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Shouvik Kanti Bhattacharya
PHY791 | 04.10.2014
“Active Cancellation of stray magnetic
fields in a Bose-Einstein Condensation
experiment”
C. J. Dedman, R. G. Dall, L. J. Byron, and A. G.
Truscott
Review of Scientific Instruments
78, 024703(2007)[1]
Phase transition of a graduate
student
 Moved to Omaha from Boston on the 10th
of August, 2013.
 Went through 3 different orientations in
the following 8 days (August 12- August
20, 2013).
 Engaged in analytical solution of finding
an optimum setup for cancelling magnetic
fields and presented my work on October
30, 2013.
Bhattacharya 2
A common example of phase transition
Bhattacharya 3
Figure 1. The front yard of my residence, picture taken April 4, 2014, 8:42 am
CST.
Sublimation/Evaporation
Bhattacharya 4
Figure 2. The front yard of my residence, picture taken April 4, 2014, 3:03 pm
CST.
Let’s remind us about the Bose-
Einstein condensate
 Bose-Einstein condensation is a phase
transition.
 All bosons are at the ground state.
 The condensate occurs at a thermal
equilibrium.
 Superfluidity of helium and
superconductivity of an electron gas are
caused by the Bose Einstein condensate.
Bhattacharya 5
Experimental Setup of the BEC
 “The possibility of creating optical fields
with many photons in a single mode of a
resonator was realized with the creation of
the laser in 1960. The possibility of
creating a matter-wave field with many
atoms in a single mode of an atom trap-
the atomic equivalent of an optical
resonator-was realized with the
achievement of Bose-Einstein
condensation(BEC) in 1995.” Wolfgang
Ketterle[2]
Bhattacharya 6
History of the BEC Experiments
Bhattacharya 7
Figure 3. History of the BEC publications over time[2]
Controlling the Magnetic fields
Bhattacharya 8
 A Stable magnetic field where the bosons
are trapped in is a key requirement for
many BEC and ultra cold atom
experiments.
 Examples: Quantum information
processing, quantum simulation with
qubits encoded in field sensitive atomic
spin states.[3]
Controlling the Magnetic fields (cont.)
Bhattacharya 9
 A complete shielding of the exterior
magnetic field is also desired in some
cases.
 Experiment on the spinor condensates
require to suppress the background
magnetic field.[3]
Bhattacharya 10
Figure 4. Magnetic Noise [1]
What did they do?
 An active system that responds to an
abrupt change in magnetic field up to 3
kHz noise.
 Their main objective was stabilizing the
magnetic field by one part in ten thousand
(10-10 T).
Bhattacharya 11
Some ways to shield a magnetic field
 Shielding by a high permeable material
 Shielding by Eddy current
 Using 3-pairs of “active” Helmholtz
Coil
Bhattacharya 12
Bhattacharya 13
Figure 5. Experimental Design[1]
Integrator
Bhattacharya 14
Figure 6. A Schematic Diagram of an Integrator Circuit, Image courtesy:
http://www.electronics-tutorials.ws/opamp/opamp_6.html
Integrating Vin
Bhattacharya 15
Figure 7.Image courtesy: http://www.electronics-
tutorials.ws/opamp/opamp_28.html
Differentiator
Bhattacharya 16
Figure 8. A Schematic Diagram of a Differentiator Circuit, Image Courtesy:
http://www.electronics-tutorials.ws/opamp/opamp_7.html
Differentiating Vin
Bhattacharya 17
Figure 9 Image courtesy: http://www.electronics-
tutorials.ws/opamp/opamp_42.html
Result
Bhattacharya 18
Scope of work
 Currently enrolled in PHY582 and hoping
to finish the geomagnetic field
suppression (passive system) experiment
this semester.
 Planning to enroll in PHY799 in summer
and start making progress in the active
magnetic field suppression.
Bhattacharya 19
Helmholtz Coils
20
1
2
Figure 10. A pair of Helmholtz coils. Image Courtesy:
http://physicsx.pr.erau.edu/HelmholtzCoils/HelmholtzCoils.jpg
Radia
Bhattacharya 21
Figure 11. Changing the separation parameter and reporting associated
magnetic field with it.
Acknowledgements
 I would like to primarily thank to Dr.
Jonathan Wrubel, Dr. Andrew Baruth, and
Dr. Michael Nichols.
 Dr. David Sidebottom and Dr. Kyle Watters
 Nathan Holman and the AMO Research
group at Creighton University (Spring
2014)
Bhattacharya 22
References
[1] C. J. Dedman, R. G. Dall, L. J. Byron, and A. G. Truscott. 2007.
Review of Scientific Instruments 78, 024703.
[2] Ketterle, Wolfgang. December, 1999. Physics Today.
[3] A Smith, B E Anderson, S Chaudhury, and P S Jessen, J. Phys. B:
At. Mol. Opt. Phys. 44 (2011) 205001 (7ppm).
