improving the detection sensitivity of dark-matter axion search with a rydberg-atom single-photon...
TRANSCRIPT
Improving the detection sensitivity
of dark-matter axion search
with a Rydberg-atom single-photon detector
M.Saeed For
newCARRACK CollaborationKyoto
FPUA2010
T. Arai, A. Fukuda, A. Matsubara,T. Mizusaki, A. Sawada,M.Saeed:
S. Ikeda, K. Imai, T. Nakanishi,Y. Takahashi:
Y. Isozumi, T. Kato, D. Ohsawa,M. Tosaki:
K. Yamamoto:
H. Funahashi,J.Uda:
Y. Kido, T. Nishimura, S. Matsuki:
Research Center for Low Temperature and Materials Sciences, Kyoto University
Department of Physics, Kyoto University
Radioisotope Center, Kyoto University
Department of Nuclear Engineering, Kyoto University
Institute for the promotion of excellence in higher education Kyoto University
Department of Physics, Ritsumeikan University
T. Arai, A. Fukuda, A. Matsubara,T. Mizusaki, A. Sawada,M.Saeed:
S. Ikeda, K. Imai, T. Nakanishi,Y. Takahashi:
Y. Isozumi, T. Kato, D. Ohsawa,M. Tosaki:
K. Yamamoto:
H. Funahashi,J.Uda:
Y. Kido, T. Nishimura, S. Matsuki:
Research Center for Low Temperature and Materials Sciences, Kyoto University
Department of Physics, Kyoto University
Radioisotope Center, Kyoto University
Department of Nuclear Engineering, Kyoto University
Institute for the promotion of excellence in higher education, Kyoto University
Department of Physics, Ritsumeikan University
newCARRACK Collaboration
(1) Principle of Rydberg-atom single-photon detector
(2) Performance of detector : measurements of blackbody radiations in a cavity at low temperature
(3) Sensitivity limit: effect of stray electric field
(4) Practical design for improving the sensitivity
Contents
AxionA hypothetical particle postulated by Peccei-Quinn in 1977 to resolve the so called strong CP problem in QCD.is a well-motivated candidate for the Dark Matter
Dark MatterRotation-velocity distribution of a typical spiral galaxy A: expected B: observed
Rotation curve of a typical spiral galaxy, i.e. rotating velocity of the galaxy versus distance from the center of the galaxy, cannot be explained only by the visible matter. Existence of a roughly spherically symmetric and centrally-concentrated matter called galaxy halo explains the rotation curve. Non-visible form of matter which would provide the enough mass and gravity is called “DDark ark MMatteratter”.
10-6[eV] < ma < 10-3[eV] 240[MHz] < f < 240 [GHz]
4s1/2
Axion
B0
ns1/2
np1/2
Diode laser 766.7nm
4p3/2
Diode laser 455nm
γ
Primakoff effect Rydberg atom
|g 〉
|e 〉
Lower state |g>Upper state |e >
Principle of the Kyoto Rydberg-atom single-photon detector
39K
Axion is resonantly converted to a single microwave photon by a Primakoff interaction ,enabling us to develop an effective axion detection by counting axion converted photons indirectly
Schematic
LaserElectron multiplier
Dilution fridge
electron
Fieldionizationelectrodes
Atomic beamMetal posts for tuning
mirror
7Tmagnet
Whole System
Liquid Helium
Dilution fridge and selective field ionization detector
Electron multiplier
Selective Fieldionization region
Laser set up
Top view of the Dilution Fridge
Noise source
Blackbody radiation in the cavity
Cavity temperature must be kept as low as possible
Stray electric field limited the
Sensitivity
Reduction of absorption probability of photon in the resonant cavity (Resonance broadening)
Degradation of the selectivity in the field ionization process (SFI) (Rotational effect of electric field)
Actual pulsed-field ionization scheme
Lower state
Upper state
111
111
111P
111S
111P
111S
M. Tada et al., Phys. Lett. A 349(2006)488
Measurement of blackbody radiationsin a resonant microwave cavity
SQL Limit
2527 MHz
p
st
sa
p
p
st
st
sa
sa
Improvements
1. Instead of Rb ,Potassium Rydberg atoms will be used (reduce the effect of Stark broadening in the microwave absorption Process)
2. Guiding field method to avoid the rotation of the electric field
3. A spatially collimated bunched packets of Rydberg atomic beam (by laser cooling)
time varying electric field will be applied to compensate the stray electric field.
Improvements
1. Instead of Rb ,Potassium Rydberg atoms will be used (reduce the effect of Stark broadening in the microwave absorption Process)
2. Guiding field method to avoid the rotation of the electric field
3. A spatially collimated bunched packets of Rydberg atomic beam (by laser cooling)
time varying electric field will be applied to compensate the stray electric field.
Improvements (1): Use of 39K Rydberg atoms instead of 85Rb
H.Haseyama et al J.Low Temp Phys150 549(2008)
39K 85Rb
Electric field [mV/cm]
2800
2900
3000
3100
0 10 20 30 40
39K: n =102
Experimental data of Stark shift in 39K for n=102
More Precise measurements are in Progress
s-p
ener
gy d
iffer
ence
[M
Hz]
Red solid circles : Preliminary experimental data for the s1/2 to p3/2 transitionsopen circles : those for the s1/2 to p1/2 transitions.
