ultracoldneutron research at lansceneutron.physics.ncsu.edu/lug2015/ucn_research... ·...
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Ultracold NeutronResearchatLANSCEBradPlaster,UniversityofKentucky
LANSCEUserGroupMeetingNovember3,2015
LANSCEUCNSource
OperatingSince2004
ProtonBeam
UCNGuide
ToExperiments
Ultracold Neutrons(UCN)T<340nano‐eVv<8m/s
A.R.Youngetal.,J.Phys.G:Nucl.Part.Phys.41(2014)114007A.Saundersetal,Rev.Sci.Instrum.84(2013)013304A.Saundersetal.,Phys.Lett.B593(2004)55 2
SolidDeuteriumUCNSource
UCNasaProbeofFundamentalInteractions
Electromagnetic
E B
Strong
Gravity
g
nnn EH ˆVg =mgz
dpn
THe3 pn
S.Burles,K.M.Nollett,andM.S.Turner,astro‐ph/9903300
Weak
J.S.NicoandW.M.Snow,Annu.Rev.Nucl.Part.Sci.55(2005)27H.Abele,Prog.Part.Nucl.Phys.60(2008)1D.Dubbers andM.Schmidt,Rev.Mod.Phys.83(2011)1111 3
LANSCEUCNSourcePerformance
A.R.Youngetal.,J.Phys.G:Nucl.Part.Phys.41(2014)114007 4
ManyUsers!
5
TheUCNScienceProgram
“ReachingfortheHorizon”,The2015LongRangePlanforNuclearSciencehttp://science.energy.gov/~/media/np/nsac/pdf/2015LRP/2015_LRPNS_091815.pdf 6
TheExperiments
7
UCNB/Nab
NeutronEDM
UCNS
PrecisionNeutron‐Decay:UCNAσ
n e–
θe
p
e
θp
“V– A”Law
ep
8
“A”
M.P.Mendenhalletal.,PRC87(2013)032501B.Plasteretal.,PRC86(2012)055501
PrecisionNeutron‐Decay:UCNB,Nab(SNS)σ
n e–
θe
p
e
θp
e
e
EmbBB 0
νp
10.6 xray
481.7 CE 975.7 CE553.8 CE565.8 CE
56.7 CE72.8 xray75.0 xray84.9 xray
1047.8 CE
9
T.Bhattacharyaetal.,PRD85(2012)054512
S.Profumo,M.J.Ramsey‐Musolf,andS.Tulin,PRD75(2007)075107
PrecisionNeutron‐Decay:UCN
“CounttheLiving”
/0)( teNtN
“CounttheDead”
0N
dtdN
10R.H.Cyburt etal.,arXiv:1505.01076K.Nollett.updateofarXiv:1312.5725
PrecisionNeutron‐Decay:UCN
P.Walstrom etal,NIMA599 (2009) 82D.J.Salvat etal.,PRC89(2014)052501 11
Magneto‐ GravitationalTrap
Halbacharray
g
steNtN /0)(
10B UCN Detector
Al Shutter AFP Spin Flipperin 130G (370 kHz)
Trap Door
Polarized UCN from 6T PPM
The UCN Experiment is operational since 2013
UCN Spectrum Cleaner (Polyethylene sheet)
He Drift Tubesnot pictured)
“Fill‐Store‐Count” cycle1. Fill polarized UCN into the trap2. Clean the UCN spectrum3. Store UCN4. Count UCN
B/ZnS UCN detector
V-foil in-situ UCN
detector
Detector R&D:2013: External UCN detector2014‐2015: V‐foil in‐situ UCN detector2015‐2016: 10B/ZnS in‐situ UCN detector
SourceUpgradeinProgress
13LDRDProject#20140015DR:“ProbingNewSourcesofTime‐ReversalViolationwithNeutronEDM”,T.Ito(PI)
SourceUpgradeinProgress NeutronEDM
NTEd
1~δ
Figures:“ReachingfortheHorizon”,The2015LongRangePlanforNuclearSciencehttp://science.energy.gov/~/media/np/nsac/pdf/2015LRP/2015_LRPNS_091815.pdf 14
SourceUpgradeinProgress NeutronEDM
NewEDMExperiment
15
OtherExcitingOpportunities
z (m)
n =1 n =2 n =3 n =41.4peV 2.5peV 3.3peV 4.1peV
nnn EH ˆVg =mgzg
V.Nesvizhevsky etal.,Nature415 (2002)297T.Jenke etal.,NaturePhys.7 (2011)468A.R.Youngetal. L.J.Broussardetal. 16
