Sterile Neutrino Searches with MINOS+ Leigh Whitehead Birmingham - - PowerPoint PPT Presentation

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Sterile Neutrino Searches with MINOS+ Leigh Whitehead Birmingham - - PowerPoint PPT Presentation

Sterile Neutrino Searches with MINOS+ Leigh Whitehead Birmingham HEP Seminar 29/04/20 Outline Introduction MINOS+ Experiment Three flavour oscillation results Four flavour oscillation results Leigh Whitehead 2 Neutrinos


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SLIDE 1

Sterile Neutrino Searches with MINOS+

Leigh Whitehead

Birmingham HEP Seminar 29/04/20

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SLIDE 2

Leigh Whitehead

Outline

  • Introduction
  • MINOS+ Experiment
  • Three flavour oscillation results
  • Four flavour oscillation results

2

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SLIDE 3

Leigh Whitehead

Neutrinos

  • Neutrino oscillations have become a well-established and

well-described phenomenon over the last 20 years.

  • The Nobel Prize in Physics 2015 was awarded jointly to Takaaki

Kajita and Arthur B. McDonald "for the discovery of neutrino

  • scillations, which shows that neutrinos have mass"
  • Oscillations arise from the quantum mechanical

interference between the neutrino mass states.

  • At least two of the neutrinos must be massive!
  • The neutrino eigenstates of the weak interaction are not

the same as the mass eigenstates.

3

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SLIDE 4

Leigh Whitehead

Neutrinos

  • For three neutrino flavours:

4 Leigh Whitehead

Flavour eigenstates: Mass eigenstates: 3x3 unitary matrix – the PMNS matrix

L

4

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SLIDE 5

Leigh Whitehead

Neutrinos

  • For three neutrino flavours:
  • Three mixing angles and a CP violating phase.
  • Oscillations are driven by mass-squared splittings

5

Muon neutrino disappearance
 (accelerator and atmospheric) Electron antineutrino disappearance (reactor) Electron neutrino appearance (accelerator) (Anti)electron neutrino disappearance
 (solar and reactor)

P (νµ → νµ) ≈ 1 − sin2 2θ23 sin2 ✓1.27∆m2

31L

E ◆

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SLIDE 6

Leigh Whitehead

Mass Hierarchy

  • The order of all the mass states isn’t completely known.
  • The sign of is known from matter effects in the Sun

and from the definition of having the largest component.

  • The sign of is still unknown.

6

Δm232 Δm221 ν1 ν2 ν3 ντ νµ νe Δm221 ν1 ν2 ν3 Δm232 Normal Hierarchy Inverted Hierarchy

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SLIDE 7

Leigh Whitehead

Current State of Measurements

  • Very successful programme 

  • f measurements.
  • The remaining unknowns:
  • Is the mass-hierarchy
  • Normal > 0?
  • Inverted < 0?

  • Is = 45o?
  • If not, is it higher or lower?

  • What is the value of ?
  • Is there CP violation in the neutrino 


sector?

7

Esteban, I., Gonzalez-Garcia, M.C., Hernandez-Cabezudo, A. et al. J. High

  • Energ. Phys. (2019) 2019: 106. https://doi.org/10.1007/JHEP01(2019)106

Nu-Fit v4.0

  • How many neutrinos are there?
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SLIDE 8

MINOS and
 MINOS+

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SLIDE 9

Leigh Whitehead

The MINOS+ Experiment

  • MINOS/MINOS+ had two functionally identical, magnetised,

tracking, sampling calorimeters.

  • Can distinguish muon charge from the curvature.
  • Exposed by the NuMI beam at Fermilab.
  • MINOS+ is the continuation of MINOS into the NOvA era at

FNAL.

9

Far Detector 735 km from beam target 5.4 kton mass Near Detector 1 km from beam target 1 kton mass

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SLIDE 10

Leigh Whitehead

The NuMI Beam

  • MINOS+ collected neutrinos from the NuMI beam at

Fermilab.

  • Neutrinos produced by decay of 


focused mesons produced in the target.

  • Polarity of the horns can be reversed to


produce an antineutrino beam.

