Precision measurement and new physics searches by neutrino ...

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物理学院 SCHOOL OF PHYSICS Precision measurement and new physics searches by neutrino oscillation experiments Jian Tang [email protected] Seminar @ SJTU & TDLi Institute, Sept. 30 Collaborators: Yong Du, Hao-Lin Li, Jiang-HaoYu (CAS-ITP) Zhuo-Jun Hu, Jia-Jie Ling, Sampsa Vihonen, Tse-Chun Wang, Yi-Bing Zhang Ref: JHEP01(2021)124, JHEP03(2021)019, arXiv: 2106.15800

Transcript of Precision measurement and new physics searches by neutrino ...

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物理学院SCHOOL OF PHYSICS

Precision measurement and new physics searches by neutrino oscillation experiments

Jian Tang

[email protected]

Seminar @ SJTU & TDLi Institute, Sept. 30

Collaborators:

Yong Du, Hao-Lin Li, Jiang-Hao Yu (CAS-ITP)

Zhuo-Jun Hu, Jia-Jie Ling,

Sampsa Vihonen, Tse-Chun Wang, Yi-Bing Zhang

Ref: JHEP01(2021)124, JHEP03(2021)019, arXiv: 2106.15800

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Table of contents

• Motivations

• Non-unitarity(NU) v.s non-standard interactions(NSIs)

• Global fits of mixing parameters without unitarity

• Constraints of NSIs based on SMEFT

• Summary

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Three-generation neutrino oscillations

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• For 3 ν framework , we have 6+1 free parameters in neutrino oscillations:

P (θ12, θ13, θ23, δ, Δm212, Δm31

2) + ρ (in matter)√ √ √ √? √?

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Where are neutrinos from?

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Natural source

Artificial source

10-4 10-3 104103 105 106 107 1010109 1011108 1012

keV MeV GeV TeV

E [eV]

~Electron mass ~Proton mass ~LHC

???

???

??

??

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Working principles of neutrino oscillation experiments

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• Get the neutrino source as clean as possible. Muon decay v.s pion decay beams.

• Deploy the best detector to reconstruct the oscillated neutrino spectra: Gd-WC, LAr

TPC, scintillator detector with flavour&charge identifications…

• Data mining: precision measurement & discovery of new physics…

Neutrino source

Near detector(cancellation of

systematics in flux&X-section...)

Far detector

Baseline

L ~ E/m2

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An example: T2K

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K. McFarland, Neutrino InteractionUncertainties @ NNN2018

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Simulations of neutrino oscillations w/o new physics

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By GLoBES

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Lots of neutrino experiments to get a new horizon

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More are coming…

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WC detectors: KamiokandeSKHyperK

• Bigger than bigger! PMT technology revolutionized!

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3 kton WC 20% coverage

with 20’’ PMT

50 kton WC 40% coverage

with 20’’ PMT

260 kton WC 40% coverage

with 20’’+HQE PMT

• Construction started in 2020.

• Data taking from 2027.

• J-PARC neutrino beam will be upgraded from 0.7 to 1.3 MW

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LAr TPC: DUNE

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Courtesy: Guang Yang@NuFact2021

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LSc: DYB (20 t*8) JUNO (20 kt)

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• Daya Bay neutrino experiment: mission completed!

Credit: Miao He

Dec. 12, 2020

MCP-PMT

20’’+HQE

MH sensitivity:

∆χ2= 15.07

By GLoBES

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NuFACT2021: WG1 proposed questions

• What is the neutrino mass ordering?

• Are there CP violations in the lepton sector?

• How much precision shall we reach to tell new physics?

• What are the current and future systematic limitations on precision measurement and how to address them?

• Is the neutrino mixing matrix unitary?

• Are there non-standard neutrino interactions?

• Are there more than three-flavor neutrinos?

• How to deal with the reactor flux deficit?

• How consistent are results from NOvA and T2K?

• How to examine neutrino mass models based on flavor symmetries (A4, S4, Modular…)?

• What’s next even after neutrino mass ordering and Dirac CP phase?

• …

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Table of contents

• Motivations

• Non-unitarity(NU) v.s non-standard interactions(NSIs)

• Global fits of mixing parameters without unitarity

• Constraints of NSIs based on SMEFT

• Future prospects

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Non-unitary neutrino mixings (NU)

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Non-Standard Interactions (NSIs)

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NSI happens to neutrino propagation in matter NSI at neutrino productions

• New physics beyond SM: new particles, new couplings,

new phenomenon...

