Top Banner
Neutrinos at the South Pole with IceCube, DeepCore and PINGU Ken Clark, SNOLAB
51

Ken Clark, SNOLAB

Dec 31, 2016

Download

Documents

phamcong
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Ken Clark, SNOLAB

Neutrinos at the South Pole with IceCube,

DeepCore and PINGU

Ken Clark, SNOLAB

Page 2: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrinos• Neutrinos obviously

need no introduction at SNOLAB

• VERY light, neutral particles

• Only interact very weakly • Very prevalent in the

universe • Three flavours

2

Page 3: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Sources of Neutrinos• Experiments study neutrinos from different

sources

• Solar neutrinos (Homestake, Borexino, SNO)

• Reactor neutrinos (KamLAND, Daya Bay, RENO)

• Neutrino Beams (MINOS, T2K, OPERA)

• Atmospheric Neutrinos (SuperK, Antares, IceCube)

3

Page 4: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Atmospheric Neutrinos

• Source of neutrinos is the interaction of particles in the atmosphere

• These interactions produce neutrinos with an understood flux and flavour content

4

Page 5: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrino Energy Spectrum

5

• Studying neutrinos at high energies was the motivation

• Success with intermediate IceCube configurations

GeV TeV PeV EeV

Page 6: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016 6

100

10Events

/km2 year

GeV TeV PeV EeV

• Studying neutrinos at high energies was the motivation

• Success with intermediate IceCube configurations

Neutrino Energy Spectrum

Page 7: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Detector Wish List

• In order to detect these neutrinos, a detector was needed which would:

1. Have a large target mass 2. Provide a very clear medium so that

light can be detected 3. Be at least somewhat shielded from

outside radiation

7

Page 8: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube/DeepCore

8

Skiway

South Pole Station

Page 9: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

The IceCube Neutrino Telescope

9

Page 10: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016 10

The IceCube Neutrino Telescope

Page 11: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Detection Method

11

muon

neutrino

interaction

Page 12: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube Events

• Usual map overlay of event?

12

Page 13: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Events in the Detector

• Events are separable using their signature in the detector

13

Time

Early Late

CC Muon Neutrino νμ + N μ + X

“Track”

NC Neutrino νX + X νX + X

“Cascade”

Page 14: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Event Selection

• Use an extensive veto to remove specific classes of events

• Want to retain only events which have their first interaction inside the detector

14

IceTop Water Tanks

1.45 km

90 m

2450m

2085m2165m

Veto Region

Dust Layer

Veto Region

Page 15: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Event Selection

15

YES NO

Page 16: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Why So Strict?

• This is 10 ms of data

• In one year IceCube will detect:

~1011 atmospheric muons (3000 per second)

~105 atmospheric ν->μ (1 every 6 minutes)

~10 cosmic ν->μ

16

Page 17: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Analysis Preparation

• Several aspects required to prepare for the full analysis of the high energy events

• Need to determine the number of neutrinos expected and their energy spectrum

• Need to verify the veto procedure with existing data/Monte Carlo

17

Anticipated Events

Atmospheric μ: Determined from experimental data using

the new veto 6±3.4

Atmospheric ν: Determined using Monte Carlo simulation

and previous data 4.6+3.7-1.2

Page 18: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube Results

1.04±0.16 PeV

• Try out these new methods on a subsample of the IceCube data

• Completely unexpectedly, two very high energy events were found (and named)

18

1.14±0.17 PeV

Page 19: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube Results

1.04±0.16 PeV

19

1.14±0.17 PeV

• Try out these new methods on a subsample of the IceCube data

• Completely unexpectedly, two very high energy events were found (and named)

Page 20: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube Results

1.04±0.16 PeV

20

1.14±0.17 PeV

• Try out these new methods on a subsample of the IceCube data

• Completely unexpectedly, two very high energy events were found (and named)

Page 21: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Predicted Results

21

Expected to see 10.6+5.0-3.6

Page 22: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Actual Results

22

Actually saw 28 (in the first 2 years of data)

Page 23: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube Results

23

(This has been updated to ~3 years)

Page 24: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Source?

24

There is no convincing source so far…

Page 25: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Highest Energy

• Ernie & Bert stood as the highest energy events for some time

• During the full analysis, a new record-setting event was found

25

2.2 PeV

Page 26: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

On to the Next Analysis

• Want to expand beyond just high energy neutrino detection

• Neutrino oscillations are very exciting field right now…

• Why not see if we can do something with those?