10

120 GeV
 protons from
 Main Injector

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SLIDE 11

Leigh Whitehead

Data Samples

  • Results shown today use all MINOS and 2/3 years of MINOS+

data

11

10.56 x 1020 POT MINOS 5.80 x 1020 POT MINOS+

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SLIDE 12

Leigh Whitehead

Neutrino Interactions in MINOS+

  • There are three main types of interactions seen in MINOS+

12

νµ charged-current ν neutral-current νe charged-current

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SLIDE 13

Leigh Whitehead

NC Event Selection

  • The first step is to select the neutral current interactions.
  • Two main selection criteria:
  • Event length and the extension of the track beyond the hadronic

shower.

13

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SLIDE 14

Leigh Whitehead

CC Event Selection

  • Charged current interactions are selected from those that

do not pass the neutral current selection.

  • Use a kNN to select CC interactions from the backgrounds.
  • Uses four topological and energy deposition variables as input.

14

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SLIDE 15

Three Flavour
 Oscillation Analysis

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SLIDE 16

Leigh Whitehead

Beam Neutrinos - Flux Prediction

  • In our three-flavour analysis we use the ND to tune the MC
  • A special sample with the magnetic horns switched off

allows us to probe hadron production effects

16

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SLIDE 17

Leigh Whitehead

Beam Neutrinos - Flux Prediction

  • In our three-flavour analysis we use the ND to tune the MC
  • We then apply these hadron production weights to the

standard horn on MC

17

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Leigh Whitehead

Beam Neutrinos - Flux Prediction

  • In our three-flavour analysis we use the ND to tune the MC
  • Finally, we fit the standard hour on MC to tune the beam

focussing component of the flux prediction

18

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SLIDE 19

Leigh Whitehead

Beam Neutrinos

  • MINOS was designed to measure the atmospheric scale
  • scillation parameters.
  • Look for disappearance of muon neutrinos in the FD relative to ND.
  • Measure muon neutrinos through charged current interactions.

19

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SLIDE 20

Leigh Whitehead

Atmospheric Neutrinos

  • The MINOS+ Far Detector has collected a large number of

atmospheric neutrinos over 12 years

  • Neutrinos and anti-neutrinos separated by curvature in

the magnetic field

20

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SLIDE 21

Leigh Whitehead

Atmospheric Neutrinos

  • The MINOS+ Far Detector has collected a large number of

atmospheric neutrinos over 12 years

  • Neutrinos and anti-neutrinos separated by curvature in

the magnetic field

21

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SLIDE 22

Leigh Whitehead

Three Flavour Oscillations

  • Fit gives 1D and 2D contours

22

Best fit Δm2

32 = 2.42x10-3 eV2

sin2θ23 = 0.42 |Δm2

32| 90% C.L. intervals

NH: (2.28 – 2.55) x 10-3 eV2 IH: (2.33 – 2.60) x 10-3 eV2 Measured to ~3.5% at 68% C.L. sin2θ23 90% C.L. interval 0.36 – 0.65

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SLIDE 23

Leigh Whitehead

Three Flavour Oscillations

  • Fit gives 1D and 2D contours

23

Best fit Δm2

32 = 2.42x10-3 eV2

sin2θ23 = 0.42 |Δm2

32| 90% C.L. intervals

NH: (2.28 – 2.55) x 10-3 eV2 IH: (2.33 – 2.60) x 10-3 eV2 Measured to ~3.5% at 68% C.L. sin2θ23 90% C.L. interval 0.36 – 0.65

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SLIDE 24

Beyond Three
 Neutrino Flavours

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Leigh Whitehead

How Many Neutrinos?

  • Invisible width of the Z-boson from LEP very strongly

measured that there are 3 neutrinos.

  • For fourth neutrino 



 must not couple to the Z-boson.

  • Hence the name sterile.
  • Results from Planck:

25

P . A. R. Ade, et al. (2016) Astron. Astrophys. 594, arXiv 1502.01589

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SLIDE 26

Leigh Whitehead

Some Anomalies

  • The majority of neutrino oscillation data is well described

by the three flavour model.

