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Optimal control theory for unitary transformations
Quantum Physics · Submitted 31 Aug 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Light fields are found that are able to implement the Fourier transform within a picosecond time scale.
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The abstract, sentence by sentence
The dynamics of a quantum system driven by an external field is well described by a unitary transformation generated by a time dependent Hamiltonian. The inverse problem of finding the field that generates a specific unitary transformation is the subject of study. The unitary transformation which can represent an algorithm in a quantum computation is imposed on a subset of quantum states embedded in a larger Hilbert space. Optimal control theory (OCT) is used to solve the inversion problem irrespective of the initial input state. A unified formalism, based on the Krotov method is developed leading to a new scheme. The schemes are compared for the inversion of a two-qubit Fourier transform using as registers the vibrational levels of the $X^1\Sigma^+_g$ electronic state of Na$_2$. Raman-like transitions through the $A^1\Sigma^+_u$ electronic state induce the transitions. Light fields are found that are able to implement the Fourier transform within a picosecond time scale. Such fields can be obtained by pulse-shaping techniques of a femtosecond pulse. Out of the schemes studied the square modulus scheme converges fastest. A study of the implementation of the $Q$ qubit Fourier transform in the Na$_2$ molecule was carried out for up to 5 qubits. The classical computation effort required to obtain the algorithm with a given fidelity is estimated to scale exponentially with the number of levels. The observed moderate scaling of the pulse intensity with the number of qubits in the transformation is rationalized.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The dynamics of a quantum system driven by an external field is well described by a unitary transformation generated by a time dependent Hamiltonian. | background 1.00 | 0.06 | 0.02 | asserted 0.98 |
| s1 | The inverse problem of finding the field that generates a specific unitary transformation is the subject of study. | background 0.69 | 0.18 | 0.04 | asserted 0.99 |
| s2 | The unitary transformation which can represent an algorithm in a quantum computation is imposed on a subset of quantum states embedded in a larger Hilbert space. | background 0.71 | 0.15 | 0.04 | asserted 0.99 |
| s3 | Optimal control theory (OCT) is used to solve the inversion problem irrespective of the initial input state. | method 0.94 | 0.64 | 0.11 | asserted 1.00 |
| s4 | A unified formalism, based on the Krotov method is developed leading to a new scheme. | contribution 0.50 | 0.91 | 0.08 | asserted 1.00 |
| s5 | The schemes are compared for the inversion of a two-qubit Fourier transform using as registers the vibrational levels of the $X^1\Sigma^+_g$ electronic state of Na$_2$. | method 0.79 | 0.88 | 0.05 | asserted 0.97 |
| s6 | Raman-like transitions through the $A^1\Sigma^+_u$ electronic state induce the transitions. | method 0.97 | 0.47 | 0.03 | asserted 1.00 |
| s7 | Light fields are found that are able to implement the Fourier transform within a picosecond time scale. | result 1.00 | 0.89 | 0.23 | asserted 1.00 |
| s8 | Such fields can be obtained by pulse-shaping techniques of a femtosecond pulse. | result 0.44 | 0.52 | 0.07 | asserted 0.80 |
| s9 | Out of the schemes studied the square modulus scheme converges fastest. | result 1.00 | 0.92 | 0.19 | asserted 1.00 |
| s10 | A study of the implementation of the $Q$ qubit Fourier transform in the Na$_2$ molecule was carried out for up to 5 qubits. | contribution 0.86 | 0.93 | 0.09 | asserted 1.00 |
| s11 | The classical computation effort required to obtain the algorithm with a given fidelity is estimated to scale exponentially with the number of levels. | result 0.84 | 0.71 | 0.17 | asserted 0.97 |
| s12 | The observed moderate scaling of the pulse intensity with the number of qubits in the transformation is rationalized. | interpretation 0.90 | 0.83 | 0.17 | asserted 0.97 |
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The paper
Original abstract
The dynamics of a quantum system driven by an external field is well described by a unitary transformation generated by a time dependent Hamiltonian. The inverse problem of finding the field that generates a specific unitary transformation is the subject of study. The unitary transformation which can represent an algorithm in a quantum computation is imposed on a subset of quantum states embedded in a larger Hilbert space. Optimal control theory (OCT) is used to solve the inversion problem irrespective of the initial input state. A unified formalism, based on the Krotov method is developed leading to a new scheme. The schemes are compared for the inversion of a two-qubit Fourier transform using as registers the vibrational levels of the $X^1\Sigma^+_g$ electronic state of Na$_2$. Raman-like transitions through the $A^1\Sigma^+_u$ electronic state induce the transitions. Light fields are found that are able to implement the Fourier transform within a picosecond time scale. Such fields can be obtained by pulse-shaping techniques of a femtosecond pulse. Out of the schemes studied the square modulus scheme converges fastest. A study of the implementation of the $Q$ qubit Fourier transform in the Na$_2$ molecule was carried out for up to 5 qubits. The classical computation effort required to obtain the algorithm with a given fidelity is estimated to scale exponentially with the number of levels. The observed moderate scaling of the pulse intensity with the number of qubits in the transformation is rationalized.
