal Downgoing Upgoing Stop

R =

+

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Teresa Montaruli, Les Houches, 25 Jan. 2002 20

Multiple Scattering: E dependence in MACRO data? Multiple Scattering: E dependence in MACRO data?

  • 25 radiation lengths of absorber+iron
  • ST system σ ~1cm saturation @

Eµ~10GeV

  • ST resolution improved to 3mm using

TDC analogue information (150 ns) µ residual energy up to 40 GeV (Eν~200 GeV) Goal: study of atm νµ oscillations using energy estimate through multiple scattering of µ↑ Given preferred oscillation parameters ∆m2 ~O(10-3 eV2) oscillation effects stronger at Eµ≤10 GeV and disappear at E> 100 GeV NIM paper to appear

log10Eµ(GeV)

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Teresa Montaruli, Les Houches, 25 Jan. 2002 21

Oscillations and Multiple Scattering Oscillations and Multiple Scattering

eV2

Preliminary

Low energy: <Eν> ~15 GeV (46 events) High energy: <Eν> ~170 GeV (55 events) Error: 11% ν flux + cross section +5% acceptance 348 of the through-going upgoing sample survived to cuts (4 ST planes with valid QTP-TDC information) NN trained to recognize residual µ energy

Next future: oscillation contour from low/high ratio

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Teresa Montaruli, Les Houches, 25 Jan. 2002 22

MACRO as a ν telescope MACRO as a ν telescope

  • Good pointing resolution using ST system (<1°); Moon shadow at 5.5σ level

Showers do not worsen angular res. ∆Ω(µsim−µrec)∼1° @ 100 TeV

  • Timing 600 ps resolution ⇒atm µ background rejection
  • Efficiency and acceptance checked at HE: monoenergetic µ beams using

Bottai&Perrone corrections to µ propagation in GEANT and rock around MACRO Area @100 TeV ~ 42% area @10 GeV due to analysis cuts (same as oscillation analysis except for 200 gr/cm2 in lower detector)

(PRD59 (1999)). MACRO Coll., AP.J., 546, 1038, 2001

MACRO area averaged over 1 day as a function of declination and energy

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Teresa Montaruli, Les Houches, 25 Jan. 2002 23

MACRO response function to astrophysics fluxes MACRO response function to astrophysics fluxes

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Teresa Montaruli, Les Houches, 25 Jan. 2002 24

Neutrino Astronomy with MACRO Neutrino Astronomy with MACRO

Search for clusters around µ↑ directions+sources from catalogues (SNRs, EGRET, NovaeX, Blazars, BATSE and BeppoSAX)

  • Atm. ν background:
  • Steady sources: 100 random associations of µ↑ local angles with times

Backg in 10º declination bands

  • Pulsed sources: coincidences in ∆t = ±(20-400) s (each 20 s), 200 time

shifts of ∆t(µ↑ and GRB) (from –4000-4000 s to -80000-80000s) No statistically significant cluster

  • f 1356 events around 42 selected

sources 12 sources with ≥2 events (expected 14.3) in 3º 7 events from GX339-4 (P=2.6·10-3) Prob to find such excess from ≥1 of the 42 sources Pmax = 6.5%

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Teresa Montaruli, Les Houches, 25 Jan. 2002 25

Point-like source search Point-like source search

MACRO SKY SURVEY 1356 µ↑ No significant cluster around 1356 events 110 clusters with with ≥4 events around a given event 107.8 expected in 3º cone Largest cluster of 9 events around (345º,-74º)

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Teresa Montaruli, Les Houches, 25 Jan. 2002 26

Neutrino Astronomy with MACRO Neutrino Astronomy with MACRO

No significant excess has been found with respect to the background 90%c.l. muon flux upper limits for 90% of signal in 3º search cones for ν flux power law with 2.1 spectral index and for Eµ ≥1 GeV Fraction

  • f signal

in 3º as a function of spectral index and cos(zenith)

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Teresa Montaruli, Les Houches, 25 Jan. 2002 27

ν ν emissions during GRBs ν ν emissions during GRBs

BATSE : 1 burst /day (4π/3sr)

Similar results for BeppoSAX

1230 MACRO µ↑ overlap in time with 2702 BATSE GRBs 10º (5º ) 96.9% (83.5%)

νs from GRBs (BATSE error box

dominates) ±200 s (98% GRBs T90s) 0 events (0.05 expected) MACRO area/average burst 133m2 90%c.l upper limit: 6.64 10-10 µ cm-2 per average burst 1 order of magnitude from Waxman&Bahcall fireball scenario

