23,653 research outputs found

    Width-tuned magnetic order oscillation on zigzag edges of honeycomb nanoribbons

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    Quantum confinement and interference often generate exotic properties in nanostructures. One recent highlight is the experimental indication of a magnetic phase transition in zigzag-edged graphene nanoribbons at the critical ribbon width of about 7 nm [G. Z. Magda et al., Nature \textbf{514}, 608 (2014)]. Here we show theoretically that with further increase in the ribbon width, the magnetic correlation of the two edges can exhibit an intriguing oscillatory behavior between antiferromagnetic and ferromagnetic, driven by acquiring the positive coherence between the two edges to lower the free energy. The oscillation effect is readily tunable in applied magnetic fields. These novel properties suggest new experimental manifestation of the edge magnetic orders in graphene nanoribbons, and enhance the hopes of graphene-like spintronic nanodevices functioning at room temperature.Comment: 22 pages, 9 figure

    Quantum Dimensionality Reduction by Linear Discriminant Analysis

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    Dimensionality reduction (DR) of data is a crucial issue for many machine learning tasks, such as pattern recognition and data classification. In this paper, we present a quantum algorithm and a quantum circuit to efficiently perform linear discriminant analysis (LDA) for dimensionality reduction. Firstly, the presented algorithm improves the existing quantum LDA algorithm to avoid the error caused by the irreversibility of the between-class scatter matrix SBS_B in the original algorithm. Secondly, a quantum algorithm and quantum circuits are proposed to obtain the target state corresponding to the low-dimensional data. Compared with the best-known classical algorithm, the quantum linear discriminant analysis dimensionality reduction (QLDADR) algorithm has exponential acceleration on the number MM of vectors and a quadratic speedup on the dimensionality DD of the original data space, when the original dataset is projected onto a polylogarithmic low-dimensional space. Moreover, the target state obtained by our algorithm can be used as a submodule of other quantum machine learning tasks. It has practical application value of make that free from the disaster of dimensionality

    Multifractal characterisation of length sequences of coding and noncoding segments in a complete genome

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    The coding and noncoding length sequences constructed from a complete genome are characterised by multifractal analysis. The dimension spectrum DqD_{q} and its derivative, the 'analogous' specific heat CqC_{q}, are calculated for the coding and noncoding length sequences of bacteria, where qq is the moment order of the partition sum of the sequences. From the shape of the % D_{q} and CqC_{q} curves, it is seen that there exists a clear difference between the coding/noncoding length sequences of all organisms considered and a completely random sequence. The complexity of noncoding length sequences is higher than that of coding length sequences for bacteria. Almost all DqD_{q} curves for coding length sequences are flat, so their multifractality is small whereas almost all DqD_{q} curves for noncoding length sequences are multifractal-like. We propose to characterise the bacteria according to the types of the CqC_{q} curves of their noncoding length sequences.Comment: 15 pages with 5 figures, Latex, Accepted for publication in Physica

    Polynomial maps with invertible sums of Jacobian matrices and of directional Derivatives

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    Let F:Cn→CmF: C^n \rightarrow C^m be a polynomial map with degF=d≥2degF=d \geq 2. We prove that FF is invertible if m=nm = n and ∑i=1d−1JF(αi)\sum^{d-1}_{i=1} JF(\alpha_i) is invertible for all ii, which is trivially the case for invertible quadratic maps. More generally, we prove that for affine lines L={β+μγ∣μ∈C}⊆CnL = \{\beta + \mu \gamma | \mu \in C\} \subseteq C^n (γ≠0\gamma \ne 0), F∣LF|_L is linearly rectifiable, if and only if ∑i=1d−1JF(αi)⋅γ≠0\sum^{d-1}_{i=1} JF(\alpha_i) \cdot \gamma \ne 0 for all αi∈L\alpha_i \in L. This appears to be the case for all affine lines LL when FF is injective and d≤3d \le 3. We also prove that if m=nm = n and ∑i=1nJF(αi)\sum^{n}_{i=1} JF(\alpha_i) is invertible for all αi∈Cn\alpha_i \in C^n, then FF is a composition of an invertible linear map and an invertible polynomial map X+HX+H with linear part XX, such that the subspace generated by {JH(α)∣α∈Cn}\{JH(\alpha) | \alpha \in C^n\} consists of nilpotent matrices

    Measure representation and multifractal analysis of complete genomes

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    This paper introduces the notion of measure representation of DNA sequences. Spectral analysis and multifractal analysis are then performed on the measure representations of a large number of complete genomes. The main aim of this paper is to discuss the multifractal property of the measure representation and the classification of bacteria. From the measure representations and the values of the DqD_{q} spectra and related CqC_{q} curves, it is concluded that these complete genomes are not random sequences. In fact, spectral analyses performed indicate that these measure representations considered as time series, exhibit strong long-range correlation. For substrings with length K=8, the DqD_{q} spectra of all organisms studied are multifractal-like and sufficiently smooth for the CqC_{q} curves to be meaningful. The CqC_{q} curves of all bacteria resemble a classical phase transition at a critical point. But the 'analogous' phase transitions of chromosomes of non-bacteria organisms are different. Apart from Chromosome 1 of {\it C. elegans}, they exhibit the shape of double-peaked specific heat function.Comment: 12 pages with 9 figures and 1 tabl

    Thermal-Mechanical Properties of Polyurethane-Clay Shape Memory Polymer Nanocomposites

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    Shape memory nanocomposites of polyurethane (PU)-clay were fabricated by melt mixing of PU and nano-clay. Based on nano-indentation and microhardness tests, the strength of the nanocomposites increased dramatically as a function of clay content, which is attributed to the enhanced nanoclay–polymer interactions. Thermal mechanical experiments demonstrated good mechanical and shape memory effects of the nanocomposites. Full shape memory recovery was displayed by both the pure PU and PU-clay nanocomposites.
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