Difference between revisions of "Quantum Control"
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[[Image:Detuning_total_v6.jpg|center|200px]] | [[Image:Detuning_total_v6.jpg|center|200px]] | ||
<center>''Fig.3: fluorescence as a function of detuning and chirp rates''</center> | <center>''Fig.3: fluorescence as a function of detuning and chirp rates''</center> | ||
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+ | <big>'''Strong-field two-photon absorption in atomic cesium: an analytical control approach</big><br> | ||
+ | [[Image:Strongfield.jpg|left|200px]] | ||
+ | |||
+ | We have considered an analytical control of two-photon absorption | ||
+ | process of atoms in the strong-field interaction regime. The experiment | ||
+ | was performed on gaseous cesium atoms strongly interacting with a | ||
+ | shaped laser-pulse from a femtosecond laser amplifier and a programmable | ||
+ | pulse-shaper. When this shaped laser-pulse transfers the atomic population | ||
+ | from the 6s ground state to the 8s excited state, we have found that both | ||
+ | positively- and negatively-chirped laser pulses, compared with a Gaussian | ||
+ | pulse, enhance this excitation in the strong-field regime of laser-atom | ||
+ | interaction. This unusual phenomena is explained because the temporal | ||
+ | shape of the laser intensity compensates the effect of dynamic Stark shift for | ||
+ | the two-photon resonant condition to be optimally maintained. We provide | ||
+ | analytic calculations using the strong-field phase matching, which show | ||
+ | good agreement with the experiment. | ||
+ | |||
+ | [http://www.opticsinfobase.org/abstract.cfm?uri=oe-17-9-7648 27 April 2009 / Vol. 17, No. 9 / OPTICS EXPRESS 7648] | ||
+ | |||
+ | |||
+ | <big>'''Strong-Field two-photon transition by phase shaping</big><br> | ||
+ | [[Image:Rb_TPA.jpg|left|150px]] | ||
+ | We demonstrate the ultrafast coherent control of a non-linear two-photon absorption in a dy- | ||
+ | namically shifted energy level structure. We use a spectro-temporal laser pulse shaping that is | ||
+ | programmed to preserve the resonant absorption condition during the intense laser ¯eld interaction. | ||
+ | Experiments carried out in the strong-¯eld regime of two-photon absorption in the ground state | ||
+ | of atomic Cesium reveal that the analytically obtained o®set and curvature of a laser spectrum | ||
+ | compensate the effect of both static and dynamic energy shifts of the given light-atom interaction. | ||
+ | |||
+ | PRA accepted Tuesday Jul 20, 2010 | ||
+ | |||
+ | |||
+ | <big>'''Coherent Control in 2D-FTES'''</big><br> | ||
+ | [[Image:2D_FTES-highlight.JPG|left|100px]] | ||
+ | |||
+ | We demonstrate the advantage of applying coherent control technique to 2D-FTES spectroscopy. By shaping individual pulses used in 2D-FTES on atomic model system, we selectively turn on and off specific couplings. This advanced 2D-FTES technique may be useful for probing time-dependent coupling paths among multilevel electronic energy states in complex systems | ||
+ | <br><br><br><br> |
Revision as of 15:25, 30 July 2010
Two photon absorption in strong field
A shaped ultrafast pulse makes it possible to stir a quantum system and thus control a quantum process via light-matter interaction. Two photon absorption(TPA) process in two-level atoms is one of the good testbed for coherent control. We study coherent control schemes for a TPA process in a strong field. For a optimal coherent scheme to enhance TPA, strong field effects(dynamic Stark shift) have been considered.
In weak field reigme, a transform-limited pulse is a optimal pulse to enhance a TPA. But it is not a optimal solution in strong field. The dynamic Stark shift disturbs a TPA process.
A linear chirped pulse is more optimal than a transform-limited pulse.
Strong-field two-photon absorption in atomic cesium: an analytical control approach
We have considered an analytical control of two-photon absorption process of atoms in the strong-field interaction regime. The experiment was performed on gaseous cesium atoms strongly interacting with a shaped laser-pulse from a femtosecond laser amplifier and a programmable pulse-shaper. When this shaped laser-pulse transfers the atomic population from the 6s ground state to the 8s excited state, we have found that both positively- and negatively-chirped laser pulses, compared with a Gaussian pulse, enhance this excitation in the strong-field regime of laser-atom interaction. This unusual phenomena is explained because the temporal shape of the laser intensity compensates the effect of dynamic Stark shift for the two-photon resonant condition to be optimally maintained. We provide analytic calculations using the strong-field phase matching, which show good agreement with the experiment.
27 April 2009 / Vol. 17, No. 9 / OPTICS EXPRESS 7648
Strong-Field two-photon transition by phase shaping
We demonstrate the ultrafast coherent control of a non-linear two-photon absorption in a dy- namically shifted energy level structure. We use a spectro-temporal laser pulse shaping that is programmed to preserve the resonant absorption condition during the intense laser ¯eld interaction. Experiments carried out in the strong-¯eld regime of two-photon absorption in the ground state of atomic Cesium reveal that the analytically obtained o®set and curvature of a laser spectrum compensate the effect of both static and dynamic energy shifts of the given light-atom interaction.
PRA accepted Tuesday Jul 20, 2010
Coherent Control in 2D-FTES
We demonstrate the advantage of applying coherent control technique to 2D-FTES spectroscopy. By shaping individual pulses used in 2D-FTES on atomic model system, we selectively turn on and off specific couplings. This advanced 2D-FTES technique may be useful for probing time-dependent coupling paths among multilevel electronic energy states in complex systems