a new determination of the fine structure constant based...
TRANSCRIPT
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Laboratoire Kastler Brossel (ENS, CNRS, UPMC) Institut National de Métrologie (CNAM)
PermanentsS. Guellati-KhélifaC. SchwobF. NezL. JulienF. Biraben
Ph.D StudentsP. CladéM. CadoretE. De Mirandes
A new determination of the fine structure constant based on Bloch oscillations of 87 Rb atoms in a vertical optical lattice
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quantum Hall effect
137.035 990 137.036 000 137.036 010
hfs muonium
h / m(neutron)h / m(Cs)
QED
h / m
Solid statephysics
g 2 of the electron (UW)
α-1
Γp,h-90
Codata98
Codata02
h / m(Rb)
Determinations of the fine structure constant α
c4e
0
2
hπε=α
CODATA 2002 P. Mohr and B. Taylor, RMP, 77, n°1, p. 1, january 2005
RK=h/e2=µ0c/2α
ae = f (α/π)
mv=h/λg 2 of the electron (Harvard)
( )( )Xmh
)e(AXA
cR2
r
r2 ∞=α
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Two photon transition : defined momentum transfer
Low spontaneous emission
Doppler sensitive
Controllable width of the transition (pulse duration) :
F=2
F=1
5P3/2
mk2 k1
ωSHF
∆
∆ΩΩ
∝Ω 21eff
(M. Kasevich et al, Phys. Rev. Lett 66, (1991) 2297)
Recoil velocity Raman transition
a
b
νħk m
vr m2kmv
21E
mkv
222rr
r
h
h
==
=
4
Principle of our experiment
Final uncertainty : σvr = σv / (2N)
N × 2ħk
Coherent acceleration
measurement(Raman transition)
selection(Raman transition)
MOT +molasses
! selection of an initial sub-recoil velocity class! coherent acceleration : N Bloch oscillations, momentum transfer 2Nħk! measurement of the final velocity class
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Momentum
Ener
gyV
eloc
ity d
istri
butio
n
|bi
~δcenter
Ener
gy
Momentum
Determination of the center of velocity distribution
F=1
Raman detuningδcenter
⇒
1) Subrecoil velocity selection 3) Velocity measurement
F=2
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F=1
MOT +Optical molasses
Selection: F=2 → F=1
δsel
π-pulse
Tuned FrequencyDetection
Measurement:F=1 → F=2
δmeas
π-pulse
-5vr 0 +5 vr-5vr 0 +5 vr-5vr 0 +5 vr
F=2
F=1
Blow awaybeam
5S1/2
F=2
5P3/2
87RbVelocity sensor
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"intensity: 100mW.cm-2 ; detuning ∆ ~ 1050 GHz
"1,8 s per point (loading of the MOT)
"300 points (~10 minutes)
~vr/50
N 2/(
N 1+
N 2)
Velocity measurement : results
15000vHz1 r
v →≈σ
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Velocity
Ener
gymk1 k2
# Light shift
# Quadratic Zeeman shift
∆Zeeman
∆ v
Reduction of constant systematic shifts
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Velocity
Ener
gymk2 k1
Compensation of energy shifts by inverting the direction of Raman beams
∆Zeeman
∆ v
Two spectra →one velocity measurement
2×10
-3v r
# Light shift
# Quadratic Zeeman shift
Reduction of systematic shifts
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Coherent acceleration of atoms
