Abstract
It has been shown by Rellich, Weidman, and Gustafson-Rejto that the one-electron Dirac operator is essentially self-adjoint on the domain of infinitely differentiable functions with compact support, for atomic numbers less than or equal to 118. We state a double perturbation theorem which shows that the one-electron Dirac operator can admit another perturbation in addition to the Coulomb potential, which satisfies a mild Stummel type bound. In addition, the domain of the closure of the perturbed operator is the same as the domain of the closure of the unperturbed operator.
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Abbreviations
- √:
-
square root
- <, ≤, >, ≥:
-
inequalities
- ∞:
-
infinity
- γ:
-
gamma
- μ:
-
mu
- ∂:
-
partial derivative
- Σ:
-
summation
- ⊗:
-
tensor product
- ||:
-
absolute value
- ±:
-
plus or minus
- α:
-
alpha
- →:
-
limit
- ρ:
-
rho
- ∩:
-
intersection
- ∫:
-
integral
- ‖‖:
-
norm
- *:
-
adjoint
- Δ:
-
Laplacian
- ω:
-
omega
- ξ:
-
xi
- η:
-
eta
- 1/2:
-
fraction
- ∈:
-
is an element of
- ⊂:
-
is a subset of
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Landgren, J.J. Some essentially self-adjoint Dirac type operators i (formulation and an extension of the rellich-kato theorem). Lett Math Phys 2, 61–70 (1977). https://doi.org/10.1007/BF00420673
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DOI: https://doi.org/10.1007/BF00420673