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      Ground states of Nonlinear Schr\"{o}dinger System with Mixed Couplings

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          Abstract

          We consider the following \(k\)-coupled nonlinear Schr\"odinger system: \begin{align*} \begin{cases} &-\Delta u_j + \lambda_j u_j = \mu_j u_j^3 + \sum_{i=1, i\not=j}^k \beta_{i,j} u_i^2 u_j \quad {\rm in}\ \mathbb{R}^N,\\ &u_j>0 \quad {\rm in}\ \mathbb{R}^N, \quad u_j(x) \to 0 \quad \text{as }|x|\to +\infty, \quad j=1,2,\cdots,k, \end{cases} \end{align*} where \(N\leq 3\), \(k\geq3\), \(\lambda_j,\mu_j>0\) are constants and \(\beta_{i,j}=\beta_{j,i}\not=0\) are parameters. There have been intensive studies for the above system when \(k=2\) or the system is purely attractive (\( \beta_{i,j}>0, \forall i \not = j\)) or purely repulsive (\(\beta_{i,j}<0, \forall i\not = j \)); however very few results are available for \(k\geq 3\) when the system admits {\bf mixed couplings}, i.e., there exist \((i_1,j_1)\) and \((i_2,j_2)\) such that \(\beta_{i_1,j_1}\beta_{i_2,j_2}<0\). In this paper we give the first systematic and an (almost) complete study on the existence of ground states when the system admits mixed couplings. We first divide this system into {\bf repulsive-mixed} and {\bf total-mixed} cases. In the first case we prove nonexistence of ground states. In the second case we give an necessary condition for the existence of ground states and also provide estimates for the Morse index. The key idea is the {\bf block decomposition} of the system ({\bf optimal block decompositions, eventual block decompositions}), and the measure of total interaction forces between different {\bf blocks}. Finally the assumptions on the existence of ground states are shown to be {\bf optimal} in some special cases.

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          Bose–Einstein condensation of the triplet states in the magnetic insulator TlCuCl3

          Bose-Einstein condensation denotes the formation of a collective quantum ground state of identical particles with integer spin or intrinsic angular momentum. In magnetic insulators, the magnetic properties are due to the unpaired shell electrons that have half-integer spin. However, in some such compounds (KCuCl3 and TlCuCl3), two Cu2+ ions are antiferromagnetically coupled to form a dimer in a crystalline network: the dimer ground state is a spin singlet (total spin zero), separated by an energy gap from the excited triplet state (total spin one). In these dimer compounds, Bose-Einstein condensation becomes theoretically possible. At a critical external magnetic field, the energy of one of the Zeeman split triplet components (a type of boson) intersects the ground-state singlet, resulting in long-range magnetic order; this transition represents a quantum critical point at which Bose-Einstein condensation occurs. Here we report an experimental investigation of the excitation spectrum in such a field-induced magnetically ordered state, using inelastic neutron scattering measurements of TlCuCl3 single crystals. We verify unambiguously the theoretically predicted gapless Goldstone mode characteristic of the Bose-Einstein condensation of the triplet states.
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            Uniform Hölder Bounds for Nonlinear Schrödinger Systems with Strong Competition

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              Standing waves of some coupled nonlinear Schrödinger equations

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                Journal
                13 March 2019
                Article
                1903.05340
                af453f3c-e88b-4d74-9c6b-5675dbd4129b

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                38 pages
                math.AP

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