• 沒有找到結果。

Neutrino and Dark Matter Physics with Low Threshold Germanium Detectors

N/A
N/A
Protected

Academic year: 2022

Share "Neutrino and Dark Matter Physics with Low Threshold Germanium Detectors"

Copied!
27
0
0

加載中.... (立即查看全文)

全文

(1)

Neutrino and Dark Matter Physics with Low Threshold Germanium Detectors

Overview : TEXONO Program/Facilities

Neutrino Physics at KSNL

New Facility CJPL & CDEX Dark Matter

Prospects & Perspectives

Henry T. Wong / 王子敬 Academia Sinica / 中央研究院

November 2017

@

(2)

TEXONO-CDEX Collaboration

TEXONO

[since 1997]

:

Neutrino Physics at Kuo-Sheng Reactor Neutrino Laboratory (KSNL)

Taiwan (AS, INER, KSNPS,NTU,NDHU)

India (BHU)

Turkey (METU,DEU)

CDEX

[birth 2009]

:

Dark Matter Searches at China Jin-Ping Underground Laboratory (CJPL)

China (THU, CIAE, NKU, SCU,YLJHD)

Taiwan EXperiment On NeutrinO

China Dark Matter EXperiment

Research Program:

Low Energy Neutrino and Dark Matter Physics

(3)

NCTS ECP (2015+)

 ν-NSI ; BSM ν-e & ν-N ;

Atomic/nuclear effects in ν/χ interactions ;

 ν/χ – em effects ;

 ν-N QM coherency effects ;

Sterile-ν DM ; dark photons ;

……

TEXONO Theory Program

[AS, NTU, NDHU, DEU(Turkey), SCU(China) …… ]

C.P. Liu (NDHU)

J.W. Chen (NTU)

Connections: Studies of EW/BSM physics involves exquisite understanding of the detection physics mechanisms which require state-of-the-art command of atomic, nuclear & QCD physics.

(4)

4

28 m from core#1 @ 2.9 GW

Shallow site : ~30 mwe overburden

~10 m below ground level

Kuo Sheng Reactor Neutrino Laboratory [KSNL]

(5)

無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無無

Configuration:

Modest yet Unique

Flexible Design:

Allows different detectors conf. for different physics

Inner Target Volume

Front View (cosmic vetos,

shieldings, control room …..)

(6)

ULB-HPGe [1 kg] CsI(Tl) [200 kg]

Multi-Disks Array [~300 Tb]

KSNL : Detectors Schematics

Sub-keV Ge Detectors (20-900 g)

Data Acquisition with FADC Readout & FPGA Capabilities

(7)

Neutrino Properties & Interactions at Reactor

quality Detector requirements mass

Threshold ~ 100 eV

Observable Spectra with Reactor Neutrino “Beam”

Magnetic Moments

[PRL03,PRD05,PRD07]

1 kg HPGe

ν-e Scattering SM [PRD10]

& NSI/BSM

[PRD10,PRD12,PRD15,PRD17]

200 kg CsI(Tl)

νN Coherent Scattering [Current Theme;PRD16]

sub-keV O(kg) ULEGe / PCGe

Dark Matter Searches @ KSNL [PRD09,PRL13,AP14]

CDEX Program@CJPL [PRD13,PRD14,PRD14;PRD16,PRD17]

Theory Program

Neutrino Milli-charge [PRD14]

sub-keV O(kg) ULEGe / PCGe

Reactor Neutrino Spectrum

(8)

CsI(Tl) 200 kg :

Probe Electroweak Physics

[PRD10]

RSM

sys stat

R =[1.08±0.21( )±0.16( )]×

) ( 024 . 0 ) (

031 . 0 251 . 0

sin2θW = ± stat ± sys

Verify SM Destructive Interference

Constraints on Various Beyond SM Effects [PRD10;PRD12;PRD15] 0

ON-BKG

200 kg CsI(Tl)

Best Measurement !

(9)

Neutrino Electromagnetic Properties : Magnetic Moments

Search of µ

ν

at low enery with Reactor νe scattering

high signal rate & robustness:

 µν>>SM [ decouple irreducible bkgunknown sources ]

T << Eνdσ/dT depends on total φν flux but NOT spectral shape [ flux well known : ~6 fission-ν~1.2

238U capture-ν per fission ]

2

2

1 1

)

(

2

µ

ν

πα ν σ ν

µ

 

 

= m TE

dT e d

e

µνe) < 7.2 X 10-11 µB [PRL03,PRL07]

……. Same approach continuing in GEMMA (Kalinin, Russia)

µνe) < 2.9 X 10-11 µB [2013]

(10)

Neutrino “Milli-charge”

[+ Theorists: Chen, Liu, Chi; PRD14]

Identify New Twist - Cross-section enhanced at low energy transfer (“minimum ionizing”)

Smoking-gun signatures for positive signals:

peaks at known K/L binding energy at known ratios [different from cosmic- activation electron-capture background]

Present Bound : δQ < 10-12

Future Sensitivity Goal (100 eVee threshold): δQ ~ 10-14

Neutrino

Electromagnetic Form Factors

Atomic Ionization Differential Cross-Section

with full atomic physics many-body “MCRRPA” calculation [PL13]

(11)

Non-Relativistic Massive Sterile Neutrino to Light SM Neutrinos Via Transition Magnetic Moment Atomic Ionization

[PRD16]

Pole structure at differential cross-section at m

ν

/2 (q

2

~0)

