bibkey: higham2006eigenstate authors: Nicholas J. Higham year: 2006 title: Functions of Matrices doi: null url: https://eprints.maths.manchester.ac.uk/310/ claim: Matrix Taylor series act scalarly on an eigenline, and the standard pure-state trace formulas give a positive normalized density matrix and zero energy variance. strata_touched:
- D5/S3/Quantum/Dynamics/EnergyEigenstateStationarity license: citation-only triage: anchor
Matrix series and pure eigenstates
Verified locator
The exact upstream locator is: https://eprints.maths.manchester.ac.uk/310/
The record identifies Higham’s 2006 chapter in the Handbook of Linear
Algebra. Its PDF, https://eprints.maths.manchester.ac.uk/310/1/fm_final.pdf,
was retrieved: section 1, fact 10 gives the matrix Taylor-series formula;
section 3 defines the matrix exponential by sum_{k>=0} A^k/k!.
The companion source is John Preskill, Ph219/CS219, Chapter 2,
Foundations I: States and Ensembles:
https://www.preskill.caltech.edu/ph219/chap2_15.pdf
The retrieved text gives mean(A)=<psi|A|psi> in (2.9), the trace expectation
in (2.62), positivity and trace one on page 20, and the pure density matrix
rho=|psi><psi| on that page.
Shared source chain and declaration bridges
exp_mulVec_of_eigenvector: ifAv=mu v, induction givesA^k v=mu^k v. Apply the continuous linear mapB -> Bvto the convergent matrix exponential series, then use uniqueness of the sum:exp(A)v = sum_k mu^k v/k! = exp(mu)v. Exponential has infinite radius of convergence. This argument applies to every finite complex matrix, including n=0, and permits v=0. It requires neither Hermitian A nor diagonalizability nor a nonzero vector; a theorem imposing those stronger conditions is not used as a substitute. The local proof implements the bridge withNormedSpace.exp_series_hasSum_exp', continuous linear evaluation andHasSum.unique.pureDensityState: a local representation of the standard construction (标准构造的本地表示). Fromv* v=1, setrho=vv*. For every x,x* rho x=|v* x|^2 >= 0, andtr(rho)=v* v=1. The localDensityStatepackages these two properties of the existing rank-one matrix; it introduces no new pure-state law.energy_eigenstate_variance_zero: the trace identity givesRe tr(rho A)=Re(v*Av). IfHv=Ev, normalized v and real E give the first moment E. AlsoH^2v=E^2v, so the second moment is E^2; subtracting the squared first moment gives zero. The Lean theorem does not assume Hermiticity of H: this algebra remains valid for any complex matrix with the stated real eigenvalue and normalized vector. Its interpretation as an energy-observable variance is on the Hermitian domain; nonnegative variance for arbitrary matrices is not asserted.
What this note does and does not attest
Attested by this repository’s own retrieval: Higham’s chapter metadata, Taylor and exponential formulas, Preskill’s formulas and pure-state paragraph at the locations above, and the local declaration boundaries. The series-evaluation and moment-subtraction bridges are explicit here.
The round-19 classification is received from issue #6298. Treating the
2006 chapter as the later standalone book, attributing these exact Lean
signatures to either source, or claiming priority would be
ASSUMED-UNVERIFIED; none is asserted. The existing Citation for
energy_eigenstate_stationary is outside this correction.