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Discovery of CPV affected by NU/NSIs

16Phys.Rev.D 95 (2017) 3, 033005JHEP 10 (2016) 138 by Dr. Shao-Feng Ge

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Table of contents

• Motivations

• Non-unitarity(NU) v.s non-standard interactions(NSIs)

• Global fits of mixing parameters without unitarity

• Constraints of NSIs based on SMEFT

• Future prospects

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• Reduced constraints without the unitary assumption in the quark mixing.

• Let’s keep the democratic way in quark and lepton mixing?18

What if there is non-unitary mixing?

?

Lepton mixing

www.nu-fit.org

No unitarity assumption here!

Quark mixing

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Simple mathematics w/o unitarity assumption

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Unitarity

Non-unitarity(NU)

• Only 4 real parameters with unitarity.

• Now we have 13 real parameters after rephrasing fields for NU!

18 real parameters in linear algebra

-5 by rephrasing fields in physics

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What if there is non-unitary mixing?

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• Correlations between 3nu mixing matrix

elements without unitarity assumption.

• Octant degeneracies get worse for NU.

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What if there is non-unitary mixing?

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• Nice precision in the first and second row/column.

• Tau neutrino physics are to be improved for better constraints on 3rd row/column!

ClosureNormalizations

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Table of contents

• Motivations

• Non-unitarity(NU) v.s non-standard interactions(NSIs)

• Global fits of mixing parameters without unitarity

• Constraints of NSIs based on SMEFT

• Future prospects

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Working principle of effective field theory (EFT)

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EFT: connecting low-energy phenomenon to high-energy scale

Credit: Adam Falkowski

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• Start from a UV theory

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• Matching by covariant derivative expansion, EoM

• Solve for classical solution

An example for demonstration

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An example for demonstration

• Put the classical solution back to Lagrangian density

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• Fierz transformation to Warsaw basis

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An example for demonstration

• Run down from scale M to electroweak scale v

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• Probably generate non-zero Wilson coefficients other than Cle

• Matching at electroweak scale to LEFT

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Matching between QM and QFT NSIs

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• QM NSIs are fully independent without much info

about the underlying theory.

• QFT NSIs allow their correlations.

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EFT: connecting low-energy phenomenon to high-energy scale

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• Dimension-6 operators only

• Neutrino masses are generated by

dimension-5 Weinberg operators

Effective operators

Cut-off scale

Wilson coefficient

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SMEFT-NSIs by T2K and NOvA

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• T2K and NOvA are already sensitive to new physics around 20 TeV.

• Correlations among different dimension-6 operators play important roles.

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SMEFT-NSIs by reactor neutrino experiments

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• Reactor neutrino experiments are sensitive to new physics around 5 TeV.

• Complementarity between LBL and reactor expts due to different sets of operators

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Table of contents

• Motivations

• Non-unitarity(NU) v.s non-standard interactions(NSIs)

• Global fits of mixing parameters without unitarity

• Constraints of NSIs based on SMEFT

• Future prospects on SMEFT-NSIs

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Democratic treatment of CKM and PMNS mixing

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Smelli

Quark mixing v.s neutrino mixing/scattering

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SMEFT-NSIs by T2HK and DUNE

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NC-NSIs

CC-NSIs

• Cover 1635 SMEFT operators in dimention-6. ND is important to constraint SMEFT-NSIs.

• DUNE has better sensitivity than T2HK due to the longer baseline.

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SMEFT-NSIs by JUNO w/o TAO and COHERENT

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CC-NSIs

NC-NSIs

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Summary

• Neutrino oscillation is the first direct evidence BSM.

• Discovery of CPV & determination of MH is around the corner. Neutrino will be used for new physics searches.

• New physics might be hidden in the uncertainties.

• Unitary mixing should not be taken by default, as tau neutrino-related part is yet to be improved.

• We can have better knowledge of underlying theory by RGE running and matching in different scales to connect the low-energy neutrino oscillation experiments and the UV completion model in SMEFT.

• Let’s work together to discover new physics with neutrinos…

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Precision measurement and tau-neutrino physics?

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• Pushing precision to sub-percent level and probe new physics

arXiv:2108.11107

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THANK YOU

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