UCNFacility“WishList”
Abilitytorun24/7(beamcurrentlyswitchedfrompRAD)
Abilitytorunwithhigherbeamcurrents
Cryogenicplant(2LHe liquefiers +3compressors)=veryloudenvironment
17
Summary
BroadscopeofresearchusingUCNaddressingfundamentalproblemsattheforefrontofnuclearphysicsresearch
IacknowledgesupportunderDOEAwardNumberDE‐SC0014622
Largeandactivecommunityofusers
18
ExtraSlides
UCNB / Nab Collaborations
UCNS
Coldvs.Ultracold
2
ultracold cold fast
MeV0.05–25meV
1– 300KmK
<350neV
T=20K
v2exp(−v2)
Superfluid4He
B.Plaster
p2/2m
dispersioncurve
4V.Nesvizhevsky etal.,Nature415,297(2002)
GravityandShort‐RangeInteractions
z (m)
n =1 n =2 n =3 n =41.4peV 2.5peV 3.3peV 4.1peV
nnn EH ˆVg =mgzg
B.Plaster
GravityandShort‐RangeInteractions
5
Spectroscopy
T.Jenke etal.,NaturePhys.7,468(2011)
Epq =Ep – Eq
NewShort‐RangeInteractions:
WeakEquivalencePrinciple:
nnn Emgzdzd
m
2
22
2
Chameleons,Axions,… Neutronsq =0NoEM
backgrounds!
“GravitationalResonanceSpectroscopy”
Casimir,vanderWaals
UCN
pqpq
Eω
B.Plaster
GravityandShort‐RangeInteractions
6
DarkEnergyChameleonFields
Gravityasapracticaltool…
T.Jenke etal.,PRL112,151105(2014);K.Tullney etal.,PRL111,100801(2013);A.N.Ivanovetal.,PRD87,105013(2013);T.Jenke etal.,arXiv:1208.3875
Axion DarkMatter
torsionpendulum
KE.00006:T.SakutaKE.00007:S.SaibaKE.00008:E.DeesKE.00009:M.Kitaguchi
B.Plaster
Neutron‐Decay: Lifetime
7
“V– A”Law
Parameters:
2) =gA /gVVud
WhatifthereareScalar, Tensor?
W.MarcianoandA.Sirlin,PRL96,032002(2006);W.Marciano,talkatSantaFeLifetimeWorkshop(2012)B.Plaster
Lifetime:Techniques
8A.Serebrov etal.,Phys.Lett.B605,72(2005);J.S.Nico etal.,PRC71,055502(2005);A.Yueetal.,PRL111,222501(2013)
“CounttheLiving”
t
N/
0)( teNtN
“CounttheDead”
/0NN
B.Plaster
Lifetime:BBNandNeff
9A.Coc etal.,arXiv:1403.6694;A.R.Youngetal.,J.Phys.G(inpress)B.Plaster
StandardModel:Neff =3.046
K.Nollett,talkatACFIWorkshopon“MeasuringtheNeutronLifetime”;updateofarXiv:1312.5725
~8s Neff ~0.12
n
n
p
p
YY
73.039.0
BBN
2
eff
eff
eff
eff 04.019.0
NN
NN
CMBBBN
Lifetime:Beam
10A.Yueetal.,PRL111,22(2013);J.S.Nico etal.,PRC71,055502(2005);F.Wietfeldt talkatACFIWorkshopon“MeasuringtheNeutronLifetime”
BL2ExperimentNIST:n ~1s
200increaseinprotonrate FE.00006:K.MishimaFE.00007:G.TanakaFE.00008:J.MulhollandFE.00011:T.YamadaKE.00010:R.Sakakibara
BL3ExperimentNIST:n <0.3s
B.Plaster
Lifetime:UCNStorage
11
Material‐wallUCNstorageexperiments
D.Salvat etal.,PRC89,052501(R)(2014)
Next‐generation:(nearly)eliminatewalllosses!
UCN
ED.00008:S.SeestromFE.00004:D.SalvatFE.00005:A.HolleyKE.00011:R.PattieKE.00012:Z.WangME.00013:N.Callahan
B.Plaster
Neutron‐Decay: AngularCorrelations
12
Differentialdistribution:
EEppD
EpB
EpA
Emb
EEppaEEEp
dEddd
e
e
e
en
e
e
e
eeee
ee
1)( 20
BSM BSM
BSM
νe
e bEmBB 0
20 3λ1)1|λ(||λ|2A
B.Plaster
Vud
13T.Bhattacharyaetal.,PRD85,054512(2012)
Vud (10–4)
10
20
30
Pion
experiment theory
Superallowed
nucleusdependent EW
Whatisneeded?
