16,818 research outputs found

    Engineering planar transverse domain walls in biaxial magnetic nanostrips by tailoring transverse magnetic fields with uniform orientation

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    Designing and realizing various magnetization textures in magnetic nanostructures are essential for developing novel magnetic nanodevices in modern information industry. Among all these textures, planar transverse domain walls (pTDWs) are the simplest and the most basic, which make them popular in device physics. In this work, we report the engineering of pTDWs with arbitrary tilting attitude in biaxial magnetic nanostrips by transverse magnetic field profiles with uniform orientation but tunable strength distribution. Both statics and axial-field-driven dynamics of these pTDWs are analytically investigated. It turns out that for statics these pTDWs are robust again disturbances which are not too abrupt, while for dynamics it can be tailored to acquire higher velocity than Walker's ansatz predicts. These results should provide inspirations for designing magnetic nanodevices with novel one-dimensional magnetization textures, such as 360∘^\circ walls, or even two-dimensional ones, for example vortices, skyrmions, etc.Comment: 14 pages, 3 figure

    Applications of degree estimate for subalgebras

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    Let KK be a field of positive characteristic and KK be the free algebra of rank two over KK. Based on the degree estimate done by Y.-C. Li and J.-T. Yu, we extend the results of S.J. Gong and J.T. Yu's results: (1) An element p(x,y)∈Kp(x,y)\in K is a test element if and only if p(x,y)p(x,y) does not belong to any proper retract of KK; (2) Every endomorphism preserving the automorphic orbit of a nonconstant element of KK is an automorphism; (3) If there exists some injective endomorphism Ο•\phi of KK such that Ο•(p(x,y))=x\phi(p(x,y))=x where p(x,y)∈Kp(x,y)\in K, then p(x,y)p(x,y) is a coordinate. And we reprove that all the automorphisms of KK are tame. Moreover, we also give counterexamples for two conjectures established by Leonid Makar-Limanov, V. Drensky and J.-T. Yu in the positive characteristic case.Comment: 12 page

    Search for C=+C=+ charmonium and XYZ states in e+eβˆ’β†’Ξ³+He^+e^-\to \gamma+ H at BESIII

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    Within the framework of nonrelativistic quantum chromodynamics, we study the production of C=+C=+ charmonium states HH in e+eβˆ’β†’Ξ³Β +Β He^+e^-\to \gamma~+~H at BESIII with H=Ξ·c(nS)H=\eta_c(nS) (n=1, 2, 3, and 4), Ο‡cJ(nP)\chi_{cJ}(nP) (n=1, 2, and 3), and 1D2(nD)^1D_2(nD) (n=1 and 2). The radiative and relativistic corrections are calculated to next-to-leading order for SS and PP wave states. We then argue that the search for C=+C=+ XYZXYZ states such as X(3872)X(3872), X(3940)X(3940), X(4160)X(4160), and X(4350)X(4350) in e+eβˆ’β†’Ξ³Β +Β He^+e^-\to \gamma~+~H at BESIII may help clarify the nature of these states. BESIII can search XYZXYZ states through two body process e+eβˆ’β†’Ξ³He^+e^-\to \gamma H, where HH decay to J/ΟˆΟ€+Ο€βˆ’J/\psi \pi^+\pi^-, J/ΟˆΟ•J/\psi \phi, or DDΛ‰D \bar D. This result may be useful in identifying the nature of C=+C=+ XYZXYZ states. For completeness, the production of C=+C=+ charmonium in e+eβˆ’β†’Ξ³+Β He^+e^-\to \gamma +~H at B factories is also discussed.Comment: Comments and suggestions are welcome. References are update
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