  • However, there are some outliers.
  • Anomalous appearance of in short-baseline beams.
  • Gallium experiment calibration sources.
  • Reactor neutrino flux deficit.
  • The main point is that all three anomalies were consistent

with oscillations at a mass-splitting scale of approximately 1 eV2

26

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SLIDE 27

Leigh Whitehead

Some Anomalies - 1

  • LSND saw an excess of
  • Could be interpreted as oscillations at 


a mass-splitting scale of approximately 
 1 eV2

  • However, KARMEN2 saw results 


consistent with expectation.

27

  • The MiniBooNE experiment was devised

to investigate these differing results…

  • Looked at and

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SLIDE 28

Leigh Whitehead

Some Anomalies - 1

  • MiniBooNE saw excess appearance in 


both neutrino and anti neutrino channels.

  • Not identical to LSND, but allowed 


similar regions of phase-space.

28

  • A. Aguilar-Arevalo et al. Phys. Rev. Lett. 121 (2018), p. 221801.
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SLIDE 29

Leigh Whitehead

Some Anomalies - 2

  • GALLEX and SAGE were two


solar neutrino experiments.

  • Calibrated using 


radioactive sources.

  • Measured rates from the 


calibration sources showed 
 consistent deficits.

  • Again, consistent with a 


1 eV2 mass-splitting.

29

Gariazzo et al. J.Phys. G43 (2016) 033001 DOI:10.1088/0954-3899/43/3/033001

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Leigh Whitehead

Some Anomalies - 3

  • The majority of reactor neutrino experiments have seen a

deficit of .

  • Again, consistent with a 1 eV2 mass-splitting, but…

30

Gariazzo et al. (2017). arXiv: 1703.00860 [hep-ex]

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SLIDE 31

Leigh Whitehead

Some Anomalies - 3

  • Daya Bay released results from studying their flux as a

function of reactor fuel cycles to extract information on the uranium and plutonium components.

  • Flux deficit appears to only come


from the uranium flux.

  • The sterile neutrino hypothesis


for the reactor anomaly is:
 “incompatible with Daya Bay’s


  • bservation at 2.6σ”.

31

An et al. (2017). arXiv: 1704.01082 [hep-ex]

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SLIDE 32

Leigh Whitehead

Null Results

  • A number of muon neutrino disappearance experiments see

no evidence of a sterile neutrino.

  • MiniBooNE + SciBooNE
  • MINOS
  • IceCube
  • CDHS
  • CCFR
  • Super-K

32

  • M. G. Aartsen et al. Phys. Rev.
  • Lett. 117, 071801 (2016)


P . Adamson et al., Phys. Rev. Lett. 117, 151803 (2016).


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SLIDE 33

Leigh Whitehead

Four Flavour Formalism

  • Most common extension to include a 4th neutrino is the 3+1

model.

  • PMNS matrix becomes 4 x 4
  • Three new mixing angles: 


θ14 , θ24 and θ34

  • Two new CP phases:


𝜀14 and 𝜀24

  • Three new mass-splittings,


but only one is independent.

  • Δm241

33

ν1 ν2 ν3 ντ νµ νe ν4 νs Δm241

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SLIDE 34

MINOS+ Four Flavour
 Oscillation Analysis

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SLIDE 35

Leigh Whitehead

Sterile Oscillations in MINOS+

  • MINOS+ is sensitive to three of the sterile oscillation

parameters.

  • Muon neutrino disappearance: θ24 and Δm241
  • Measured with muon neutrino charged-current events.
  • Active neutrino disappearance: θ24 , θ34 and Δm241
  • Measured using neutral-current interactions.
  • Sensitivity reduced compared to CC due to worse energy resolution

and lower cross-section.

  • Oscillations can cause effects in both detectors depending
  • n the value of Δm241

35

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SLIDE 36

Leigh Whitehead

Sterile Oscillations in MINOS+

36

P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41

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SLIDE 37

Leigh Whitehead

Sterile Oscillations in MINOS+

37

P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41

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SLIDE 38

Leigh Whitehead

Sterile Oscillations in MINOS+

38

P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41

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SLIDE 39

Leigh Whitehead

Sterile Oscillations in MINOS+

39

P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41

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SLIDE 40

Leigh Whitehead

Sterile Oscillations in MINOS+

40

P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41

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SLIDE 41
  • The previous MINOS sterile neutrino 


analysis used the ratio of the Far and 
 Near spectra.