Neutron
EW
T=½Mirror
EW
nucleusdependent
a/a,A/A<0.1%
<0.3s
B.Plaster
PDG :
PDG :
4.1ν/χ 2
9.1ν/χ 2
AngularCorrelations: BSMPhysics
14T.Bhattacharyaetal.,PRD85,054512(2012);S.GardnerandB.Plaster,PRC87,065504(2013)
EEppD
EpB
EpA
Emb
EEppaEEEp
dEddd
e
e
e
en
e
e
e
eeee
ee
1)( 20
νe
e bEmBB 0
“a”,“A”to0.03%+n to…b,b(disentangled)
Neutronsvs.LHC
BP,S.K.L.Sjue,andA.R.Young,inpreparation
FE.00010:K.Hickerson
Nab:b~3 10–3
pp e +X
B.Plaster
A0
15
FE.00002:M.BrownFE.00003:A.SaundersME.00006:X.Ding
UCNAatLANL
DNPThesisPrize:M.P.Mendenhall
S/B:124
2010:0.94%
2011– 2013
Statistics~0.45%Systematics<0.5%
M.P.Mendenhalletal.PRC87,032501(R)(2013);BPetal.,PRC86,055501(2012)B.Plaster
a0
16
aCORN atNIST
Courtesy:F.Wietfeldt
2013:~3%
movingtonewguidehall
2015:~1%
B.Plaster
TheProblemoftheBaryonAsymmetry
17
Howcanthisbe?
Funtidbit:1975NobelPeacePrize!
0
BaryonNumberViolation
CandCPViolation
InteractionsoutofThermalEquilibrium
B.Plaster
BViolation:n‐n Oscillations
18
Canonicalidea:2 2matrix
2222
2
δ~)(sin)(
δ~)( ttEE
tPn
nn
EE
nn
in
nt
nn EEE δ
D.G.Phillipsetal.,arXiv:1410.1100[hep‐ex];S.GardnerandE.Jafari,arXiv:1408.2264
ILL(1994): >8.6 107 s EuropeanSpallationSource:
1011/s;t~0.1s
58Niguidem~6supermirrorsIncreaseinflightpathGainFactorsof100–1000
But…alsonewidea!nandnofoppositespinsinanexternalmagneticfieldhavesameenergy!
KE.00001:S.Gardner
B.Plaster
CPViolation:NeutronEDM
19
Sensitivitypermeasurementcycle:
NTEdn
1~δ
ILL:
E~10kV/cmT~130sN~14000density~0.7/cm3
Therefore,for~10–28 e‐cm:
E~5T~4N~25
Minimum:HigherUCNdensities!
ME.00001:M.MakelaME.00002:T.ItoME.00003:E.PierreME.00004:J.Martin
B.Plaster
Stat:1.6 10–26 e‐cm
WorldwideEffort:~10Experiments
20Tablefrom:B.Filippone etal.,SNSnEDM ExperimentPositionPaper
Differencesinexperimentaltechniques:Measure oraccumulatedphase =t?Magneticfieldmonitoring?“Co‐magnetometer”?UCNproduction/transport?
LANL SolidD2 Vacuum R&D ~30
B.Plaster
SNSnEDM Experiment
21
Stronginteraction
UCN 3He
superfluid4He
8.9Å n
BE
3He
3n
3
n
,BE
,BE
3Hen + p+T
ED.00006:A.ReidED.00007:R.DipertME.00010:C.SwankME.00011:N.NouriME.00012:S.Slutsky
R.Golub andS.K.Lamoreaux,Phys.Rept.237,1(1994)B.Plaster
Hadronic ParityViolation
22
ParityConserving
B.R.Holstein,J.Phys.G36,104003(2009);J.S.Nico andW.M.Snow,Annu.Rev.Nucl.Part.Sci.55,27(2005)
ParityViolatingWeakCouplings
Wikipedia!
DDH:QuarkModel+SU(6) “DDHReasonableRange”
B.Plaster
Hadronic ParityViolation:NPDGamma
23Courtesy:C.Crawford
pn + d+
θcos141
Add
n k
fA 11.0DDH
KE.00003:D.Blyth
NPDGammaSensitivity:
A ~1 10–8
J.Wasem,PRC85,022501(R)(2012)f =(1.099 0.505 0.061) 10–7
B.Plaster
Hadronic ParityViolation:n‐3He
24
3Hen + p +T
ProtonAsymmetry!
n pp
Single‐WireSpinAsymmetries!
KE.00005:M.McCrea
Courtesy:C.CrawfordB.Plaster