A mixed graph is a that can be obtained from simple undirected by replacing some of the edges arcs in precisely one two possible directions. The Hermitian adjacency matrix $G$ order $n$ $n \times n$ $H(G)=(h_{ij})$, where $h_{ij}=-h_{ji}= \boldsymbol{\mathrm{i}}$ (with $\boldsymbol{\mathrm{i}} =\sqrt{-1})$ if there exists an arc $v_i$ to $v_j$ (but no $v_i$), $h_{ij}=h_{ji}=1$ edge (and arcs) b...

In case of an anisotropic superconductor non-magnetic disorder leads eventually to pair breaking effect via Abrikosov–Gorkov formula [1, 2, 3, 4, 5], like for magnetic impurities, for any value of a coherence length ξ. By analogy to an isotropic s–wave pairing, for superconductors with an enough large coherence length ξ, the amplitude of paring potential |∆(ij)| tends be the same for all bonds ...

E gávnnu åvdep guoradallama ma li gehtjadam iellemguojme vahágahttemav sáme álmmuga gaskan. Diehtep vahágahttem åbbålattjat, ja sierraláhkáj, vájkkut psykalasj varresvuohtaj nievres láhkáj, árvvedahtte sámij gaskan la sæmmi láhkáj. SAMINOR 2 – gatjálvissjiemáguoradallama dáhtáj milta lip man dábálasj iellemguojmev dåbdulattjat, rubbmelattjat sevsalattjat vahágahttet. Lep aj gåktu goavge depresj...

It is shown that, if IJ is a subvariety of the join of a nilpotent variety and a metabelian variety and if V̂ is a variety with a finite basis for its laws, then UV also has a finite basis for its laws. The special cases IJ nilpotent and IJ metabelian have been established by Higman (1959) and Ivanjuta (1969) respectively. The proof here, which is independent of Ivanjuta's, depends on a rather g...

We prove that the Bohmian arrival time of the 1D Schrödinger evolution violates the quadratic form structure on which Kijowski's axiomatic treatment of arrival times is based. Within Kijowski's framework, for a free right moving wave packet Ψ, the various notions of arrival time (at a fixed point x on the real line) all yield the same average arrival time tK ij (Ψ). We derive the inequality tB ...

i x i s = 1, x i s ≥ 0, x ij s ≥ 0 . • x i s ∈ [0, 1]: indicates whether label i is chosen at voxel s • y ij s = x ij s − x s ∈ [−1, 1]: presence of a surface and its direction • ρs: unary term, cost for label i at location s •φij s : convex smoothness term at voxel s for labels i and j • ek ∈ R: k-th canonical basis vector • T : alignment between prior and input data •α: normalization factor f...

We describe here the characteristics of two types of high-quality PbTe p-njunctions, prepared in this work: (1) by thermal diffusion of In4Te3 gas (TDJ), and (2) by ion implantation (implanted junction, IJ) of In (In-IJ) and Zn (Zn-IJ). The results, as presented here, demonstrate the high quality of these PbTe diodes. Capacitance-voltage (C-V) and current-voltage (I-V) characteristics have been...

24 bounded regions of spacetime. Gravitational physics and its mathematical expression have been smoothly melded. 23 ^ @ 0 g ij = ?2NK ij ; (82) that has no slicing term analogous to S ij. It has characteristics along the light cone and @ 0. It is not quasi-diagonal because of third order derivatives of g ij arising in (81) from r 2 N. This system is hyperbolic non-strict 21]. On the other hand...

In many area of medical research, a relation analysis between one response variable and some explanatory variables is desirable. Regression is the most common tool in this situation. If we have some assumptions for such normality for response variable, we could use it. In this paper we propose a nonparametric regression that does not have normality assumption for response variable and we focus ...

Electrons confined in silicon quantum dots exhibit orbital, spin, and valley degrees of freedom. The degree freedom originates from the bulk bandstructure silicon, which has six degenerate electronic minima. degeneracy can be lifted wells due to strain confinement, but "valley splitting" two lowest lying valleys is known sensitive atomic-scale disorder. Large splittings are desirable have a wel...