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Owing to the small number of patients with tyrosine hydroxylase (TH) deficiency, no genotype-phenotype correlations have yet been identified. To investigate the genotype-phenotype correlation of R233H mutation in TH deficiency, we analyzed the clinical manifestations and treatment responses of four patients with the R233H homozygous mutation. Thirty-eight additional patients, available from the literature, known to be homozygous or heterozygous for the R233H mutation, were combined with the four cases from our hospital. Data for a total of 42 patients were retrieved. Our four patients showed clinical presentation consistent with Type A TH deficiency, and responded well to levodopa therapy, with an improvement in clinical symptoms within 1–2 weeks. In the 42 patients, 20 of 42 patients (48%) were homozygous and 22 (52%) were heterozygous for the R233H mutation. Of the 20 patients who were homozygous for the R233H mutation, a majority (80%) suffered from Type A TH deficiency. Of the 8 patients that were heterozygous for the R233H/the mutation located downstream of exon 11, 7 patients (86%) suffered from Type B TH deficiency. Of the 7 patients who were heterozygous for the R233H/nonsense mutation, 6 (86%) suffered from Type B TH deficiency. Genotype-phenotype correlation of R233H mutation was observed in TH deficiency. The homozygous R233H mutation frequently manifests as Type A TH deficiency, whereas R233H/nonsense mutation or any mutation located downstream of exon 11 manifests as Type B TH deficiency. [ABSTRACT FROM AUTHOR]

CuAlS2 has attracted much attention recently as a p-type transparent conductive material. In this paper, we investigate the site preference of substitutional Be in CuAlS2 and the transition level of BeAl using the first-principles calculation. We find that Be would be doped effectively at Al sites in CuAlS2 as a good p-type dopant. In addition, we speculate that Be-Mg or Be-Zn codoped CuAlS2 could have a mobility enhancement and thus a good p-type conductivity due to low lattice distortion. [ABSTRACT FROM AUTHOR]

Through comparisons with an entanglement breaking (EB) channel, we characterize the local quantum channels that destroy quantum correlations, especially for quantum discord, and give a detailed description of a discord-breaking (DB) channel. We prove that the quantum discord can be broken if and only if the local quantum channel is a commutativity-creating (CoC) channel. Then we show which kind of channels is a CoC channel, and address the relation between EB and DB channels. Furthermore we apply our results to three typical noise channels. [ABSTRACT FROM AUTHOR]

Noisy entangled resource and non-standard teleportation operations result in imperfect teleportation. In this paper, we derive an explicit expression for the output states of imperfect teleportation processes, thereby establishing a correspondence between teleportation and quantum channels. This result offers a different insight into teleportation. Also, it enables us to derive an expression for the fidelity of teleportation. Our results analytically reveal the dependence of the output states and the fidelity on the entangled resource and teleportation operations. The Nielsen–Caves teleportation formalism is used in the derivation. [ABSTRACT FROM AUTHOR]

The speed of evolution of a qubit undergoing a nonequilibrium environment with spectral density of general ohmic form is investigated. First we reveal non-Markovianity of the model, and find that the non-Markovianity quantified by information backflow of Breuer et al. [Phys. Rev. Lett. 103 210401 (2009)] displays a nonmonotonic behavior for different values of the ohmicity parameter s in fixed other parameters and the maximal non-Markovianity can be achieved at a specified value s. We also find that the non-Markovianity displays a nonmonotonic behavior with the change of a phase control parameter. Then we further discuss the relationship between quantum speed limit (QSL) time and non-Markovianity of the open-qubit system for any initial states including pure and mixed states. By investigation, we find that the QSL time of a qubit with any initial states can be expressed by a simple factorization law: the QSL time of a qubit with any qubit-initial states are equal to the product of the coherence of the initial state and the QSL time of maximally coherent states, where the QSL time of the maximally coherent states are jointly determined by the non-Markovianity, decoherence factor and a given driving time. Moreover, we also find that the speed of quantum evolution can be obviously accelerated in the wide range of the ohmicity parameter, i.e., from sub-Ohmic to Ohmic and super-Ohmic cases, which is different from the thermal equilibrium environment case. [ABSTRACT FROM AUTHOR]