  • Can’t use the ND to tune the MC like


in our three-flavour analysis.

  • Many systematics cancel in the ratio.
  • Uncertainty in the ratio was dominated by FD statistics.

Leigh Whitehead

Analysis Method

41

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SLIDE 42
  • We have now moved to a simultaneous two detector fit.
  • Use the a-priori flux prediction from MINERvA [1]
  • We use a single covariance matrix that encapsulates the

correlations between the systematic uncertainties.

  • This still enables us to have some cancellation of the systematic

uncertainties without using the Far-over-Near ratio.

  • Consider a total of 44 systematic uncertainties across the

different event selections.

Leigh Whitehead

The Two Detector Fit

42 [1] L. Aliagia, et al, Phys. Rev. D 94, 092005, 2016

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SLIDE 43

Leigh Whitehead

Systematic Uncertainties: NC

43

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SLIDE 44

Leigh Whitehead

Systematic Uncertainties: NC

44

Diagonal components
 form the bands below Correlations between the two detectors Near Detector Far Detector Near Detector Far Detector

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SLIDE 45

Leigh Whitehead

Systematic Uncertainties: CC

45

Near Detector Far Detector

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SLIDE 46

Leigh Whitehead

Systematic Uncertainties: CC

46

Strong correlations between the detectors gives strong cancellation of systematic uncertainties

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SLIDE 47
  • Perform a fit to minimise the following for both the CC and

NC samples

  • We fit for Δm241, Δm232, θ23, θ24 and θ34
  • Global best fit values are used for Δm221, θ12 and θ13
  • The other parameters have a negligible effect on the

analysis and are set to zero: θ14, δ13, δ14 and δ24

  • Penalty term prevents from Δm232 becoming degenerate

with Δm241

Leigh Whitehead

The Fit Procedure

47

χ2 =

N

X

i=1 N

X

j=1

(xi − µi) ⇥ V −1⇤

ij (xj − µj) + penalty

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SLIDE 48
  • Spectra shown after correcting the prediction after

decorrelation of the covariance matrix

Leigh Whitehead

Event Spectra: NC Selection

48

P . Adamson et al., Phys. Rev. Lett. 122, 091803 (2019).

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SLIDE 49
  • Spectra shown after correcting the prediction after

decorrelation of the covariance matrix

Leigh Whitehead

Event Spectra: CC Selection

49

P . Adamson et al., Phys. Rev. Lett. 122, 091803 (2019).

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SLIDE 50
  • Best fit point:

Δm2

41 = 2.33x10-3 eV2

sin2θ24 = 1.1x10-4 θ34 < 8.4x10-3 sin22θ23 = 0.92 χ2

min/dof = 99.3/140

χ2(4ν) – χ2(3ν) = 0.01

Leigh Whitehead

The Fit Result

50

P . Adamson et al., Phys. Rev. Lett. 122, 091803 (2019).

Excluded region

slide-51
SLIDE 51
  • Best fit point:

Δm2

41 = 2.33x10-3 eV2

sin2θ24 = 1.1x10-4 θ34 < 8.4x10-3 sin22θ23 = 0.92 χ2

min/dof = 99.3/140

χ2(4ν) – χ2(3ν) = 0.01

Leigh Whitehead

Comparison with Other Results

51

P . Adamson et al., Phys. Rev. Lett. 122, 091803 (2019).

slide-52
SLIDE 52
  • MINOS+ sensitive to
  • Daya Bay ve disappearance sensitive to
  • Combine to probe the same parameter-space as LSND and

MiniBooNE:

Leigh Whitehead

Combination with Daya Bay

52

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SLIDE 53

Leigh Whitehead

Combination with Daya Bay

53 P . Adamson, et al., https://arxiv.org/abs/2002.00301

slide-54
SLIDE 54
  • MINOS/MINOS+ has produced


its final three flavour muon
 neutrino disappearance 
 result

  • Very high statistics 


covering the entire 


  • scillation dip
  • Measured Δm2

32 to 3.5%


  • The four-flavour analysis gives a leading exclusion on the

sterile neutrino hypothesis over many orders of magnitude in Δm2

41

Leigh Whitehead

Summary

54

slide-55
SLIDE 55

Thank You!
 Any Questions?