PT Symmetry in Optics, Exceptional Points and Bound States in the Continuum

PT Symmetry in Optics, Exceptional Points and Bound States in the Continuum

International Centre for Theoretical Sciences via YouTube Direct link

Modified KdV Equations

18 of 23

18 of 23

Modified KdV Equations

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PT Symmetry in Optics, Exceptional Points and Bound States in the Continuum

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  1. 1 INTERNATIONAL
  2. 2 NON-HERMITIAN PHYSICS PHHQP XVIII
  3. 3 PT Symmetry in Optics, Exceptional Points and Bound States in the Continuum
  4. 4 PT Symmetric Systems Outline of the talk
  5. 5 The norm has to be redefined Das et al., Bender, Mostafazadeh: olun:=only.
  6. 6 PT Symmetric Potential: Example
  7. 7 SUSY and PT symmetric Phases Potential is invariant under the transformation A + + B - S:
  8. 8 E? = -B- " - na2.
  9. 9 Phases of SUSY Broken phases of SUSY occur for different parameter domains with real eigenvalues.
  10. 10 Bound States in Continuum In the PT-broken phase, energy can be still real provided
  11. 11 Scattering by PT Symmetric Systems
  12. 12 sospectral Deformation and Connection with KdV The earlier mentioned two superpotentials WI and W2 Eq.
  13. 13 Light Stops at Exceptional Point The group velocity of light has been shown to vanish at except tonal point.
  14. 14 Experimental observation of PTSY-QM
  15. 15 Coherent Perfect Absorber CPA
  16. 16 PT-CPA Laser
  17. 17 PT Symmetric Solutions in Modified KdV Equation
  18. 18 Modified KdV Equations
  19. 19 Complex superposed solutions
  20. 20 Some remarks
  21. 21 - 602Ur + Vers = 0, there exist solutions in the form of complex superposition.
  22. 22 Conclusions
  23. 23 Thank you for your patience and attention

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