Global Alliance in Management Education

About: Global Alliance in Management Education is a based out in . It is known for research contribution in the topics: Magnetic field & Skyrmion. The organization has 577 authors who have published 2057 publications receiving 72848 citations. The organization is also known as: CEMS & The Global Alliance in Management Education.

Full reconstruction of a 14-qubit state within four hours

Abstract: Full quantum state tomography (FQST) plays a unique role in the estimation of the state of a quantum system without a priori knowledge or assumptions. Unfortunately, since FQST requires informationally (over)complete measurements, both the number of measurement bases and the computational complexity of data processing suffer an exponential growth with the size of the quantum system. A 14-qubit entangled state has already been experimentally prepared in an ion trap, and the data processing capability for FQST of a 14-qubit state seems to be far away from practical applications. In this paper, the computational capability of FQST is pushed forward to reconstruct a 14-qubit state with a run time of only 3.35 hours using the linear regression estimation (LRE) algorithm, even when informationally overcomplete Pauli measurements are employed. The computational complexity of the LRE algorithm is first reduced from∼1019 to∼1015 for a 14-qubit state, by dropping all the zero elements, and its computational efficiency is further sped up by fully exploiting the parallelism of the LRE algorithm with parallel Graphic Processing Unit (GPU) programming. Our result demonstrates the effectiveness of using parallel computation to speed up the postprocessing for FQST, and can play an important role in quantum information technologies with large quantum systems.

Quantum Hall states stabilized in semi-magnetic bilayers of topological insulators.

Abstract: By breaking the time-reversal symmetry in three-dimensional topological insulators with the introduction of spontaneous magnetization or application of magnetic field, the surface states become gapped, leading to quantum anomalous Hall effect or quantum Hall effect, when the chemical potential locates inside the gap. Further breaking of inversion symmetry is possible by employing magnetic topological insulator heterostructures that host non-degenerate top and bottom surface states. Here we demonstrate the tailored-material approach for the realization of robust quantum Hall states in the bilayer system, in which the cooperative or cancelling combination of the anomalous and ordinary Hall responses from the respective magnetic and non-magnetic layers is exemplified. The appearance of quantum Hall states at filling factor 0 and +1 can be understood by the relationship of energy band diagrams for the two independent surface states. The designable heterostructures of magnetic topological insulator may explore a new arena for intriguing topological transport and functionality.

Spin injection into a superconductor with strong spin-orbit coupling.

Abstract: We demonstrate spin injection into superconducting Nb by employing a spin absorption technique in lateral spin valve structures. Spin currents flowing in a nonmagnetic Cu channel are preferably absorbed into Nb due to its strong spin-orbit interaction, the amount of which dramatically changes below or above the superconducting critical temperature (${T}_{C}$). The charge imbalance effect observed in the $\mathrm{Cu}/\mathrm{Nb}$ interface ensures that superconducting Nb absorbs pure spin currents even below ${T}_{C}$. Our analyses based on the density of states calculated using the Usadel equation can well reproduce the experimental results, implying that the strong spin-orbit interaction of Nb is still effective for the spin absorption even below ${T}_{C}$. Most importantly, our method allows us to determine the intrinsic spin relaxation time in the superconducting Nb, which reaches more than 4 times greater than that in the normal state.

End-on orientation of semiconducting polymers in thin films induced by surface segregation of fluoroalkyl chains.

Abstract: Controlling the orientation of highly anisotropic structures of polymers is important because the majority of their mechanical, electronic, and optical properties depend on the orientation of the polymer backbone. In thin films, the polymer chains tend to adopt an orientation parallel to the substrate; therefore, forcing the chains to stand perpendicular to the substrate is challenging. We have developed a simple way to achieve this end-on orientation. We functionalized one end of a poly(3-butylthiophene) (P3BT) chain with a 1H,1H,2H,2H,3H,3H-perfluoroundecyl group, which caused spontaneous self-segregation of the polymer (P3BT-F17) to the surface of the polymer film. In P3BT-F17/polystyrene (PS) blend films, a highly ordered end-on orientation of the conjugated backbone was observed in the surface-segregated layer of the crystalline P3BT-F17. Furthermore, when the film was spin-coated from a mixture of P3BT-F17 and P3BT, the chain orientation of P3BT-F17 at the surface forced the P3BT in the bulk of the film to adopt the end-on orientation because of the high crystallinity of P3BT. The electronic conductivity measured perpendicular to the film surface also reflected the end-on orientation in the bulk, resulting in a more than 30-fold enhancement of the hole mobility.

Liouvillian Skin Effect: Slowing Down of Relaxation Processes without Gap Closing.

Abstract: It is highly nontrivial to what extent we can deduce the relaxation behavior of a quantum dissipative system from the spectral gap of the Liouvillian that governs the time evolution of the density matrix. We investigate the relaxation processes of a quantum dissipative system that exhibits the Liouvillian skin effect, which means that the eigenmodes of the Liouvillian are localized exponentially close to the boundary of the system, and find that the timescale for the system to reach a steady state depends not only on the Liouvillian gap $\mathrm{\ensuremath{\Delta}}$, but also on the localization length $\ensuremath{\xi}$ of the eigenmodes. In particular, we show that the longest relaxation time $\ensuremath{\tau}$ that is maximized over initial states and local observables is given by $\ensuremath{\tau}\ensuremath{\sim}{\mathrm{\ensuremath{\Delta}}}^{\ensuremath{-}1}(1+L/\ensuremath{\xi})$ with $L$ being the system size. This implies that the longest relaxation time can diverge for $L\ensuremath{\rightarrow}\ensuremath{\infty}$ without gap closing.