Sterile Neutrino Searches with MINOS+ Leigh Whitehead Birmingham - - PowerPoint PPT Presentation
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
Leigh Whitehead
Outline
- Introduction
- MINOS+ Experiment
- Three flavour oscillation results
- Four flavour oscillation results
2
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
Leigh Whitehead
Neutrinos
- For three neutrino flavours:
4 Leigh Whitehead
Flavour eigenstates: Mass eigenstates: 3x3 unitary matrix – the PMNS matrix
L
4
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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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
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?
MINOS and MINOS+
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.
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Far Detector 735 km from beam target 5.4 kton mass Near Detector 1 km from beam target 1 kton mass
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
Leigh Whitehead
Data Samples
- Results shown today use all MINOS and 2/3 years of MINOS+
data
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10.56 x 1020 POT MINOS 5.80 x 1020 POT MINOS+
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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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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.
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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
Three Flavour Oscillation Analysis
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
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
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
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
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
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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
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
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
Beyond Three Neutrino Flavours
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
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
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
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.
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
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]
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]
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).
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
MINOS+ Four Flavour Oscillation Analysis
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
Leigh Whitehead
Sterile Oscillations in MINOS+
36
P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41
<latexit sha1_base64="x/LYc86yKUOtQl4+Uz2kQjK8J4k=">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</latexit>Leigh Whitehead
Sterile Oscillations in MINOS+
37
P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41
<latexit sha1_base64="x/LYc86yKUOtQl4+Uz2kQjK8J4k=">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</latexit>Leigh Whitehead
Sterile Oscillations in MINOS+
38
P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41
<latexit sha1_base64="x/LYc86yKUOtQl4+Uz2kQjK8J4k=">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</latexit>Leigh Whitehead
Sterile Oscillations in MINOS+
39
P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41
<latexit sha1_base64="x/LYc86yKUOtQl4+Uz2kQjK8J4k=">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</latexit>Leigh Whitehead
Sterile Oscillations in MINOS+
40
P (νµ → νµ) ≈1 − sin2 2θ23 cos 2θ24 sin2 ∆31 − sin2 2θ24 sin2 ∆41
<latexit sha1_base64="x/LYc86yKUOtQl4+Uz2kQjK8J4k=">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</latexit>- 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
- 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
Leigh Whitehead
Systematic Uncertainties: NC
43
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
Leigh Whitehead
Systematic Uncertainties: CC
45
Near Detector Far Detector
Leigh Whitehead
Systematic Uncertainties: CC
46
Strong correlations between the detectors gives strong cancellation of systematic uncertainties
- 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
<latexit sha1_base64="g9erNhbBxtvSR6tmR+krIZHNug=">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</latexit>- 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).
- 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).
- 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
- 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).
- 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
Leigh Whitehead
Combination with Daya Bay
53 P . Adamson, et al., https://arxiv.org/abs/2002.00301
- 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