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The relevant nonlinear generalized singular vector relation, without imposing unit-data normalization, isThis is a generalized eigenfunction in the forward-operator metric, rather than a distributional generalized eigenfunction of a linear operator. It supplies the normal-operator source condition with $v=\lambda u^{†}$. For a convex positively one-homogeneous functional, the subgradient inequality applied at zero and at $2u^{†}$ gives $⟨p,u^{†}⟩=J(u^{†})$. If $K{u}^{†}\ne 0$, thenAssume the usual positive eigenvalue $\lambda >0$ and $0<\alpha \lambda \le 1$. By positive homogeneity,The shifted-comparator Bregman bound therefore yieldsThe vector $(1-\alpha \lambda )u^{†}$ is itself a minimizer: $p$ remains a subgradient along the nonnegative ray, and substitution satisfies the subgradient optimality condition. If $K$ is injective, this also proves $u_{\alpha }=(1-\alpha \lambda )u^{†}$. Otherwise distinct minimizers can differ in the kernel while sharing the same predicted data.

For a nonnegative convex positively one-homogeneous functional, the branch continues as $(1-\alpha \lambda {)}_{+}{u}^{†}$ above the threshold, since $p/(\alpha \lambda )\in \partial J(0)$ there. Nonnegativity is needed for that clipping argument; bare positive homogeneity allows signed linear functionals.

Zero Bregman distance does not imply exact recovery. For $K=I$, $J(s)=|s|$, $u^{†}=a>0$ and $0<\alpha <a$, the minimizer is $u_{\alpha }=a-\alpha \ne a$, but $D_J^1(a-\alpha ,a)=0$. Both points touch the same supporting line, as described by zero Bregman distance and supporting faces.

Let $w=K^{\ast }Kv\in \partial J(u^{†})$ from the normal-operator source condition, and set $e=u-u^{†}$. Since $u^{†}$ is a least-squares solution, the normal equation for a linear inverse problem gives $K^{\ast }(K{u}^{†}-f)=0$. Expand the objective difference and use the Bregman distance definition:The cross term with the residual of the least-squares solution vanishes by the normal equation; exact data are not required. Compare the minimizing $u_{\alpha }$ with $z=u^{†}-\alpha v$. At $z$, the completed square is zero. Dividing the resulting inequality by $\alpha$ proves the stronger shifted-comparator Bregman boundDropping the nonnegative squared term gives the requested estimate. If the comparator lies outside the effective domain of $J$, its distance is infinite and the inequality is valid but gives no finite error bound.