Difference between revisions of "Quantum Control"

From KAIST Quantum Computing Lab Wiki
Jump to navigationJump to search
Line 8: Line 8:
 
<center>Fig.1: schematic diagram of the experimental setup</center>
 
<center>Fig.1: schematic diagram of the experimental setup</center>
  
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.  
+
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.  
  
 
[[Image:Intensity_total_v4.jpg|center|400px]]
 
[[Image:Intensity_total_v4.jpg|center|400px]]

Revision as of 04:27, 28 August 2009

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) processes between two states is one of famous systema of 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) has to be considered.

Setup dazzler.jpg
Fig.1: schematic diagram of the experimental setup

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.

Intensity total v4.jpg
Fig.2: fluoresence as a function of chirp rates and transform-limited intensity of pulses

A linear chirped pulse is more optimal than a transform-limited pulse.


Detuning total v6.jpg
Fig.3: fluorescence as a function of detuning and chirp rates