2009
DOI: 10.1109/tac.2009.2031212
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Time-Minimal Control of Dissipative Two-Level Quantum Systems: The Generic Case

Abstract: The objective of this article is to complete preliminary results from [4,13] concerning the time-minimal control of dissipative two-level quantum systems whose dynamics is governed by Lindblad equations. The extremal system is described by a 3D-Hamiltonian depending upon three parameters. We combine geometric techniques with numerical simulations to deduce the optimal solutions.

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Cited by 71 publications
(51 citation statements)
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“…Typically, this requires understanding of the geometry of the control problem from which one can deduce the structure of the optimal solution, a proof of global optimality and physical limits, such as the minimal time to reach the target [5]. Mathematical tools that were developed recently [11][12][13][68][69][70] could tackle problems of increasing difficulty, including fundamental control problems for closed [14,[71][72][73][74][75] and open quantum systems [76][77][78][79][80][81]. This method is able to treat quantum control problems ranging from two and three level quantum systems or two and three coupled spins to two-level dissipative quantum systems with dynamics governed by the Lindblad equation.…”
Section: Geometric Optimal Control -State Of the Artmentioning
confidence: 99%
See 1 more Smart Citation
“…Typically, this requires understanding of the geometry of the control problem from which one can deduce the structure of the optimal solution, a proof of global optimality and physical limits, such as the minimal time to reach the target [5]. Mathematical tools that were developed recently [11][12][13][68][69][70] could tackle problems of increasing difficulty, including fundamental control problems for closed [14,[71][72][73][74][75] and open quantum systems [76][77][78][79][80][81]. This method is able to treat quantum control problems ranging from two and three level quantum systems or two and three coupled spins to two-level dissipative quantum systems with dynamics governed by the Lindblad equation.…”
Section: Geometric Optimal Control -State Of the Artmentioning
confidence: 99%
“…Both analytical and numerical methods have proven very effective for two-and three-level systems [72,[74][75][76][77]80,159,[336][337][338][339][340][341][342][343][344][345][346][347][348], two uncoupled spins [349,350], and two coupled spins [83,85,89,[351][352][353][354][355]. Significant progress has been made in understanding of how to optimally control coupled spin systems with more than two spins [65,71,86,87,[313][314][315][356][357][358][359][360][361][362][363][364][365][366]…”
Section: State Of the Artmentioning
confidence: 99%
“…M 0 is the magnitude of the Bloch vector at thermal equilibrium. Using the symmetry of revolution of the system around the z-axis, we can restrict the problem to only one control field [19,20]. In the following of the paper, we will assume without loss of generality that ω y = 0, which implies that the x-coordinate of the Bloch vector is not coupled to the other components.…”
Section: The Model Systemmentioning
confidence: 99%
“…In recent years, significant progress has been made in quantum control for both numerical [24][25][26][27][28][29][30][31][32][33][34][35][36][37] and analytical [38][39][40][41] methods. Extensive knowledge has been gained on optimal pulse sequences for two-and three-level systems [42][43][44][45][46][47][48][49][50][51][52][53][54][55][56], two uncoupled spins [57,58], and two coupled spins [59][60][61][62][63][64][65]. Further advances have been made on how to optimally control multiple coupled spins .…”
Section: Introductionmentioning
confidence: 99%