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DAMA/LIBRA-phase2 in WIMP effective models SUNGHYUN KANG IN COLLABORATION WITH S. SCOPEL, G. TOMAR, J.H. YOON SOGANG UNIVERSITY

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Page 1: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

DAMA/LIBRA-phase2 in WIMP effective modelsSUNGHYUN KANG

IN COLLABORATION WITH S . SCOPEL , G. TOMAR, J .H. YOON

SOGANG UNIVERSITY

Page 2: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

Introduction

Many evidences of Dark Matter

CDM(Cold Dark Matter)

Neutrino

WIMP

(Weakly Interacting Massive Particle)

"Content of the Universe - Pie Chart“Wilkinson Microwave Anisotropy Probe.

National Aeronautics and Space Administration. Retrieved 9 January 2018.

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DAMA/LIBRA-phase2 analyses

Bernabei et al. (DAMA Collaboration), 1805.10486

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DAMA/LIBRA-phase2 analyses

A. L. Fitzpatrick, W. Haxton, E. Katz, N. Lubbers, and Y. Xu, The Effective Field Theory of Dark Matter Direct Detection, JCAP 1302 (2013) 004

τ : isospinj : interaction type

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DAMA/LIBRA-phase2 analyses

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon DAMA/LIBRA-phase2 in WIMP effective models, JCAP07(2018)016

𝑅𝑙ττ′: WIMP response function

𝑊𝑙ττ′: nucleus response function: M, Σ’, Σ’’, Δ, φ’’, φ’ (M=SI, , Σ’, Σ’’=SD)

(from Nikhil Anand, A. Liam Fitzpatrick, W. C. Haxton,Model-independent WIMP Scattering Responses and EventRates : A Mathematica Package for Experimental Analysis)

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DAMA/LIBRA-phase2

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon DAMA/LIBRA-phase2 in WIMP effective models, JCAP07(2018)016

Considering one EFT coupling at a time

Page 7: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

DAMA/LIBRA-phase2 analyses

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon DAMA/LIBRA-phase2 in WIMP effective models, JCAP07(2018)016

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DAMA/LIBRA-phase2 analyses

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon DAMA/LIBRA-phase2 in WIMP effective models, JCAP07(2018)016

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DAMA/LIBRA-phase2 analyses

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon DAMA/LIBRA-phase2 in WIMP effective models, JCAP07(2018)016

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DAMA/LIBRA-phase2

Page 11: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

DAMA/LIBRA-phase2

Page 12: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

Anapole Dark Matter(ADM)

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon, P. Gondolo, Anapole Dark Matter after DAMA/LIBRA-phase2, arXiv:1808.04112

Electric, velocity dependent part

Magnetic, velocity independent part

Page 13: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

Anapole Dark Matter(ADM)

Experimental form factorHaxton(blue dot-dash) vs

experimental form factor(purple)

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Anapole Dark Matter(ADM)

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon, P. Gondolo, Anapole Dark Matter after DAMA/LIBRA-phase2, arXiv:1808.04112

Maxwellian velocity distribution Maxwellian velocity distribution

Page 15: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

Anapole Dark Matter(ADM)

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon, P. Gondolo, Anapole Dark Matter after DAMA/LIBRA-phase2, arXiv:1808.04112

Halo independent case

Page 16: DAMA/LIBRA-phase2 in WIMP effective modelsevents.kias.re.kr/ckfinder/userfiles/201901/files/Kang... · 2019-01-17 · non-relativistic effective models can fit the DAMA/LIBRA-phase2

pSIDM

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon, Proton-philic spin-dependent inelastic Dark Matter (pSIDM) as a viable explanation of DAMA/LIBRA-phase2, arXiv:1810.09674

χ 𝑚χ′ −𝑚χ = δ

Inelastic case : δ ≠ 0

pp

Χ’

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pSIDM

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon, Proton-philic spin-dependent inelastic Dark Matter (pSIDM) as a viable explanation of DAMA/LIBRA-phase2, arXiv:1810.09674

How pSIDM evades constraints

Xe, Ge: spin-dependent WIMP-proton cross section(no interaction with neutron)

F : 𝑣𝑚𝑖𝑛∗𝐹 > 𝑣𝑒𝑠𝑐

DAMA signal is okay since 𝑣𝑚𝑖𝑛∗𝑁𝑎, 𝑣𝑚𝑖𝑛

∗𝐼 < 𝑣𝑒𝑠𝑐

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pSIDM

Sunghyun Kang, S.S., G. Tomar, J.H. Yoon, Proton-philic spin-dependent inelastic Dark Matter (pSIDM) as a viable explanation of DAMA/LIBRA-phase2, arXiv:1810.09674

Halo independent caseMaxwellian velocity distribution

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Conclusions

non-relativistic effective models can fit the DAMA/LIBRA-phase2 data with less fine tuning compared to a standard SI interaction- all model excluded by fluorine&xenon detectors

Anapole Dark Matter could explain DAMA/LIBRA-phase1 in compliance with constraints from other experiments. It is now excluded after DAMA/LIBRA-phase2.

pSIDM could explain DAMA/LIBRA-phase1 in compliance with constraints from other experiments. Still OK after DAMA/LIBRA-phase2 if WIMP velocity distribution departs from a Maxwellian.