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References
How later papers used it
48 later papers cite it
9 later papers by other authors are listed below: 9 used its method or tool.
Uses its method or tool 9 of 18 papers with this label
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Employed a linear variant of Krotov's method to obtain a monotonically convergent optimization algorithm.
Prospects for fast Rydberg gates on an atom chip (2011) · 1.00 · paraphrased: the licence does not allow quoting
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Defined the specific form of its step-size parameter and shape function as given in this paper.
Optimal Control Design of Robust Raman Pulses for High-Fidelity Cold-Atom Interferometry (2026) · 0.88 · paraphrased: the licence does not allow quoting
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We take [ref] [equation] where $Ω_k^(t)$ is a reference field for each $Ω_k(t)$, $S(t)$ the shape function from Eq. [ref] and $λ_k$ a numerical parameter that controls the magnitude of update in each iteration.
Engineering Strong Beamsplitter Interaction between Bosonic Modes via Quantum Optimal Control Theory (2021) · Quantum Optimal Control Theory · 0.98
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Assumed the function g to take the form given in this paper to minimize the total functional.
Optimally controlled quantum discrimination and estimation (2020) · 0.98 · paraphrased: the licence does not allow quoting
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Used a square-modulus overlap functional from this paper to optimize an effective pi/2 pulse.
Robust Optimized Pulse Schemes for Atomic Fountain Interferometry (2022) · 0.87 · paraphrased: the licence does not allow quoting
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In order to optimize for quantum gates, we use the error-measure [ref] [equation] and take $|ψ_l^⟩ = O |ψ_l^⟩$ as the desired target states for the target gate $O$.
Comparing planar quantum computing platforms at the quantum speed limit (2023) · Quantum optimal control theory · 0.99
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Within 300 iterations, using a square-modulus functional [ref] , we can bring the separation error from 0.648, see Fig. [ref], to $1.26 ×10^-5$.
Rotation Sensing using Tractor Atom Interferometry (2023) · Optimal Control · 0.94
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Introduced real and imaginary parts of its coefficient vectors, an arrangement also used in this paper.
Gradient-based reconstruction of molecular Hamiltonians and density matrices from time-dependent quantum observables (2022) · 0.84 · paraphrased: the licence does not allow quoting
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Considered Krotov's method from this paper as another quantum optimal control protocol.
Hamiltonian Quantum Generative Adversarial Networks (2022) · 0.89 · paraphrased: the licence does not allow quoting
How the literature uses it
1 arXiv paper cite this in 6 sentences
Papers citing it · 2 sentences without a confident label
Uses its method or tool 1 paper
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In the following, we use Krotov's method [ref] in its adaption to quantum dynamics [ref] to carry out the optimization.
Fast and accurate circularization of a Rydberg atom · Optimal control theory · 1.00
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