Raman transitions in a same internal state
E = P2/2M
p2~k 4~k 6~k
δ= 10 k vr
δ= 6 k vr δ= 2 k vr
ν1
ν2
Laboratory frame
( ) tak222 21' =−= υυπδπ
coherent acceleration, 2 ~ k per cycle
E
p
ν1 ν1
+hk−hk
ν1
ν1
g
νBmg2 k
=h
Acceleration Stationary
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E
p
n, n
n-1, n+1 n-2, n+2 n-3, n+3
0 2hk 4hk
Coherent acceleration of atoms
Bloch oscillations in the fundamental energy band
M. Ben Dahan et al , Phys. Rev. Lett. 76 (1996) 4508.
E. Peik et al, Phys. Rev. A 55 (1997) 2989.
Dressed atom
Accelerated frame
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t1, N1t2, N2
! Differential measurement to cancel systematic effects
! Atomic cloud dont move between selection and measurement → g measurement at the same place
Stationary experiment
Measurement of g/vr à 10-6
Cladé et al, Europhys Lett. (2005) p.730
( )
( ) ( )21
21r21
r
Biii
ttNN2vvv
vg
Ntgv
−−+−=
τ−=
τB=1,2 ms and U0 = 2,7 Ermg
k2B
h=τ E
p
ν1ν1
+hk−hk
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MOTOptical molasses
87RbDetection
blow awaybeam
Selection: F=2 → F=1
δsel
π-pulse
Measurement: F=1 → F=2
δmeas
π-pulse
Acceleration accelerationDeceleration
Velocity variation
t : time between the two Raman pulsesN: Number of Bloch oscillations
Acceleration in both opposite directions
Experimental sequence (acceleration)
Acceleration
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Blow-awaybeam
Bloch beam
Raman beam 1and
Raman beam 2
Bloch beam
Detection beams
Signal from F=2Signal from F=1
Raman beam 2
Co ld atomic cloud
Repumping beam
Partially reflect ingplate
λ/2 waveplate
gUpper optical fiber
Lower op tical fiber
Experimental set up
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about 450 Bloch oscillations in each direction : 1800 recoils
ResultsTransfer efficiency : > 99.95% per oscillation (2 recoils)
measurements performed in April 2005
α-1 = 137.035 998 78 (91) 10-7
-1
uncertainty 6.7 × 10- 9
Cladé et al, PRL 96, 033001 (2006)
1 point = 4 spectra
Statistical uncertainty on α = 4.4×10-9
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Systematic effects
!Lasers frequencies : FP cavity → uncertainty 300kHz →
!Beams misalignment : Optical fibers to couple Raman/Bloch beams into the cell
maximum misalignment :
θr = 3×10-5 radθB=1.6×10-4 rad
Correction on α-1: -( 2 ± 2 )×10-9
θr θB
kB
kB
kR
kR
ur(α) = 8 × 10-10
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Systematic effects!Gravity gradient :
R : Earth radiust : spacing time / sel-meas = 12 ms
!Level shifts :- Light shift
F=2
F=1
5P3/2
k2
k1
ωSHF
∆=1050GHzExpansion of the cloud ∆I=10% when k²R ↔ k1
R
ur(α) = 3 × 10-10
-Magnetic field gradient = trajectory effect
up acc.
down acc.
meas.
meas.
sel.
sel.
∆z=0.3mm when k²R ↔ k1R
Correction on α-1 ~ (6.6 ± 2) × 10-9
!Quadratic magnetic force :
Correction on α-1~ ~ 10-10
Rtg 2
−
Correction on α-1~ ~(-1.3 ± 0.4) × 10-9
rvN2t)M/F(
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! What is the momentum transferred to the atoms by laser beams ?
Momentum transferred = gradient of the phase
Gaussian beam : Plane waves superposition :
! Gaussian beam:
Gouy phase
Curvature radius
keff can be measured with a wave front analyzer (R, w)
2
22
2
22// c
kc
k ωω<−= ⊥
( ) ( ) ( ) ( ) ( )z,rz,rkaveckpperEz,rE zeffeffz,ri φ∂=+→= φ h
( ) ( )R2
rkzzkz,r2
G +−= φφ
( )k
dzdR
R2r
zwk2kk 2
2
2eff ××−−=
Gouy phase and wave front curvature
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ρ: densityΓ: natural width∆: detuning
Recoil transmitted by one Bloch oscillation : 2~k or 2n~k ?Doppler effect for the Raman transitions : 2kv or 2nkv ?
( )3
21n
πλ
∆Γ
ρπ=−∆
22
nk Γσ=∆
For the background vapordensity: 8.108 atoms/cm3
Raman beams : ∆= 1050 GHz : (n-1)= 4.10-10 (selection)(n-1)<10-12 (measure)
Bloch beams : ∆ = 40 GHz: (n-1)=2.10-10 (selected atoms)
For the cold atomsInitial atomic density : 1011 atoms/cm3
(n-1) ~ 4.10-10
Refractive index
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PRL 94 170403 (2005) (MIT): Photon Recoil Momentum in Dispersive Media
Observation : modification of recoil energy in a dispersive medium (BEC).
N1 << Ntot
Ntot N0 N1
2n~k2(1-n)N1/N0~k
Dispersive medium Atoms
n : index ofrefraction
Bloch oscillations :
pfinal = 2n~k + 2(1-n) ~k Ntot/Ntot = 2~k if η= 100%
Index of refraction
Accelerated atoms $ dispersive medium
ω= ω - kvatom
otherwise ~(1-η)(n-1)
+ (n-1)kvmediumn
Raman transition :
vmedium
vatom
Atomic cloud
Lω= ω - kvatom+ (n-1)k(vmedium-vatom)
dL/dt = 0 ⇔ vmedium=vatom no effect
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Error budgetSource Correction Uncertainty
(α-1)(ppb) (α-1)(ppb)
"Laser frequencies 0 0.8"Beams alignment - 2 2"Wave front curvature and Gouy phase - 8.2 4"2nd order Zeeman effect 6.6 2"Quadratic magnetic force - 1.3 0.4"Gravity gradient - 0.18 0.02"Light shift (one photon transition) 0 0.2"Light shift (two photon transition) - 0.5 0.2"Light shift (Bloch oscillations) -0.41 0.4"Index of refraction (cold atomic cloud) <0.1 0.3"Index of refraction (background vapor) - 0.37 0.3
Global systematic effects - 6.36 5.0Statistical uncertainty 4.4
TOTAL 6.7
Cladé et al (paper in preparation) α-1 = 137.035 998 84 (91)