3rd Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Volume 54, Number 10
Tuesday–Saturday, October 13–17, 2009;
Waikoloa, Hawaii
Session 1WD: Workshop on Neutrinoless Double Beta Decay I
9:00 AM–12:30 PM,
Tuesday, October 13, 2009
Room: Kohala 2
Chair: M. Nomachi, Osaka University
Abstract ID: BAPS.2009.HAW.1WD.2
Abstract: 1WD.00002 : CANDLES for the study of $^{48}$Ca double beta decay
9:30 AM–10:00 AM
Preview Abstract
Abstract
Author:
Izumi Ogawa
(Graduate School of Science, Osaka University)
CANDLES is the project to search for double beta decay (DBD) of
$^{48}$Ca by using CaF$_2$ scintillators.
The $Q$-value of $^{48}$Ca, which is the highest (4.27~MeV) among
potential DBD nuclei, is far above energies of $\gamma$-rays from
natural radioactivities (maximum 2.615~MeV from $^{208}$Tl
decay), therefore we can naturally expect small backgrounds in
the energy region we are interested in.
We gave the best lower limit on the half-life of neutrino-less
double beta decay of $^{48}$Ca by using CaF$_2$(Eu) detector
system, ELEGANT VI though further development is highly desirable
to reach the mass region of current interest.
We have constructed the prototype detector, CANDLES III in our
laboratory (Osaka U.) at sea level and studied the basic
performance of the system, including the light collection,
position reconstruction and background rejection.
We are now moving the detector system to new experimental room
(room D) at Kamioka underground laboratory (2700~m.w.e.) to avoid
large background originated from cosmic rays.
At the same time, we are increasing the total mass of the
$^{48}$Ca compared to the one in the prototype detector.
96 (instead of 60 in prototype) CaF$_2$ modules which contains
350~g of $^{48}$Ca are immersed in a liquid scintillator (LS)
which acts as an active veto (veto phase).
The conversion phase contains wavelength shifter (Bis-MSB) which
converts the emission light of CaF$_2$(pure) which has a peak in
the UV region to the visible one where the quantum efficiency of
the PMTs is high enough (maximum at $\sim400$~nm) and materials
at the optical path have good transparencies.
Scintillation lights from both the CaF$_2$ modules and the liquid
scintillator in veto phase are viewed by large PMTs ($48 \times
13$'' and $14 \times 17$'' tubes).
All the detector system described above are contained in a water
tank which is 3~m in diameter and 4~m in height.
The water tank and a purification system of the LS together with
LS storage tanks were installed at room D.
The purification system of the LS removes the radioactive
impurities especially U and Th using the techniques of
water-extraction and N$_2$ purge.
Other components including the CaF$_2$ modules, the PMTs, the
liquid scintillator vessel and DAQ system will be installed soon.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2009.HAW.1WD.2