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Stark Spectroscopy of PbF molecule Tao Yang, Priyanka Milinda Rupasinghe, James Coker, Haoquan Fan, John Moore-Furneaux, Neil E. Shafer-ray Homer L. Dodge Department of Physics and Astronomy University of Oklahoma June 23 th, 2011
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Table of Contents History and motivation PbF as a probe for e-EDM 208 Pb 19 F Stark spectroscopy Summary
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History and motivation The existence of the permanent e-EDM results in violations of two fundamental symmetries: Charge- Parity Symmetry and Time Reversal Symmetry. 1950195319561964 2011 Future How time flies * J. J. Hudson, D. M. Kara, I. J. Smallman, B. E. Sauer, M. R. Tarbutt and E. A. Hinds, Nature 473, 493–496 (2011).
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PCT --+ +-- +-- T (CP)
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We do not measure e-EDM directly, however, we measure EDM of an atom or a molecule instead. PbF as a probe for e-EDM E ext E eff
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In practice, we need only a 8kV/cm to get Eeff= ~30GV/cm 10 -30 -15 0 E lab (kV/cm) E eff (GV/cm)
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Possible problem with PbF as a probe of an e-EDM is MAGNETIC MOMENT DEPENDS ON THE MAGNITUDE OF E.
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PbF beam E0E0 Optical Alignment of PbF Optical Probe of PbF To gain sensitivity to the e-EDM,
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Pseudocontinuous resonant enhanced multiphoton ionization (pc-REMPI) 208 Pb 19 F Stark spectroscopy
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PbF + e-e- MCP multichannel scalar 476nm or 468nm 76MHz 6ps 800 mW 436nm or 444nm cw 10MHz ---P. Sivakumar, C. P. McRaven, P. M. Rupasinghe, T. Yang, N. E. Shafer-Ray, Trevor J. Sears and Gregory E. Hall, Molecular Physics: An International Journal at the Interface Between Chemistry and Physics, Volume 108, Issue 7 & 9 (2010).
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Experimental configuration
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---P. Sivakumar, C. P. McRaven, P. M. Rupasinghe, T. Yang, N. E. Shafer-Ray, Trevor J. Sears and Gregory E. Hall, Molecular Physics: An International Journal at the Interface Between Chemistry and Physics, Volume 108, Issue 7 & 9 (2010).
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Numerical solution for the hyperfine and Stark interaction eigenvalues of the effective spin-rotational Hamiltonian ---R. A. Frosch and H. M. Foley, Phys. Rev. 88, 1337–1349 (1952) ---M.G. Kozlov, V.I.Fomichv, Yu Yu Dmitriev, L.N. Labzovsky and A.V. Titov, J. Phys. B: At. Mol. Phys. 20(1987) ---M.G. Kozlov, L.N. Labzowsky, J. Phys. B: At. Mol. Phys. 28(1995)
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Simulation of Stark shift on two branches
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---Lukas D. Alphei, Jens-Uwe Grabow, A. N. Petrov, Richard Mawhorter, Benjamin Murphy, Alexander Baum, Trevor J. Sears, T. Yang, P. M. Rupasinghe, C. P. McRaven and N. E. Shafer-Ray, Phys. Rev. A 83, 040501(R) (2011). This work(66% C.L.) Ref. Y.Y. Dmitriev, et al, Phys. Lett. A 167, 280(1992) Ref. K. I. Baklanov, et al, Phys.Rev.A 82, 060501 (2010) 4.62 D4.26 D ——2.51 D
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Simulation of Stark shift on two branches Q fe (1/2) Ability to do state-selective ionization In an strong electric field depends critically on the curvature of these lines!
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IT WORKS!!! Expected Spectra of the Q[1/2] Transition in an E Field (95% Uniformity)
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---P. Sivakumar, C. P. McRaven, P. M. Rupasinghe, T. Yang, N. E. Shafer-Ray, Trevor J. Sears and Gregory E. Hall, Molecular Physics: An International Journal at the Interface Between Chemistry and Physics, Volume 108, Issue 7 & 9 (2010).
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Summary PbF is a promising candidate for measuring the e-EDM. We have measured the electric dipole moment of the X 1 and A states. The dipole moments of the X 1 and A states allow for an F=1 to F=1 transition that is relatively immune to variations in electric field. This allows for a magnetic field free measurement of the e-EDM eliminating many possible sources of systematic error. This work(66% C.L.) Ref. Y.Y. Dimitiev, et al, Phys. Lett. A 167, 280(1992) Ref. K. I. Baklanov, et al, Phys.Rev.A 82, 060501 (2010) 4.62 D4.26 D 2.51 D
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Professors Neil E. Shafer-ray, John Moore-Furneaux Graduate students Priyanka Milinda Rupasinghe, Tao Yang, James Coker, Haoquan Fan Undergraduate students Jacob Stinnett, Jeffery Gillean Lab members Last Generation of graduate students Poopalasingam Sivakumar, Christopher P. McRaven
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Acknowledgements Supported by the National Science Foundation and the University of Oklahoma’s Office of the Vice President for Research. Thank you!
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