Improvements
1. Instead of Rb ,Potassium Rydberg atoms will be used (reduce the effect of Stark broadening in the microwave absorption Process)
2. Guiding field method to avoid the rotation of the electric field
3. A spatially collimated bunched packets of Rydberg atomic beam (by laser cooling)
time varying electric field will be applied to compensate the stray electric field.
Guiding electric fieldImprovements(2): Cavity and electrodes
cavityStark electrode
SFI electrodes
electrodes forfield rotation
atomic beam
y
zfield direction
Stark field direction
Cavity electro-magnetic field: TM010
E
M.Shibata et al J.Low Temp Phys 151 1043(2008)
-40
-30
-20
-10
0
10
20
30
40
x=0,y=0excitation point
cavity SFI box
-100
-50
0
50
100x=0,y=0
θ
φ
excitation point
cavity SFI box
50 100 150 200
z [mm]
[m
V/c
m]
Ang
le [
deg
r ee]
xy
z
θ
φ
|E|
Ex
Ey
Ez
Ele
ctri
c fi
eld
Cavity and electrodes structure
i.d. 90, length 958cylindrical TM010 mode
A distinctive step to overcome the stray electric field dynamically
• Instead of continuous beam a spatially collimated bunched packets of Rydberg atomic beam will be used by laser cooling technique and by applying time varying field to compensate the stray field
• Increasing absorption probability and state selectivity
Improvements
1. Instead of Rb ,Potassium Rydberg atoms will be used (reduce the effect of Stark broadening in the microwave absorption Process)
2. Guiding field method to avoid the rotation of the electric field
3. A spatially collimated bunched packets of Rydberg atomic beam (by laser cooling)
time varying electric field will be applied to compensate the stray electric field.
Time to reach the bunched beam from trap to Resonant Cavity
S=1.365 mV=350 m/st = 3.9 ms
Spatial Spread of 39K at the position of the Resonant Cavity
V = 350m/st 1(time taken for accelerated motion)=1.4
ms
S1(Distance Traveled to attain V ) = 0.24 m
S2(Distance to Resonant Cavity)=1.365m
t2(Time to reach the Cavity)=3.9 ms
Velocity spread after acceleration=2m/s
Spatial spread after acceleration is about 2mm
at the position of cavity spatial spread increase
Improvements(3): Laser cooled bunched beam
T=145mK
Summary
Obtained preliminary data of Stark Shift of 39K Constructed the Guiding Field system in the cavity.
More precise measurement of Stark Shifts of 39K Experimental testing of Guiding electric field and sensitivity up to 10 mK Designing and construction of laser cooling apparatus for collimated bunched beam of 39K Rydberg atoms
Improvements in Progress
Present Status
Thank you For
your kind Attention
Room Temp39K source
Ion Pump
Anti Helmotz coils
Laser Beams
s+
s-
s-
-
C.Monroe et all Phy.Rev.Lett,65,1571(1990)
Omit this slide
B=monIr2/2(r2+z2)3/2
If separation is twice of the Radius of the coilB= (4/5)3/2monI/rCoil Radius (r) = 30mmSeparation (z) = 60mmNumber of turns (n)=25Current=3ARequired Field Gradient=0.20T/m
Anti -Helmholtz coils
z
x
y
I
I
s-
s+
s+
s-
s-
s+
n=10 n=100 n=1000
Mean radius
n2 53A0 0.53micro meter
53micrometer
Binding energy
1/n2 1100cm-1 11cm-1 0.1m-1c
Period of electronic motion
n3 0.15pico second
0.15ns 0.1micro second
Polarizebility
n7 0.2 0.2x107 0.2x1014
Spacing between adjacent level
n-3 200cm-1 0.2cm-1 2x10-4cm-1
Ionization field
n-4 33000v/cm
3.3v/cm
3.3x10-4 v/cm
Some parameters regarding axion-photon-atom system
Initial average quantum state occupation number of axion=5.7x1025
Spread in the axion energies=10-11eV/h
Axion- photon- photon coupling constant=4x10-26eV/h
Collective coupling constant between the resonant photons and the N
Rydberg atoms=1x10-10eV/hCavity length=20cmV=350m/s
Ma=10-5ev
Q=2x10-4
Loading Rate Coefficient also depends upon the beam diameter and the Total intensity of the trapping laser as shown in fig.3
Fig. 3 .Loading rate coefficient l as a function of (a) beam
diameter d and of (b) intensity Itot
Some Parameters dependence of 39K Trap
1.Number of Trapped atoms(N)
2.Loading Rate Coefficient(l)
3.Trapped atoms density(n)
4.Loss Rate
Itot=220mW/cm2 and beam diameter is 1.2cm Williamson III JOSA B Vol 12 ,1393(1995)
Kitagawa, Yamamoto, and Matsuki, 2000.
From Kitagawa,Yamamoto, and Matsuki, 1999.
33
Shibata et al., Rev.Sci.Inst. 74(2003)3317.
atomic beamatomic beam
e-
0.15kV
1kV
CEM
Cross Sectional View
20K