无界锥上MIT袋模型的自伴性
Self-adjointness for the MIT bag model on an unbounded cone
AI总结:
该研究针对无界三维圆锥上带MIT袋边界条件的无质量Dirac算子,证明凸锥下其在四分量$H^1$函数域上自伴,给出非凸锥情形的数值证据,还得到凸锥上的Hardy型不等式及扰动稳定性,并讨论了向量子点边界条件的推广。
摘要:
我们研究了无界三维圆锥上满足MIT袋边界条件的无质量Dirac算子。对于凸锥,我们证明了该算子在满足MIT袋边界条件的四分量$H^1$函数定义域上是自伴的,证明依赖于变量分离法和一维纤维Dirac型算子的谱估计。此外,我们提供了数值证据,表明非凸锥上该算子在相同定义域下也具有自伴性。我们还证明了凸锥上此类Dirac算子的Hardy型不等式,该不等式尤其能得到自伴性在一类无界势扰动下的稳定性。文中还讨论了将结果推广到带量子点边界条件的Dirac算子的相关内容。
英文摘要:
We consider the massless Dirac operator with the MIT bag boundary conditions on an unbounded three-dimensional circular cone. For convex cones, we prove that this operator is self-adjoint defined on four-component $H^1$--functions satisfying the MIT bag boundary conditions. The proof of this result relies on separation of variables and spectral estimates for one-dimensional fiber Dirac-type operators. Furthermore, we provide a numerical evidence for the self-adjointness on the same domain also for non-convex cones. Moreover, we prove a Hardy-type inequality for such a Dirac operator on convex cones, which, in particular, yields stability of self-adjointness under perturbations by a class of unbounded potentials. Further extensions of our results to Dirac operators with quantum dot boundary conditions are also discussed.
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