Definition. Leading squared singular-energy share [ftip-0086]

Let \(\Delta W\in \mathbb R^{m\times n}\) be nonzero, set \(q=\min (m,n)\), and order its singular values as \(\sigma _1\geq \cdots \geq \sigma _q\geq 0\). Its leading squared singular-energy share is \[ \rho _1(\Delta W) =\frac {\sigma _1(\Delta W)^2}{\sum _{j=1}^q\sigma _j(\Delta W)^2} =\frac {\sigma _1(\Delta W)^2}{\|\Delta W\|_F^2}. \] The nonzero hypothesis prevents an undefined \(0/0\); the value lies in \([1/q,1]\).

NExt instead reports \(E_1=\sigma _1/\sum _j\sigma _j\) in Section 3.2 Low-rank optimization trajectories modeling for LLM RLVR acceleration[chen2026lowrank]. That nuclear-share statistic and \(\rho _1\) answer different questions. The squared share measures contribution to squared Frobenius norm.