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Nuestro Coloquio de Hoy




 Estimados Colegas,
 
 En nuestro Coloquio de hoy contaremos con la presencia del Dr. Roland
 Lefebvre del Laboratorio de Fotofísica Molecular del CNRS en Orsay,
 Francia. Su platica se intitula:
 
           "Zero-Width Resonances and Exceptional Points
                  in Molecular Photodissociation"
                 
 Nos dará mucho gusto contar con su amable presencia, el día de hoy
 miércoles 24 de febrero a las 5:30 PM, en el auditorio del Instituto
 de Ciencias Físicas de la UNAM- Campus Morelos.
 
 Atentamente:
 
 Maximino Aldana y Guillermo Hinojosa.
                 
                                ~ Abstract ~
                               
 The interaction of a molecule with a cw laser field is described by a
 time-periodic Hamiltonian. The wave equation has solutions given by the
 Floquet formalism, with eigenvalues called the quasi-energies. If the field
 can lead to photodissociation of the molecule, these quasi-energies are
 complex, with an imaginary part yielding the photofragmention rate. In the
 case of intense fields, there is a richness of new processes. We are here
 interested[1] by the possibility, with an appropriate choice of laser
 intensity, to reduce to zero the imaginary part of the energies of some
 of the resonances associated with field-free vibrational states of a
 diatomic molecule. The example is the molecular ion H2+. Not all resonances
 present this property for a given wavelength. The Floquet formalism is
 applicable even for a pulsed laser if the amplitude of the field is varying
 smoothly enough. It is then possible to build filtration scenarios where
 only the resonances passing through the zero-width phenomenon during the
 pulse will survive. Another situation which is possible with an appropriate
 choice of both wavelength and intensity is to provoke the coalescence of
 two quasi-energies. The corresponding point in parameter plane is called
 exceptional. Such points have recently been studied in many areas of physics,
 either classical or quantum. They have a number of very important consequences
 which will be presented for the case of molecular photodissociation [2].
 A condition for two resonances to yield such a point is that they correspond
 to respectively a shape-like resonance and a Feshbach-like one. At an
 exceptional point the two resonance wave functions merge into a single one,
 which is said to be ”self-orthogonal”. With an adiabatic variation
 of the parameters along a closed contour around an exceptional point, it is
 possible to go from one non-degenerate resonance pole to another. In order to
 realize such a transfer, it is necessary to reach a compromise between two
 conflicting conditions: the laser pulse must vary slowly enough for an adiabatic
 transfer to take place, but fast enough to keep a fair amount of undissociated
 molecules. This can be checked through the adiabatic Floquet theory.
 
 [1] O. Atabek, R. Lefebvre, C. Lefebvre and T.T. Ngyugen-Dang,
 Phys. Rev. A 74, 063412(2008)
 [2] R. Lefebvre, O. Atabek, M. ¢ Sindelka and N. Moiseyev, Phys. Rev. Lett.
 103, 123003(2009).