Direct Search of Sterile Neutrinos as Dark Matter

(12)

Current Research Theme:

“sub-keV” Ge Detectors

Physics Goals for O[100 eV threhold1 kg mass1 cpkkd] detector :

νN coherent scattering , potential applications to reactor monitoring

Low-mass WIMP searches [CDEX Program @CJPL]

Explore ν/WIMP electromagnetic properties &

interactions

Open & Explore new detector window & detection

channel & physics parameter space

(13)

p- PCGe

[500g – 1 kg]

p+

n+(~1mm Li diffused)

n- PCGe

[500 g]

n

+

p

+(~0.5 μm Boron implanted) 500 g

4x5g ULEGe

Baseline Hardware Design

[Both TEXONO@KSNL & CDEX-1@CJPL]

Electro-Cooled p-PCGe[1430 g]

(14)

Neutrino-Nucleus Coherent Scattering :

Standard Model allowed and predicted processes :

ν (χ)

ν (χ)

Neutral current process (same for all ν-flavor)

σ ∝ N2 @ Eν < 50 MeV

“Coherent” [probe “sees” the whole nucleus]

sensitive probe for BSM ; interest in reactor monitoring

important process in stellar collapse & supernova explosion

analogous interaction used in dark matter detection

Ge at KSNL @ QF~0.2 : cut-off ~ 300 eV ;

Rate ~10 kg-1 day-1 @ threshold~100 eVee

(15)

Partial Coherent νN Elastic Scattering Observed by COHERENT@ORNL, ν @ π-DAR

(Science-2017)

!

Complementarity (Extensions) of Reactor Neutrinos:

Different kinematics regimes : q20 ; FF(q2)=1

Full QM Coherency [DAR-νN @ ~0.6 - 0.7 for CsI , threshold 4 keVnr]

Sensitive to different BSM/NSI (e.g. photon-like massless mediator)

Interest in Potential Applications to reactor monitoring

<φ> : averaged decoherence angle.

Coherency in Neutrino-Nucleus Elastic Scattering

[PRD16]

Quantify transitions between Coherency & Decoherency

Complementarity between different Sources & Target

(16)

Standard Model Cross-Sections at KSNL

[ with Quenching Function for Ge for nuclear recoils ]

Needs Background < 10 cpkkd, Target 1 cpkkd

Needs Threshold < 200 eVee, Target  100 eVee

Current Focus !!

(17)

Merits: 2400+ m rock overburden ; drive-in road tunnel access ; superb supporting infrastructures

Operated & Managed by THU & YLRHDC

CJPL-I (2010): 6X6X40 m cavern

CJPL-II (2017-18) : [ 4X(14X14X130 m) Halls ] + Pits

(18)

~2400 m

~9000 m

Physics Today September 2010

6 m (H) X 6 m (W) X 40 m (L)

CDEX-

TEXONO PandaX

Starting with plans &

sketches ….

(19)

CDEX-1 @ CJPL-I

Threshold (published results): 450 eVee

(20)

CDEX-1 Results on χN SI/SD ; solar & DM Axions

leading sensitivities

(21)

CJPL-Phase II

~500m west to CJPL-1

Construction started 2014

Rock Excavation completed May 2016

To be Commissioned Soon…

(22)

CJPL-II Layout

Four 14m*14m*130m Main Halls

Two Pits: (1) 18( φ )X18(H)m ; (2) 27(L)X16(w)X14(D)m

Total space: ~300K m³

(23)

CJPL-II Civil Engineering

(24)

Plan of Ground Laboratory (~2020)

offices, workshops, meeting venues, accommodation,

logistics (~150 people)

(25)

CDEX-1T (HPGe DM & 0νββ) Projects

CJPL-II Hall-C Pit

(Foreseen)

(26)

Towards Ton-scale enriched-Ge76 experiment for neutrinoless double beta decay experiment to cover the “Inverted Hierarchy”

Cast : mainly GERDA, Majorana, CDEX groups

CDEX group – build a case of hosting this experiment at CJPL-II

Great Opportunities (Expensive Problems) in Nuclear Physics –

nuclear matrix elements, gA in nuclear process…….

(27)

Summary & Outlook

TEXONO@KSNL contributed to neutrino electro-

magnetic and electro-weak physics, incl. best cross- section measurement among two of the fundamental leptons.

CDEX@CJPL (+TEXONO)  competitive results in low- mass WIMPs with sub-keV detectors

Frontline for low threshold germanium detectors &

physics applications like νN measurement

CJPL @ China adds to the world’s arsenal of low- background facility.

Collaboration with Atomic/Nuclear/QCD communities

has yielded fruits and expanded horizons to both.

參考文獻

相關文件

Wave Function of the Hydrogen Atom’s Ground

 Light travels between source and detector as a probability wave.

• Both the galaxy core problem and the abundance problem are associated with dwarf galaxies on the scale &lt; few kpc !!..

Macro Evolution of core-collapse supernovae (giant P violation) Chiral kinetic theory. Son, Yamamoto (2012); Stephanov, Yin

The observed small neutrino masses strongly suggest the presence of super heavy Majorana neutrinos N. Out-of-thermal equilibrium processes may be easily realized around the

• Many-body physics is essential for sub-keV detectors of neutrinos and dark matter. • High-quality many-body calculations can substantially reduce

• Dark matter appears as missing transverse momentum in collider

These experiments observed atmospheric neutrinos and confirmed neutrino oscillations..