We consider continuous Dirac operators defined on $\mathbf{R}^d$, $d\in\{1,2,3\}$, together with various discrete versions of them. Both forward-backward and symmetric finite differences are used as approximations to partial derivatives. We also allow a bounded, H\"older continuous, and self-adjoint matrix-valued potential, which in the discrete setting is evaluated on the mesh. Our main goal is to investigate whether the proposed discrete models converge in norm resolvent sense to their continuous counterparts, as the mesh size tends to zero and up to a natural embedding of the discrete space into the continuous one. In dimension one we show that forward-backward differences lead to norm resolvent convergence, while in dimension two and three they do not. The same negative result holds in all dimensions when symmetric differences are used. On the other hand, strong resolvent convergence holds in all these cases. Nevertheless, and quite remarkably, a rather simple but non-standard modification to the discrete models, involving the mass term, ensures norm resolvent convergence in general.
翻译:我们考虑连续的Dirac操作员定义在$\mathbf{R ⁇ d$,$d\in ⁇ 1,2,3 ⁇ $,以及各种离散版本中。 前向和对称的有限差异都用作部分衍生物的近似值。 我们还允许一个受约束的、H\'older连续和自对称的矩阵价值潜在值,在离散环境中,在网状上对其进行评估。我们的主要目标是调查拟议的离散模型是否在正常意义上与连续的对等方相融合,因为网状大小往往为零,直至离散空间自然嵌入连续的对等方。 在维度一中,我们显示,前向后偏差导致标准固态趋同,而在二维和三维中则没有。在使用对称差异时,所有维度都存在相同的负结果。另一方面,在所有这些案例中,都存在强烈的固态趋同。然而,相当明显的是,对离散模型进行了相当简单但非标准的修改,涉及质量术语,确保规范的常态固性趋同。