lemmaroutine

Divergence-free positive source tensor from holomorphic flow

Holomorphic flow gives a symmetric PSD tensor with divergence-free columns
abstract positive conserved tensor for the wave current
Lemma·lem:current-flow·§2.2 Two auxiliary flows

Statement (paper)

Let P=∑μCμ∂Xμ\mathscr P=\sum_\mu C^\mu\partial_{\mathsf X^\mu} have constant real symmetric coefficients. For a holomorphic solution Pfsys=0\mathscr P f_{\rm sys}=0 and the real displacement , put, wherever defined, G=fsys(X−iq)‾,Vℓa=∑μ(Cμwℓ)a ∂Xμ,Dℓa=∂wℓa+iVℓa,Zℓ=∑aGaDℓa. G=\overline{f_{\rm sys}(\mathsf X-\mathrm i q)},\qquad V_{\ell a}=\sum_\mu(C^\mu w_\ell)_a\,\partial_{\mathsf X^\mu},\qquad D_{\ell a}=\partial_{w_{\ell a}}+\mathrm i V_{\ell a},\qquad \mathcal Z_\ell=\sum_a G_aD_{\ell a}. In the real coordinates (X,w1,w2)(\mathsf X,w_1,w_2), the tensor B=Re⁡∑ℓ=12Zℓ⊗Zℓ‾ B=\Rea\sum_{\ell=1}^2\mathcal Z_\ell\otimes\overline{\mathcal Z_\ell} is symmetric and positive semidefinite, and each of its columns has zero divergence.

In plain English

For a first-order system Pfsys=0\mathscr P f_{\rm sys}=0 with constant real symmetric coefficients and holomorphic fsysf_{\rm sys}, the tensor B=Re⁡∑ℓ=12Zℓ⊗Zℓ‾B=\Rea\sum_{\ell=1}^2\mathcal Z_\ell\otimes\overline{\mathcal Z_\ell} in the real coordinates (X,w1,w2)(\mathsf X,w_1,w_2) is symmetric and positive semidefinite, and each of its columns is divergence-free.

Why it's here

This is the structural input for the wave current: positivity makes the current a nonnegative quantity, and zero divergence of the columns gives conservation, so the later propositions can treat the current as a conserved flux. The mechanism is that the operators Dℓa=∂wℓa+iVℓaD_{\ell a}=\partial_{w_{\ell a}}+\mathrm i V_{\ell a} combine with the holomorphic equation Pfsys=0\mathscr P f_{\rm sys}=0, so the divergence terms cancel, while BB is a real part of a sum of rank-one Hermitian terms, which gives symmetry and positivity.
Classified routine:
Direct computation: symmetry and positivity hold because B is the real part of a sum of Hermitian rank-one terms, and the divergence cancels using holomorphy and the constant-coefficient equation, much as divergence-free energy-momentum tensors arise for constant-coefficient symmetric systems. It is an auxiliary structural lemma, not one of the paper's main new ideas.

Sources

PaperOpen
Section
§2.2 Two auxiliary flows
Page
—
Label
lem:current-flow
Line
sections/current.tex:104
Leannot aligned

Phase 2 aligns this node to a Lean declaration.