Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Realizing Controllable Quantum States

Hideaki Takayanagi, Junsaku Nitta

Published Jan 1, 2005• 12 citations
OpenAlex

Related papers

Control of Quantum Systems

Manoj Kumar

•Jan 1, 2019•0 citations

Preparation of the entanglement states by realizing the Hadamard and CNOT quantum gates

Nourallah Ghaeminezhad, Shuang Cong

The preparation of the maximum entangled states, i.e., the Bell states is studied in this paper. The Cartan decomposition and the Lyapunov control methods are used to design the control laws for some operations in realizing the Hadamard and CNOT gates to prepare the Bell states. The numerical simulation experiments show that for some proper control parameters in the designed control laws, the Hadamard and CNOT gates are realized and the stable Bell states are prepared in a short time.

IEEE Information Technology, Networking, Electronic and Automation Control Conference (ITNEC)•Mar 1, 2019•1 citation

Stochastic feedback control of quantum transport to realize a dynamical ensemble of two nonorthogonal pure states

Shakib Daryanoosh, Howard M. Wiseman, Tobias Brandes

A Markovian open quantum system which relaxes to a unique steady state ${\ensuremath{\rho}}_{\mathrm{ss}}$ of finite rank can be decomposed into a finite physically realizable ensemble (PRE) of pure states. That is, as shown by R. I. Karasik and H. M. Wiseman [Phys. Rev. Lett. 106, 020406 (2011)], in principle there is a way to monitor the environment so that in the long-time limit the conditional state jumps between a finite number of possible pure states. In this paper we show how to apply this idea to the dynamics of a double quantum dot arising from the feedback control of quantum transport, as previously considered by C. P\"oltl, C. Emary, and T. Brandes [Phys. Rev. B 84, 085302 (2011)]. Specifically, we consider the limit where the system can be described as a qubit, and show that while the control scheme can always realize a two-state PRE, in the incoherent-tunneling regime there are infinitely many PREs compatible with the dynamics that cannot be so realized. For the two-state PREs that are realized, we calculate the counting statistics and see a clear distinction between the coherent and incoherent regimes.

arXiv:1510.05180•Physical review. B./Physical review. B•Feb 18, 2016•10 citations

Control of Quantum Systems

Shuang Cong

Wiley eBooks•Mar 4, 2014•65 citations

Control of Quantum Systems

P. Zoller, J. I. Cirac, S. M. Girvin +1 more

WORLD SCIENTIFIC eBooks•Mar 26, 2013•0 citations

Optimal Control-Assisted Rapid Quantum State Transfer on 1-D Spin Chain

Kai Zhang, Sen Kuang

Traditional many-body teleportation relies on the strong interaction property of a quantum many-body system, which usually requires numerous qubits and entanglement resources, making it difficult to realize experimentally. A natural scheme is to use a 1D spin chain with simple structure to realize many-body teleportation. In this paper, we analyze the conditions for general quantum many-body teleportation and construct an effective control Hamiltonian, realizing quantum many-body teleportation on the controlled 1D spin chain. Our scheme, which only requires forward evolution and local measurements, can be used to perform quantum state transfer without the special presetting and modulation of coupling parameters of the chain and without strict control over the evolution time, thereby enhancing the experimental realizability. Furthermore, we improve the efficiency and accuracy of quantum state transfer by introducing quantum optimal control (QOC) technique to optimize the control pulse sequences.

IEEE Transactions on Quantum Engineering•Dec 8, 2025•0 citations
A Markovian open quantum system which relaxes to a unique steady state ${\ensuremath{\rho}}_{\mathrm{ss}}$ of finite rank can be decomposed into a finite physically realizable ensemble (PRE) of pure states. That is, as shown by R. I. Karasik and H. M. Wiseman [Phys. Rev. Lett. 106, 020406 (2011)], in principle there is a way to monitor the environment so that in the long-time limit the conditional state jumps between a finite number of possible pure states. In this paper we show how to apply this idea to the dynamics of a double quantum dot arising from the feedback control of quantum transport, as previously considered by C. P\"oltl, C. Emary, and T. Brandes [Phys. Rev. B 84, 085302 (2011)]. Specifically, we consider the limit where the system can be described as a qubit, and show that while the control scheme can always realize a two-state PRE, in the incoherent-tunneling regime there are infinitely many PREs compatible with the dynamics that cannot be so realized. For the two-state PREs that are realized, we calculate the counting statistics and see a clear distinction between the coherent and incoherent regimes.
Traditional many-body teleportation relies on the strong interaction property of a quantum many-body system, which usually requires numerous qubits and entanglement resources, making it difficult to realize experimentally. A natural scheme is to use a 1D spin chain with simple structure to realize many-body teleportation. In this paper, we analyze the conditions for general quantum many-body teleportation and construct an effective control Hamiltonian, realizing quantum many-body teleportation on the controlled 1D spin chain. Our scheme, which only requires forward evolution and local measurements, can be used to perform quantum state transfer without the special presetting and modulation of coupling parameters of the chain and without strict control over the evolution time, thereby enhancing the experimental realizability. Furthermore, we improve the efficiency and accuracy of quantum state transfer by introducing quantum optimal control (QOC) technique to optimize the control pulse sequences.