Non-Standard Interaction of Solar Neutrinos in Dark Matter ... · Dark Matter Detectors Shu Liao...

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MotivationCombination of oscillation and CEnNS

Future work and conclusion

Non-Standard Interaction of Solar Neutrinos inDark Matter Detectors

Shu Liao

Texas A&M University

Collaboration with: J. Dent, B. Dutta, J. Newstead, L. Strigariand J. Walker

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Outline

1 MotivationNon-standard interactions of neutrinoTransition probability of solar neutrinoCurrent constrains

2 Combination of oscillation and CEnNSExpected number of events under NSIOscillation effects

3 Future work and conclusionResolving degeneraciesConclusion

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Non-standard interactions of neutrinoTransition probability of solar neutrinoCurrent constrains

Non-standard interactions of neutrinos

General four fermion interaction:

Lint = 2p2GF ⌫↵L�

µ⌫�L

⇣✏fL↵� fL�µfL + ✏fR↵� fR�µfR

⌫�

⌫↵

f

f

= SM +BSM

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Non-standard interactions of neutrinoTransition probability of solar neutrinoCurrent constrains

Differential cross section

Differential cross section of ⌫� + f ! ⌫↵ + f as a function of recoilenergy Er:

d�

dEr=

2

⇡G2

Fmf⇥"���✏fL↵�

���2+���✏fR↵�

���2✓1� Er

E⌫

◆2

� 1

2

⇣✏fL⇤↵� ✏fR↵� + ✏fL↵�✏

fR⇤↵�

⌘ mfEr

E2⌫

#

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Non-standard interactions of neutrinoTransition probability of solar neutrinoCurrent constrains

Cross section on nucleus

✏L↵↵ ! 1

2Z✏pV↵↵ +

1

2(Z+ � Z�) ✏

pA↵↵ +

1

2N✏nV↵↵ +

1

2(N+ �N�) ✏

nA↵↵

✏R↵↵ ! 1

2Z✏pV↵↵ � 1

2(Z+ � Z�) ✏

pA↵↵ +

1

2N✏nV↵↵ � 1

2(N+ �N�) ✏

nA↵↵

d�

dEr! d�

dEr⇥ F 2

�Q2

✏pV↵↵ =1

2� 2 sin2 ✓w + 2✏uV↵↵ + ✏dV↵↵

✏pA↵↵ =1

2+ 2✏uA↵↵ + ✏dA↵↵

✏nV↵↵ = �1

2+ ✏uV↵↵ + 2✏dV↵↵

✏pA↵↵ = �1

2+ ✏uA↵↵ + 2✏dA↵↵

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Non-standard interactions of neutrinoTransition probability of solar neutrinoCurrent constrains

Transition probability of solar neutrino

The propagation of neutrino is described by:

H�↵ =

Udiag

✓0,

�m221

2E,�m2

31

2E

◆U †

�↵

+p2GF

X

f

nf

⇣�ef�e↵ + ✏f�↵

U : mixing matrix, �m2ij = m2

i �m2j , nf : number density of

fermion f .Neutrino propagates through the sun adiabatically (diagonalize Hinto UdiagU †):

P�!↵ =���U (t)↵k

���2��A1

jk

��2��A2ij

��2���U (0)�i

���2

A: transition probability between mass eigenstate when resonancehappens.

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Non-standard interactions of neutrinoTransition probability of solar neutrinoCurrent constrains

Current constraints

(a) Gonzalez-Garcia et al,

arXiv:1307.3092

(b) Coloma et al, arXiv:1701.04828

Figure: Current constraints

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Expected number of events under NSIOscillation effects

Electron scattering ⌫� + e ! ⌫↵ + e

Figure: Number of events above an equivalent electron recoil energythreshold of 1 keV as each ✏ varies over its allowable range (blue curves).Orange curve: SM contribution.

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Expected number of events under NSIOscillation effects

Nucleus scattering ⌫� +N ! ⌫↵ +N

Figure: Number of events above an equivalent nucleus recoil energythreshold of 1 keV as each e varies over its allowable range (blue curves).Orange curve: SM contribution.

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Expected number of events under NSIOscillation effects

LMA-Dark solution

✓12 ! ⇡

2� ✓12

✓13 ! ⇡ � ✓13

� ! ⇡ � �

�m231 ! ��m2

32

✏ ! �✏⇤

H ! �H⇤

Figure: Number of events for LMA-d solution withdifferent threshold energies.

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Expected number of events under NSIOscillation effects

Threshold

Figure: Number of events with different threshold energies.

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Expected number of events under NSIOscillation effects

Oscillation vs. no oscillation

✏eLee = 0.052 ✏uee = 0.2 ✏dee = 0.17U�mU † +

p2Gfdiag (1, 0, 0) +

p2Gf ✏ 1.10 0.69 0.69

U�mU † +p2Gfdiag (1, 0, 0) +

p2Gf ✏ 1.12 0.67 0.67

U�mU † +p2Gfdiag (1, 0, 0) +

p2Gf ✏ 1.13 0.44 0.44

U�mU † +p2Gfdiag (1, 0, 0) +

p2Gf ✏ 1.72 3.88⇥ 10�5 1.18⇥ 10�3

Table: Ratio to only SM prediction N/NSM

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Expected number of events under NSIOscillation effects

Survival probability due to NSI

Figure: Electron neutrino survival probability for the SM (blue) comparedto cases in of NSI.

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Resolving degeneraciesConclusion

Oscillations

Figure: Oscillation experiment can only detect ✏ee � ✏µµ, Coloma et al.2017

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Resolving degeneraciesConclusion

Complementarity of various experiments

Reactor + SNS + Solar-DM = constraints on ✏ee � ✏µµ? u and ddegeneracy?

Figure: Combining different result togetherShu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

+
=

MotivationCombination of oscillation and CEnNS

Future work and conclusion

Resolving degeneraciesConclusion

Conclusion

1 Direct dark matter searches are able to probe NSI parameterspace that cannot be probed by current neutrino experiments.

1 A low threshold detector is more likely to be able to observesignificant number of events

2 Due to interference between SM and BSM, number ofobserved events can be lower than SM expectations.

2 Uncertainties of additional NSI parameters will not only affectthe detection side, but also affect the solar neutrino flux.

Shu Liao Non-Standard Interaction of Solar Neutrinos in Dark Matter Detectors

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