double beta decay spectroscopy and neutrino mass sensitivities hiro ejiri*, t. shima
DESCRIPTION
Double Beta Decay Spectroscopy and Neutrino mass sensitivities Hiro Ejiri*, T. Shima RCNP Osaka Univ. * NIRS & CTU, Praha For the MOON collaboration Sendai TAUP Sep. 07. H. Ejiri, J. Phys. Soc. Japan, Invited Review, 74 (2005) 2101. - PowerPoint PPT PresentationTRANSCRIPT
Double Beta Decay Spectroscopy and Neutrino mass sensitivities
Hiro Ejiri*, T. Shima
RCNP Osaka Univ. *NIRS & CTU, Praha
For the MOON collaboration
Sendai TAUP Sep. 07
1.Doublr beta decay spectroscopy2. Majorana mass sensitvity
3.Double beta decays to excited states4.Nuclear matrix element
H. Ejiri, J. Phys. Soc. Japan, Invited Review, 74 (2005) 2101.H. Ejiri, Mod. Phys. Lett. A, Vol. 22, No. 18 (2007) pp. 1277-1291.
by RHC, Heavy , SUSY, and others
A2=GM AgM>
Energy spectra 4,3,2 body
LHC m / SUSY m M + kMS
different isotopes and states with different M
ALHC + RHC <m> +SUSY ~k(ML/MR)2
LHC / RHC 21 and E12 correlations
Spectroscopic detectors
ELEGANT- MOON, DCBA NEMOIII - Super NEMO
1. E12-12 identify m term 2. Detector ≠ source Select nuclide by Q, Z, Enrichment, 2 3. Small RI-BG :E(RI) < Q
separation
Major BG : 2tail inwindow. E-resolution !
Interference A0 = XL + XR XL = Light + SUSY (+Heavy )
= m M + kMS = m M [(1 + (k/ m) (Ms/M) ] Cancellation at A=76 (left fig.) or 136(right), but not at other A’ b
ecause of the different short-range/long range matrix elements.
Need measurements with different nuclides.
.
Vergados 07
Nuclear matrix elements QRPA
0.1
1
10
70 80 90 100
Rodin07 RQRPA QRPA Suhonen07 UCOM Jastraw
Nuclear matrix elements M
)
Ge Se Mo Cd Te Xe A
M ~ 24 /r = 18/A1/3 within a factor 1.3
Mass sensitivities and nuclear sensitivity
<m> = SN- 1 /2 (Neff)-1/2 1/2
B=[B(RI) + B(2)]
B(2)=4.2(/t1/2)(100/A), 10-7 and t1/2 1020
SN- 1 /2 = 13 (GM2 /0.01 A)- 1 /2
Nuclear sensitivity : m
N=1 t y and Y = = 1 SN
- 1 /2 =20~10 meV for M=25/R
eff = N ton year
= No signals for 90 % CL ~2.3 if B~0 ~1.6 + 1.7 (BN)1/2 BG =B/t y N ton year
M ; excited state and Nd M = M/3
Mass sensitivities and nuclear sensitivity
<mn> meV= (SN)- 1 /2 ( N)-1/2 1/2
SN = GM2 /0.01A/170)
M=25/R ~ 4
Small BG or N
~ 2.3 <m> = 2.3 SN
- 1 /2 ( N)-1/2 Large BG or N
~ 1.7 (BN)1/2 <m> = 1.3 SN
- 1 /2 ()-1/2
N-1/4 B1/4
N-1/2
N-1/4
10
100
0.1 1 10
Neutrino mass sensitivity
Se82 =1.7%,2.2%, Mo100 =1.7%, 2.2%
BCDE
Effective neutrino mass in meV
N ton year
Spectroscopic DBD BG=
130Te B =6000 for CUORITINO B=200 for 0.01 /y kev kg of TeO2
Excited 0+ states
Isotope
State
100Mo
GRS
100Mo
EXS
150Nd
GRS
150Nd
EXS
Q (MeV) 3.034 1.903 3.368 2.113
SN1/2 meV 9.6 19.5 19.5 42
<m> meV /5 y t 44 39 78 96
reduce BG’s 2, RI.• Cancellation, but not at both.• GRS and EXS
T = G |Mm +Ms|2 MJ>1+)
Nd M/3 is assumed for deformation change.
