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BibTeX

@misc{bai2026_260513aa1dp1,
  title        = {A no-go theorem for purely local $(\rho,T)$ Dirac interpolation},
  author       = {Dong Bai},
  year         = {2026},
  note         = {PreXiv id: prexiv:260513.aa1dp1},
  doi          = {10.99999/prexiv:260513.aa1dp1},
  url          = {https://prexiv.example/m/prexiv:260513.aa1dp1},
}

RIS

TY  - GEN
TI  - A no-go theorem for purely local $(\rho,T)$ Dirac interpolation
AU  - Dong Bai
PY  - 2026
DO  - 10.99999/prexiv:260513.aa1dp1
ID  - prexiv:260513.aa1dp1
UR  - https://prexiv.example/m/prexiv:260513.aa1dp1
AB  - We prove a sharp impossibility result for local Lieb--Oxford-type lower bounds on the indirect Coulomb energy of antisymmetric fermionic states. For a normalized \(N\)-fermion wavefunction \(\Psi\) write \(\rho_\Psi\) for its one-particle density, \(T_\Psi\) for its local kinetic energy density, and \(E_{\rm xc}(\Psi)\) for its indirect (exchange-correlation) energy. Let \(\mathcal R_\Psi\) be the dimensionless local kinetic ratio. Two constants control the discussion: the Dirac exchange constant \(C_D(q)=\tfrac{3}{4}(6/\pi)^{1/3}q^{-1/3}\) and the \emph{one-cell self-interaction constant} \(C_{\rm cell}=\tfrac{3}{5}(4\pi/3)^{1/3}\), which is strictly larger than \(C_D(q)\) for every spin multiplicity \(q\ge 1\). We show that any bounded function \(F\) with \(\limsup_{r\downarrow 0}F(r)<C_{\rm cell}\) cannot serve as the integrand of a universal pointwise lower bound \(E_{\rm xc}(\Psi)\ge -\!\int F(\mathcal R_\Psi)\rho_\Psi^{4/3}\) for arbitrarily large \(N\). The proof constructs antisymmetric many-cell states whose local data \((\rho_\Psi,T_\Psi)\) look like a flat Fermi sea but whose indirect energy is dominated by one-particle self-interaction. Consequently, no universal pointwise bound depending only on \((\rho_\Psi,T_\Psi)\) can have \(C_D(q)\) as its small-\(\mathcal R\) limit.
ER  -

Plain text

Dong Bai (2026). A no-go theorem for purely local $(\rho,T)$ Dirac interpolation. PreXiv prexiv:260513.aa1dp1, doi:10.99999/prexiv:260513.aa1dp1.

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