26

Page 27: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrino Oscillations

27

• SNOLAB users probably don’t need an introduction to oscillations

• The oscillation pattern is shown here

Blue: muon neutrino Red: tau neutrino

Black: electron neutrino

Image credit: Wikipedia

Page 28: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Atmospheric Neutrinos

• Source of neutrinos is the interaction of particles in the atmosphere

• These interactions produce neutrinos with an understood flux and flavour content

28

Page 29: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrino Oscillations

29

Blue: muon neutrino Red: tau neutrino

Black: electron neutrino

Image credit: Wikipedia

• IceCube has a maximum path length of ~13000 km • If the lower energy threshold is ~200 GeV, L/E <~65

Page 30: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrino Oscillations

30

• IceCube has a maximum path length of ~13000 km • If we can lower the energy threshold to ~10 GeV, L/

E <~1300

Blue: muon neutrino Red: tau neutrino

Black: electron neutrino

Image credit: Wikipedia

Page 31: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube

31

• 78 Strings

• 125m string spacing

• 17m DOM spacing

• Add 8 strings

• 75m string spacing

• 7m DOM spacing

• Add 20 strings

• 26m string spacing

• 5m DOM spacing10 TeV 1 EeV1 TeV100 GeV10 GeV1 GeV100 MeV10 MeV

IceCube

Page 32: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube

32

• 78 Strings

• 125m string spacing

• 17m DOM spacing

• Add 8 strings

• 75m string spacing

• 7m DOM spacing

• Add 20 strings

• 26m string spacing

• 5m DOM spacing10 TeV 1 EeV1 TeV100 GeV10 GeV1 GeV100 MeV10 MeV

IceCube

125m

Page 33: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube + DeepCore

• 78 Strings

• 125m string spacing

• 17m DOM spacing

• Add 8 strings

• 75m string spacing

• 7m DOM spacing

• Add 20 strings

• 26m string spacing

33

75m

10 TeV 1 EeV1 TeV100 GeV10 GeV1 GeV100 MeV10 MeV

DeepCore IceCube

125m

Page 34: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

The IceCube Neutrino Telescope

34

IceCube

DeepCore

Skiway

South Pole Station

Page 35: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

DeepCore Results

35

Phys. Rev. D 91 072004 (2015)

• Approximately 3 years of data analyzed

• High rate in detector provides large event sample

• Oscillation parameter constraints approaching those of dedicated experiments

Page 36: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

DeepCore Results

36

• Approximately 3 years of data analyzed

• High rate in detector provides large event sample

• Oscillation parameter constraints approaching those of dedicated experiments

Phys. Rev. D 91 072004 (2015)

Page 37: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Even Lower Energies

• Deep Core is a success, but we get access to more physics with a lower threshold

37

• muon neutrino disappearance

• maximal θ23 measurement

• lower energy dark matter

• neutrino mass hierarchy

Page 38: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

IceCube + DeepCore• 78 Strings

• 125m string spacing

• 17m DOM spacing

• Add 8 strings

• 75m string spacing

• 7m DOM spacing

• Add 20 strings

• 26m string spacing

38

75m

10 TeV 1 EeV1 TeV100 GeV10 GeV1 GeV100 MeV10 MeV

DeepCore IceCube

125m

Page 39: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

• 78 Strings

• 125m string spacing

• 17m DOM spacing

• Add 8 strings

• 75m string spacing

• 7m DOM spacing

• Add 40 strings

• 22m string spacing

• 3m DOM spacing

39

IceCube + DeepCore + PINGU

125m22m

75m

10 TeV 1 EeV1 TeV100 GeV10 GeV1 GeV100 MeV10 MeV

DeepCorePINGU IceCube

Page 40: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Improvement with PINGU

40

DeepCore PINGU

Neutrino energy: 12 GeV Lepton energy: 10 GeV

Page 41: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

The IceCube Neutrino Telescope

41

IceCube

DeepCore

PINGU

High EnergyExtension

Skiway

South Pole Station

Page 42: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Mass Hierarchy Determination

42

1

1

Page 43: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016 43

1

1

2

2

Mass Hierarchy Determination

Page 44: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrino Oscillograms

• The cross-section and flux are different for νμ and νμ

• The patterns are therefore different!

44

Page 45: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrino Oscillograms

• Sum of νμ and νμ

• Reconstruction and PID not included here

45

Page 46: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Neutrino Oscillograms

46

• Sum of νμ and νμ

• Reconstruction and PID not included here

Page 47: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

So Why am I Talking Here?

• PINGU is investigating using new DOMs with multiple PMTs

• Need to study how these would work in a low background environment

47

Page 48: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

So Why am I Talking Here?

• PINGU is investigating using new DOMs with multiple PMTs

• Need to study how these would work in a low background environment

48

Page 49: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Conclusion

• IceCube and DeepCore have been very successful and have shown that particle physics is possible in ice

• PINGU will provide insight into the nature of the NMH as well as the oscillation parameters

• SNOLAB is an ideal site to test the new PMT structures

49

Page 50: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016

Exciting Times To Come!

50

Page 51: Ken Clark, SNOLAB

SNOLAB Users Meeting - Sept 1, 2016 51

SNOLAB