Problem 6: Large epsilon-light vertex subsets -- Barrier Potential #
BSS barrier potential Phi_u(M) = tr((uI - M)^{-1}), trace
monotonicity, barrier shift/decrease/gap lemmas, eigenvalue bounds,
unitary conjugation, and the Neumann-Loewner trace bound.
Main definitions #
Problem6.barrierPotential: the upper barrier potential
Main theorems #
Problem6.trace_mul_nonneg_of_posSemidef:tr(PQ) >= 0for PSDProblem6.trace_mul_le_of_loewner: trace monotonicity under LoewnerProblem6.barrier_potential_decrease: barrier decrease estimateProblem6.barrier_gap_pos: positivity of barrier gapProblem6.barrier_rearrange: algebraic rearrangement lemmaProblem6.eigenvalue_le_trace_of_posSemidef: eigenvalue-trace bound
The upper barrier potential Φ_u(M) = tr((uI - M)⁻¹), defined for symmetric M with eigenvalues < u.
Instances For
Real form of the spectral theorem: a real Hermitian matrix equals
U * diagonal eigenvalues * star U for its eigenvector unitary U.
PSD factorization via spectral theorem: P PSD implies P = Nᴴ * N for some N.
For PSD matrices P, Q over ℝ, tr(P * Q) ≥ 0. Proof: write P = Nᴴ * N, then tr(PQ) = tr(NQNᴴ) ≥ 0 since NQNᴴ is PSD.
Trace monotonicity under Loewner order: if X ≤ Y (Loewner) and C ≥ 0, then tr(X * C) ≤ tr(Y * C). This follows from tr((Y-X)*C) ≥ 0 since Y-X ≥ 0 and C ≥ 0.
For a PSD matrix, each eigenvalue is at most the trace.
If K is PSD with trace < 1, then I - K is positive definite.