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Teresa Montaruli, Les Houches, 25 Jan. 2002 28

Search for high multiplicity events in coincidence with GRBs Search for high multiplicity events in coincidence with GRBs

MACRO dedicated SN trigger PHRASE looks for clusters of ν-like events 1453 BATSE GRBs occurred in ∼5 yrs of SN trigger up-time

  • GRB-induced variations of single event

trigger rate: ±1, ±5, ±10min intervals

RESULT: no evidence for variations Events within 10 min before and after BATSE GRBs vs SN trigger rate (= backg) Line = probability of 10-1 for

  • bserving a given number of

events in a 10min interval for a detector running time

  • f 5 yr
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Teresa Montaruli, Les Houches, 25 Jan. 2002 29

Search for diffuse ν flux in MACRO Search for diffuse ν flux in MACRO

MACRO does not directly measure µ energy but energy released in SC boxes helps in selecting HE events after energy calibrations including non-linear terms in light yield/ADC count relation accounting for PMT saturation + tests on reliability of response @ HE using full simulation and atm µ data Released energy distribution for a sample of atm µs Calibrations @ HE for 1 box: ERP attenuated ADC response to laser light

Calibration reliable to released energy >500 MeV Linear response With higher

  • rders
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Teresa Montaruli, Les Houches, 25 Jan. 2002 30

ENTRIES 7547

Log10(EIni(GeV)) Log10(ERel(MeV))

1 1.5 2 2.5 3 3.5 4 4.5 5 1 2 3 4 5 6 7 8

Total energy released Initial µ energy

Analysis for diffuse ν flux search Analysis for diffuse ν flux search

AGN simulation: 2988 yrs, CTEQ3-DIS, Stecker et al. model, proper µ transport 10 TeV in GEANT, rock around detector to account for showering events

+ box with >500 MeV at d<1m

No ST tracking required Weighted mean time by energy release for scintillator plane ⇒upward direction 1/β from ‘scintillator’ track Reasonable decrease in efficiency with energy >500 MeV in 1 box

100TeV 1TeV 10TeV

>500 MeV in another box

Radiative processes

Ionization

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Teresa Montaruli, Les Houches, 25 Jan. 2002 31

MACRO µ upper limit on diffuse ν flux MACRO µ upper limit on diffuse ν flux

livetime area efficiency c.l.) (90% limit Upper c.l.) (90% Φ × × =

µ

Φµ ~ 1.7 10-14 cm -2 s -1 sr -1

Prepint astro- ph/0105269

104<E<107

1.3 ÷ 1.9 10-5

BAIKAL (νe)

Nucl.Phys.Proc.S 91, 423 (2000)

E<106

1.0 10-6

AMANDA

This analysis

104 <E<106

4.5 10-6

MACRO (this analysis)

  • Astrop. Phys 4, 217

(1996)

E ~2.6 103

5.0 10-6

Frejus

  • Astrop. Phys 14, 61

(2000)

104<E<107

1.4 10-5

BAIKAL

Proc XXV ICRC, Durban (1997)

105<E<106

6.0 10-4

SPS- DUMAND

Phys Lett. B 333 , 555 (1994)

105<E<106

2.0 10-3

EAS – TOP

Reference ν ν Energy range (GeV) ν flux limit

(90% cl) E2Φν (GeV cm-2 s -1 sr-1)

power law index γ

γ =2

No significant signal has been found with respect to the statistical fluctuations of the atmospheric neutrino background

2

DATI

0.54±0.03stat

AGN

1.1±0.5stat

ATMO Rate of survived events in 5.8 yr

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Teresa Montaruli, Les Houches, 25 Jan. 2002 32

MACRO ν upper limit on diffuse ν flux MACRO ν upper limit on diffuse ν flux

Log10(Eν(GeV)) E2Φν(GeV cm-2 s-1 sr-1)

10

  • 9

10

  • 8

10

  • 7

10

  • 6

10

  • 5

2 3 4 5 6 7 8 9

Upper limit on ν ν flux (power law index γ

γ =2) Φµ ~ 1.7 10-14 cm -2 s -1 sr -1

(model dependent limit: ν spectrum, cross sections, µ energy losses)

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Teresa Montaruli, Les Houches, 25 Jan. 2002 33

Candidates selected by the diffuse flux analysis Candidates selected by the diffuse flux analysis

381 tracks!

