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Gravitational Aharonov-Bohm effect حمد نوری زنوز م تهراننشگاه داIPM Azar 92
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Gravitational Aharonov-Bohm effect

Jan 26, 2022

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Page 1: Gravitational Aharonov-Bohm effect

Gravitational

Aharonov-Bohm effect

محمد نوری زنوز

دانشگاه تهران

IPM Azar 92

Page 2: Gravitational Aharonov-Bohm effect

Outline of the talk

1-The ColellaOwerhauserWerner effect

2-Aharonov-Bohm effect

3-1+3 formulation of spacetime decomposition

4-Gravitoelectromagnetism and Quasi-

Maxwell form of EFEs

5-Two different versions of GAB effect

6-GA-B in stationary and static spacetimes

7-Gaussian curvature and global effects

Page 3: Gravitational Aharonov-Bohm effect

The COW effect (experiment)

Gravity in quantum mechanics?

A.W. Overhauser, R.

Colella, PRL (1974)

Page 4: Gravitational Aharonov-Bohm effect

Neutron interferometry

How the COW happened?

R. Colella, A.W. Overhauser,

S. A. Werner, PRL (1975)

Page 5: Gravitational Aharonov-Bohm effect

Aharonov-Bohm (Ehrenberg-Siday)

effect

I-Electrons move in field-free region: B = 0 outside the solenoid

II-Classically fields interact locally

Theoretical study:

Page 6: Gravitational Aharonov-Bohm effect

Classically A does not have any direct physical significance

Page 7: Gravitational Aharonov-Bohm effect

In the absence of a

magnetic field

In the presence of

a magnetic field

The solutions are related by a phase factor

Page 8: Gravitational Aharonov-Bohm effect
Page 9: Gravitational Aharonov-Bohm effect

If we want to describe the

influence of B NOT as an

ACTION AT A DISTANCE

(A NON-LOCAL effect) we

MUST use the vector

potential.

R. P. Feynman

Page 10: Gravitational Aharonov-Bohm effect

Experimentally verified by R. G. Chambers

PRL,1960; A. Tonomura et al., PRL, 1982

Page 11: Gravitational Aharonov-Bohm effect

Energy and angular momentum in A-B

effect

Torus is so narrow that is taken as a

constant inside it

Page 12: Gravitational Aharonov-Bohm effect

Distances and time intervals in

spacetimes

Space-time decomposition into spatial

and temporal sections: why?

Measurement : 4d 3d

I-A-observer B-observable

II-1+3 vs 3+1 formulations

Threading and foliation

Page 13: Gravitational Aharonov-Bohm effect

Distances and time intervals

1+ 3 : Threading(projection formalism) Gravitoelectromagnetism

3+1 : Foliation

ADM lapse and shift

For stationary space-times

Page 14: Gravitational Aharonov-Bohm effect

Quasi-Maxwell form of EFEs

D. Lynden-Bell and M. N-Z, RMP, 1998

Page 15: Gravitational Aharonov-Bohm effect

Gravitational Aharonov-Bohm effect

Two versions of GA-B effect :

II-Static space-time (static mass dist.)

Gravitoelectric A-B effect

I- Stationary (non-static) space-time Gravitomagnetic A-B effect (Rotating mass dist.)

Closer analogy to EM A-B effect

due to the appearance of B g

Spacetime has a time-like killing vector field

g0i are non-zero

Time-like Killing vector field is (globally) hypersurface orthogonal

Page 16: Gravitational Aharonov-Bohm effect

GA-B in stationary space-times

When there is a Bg field one could think of Gravitomagnetic Aharonov-Bohm effect

Weak field approximation

Einstein field eqs.

E. G. Harris, AJP 1995

Page 17: Gravitational Aharonov-Bohm effect

Solving Klein-Gordon eqn.

for a scalar field of mass M

H = 0 for r > r0

Page 18: Gravitational Aharonov-Bohm effect

Globally stationary but locally static

space-times

Stachel PRD, 1981

For a globally stationary but locally static space-time

The integral of the gravitomagnetic potential over a

closed path is non- zero

Van Stockum solution of a rigidly

rotating dust cylinder has such a property.

Page 19: Gravitational Aharonov-Bohm effect

GA-B in Static space-times

Particles constrained to move in a region where the Riemann tensor vanishes may nonetheless exhibit physical effects arising from non-zero curvature in a region from which they are excluded

Page 20: Gravitational Aharonov-Bohm effect

Ford & Vilenkin’s approach Space-time of a Tube like distribution of matter with a time-like and a space-like

Killing vector fields generating time translation and translations along the z-axis.

S

S0

C

Tube like distribution of matter

With non-zero curvature interior

2-surface orthogonal

to the Killing vectors

C in the asymptotically

flat region

Gauss-Bonnet

formula S is asymptotically a conical

surface rather than a plane

Page 21: Gravitational Aharonov-Bohm effect

Consider the static metric

Metric of the 2-surface is

Choose the coordinates so that

angle subtended at the apex R

0 < b < 1

Page 22: Gravitational Aharonov-Bohm effect

The Gaussian curvature K of S in terms of

the Riemann tensor of the 4-dim space-time

Assuming the source to be independent of t and z

For a dust source with only

i.e mass per unit length of the tube

Page 23: Gravitational Aharonov-Bohm effect

Gaussian curvature & global effects

M.N-Z and A. Parvizi, PRD, 2013

Page 24: Gravitational Aharonov-Bohm effect

Static tube-like dust space-time In asympt. Flat region

Page 25: Gravitational Aharonov-Bohm effect

Cylindrically symmetric dust spacetime

Page 26: Gravitational Aharonov-Bohm effect
Page 27: Gravitational Aharonov-Bohm effect
Page 28: Gravitational Aharonov-Bohm effect

Experiment proposal

Page 29: Gravitational Aharonov-Bohm effect

Yet another Gravitational analogue of the electrostatic A-B effect: Gravitostaic A-B effect

Page 30: Gravitational Aharonov-Bohm effect

Conclusions

1-Gravitoelectric A-B within full EFEs i.e NO weak field approx.

2-GA-B and COW effect both as geometrical effects and under

the same flag!

Page 31: Gravitational Aharonov-Bohm effect

Thank you for your

attention