Optimal pulse sequences for population transfer in multilevel systems

1999 ◽  
Vol 60 (4) ◽  
pp. 3081-3090 ◽  
Author(s):  
Ignacio R. Solá ◽  
Vladimir S. Malinovsky ◽  
David J. Tannor
1995 ◽  
Vol 52 (1) ◽  
pp. 566-582 ◽  
Author(s):  
B. W. Shore ◽  
J. Martin ◽  
M. P. Fewell ◽  
K. Bergmann

1996 ◽  
pp. 287-294
Author(s):  
K. Bergmann ◽  
J. Martin ◽  
B. W. Shore

Author(s):  
Y. Ohta ◽  
T. Yoshimoto ◽  
T. Bando ◽  
H. Kizu ◽  
H. Nagao ◽  
...  

2012 ◽  
Vol 350 ◽  
pp. 012004 ◽  
Author(s):  
V Chaltykyan ◽  
E Gazazyan ◽  
G Grigoryan ◽  
A Hovhannisyan ◽  
O Tikhova

2017 ◽  
Vol 66 (21) ◽  
pp. 213301
Author(s):  
Zhang Lu ◽  
Yan Lu-Yao ◽  
Bao Hui-Han ◽  
Chai Xiao-Qian ◽  
Ma Dan-Dan ◽  
...  

1986 ◽  
Vol 6 (1) ◽  
pp. 47-60 ◽  
Author(s):  
Mark A. Banash ◽  
Warren S. Warren

Conventional coherent pulse sequences such as photon echoes measure only highly averaged relaxation rates in complex multilevel systems, such as molecules undergoing state-changing collisions. Pulse frequency, phase, and shape control lets us generate sequences which give a more detailed understanding of the dynamics. Results of dual frequency, crafted shape sequences on I2 are presented which show that the "coherence dephasing" time T2 is primarily due to population redistribution (energy changing collisions) in the electronically excited state, and that the electronic ground state has a much smaller cross section for such collisions. Quantitative analysis is only possible with modified laser pulse shapes which excite a single velocity component, and requires pulse sequences which correct for the hyperfine dependence of predissociation. Since this correction is rarely made in previously reported coherent transient measurements, literature values of T2 and T1 may not be reliable in the zero pressure limit.


Author(s):  
Zhicheng Shi ◽  
Cheng Zhang ◽  
Du Ran ◽  
Yan Xia ◽  
Reuven Ianconescu ◽  
...  

Abstract In this work, we propose a composite pulses scheme by modulating phases to achieve high fidelity population transfer in three-level systems. To circumvent the obstacle that not enough variables are exploited to eliminate the systematic errors in the transition probability, we put forward a cost function to find the optimal value. The cost function is independently constructed either in ensuring an accurate population of the target state, or in suppressing the population of the leakage state, or both of them. The results demonstrate that population transfer is implemented with high fidelity even when existing the deviations in the coupling coefficients. Furthermore, our composite pulses scheme can be extensible to arbitrarily long pulse sequences. As an example, we employ the composite pulses sequence for achieving the three-atom singlet state in an atom-cavity system with ultrahigh fidelity. The final singlet state shows robustness against deviations and is not seriously affected by waveform distortions. Also, the singlet state maintains a high fidelity under the decoherence environment.


Sign in / Sign up

Export Citation Format

Share Document