Bhattacharya 23
Questions
Bhattacharya 24
Figure 12. Bose Residency: Image Courtesy:
http://upload.wikimedia.org/wikipedia/commons/2/22/Bose_Institute_-
_Kolkata_7354.JPG

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PHY791 | Thesis Presentation (Spring 2014)

  • 1. Shouvik Kanti Bhattacharya PHY791 | 04.10.2014 “Active Cancellation of stray magnetic fields in a Bose-Einstein Condensation experiment” C. J. Dedman, R. G. Dall, L. J. Byron, and A. G. Truscott Review of Scientific Instruments 78, 024703(2007)[1]
  • 2. Phase transition of a graduate student  Moved to Omaha from Boston on the 10th of August, 2013.  Went through 3 different orientations in the following 8 days (August 12- August 20, 2013).  Engaged in analytical solution of finding an optimum setup for cancelling magnetic fields and presented my work on October 30, 2013. Bhattacharya 2
  • 3. A common example of phase transition Bhattacharya 3 Figure 1. The front yard of my residence, picture taken April 4, 2014, 8:42 am CST.
  • 4. Sublimation/Evaporation Bhattacharya 4 Figure 2. The front yard of my residence, picture taken April 4, 2014, 3:03 pm CST.
  • 5. Let’s remind us about the Bose- Einstein condensate  Bose-Einstein condensation is a phase transition.  All bosons are at the ground state.  The condensate occurs at a thermal equilibrium.  Superfluidity of helium and superconductivity of an electron gas are caused by the Bose Einstein condensate. Bhattacharya 5
  • 6. Experimental Setup of the BEC  “The possibility of creating optical fields with many photons in a single mode of a resonator was realized with the creation of the laser in 1960. The possibility of creating a matter-wave field with many atoms in a single mode of an atom trap- the atomic equivalent of an optical resonator-was realized with the achievement of Bose-Einstein condensation(BEC) in 1995.” Wolfgang Ketterle[2] Bhattacharya 6
  • 7. History of the BEC Experiments Bhattacharya 7 Figure 3. History of the BEC publications over time[2]
  • 8. Controlling the Magnetic fields Bhattacharya 8  A Stable magnetic field where the bosons are trapped in is a key requirement for many BEC and ultra cold atom experiments.  Examples: Quantum information processing, quantum simulation with qubits encoded in field sensitive atomic spin states.[3]
  • 9. Controlling the Magnetic fields (cont.) Bhattacharya 9  A complete shielding of the exterior magnetic field is also desired in some cases.  Experiment on the spinor condensates require to suppress the background magnetic field.[3]
  • 10. Bhattacharya 10 Figure 4. Magnetic Noise [1]
  • 11. What did they do?  An active system that responds to an abrupt change in magnetic field up to 3 kHz noise.  Their main objective was stabilizing the magnetic field by one part in ten thousand (10-10 T). Bhattacharya 11
  • 12. Some ways to shield a magnetic field  Shielding by a high permeable material  Shielding by Eddy current  Using 3-pairs of “active” Helmholtz Coil Bhattacharya 12
  • 13. Bhattacharya 13 Figure 5. Experimental Design[1]
  • 14. Integrator Bhattacharya 14 Figure 6. A Schematic Diagram of an Integrator Circuit, Image courtesy: http://www.electronics-tutorials.ws/opamp/opamp_6.html
  • 15. Integrating Vin Bhattacharya 15 Figure 7.Image courtesy: http://www.electronics- tutorials.ws/opamp/opamp_28.html
  • 16. Differentiator Bhattacharya 16 Figure 8. A Schematic Diagram of a Differentiator Circuit, Image Courtesy: http://www.electronics-tutorials.ws/opamp/opamp_7.html
  • 17. Differentiating Vin Bhattacharya 17 Figure 9 Image courtesy: http://www.electronics- tutorials.ws/opamp/opamp_42.html
  • 19. Scope of work  Currently enrolled in PHY582 and hoping to finish the geomagnetic field suppression (passive system) experiment this semester.  Planning to enroll in PHY799 in summer and start making progress in the active magnetic field suppression. Bhattacharya 19
  • 20. Helmholtz Coils 20 1 2 Figure 10. A pair of Helmholtz coils. Image Courtesy: http://physicsx.pr.erau.edu/HelmholtzCoils/HelmholtzCoils.jpg
  • 21. Radia Bhattacharya 21 Figure 11. Changing the separation parameter and reporting associated magnetic field with it.
  • 22. Acknowledgements  I would like to primarily thank to Dr. Jonathan Wrubel, Dr. Andrew Baruth, and Dr. Michael Nichols.  Dr. David Sidebottom and Dr. Kyle Watters  Nathan Holman and the AMO Research group at Creighton University (Spring 2014) Bhattacharya 22
  • 23. References [1] C. J. Dedman, R. G. Dall, L. J. Byron, and A. G. Truscott. 2007. Review of Scientific Instruments 78, 024703. [2] Ketterle, Wolfgang. December, 1999. Physics Today. [3] A Smith, B E Anderson, S Chaudhury, and P S Jessen, J. Phys. B: At. Mol. Opt. Phys. 44 (2011) 205001 (7ppm). Bhattacharya 23
  • 24. Questions Bhattacharya 24 Figure 12. Bose Residency: Image Courtesy: http://upload.wikimedia.org/wikipedia/commons/2/22/Bose_Institute_- _Kolkata_7354.JPG