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MOMENT Overview MOMENT Overview

MOMENT Overview - PowerPoint Presentation

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MOMENT Overview - PPT Presentation

Jingyu Tang Institute of High Energy Physics CAS NuFact16 Quy Nhon Vietnam Aug 2226 2016 Outline Brief introduction to the MOMENT Recent study progress Physics potential RampD efforts at ID: 617559

neutrino beam target decay beam neutrino decay target moment physics mev linac muon cavities study amp detector csns ads

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Slide1

MOMENT Overview

Jingyu Tang

Institute of High Energy Physics, CAS

NuFact16,

Quy

Nhon

, Vietnam, Aug. 22-26, 2016Slide2

Outline

Brief introduction to the MOMENT

Recent

study progress

Physics potential

R&D efforts at

CSNS/

EMuS

SummarySlide3

Brief introduction to MOMENTSlide4

MOMENT study

MOMENT: A muon-decay medium baseline neutrino beam

facility

MOMENT was launched in 2013

as

the third phase of neutrino experiments in

China, following

Daya

Bay and JUNO

Originally as a

dedicated machine to measure CP phase in the future, if

there are still the needs then. Physics goals should be modified along with the neutrino physics development.

As a driving force to attract researchers from China as well international collaborators to work on neutrino experiments based on acceleratorsSlide5

Features:

Using

a CW proton linac as the proton

driver: 15 MW

China-ADS

linac

development

Fluidized target in high-field SC solenoidMuon transport and decay channel (Pure + or - decay, managed beam)Also possible with -decayed beam and Decay-at-Rest neutrinos Slide6

Proton driver

Design goal:

Beam power: 15 MW

Beam energy: 1.5 GeV

Beam current: 10 mA

Using the China-ADS

linac

or a dedicated linac with large simplification (much less redundancy)3.2-MeV RFQ (room-temperature)Three sections SC spoke cavities (160 MeV)Two sections SC elliptical cavities (1.5 GeV)In total, 196 SC cavities in 42 cryostats, linac length: ~ 300 mSlide7

Estimate of neutrino flux

POT (5000 h): 1.125

10

24

proton/year

Muon yield: 1.62

 10-2 /protonTotal neutrino yield: 4.8

 10-3

/proton (in pair) 5.4 

10

21

/year (in pair)

(NF

: 1.1  1021 /year )Neutrino flux at detector: dependent on the distance 4.7  1011 /m2/year (@150 km)

 Slide8

Recent progressSlide9

ADS linac

development

Parallel efforts at IHEP and IMP on the

linac

front (RFQ + low-

 cavities, 10 MeV)

Very successful from both teams (different schemes)

RFQ CW operation (IMP: 100%, IHEP: 99%)Low- superconducting cavities (10 MeV at IHEP, 5 MeV at IMP, 10 mA, pulsed)Prototypes of different SC cavities (Spoke, HWR, Elliptical)Second ADS phase (CIADS) approved Will be in Huizhou, Guangdong (not far from Daya Bay)

250 MeV -10 mA, CW mode

Test-stand at IMPSlide10

Target Station

Further optimization of the mercury

jet

target design

More

interests in developing fluidized granular target in collaborating with the C-ADS target team, and also waiting for study result with fluidized

tungsten-powder

target in Europe

Vassilopoulos’ talkSlide11

Schematic of a waterfall-like granular target

Preliminary study shows good heat transfer and pion capture efficiency

Implantation method (such as cutting slots in the inner shielding) is still under developmentSlide12

A selection section to select

+/+ from -/-, as either 

+

beam or - beam is used for producing the required neutrinos

Reverse the fields when changing from 

+

to -

Also for removing very energetic pions who still surviveVery difficult due to extremely large beam emittance (T/L)Two schemes:

based on 3 SC dipoles with strong gradient (or FFAG), and bent SC solenoidsPresent study shows

Dipole+solenoid solution works for smaller emittance, bent solenoid solution works for very large emittance

Charge selectionSlide13

Spent protons extraction

Features

Very important to avoid huge heat deposit and radiation in the target station (also meaningful for NF)

Spent protons can be reused

Very difficult in practice

Method

Extract only high-energy

protons (scattered from target)Collimation and bent solenoids (+dipole field) Slide14

Physics potentialsSlide15

Physics potential in CP

15

Detecting CP-violating phase in the lepton sector

Absolute measurement: P(

ν

μ

→ν

e

)

Relative measurement:

P(

ν

μ

→ν

e

)-

P(

ν

μ

→νe

)

Advantages of MOMENT

High intensity neutrino beam : >10

21

/year

Relative low energy (~300 MeV) and short baseline (~150 km)

M

inimum interference from matter effect

Low

π

0

background

Muon decay neutrinos

Measure multiple oscillation channels at the same time

Low beam intrinsic background

Requirement to the detector

e/

μ

identification

Neutrino/antineutrino identificationSlide16

Detector optionsLiquid scintillator

Gd

-doped water Cherenkov detector

Signals (

μ

+ decay, 5,000kton×year, 100% efficiency)

IBD: 435 (easy to be identified with neutron tagging)

νe CC: ~1,600 (large contamination of νe without magnetized detector)Oscillation signal of μ- decay is ~1/3 compared to μ+

decay Major background

Atmospheric neutrinosCharge mis-identification

Signal and background16

IBD spectrum in the detector

Another calculation can be found

in

arXiv:1511.02859Slide17

e/μ identification in the liquid scintillator

MC studies are ongoing

Improve charge identification

A large magnetized detector?

Reduce atmospheric background

Reconstructing neutrino direction

Sending neutrino in short bunches

(arXiv:1511.02859)?Not realistic in ADS-type accelerator (CW beam)Perspective

17

μ

+

e

+

Cherenkov ring

Cherenkov light

S

cintillation light

Direction of e

+

from IBDSlide18

Make use of decay-at-rest neutrinos?

Another possibility

18

DAE

δ

ALUS

MOMENT-DAR

PRL

104, 141802 (2010

)Slide19

Other physics potentials

Search for sterile neutrinos

DAR at the two beam dumps: target station and beam dump

Neutrino cross-section measurement

Both

-decay and -decay neutrinos in 0-500 MeV

Muon physics

Very high intensity DC muon beamSlide20

Some related R&D efforts at CSNS Slide21

EMuS at CSNS

We plan to build an experimental muon source (

EMuS

) at China Spallation Neutron Source (CSNS).

CSNS is under construction, expected to complete in March 2018, 100 kW at Phase I and 500 kW at Phase II

EMuS

will use 4% beam power to produce intense muon beams for

MOMENT R&D studies and SR multidisciplinary applications. Potentially it may be also used for neutrino cross-section measurements and

muon physics.MOMENT R&D studies include muon capture in high-field, charge selection, spent proton extraction etc. Present EMuS study is supported by

an NSFC fund for R&D and prototypes

Yuan’s talkSlide22

22

22

2009

5

9

日Slide23

Summary

MOMENT

is

a driving force to attract Chinese researchers to collaborate on neutrino

experiments

based on accelerator-based neutrino beams

Also participating international projects: LBNF, MICE, …

Current studies focus onSuitable detector and physics potential with different neutrino sources Fluidized granular target and spent protons extractionCharge selection methods Some R&D will be done at CSNS/EMuSSlide24

Thank you for attention!