Excited state for = 2/3 of GR by , and M= same as GR
150Nd E(2) 0.13 MeV Q MeV G
150Sm GS 0+ E(2) 0.334 MeV 3.36 13.4 0.74 MeV E(2) 0.34 MeV 2.63 3 E0 1.255 MeV E(2) 0.16 MeV 2.11 1.3 E2
150Nd -- 150Sm deformation
M due to change of deformation is 1/3?
M to the excited, but same deformation is 1
RCNP/MSU3He,t t, 3HeZergers R
Simucovic 1/4 ~ 1/6 of M due to deformation change.
RCNP Osaka High E response at low and hi
gh 1+ 2- states
D. Freckers, R. Zegers, MSU/RCNP/KVI
Charge exchange reactions
H. Ejiri, PR 380 ‘2000
2-
1+
Suhonen
z=5,5z=6,6T,Tz=6,6
z=5,5
,Tz=5,4
z=4,4
S
H. Ejiri PRL 21 ’68, H. Ejiri
PR 38 ‘78
Polarized GeV-MeV photons from laser scattered off GeV ele
ctronsfor electric and magneic trasitions.
Photon probes
MOON detector conceptional sketch
Multi-layers, 2 for and all others active shields
Each with 1PL+2PS 1.3 m-1.3 m- 4 cm 25 kg
One unit 100 mod., :30 kg, 1 m2–4m,
Based on ELEGANT V
H. Ejiri, et al., PRL, 85, 2000, 2917.H. Ejiri et al., Czech. J. Phsy. 54, 2004, 317.
Concluding remarks
1. DBD studies of E- correlations for 2-3 isotopes and/or states are indispensable for identifying the -mass processes.
2. They can be realistic by spectroscopic DBD studies with detector≠ souces. 82Se , 100Mo 150Nd are good candidates.
3. Recent QRPA/RQRPA give M~18/A1/3. Nuclear sensitivity, the mass for N=1 t y Y=1, is 20 meV for 76Ge and 10 meV for 82Se, 10
0Mo, 130Te, 136Xe.
5. Then QD ~100 meV and IH~30 meV masses are studied by N~0.1 and 1 t y with 76Ge and 82Se, 100Mo, 130Te, 136Xe .
6. Spectroscopic experiments (MOON, SuperNEMO) can access the IH masses with realistic ~ 2.2 % and ~20 mBq/t .
7. Charge exchange nuclear reactions and photo nuclear reactions are used to check the M calculations.
H. Ejiri, J. Phys. Soc. Japan, Invited Review, 74 (2005) 2101.
H. Ejiri, Mod. Phys. Lett. A, Vol. 22, No. 18 (2007) pp. 1277-1291.
MOON collaboration
H.Ejiri*, T.Itahashi, K.Matsuoka, M.Nomachi, T. Shima,
• S. Umehara, RCNP and Physics OULNS, Osaka Univ.• P.J.Doe, R.G.H.Robertson*, D.E.Vilches, J.F.Wilkerson 、 D. I. Will.
CENPA, Univ. Washington.• S.R.Elliott, V. Gehman, LANL• J.Engel. Phys.Astronomy, Univ. North Carolina. • M.Finger, M. Finger, K. Kuroda, M. Slunecka , V. Vrba.• Phys. Charles Univ. and CTU Prague • K.Fushimi, H. Kawauso, K. Yasuda, GAS, Tokushima Univ. Tokushima • M. Greenfield, ICU, Tokyo.• R. Hazama, Hiroshima Univ. • H. Nakamura, NIRS. • A. Para FNAL• A. Sissakian, V. Kekelidze, V. Voronon, G. Shirkov A. Titov, JINR • V. Vatulin, P. Kavitov, VNIIEF• S. Yoshida, Tohoku Univ. Sendai
• * Contact persons.
Thank you for your attention
• .
3 GeV-p
Neutrino Weak probes
SNS 1 6 1015 7 1014
J - PARC 3 1.2 1015 3 1014
p + Hg n +, + + + + e+ + e + anti-
C.Volpe