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Teresa Montaruli, Les Houches, 25 Jan. 2002 34

Weakly Interacting Massive Particles in Earth and Sun Weakly Interacting Massive Particles in Earth and Sun

χ+χ→ χ+χ→ νµ+… Earth: data>background in signal region (oscillations)⇒expected background

  • f atm neutrinos normalized by ratio of observed to expected events
  • utside search cones

Sun: expected backg mixing randomly times and local angles of measured events⇒the method accounts for oscillations

  • Phys. Rev. D60 (1999) 082002

Exposure ~ 4500m2yr

MC 1139±194

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Teresa Montaruli, Les Houches, 25 Jan. 2002 35

∆m2 = 3 10-3 eV2

Models by Bottino et al

(Astrop. Phys 3 (1995)65) Circles already excluded by direct searches ρχ=0.5GeVcm-3

Effect of νµ→ντ oscillations on ν fluxes from χ annhilation

  • N. Fornengo, hep-ph/0011030

ντ→νµ does not balance νµ→ντ because

Φντ<Φνµ ⇒ reduction of µ↑ χ+χ→ χ+χ→ νµ+…

Neutralinos in Earth and Sun Neutralinos in Earth and Sun

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Teresa Montaruli, Les Houches, 25 Jan. 2002 36

Current results

χ+χ→ χ+χ→ νµ+… SK: exposure from Neutrino2000 1028 events/923d, limits from ICRC2000 1416/1268 d

Baksan: 1056 events, 14.8 yr (Suvorova, hep-ph/9911415)

Lake Baikal 35 vertical,/ 234 d (ICRC2000) (10 GeV) AMANDA B10: 15 vertical/135d (astro-ph/0012285)

Current results

Sorry: could not be latest results but no published ref

Different methods for upper limits! i.e. SK limits do not account for cone collection Efficiency, MACRO 90% signal included

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Teresa Montaruli, Les Houches, 25 Jan. 2002 37

DAMA/NaI annual modulation indication DAMA/NaI annual modulation indication

Earth crossed by larger WIMP flux in June (December): VEarth rotation around Sun +(-) Vsolar system in Galaxy

v0=170km/s v0=270km/s

Earth fluxes

(Bottino et al. models PRD62(2000))

include νµ→ντ

DAMA/NaI (PLB480(2000)23): ~7%effect for ~4annual cycles favor MW=43 (72) GeV (local WIMP velocity v0 = 220km/s (170km/s))

CDMS (PRL84(2000)5699) excludes at 84%cl 3σ allowed DAMA region and

claims n background at a rate close to intensity of DAMA signal

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Teresa Montaruli, Les Houches, 25 Jan. 2002 38

νs from WIMPs in the Galactic Center

Gondolo and Silk

(PRL83(1999)):

if CDM exists in Gal Center can be accreted by black hole with formation

  • f “central spike”

If CDM = neutralinos Φν ~10-15-10-14cm-2 s-1 for mχ>50 GeV MACRO limits excludes most models with central spike

νs from WIMPs in the Galactic Center

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Teresa Montaruli, Les Houches, 25 Jan. 2002 39

AMANDA, Lake Baikal

ANTARES, NEMO-RD, NESTOR

1) High energy event angular distribution more regular than in the past

χ2/dof=9.6/9 for νµ→ντ (∆m2 = 0.0025 eV2 sin22θ=1) P = 37% (only from shape) 66% (shape + normalization) Two flavor sterile ν oscillations disfavored respect to νµ→ντ @ 99% c.l. for all mixings 2) Low energy events: flat angular distribution deficit, double ratio independent on theoretical errors⇒confirm HE µs preferred parameters 3) Multiple scattering analysis provides L/E indication 4) Upper limits to µ and ν fluxes from point-like and diffuse sources and from WIMPs at the level of expected capabilities in proposal through deep understanding of detector performances, backgrounds and development of adequate simulation tools

Conclusions Conclusions

FUTURE: neutrino telescopes (AMANDA, Lake Baikal, ANTARES, NEMO, ICECUBE) will take us in the new era of SIGNALS following all those upper limits!