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Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Shekhar S. Chandra1
October 22, 2005
1Supervisor: Assoc. Prof. Michael MorganShekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Project Overview
The main objective of the project was to numerically simulateBose-Einstein Condensates (BECs) and study the Aharonov-BohmEffect in BECs. We also provided an unambiguous way toexperimentally retrieve the phase of the complex scalar fieldassociated with BECs for this result.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Outline
1 IntroductionBose-Einstein CondensationGross-Pitaevskii Theory
2 Aharonov-Bohm (AB) EffectThe SetupThe Classical AnalogueThe Quantum AB Effect
3 Phase RetrievalGeneralised Gerchberg-Saxton (GGS) AlgorithmResults
4 SolitonsGross-Pitaevskii Theory for Two-Component BECsResults
5 Conclusion
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Introduction
Bose-Einstein Condensation
Bose-Einstein Condensation
The de Broglie Wavelength isgiven as
λdB =h
p, (1)
where the thermal momentump =
√2mkbT
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Introduction
Gross-Pitaevskii Theory
Gross-Pitaevskii Theory
This is the mean field theory that is encompassed in the TimeDependent Gross-Pitaevskii (TDGP) Equation, independentlydeveloped by Gross & Pitaevskii in 1961.
i~∂Ψ
∂t=
[− ~2
2m∇2 +
1
2mω2|r |2 + g |Ψ|2
]Ψ, (2)
where Ψ is the complex order parameter, m is the mass of theatom involved, ω is the angular frequency of the trap and g is theself-interaction co-efficient.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Aharonov-Bohm (AB) Effect
The Setup
Aharonov-Bohm (AB) Effect
Although the B field is zero outside the solenoid, the chargedparticles undergo path dependent phase changes due to thenon-zero vector potential in and outside the solenoid.
Figure: Aharonov-Bohm effect setup where the two paths (ABF & ACF)undergo different phase shifts.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Aharonov-Bohm (AB) Effect
The Classical Analogue
The Classical Analogue
Berry et al. constructed a water wave analogue to theAharonov-Bohm Effect.
Figure: Aharonov-Bohm effect in water waves.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Aharonov-Bohm (AB) Effect
The Classical Analogue
The Classical Analogue
Berry et al. constructed a water wave analogue to theAharonov-Bohm Effect.
Figure: Aharonov-Bohm effect in water waves.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Aharonov-Bohm (AB) Effect
The Quantum AB Effect
Quantum Construct qC++ & Closing the AB Effect Loop
qC++ is a C++ Toolkit withObject Oriented Design torapidly develop QuantumMechanical Simulations,visualize them and is fullyopen source.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Aharonov-Bohm (AB) Effect
The Quantum AB Effect
The Quantum AB Effect - Results
Figure: The phase dislocations observed in the numerically simulatedBEC as an analogue to the Aharonov-Bohm Effect.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Phase Retrieval
Generalised Gerchberg-Saxton (GGS) Algorithm
Generalised Gerchberg-Saxton (GGS) Algorithm
The Generalised Gerchberg-Saxton Algorithm (iterative phaseretrieval technique) developed by Tan et al. (2003) wasimplemented for the study of the phase dislocations and solitons.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Phase Retrieval
Results
Results
Figure: The results of the GGS Phase Retrieval Technique of Tan et al.(2003) to nucleated vortices. Phase retrieval is valid only to the phases ofthe inner region for the above image.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Solitons
Gross-Pitaevskii Theory for Two-Component BECs
Gross-Pitaevskii Theory for Two-Component BECs
Each component is described by a TDGP equation withself-interaction and inter-component interaction terms, whichinclude examples of a mixture of two different bosonic atoms, suchas 41K & 87Rb, as well as bosons with different internal spin states.
i~∂Ψ1
∂t=
[− ~2
2m∇2⊥ +
1
2mω2|r |2 + g11|Ψ1|2 + g12|Ψ2|2
]Ψ1, (3)
i~∂Ψ2
∂t=
[− ~2
2m∇2⊥ +
1
2mω2|r |2 + g21|Ψ1|2 + g22|Ψ2|2
]Ψ2, (4)
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Solitons
Results
Results
Solitons are spatially confined (localised) solutions to non-linearsystems. In other words, they are non-dispersive solutions withoutthe superposition principle.
Figure: The observation of dark soliton rings in one of the components ofa two-component BEC.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Conclusion
Conclusion
Phase retrieval can be used to study the exotic phase structures ofphase dislocations and solitons in BECs. Future work may include:
Using the phase retrieval technique to measure of theself-interaction co-efficient in BECs.
Using the phase retrieval technique to study the diverse rangeof topological defects in BECs.
The extension of the above into multi-component BECs andinto 3-dimensions.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Conclusion
Conclusion
Phase retrieval can be used to study the exotic phase structures ofphase dislocations and solitons in BECs. Future work may include:
Using the phase retrieval technique to measure of theself-interaction co-efficient in BECs.
Using the phase retrieval technique to study the diverse rangeof topological defects in BECs.
The extension of the above into multi-component BECs andinto 3-dimensions.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Conclusion
Conclusion
Phase retrieval can be used to study the exotic phase structures ofphase dislocations and solitons in BECs. Future work may include:
Using the phase retrieval technique to measure of theself-interaction co-efficient in BECs.
Using the phase retrieval technique to study the diverse rangeof topological defects in BECs.
The extension of the above into multi-component BECs andinto 3-dimensions.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates
Phase Dislocations in Bose-Einstein Condensates
Conclusion
Acknowledgements
I wish to thank my Supervisor Assoc. Prof. Michael Morgan for hisinsight, guidance and critique, without him this project would nothave been possible. Dr. Rotha Yu for his experience and expertisepertaining to the numerical work of the project. Dr. DavidPaganin for his insight and input into the project.
Shekhar S. Chandra Phase Dislocations in Bose-Einstein Condensates