Title: Derek F' Jackson Kimball
1A new search for aspin-gravity interaction
Eric Bahr, Valentin Dutertre, Srikanth
Guttikonda, Rene Jacome, and Khoa Nguyen
Funded by the National Science Foundation
2Dima Budker and friends.
Only 30 min from UC Berkeley!
3Guess
Within next 10-50 (?) years, our
present understanding of gravity will be
radically revised.
- Gravity is very weak, experiments are hard.
- Most tests of General Relativity are
observational. - Lots of mysteries are somehow associated with
gravity - - Dark Matter
- - Dark Energy
- GR and quantum mechanics dont fit together
nicely.
4A spin-gravity coupling?
Many physicists have proposed the possibility of
a long-range spin-gravity coupling...
Hamiltonian in Earths field
Shift of Zeeman sublevels
Spin precession
?
g
?
S
?0
?E
M -1 M 0 M 1
F1 ? F0
5A spin-gravity coupling?
What might cause a spin-gravity interaction?
Truth Who knows?
Guesses
- Einstein-Cartan Theory incorporates spin into
- General Relativity, so that spin becomes
generator of - a form of space-time curvature called torsion,
- leads to various spin-mass couplings.
- Quantum theories of gravity often propose
spin-1 and - spin-0 partners of the standard spin-2
graviton. - Spin-1, spin-0 gravitons can generate
spin-mass couplings.
6Violates Equivalence Principle!
?
?
g
a
No spin precession in accelerating frame.
Gravitational field causes spin precession.
Violates parity conservation and time-reversal
invariance!
7Distinct from some other sources of spin-mass
couplings
Lense-Thirring precession
General relativistic frame-dragging (Gravity
Probe B)
Axions
8Previous Searches
9Previous Searches
Best limit on gravitational dipole
moment Venema, Majumder, Lamoreaux, Heckel,
Fortson (1992). PRL 68, 135.
10Need sensitive measurement of atomic
spin-precession...
See Rene Jacomes talk to follow...
Nonlinear Magneto-Optical Rotation with
Frequency-modulated Light (FM NMOR)
11Projected sensitivity of FM NMOR to Zeeman shifts
Sensitivity to precession frequency is
sufficient to search for k1.
Improvement of 100 times!
12FM NMOR Gyroscope
87
Rb
13Electron spin serves as co-magnetometer for
nuclear spin
14Experimental Setup
15Systematic Effects
- Magnetic fields and gradients
- Earths rotation
- Collisional effects
- Nonlinear Zeeman effect
- AC Stark shifts due to optical fields
- Apparatus misalignments
- Geometric (Berrys) Phase
16Systematic Effects
Nuclear magnetic moment can generate ??
0.3 Hz for B 1 mG!
Controlled by magnetic field reversal and precise
measurement of B via FM NMOR.
?? ? 10-9 Hz
nucl
17Systematic Effects
Earths rotation can generate ??
Atomic spins are effectively decoupled from
laboratory spins inertial frame viewed from
noninertial lab frame.
?
? 11.6 ?Hz
E
?
1
B
1
?
E
?
1
g
Solution? Align B along ? to make effect
quadratic in misalignment, transverse field
resonances enable precise alignment.
1
1
E
18Where are we now?
5-layer magnetic shield constructed magnetic
field reduced 10,000,000 times!
19Where are we now?
Set of 7 independent coils designed and mount
built for precise control of magnetic fields.
Special antirelaxation- coated cells manufactured
20Where are we now?
Laser system and optics being tested...
21Where are we now?
Having lots of fun!
22Future
- Working on FM NMOR setup, optimizing
- magnetometric sensitivity...
- Demonstrate FM NMOR gyro and optimize
- sensitivity (amplitudes of F2,1 resonances).
- Detect nuclear magnetic moments, Earths
- rotation ? sensitivity test.
- Study collisional effects, Berrys phase.
- Look for spin-gravity coupling!