\documentclass[11pt,reqno]{amsart} \usepackage[margin=1.1in]{geometry} \usepackage[T2A,OT2,T1]{fontenc} \usepackage{amsmath,amssymb,amsthm,mathtools,mathrsfs, tikz} \usepackage{xcolor} \usepackage{microtype} \usepackage[hidelinks]{hyperref} \usepackage{orcidlink} \usepackage[backend=biber,style=alphabetic,maxnames=10,giveninits=true]{biblatex} \addbibresource{references.bib} \definecolor{vegasgold}{rgb}{0.77, 0.7, 0.35} \definecolor{darkgoldenrod}{rgb}{0.72, 0.53, 0.04} \definecolor{gold(metallic)}{rgb}{0.83, 0.69, 0.22} \hypersetup{ colorlinks=true, linkcolor=darkgoldenrod, filecolor=brown, urlcolor=gold(metallic), citecolor=darkgoldenrod, } \usepackage{enumitem} \numberwithin{equation}{section} \newtheorem{theorem}{Theorem}[section] \newtheorem{proposition}[theorem]{Proposition} \newtheorem{lemma}[theorem]{Lemma} \newtheorem{corollary}[theorem]{Corollary} \newtheorem{conjecture}[theorem]{Conjecture} \newtheorem{question}[theorem]{Question} \theoremstyle{definition} \newtheorem{definition}[theorem]{Definition} \newtheorem{remark}[theorem]{Remark} \newtheorem{example}[theorem]{Example} \newcommand{\Q}{\mathbb Q} \newcommand{\Z}{\mathbb Z} \newcommand{\cO}{\mathcal O} \newcommand{\op}[1]{\operatorname{#1}} \newcommand{\Tr}{\operatorname{Tr}} \newcommand{\Fp}{\mathbb{F}_p} \newcommand{\Div}{\operatorname{div}} \newcommand{\Zp}{\mathbb Z_p} \newcommand{\Qp}{\mathbb Q_p} \newcommand{\LambdaIw}{\Lambda} \DeclareFontFamily{U}{wncy}{} \DeclareFontShape{U}{wncy}{m}{n}{<->wncyr10}{} \DeclareSymbolFont{mcy}{U}{wncy}{m}{n} \DeclareMathSymbol{\Sh}{\mathord}{mcy}{"58} \newcommand{\AR}[1]{\textcolor{blue}{#1}} \newcommand{\Gal}{\operatorname{Gal}} \newcommand{\Cl}{\operatorname{Cl}} \newcommand{\rk}{\operatorname{rank}} \newcommand{\gr}{\operatorname{gr}} \newcommand{\ord}{\operatorname{ord}} \newcommand{\expn}{\operatorname{exp}} \newcommand{\cd}{\operatorname{cd}} \newcommand{\Iw}{\mathrm{Iw}} \newcommand{\lc}{\mathrm{lc}} \newcommand{\ur}{\mathrm{ur}} \newcommand{\ab}{\mathrm{ab}} \newcommand{\cF}{\mathcal F} \newcommand{\cG}{\mathcal G} \newcommand{\cX}{\mathcal X} \newcommand{\cH}{\mathcal H} \newcommand{\cI}{\mathcal I} \newcommand{\cK}{\mathcal K} \newcommand{\eps}{\varepsilon} \newcommand{\mob}{\mu_{\mathrm{Mob}}} % Additional notation used in this paper. \newcommand{\F}{\mathbb F} \newcommand{\Sel}{\operatorname{Sel}} \newcommand{\Frob}{\operatorname{Frob}} \newcommand{\corank}{\operatorname{corank}} \newcommand{\charac}{\operatorname{char}} \newcommand{\Hom}{\operatorname{Hom}} \newcommand{\LambdaE}{\mathcal O[[\Gamma]]} \title[Erd\H{o}s--Kac theorem for signed Iwasawa invariants] {An analogue of the Erd\H{o}s--Kac theorem for signed Iwasawa invariants of modular forms} \author[A.~Ray]{Anwesh Ray\, \orcidlink{0000-0001-6946-1559}} \address{Chennai Mathematical Institute, H1, SIPCOT IT Park, Siruseri, Kelambakkam 603103, Tamil Nadu, India.} \email{anwesh@cmi.ac.in} \subjclass[2020]{Primary 11R23; Secondary 11N60, 11F33, 11F80} \keywords{Signed Iwasawa invariants, non-ordinary modular forms, signed Selmer groups, level raising, Erd\H{o}s--Kac theorem} \begin{document} \begin{abstract} Erd\H{o}s and Kac proved that the number of distinct prime factors of an integer has a Gaussian limiting distribution. We prove an analogue for the signed Iwasawa invariants of non-ordinary weight-two modular forms. Under the hypotheses of this paper, we construct infinitely many forms congruent to a given form $g$ that realize every common nonnegative increase of its two signed $\lambda$-invariants. We count the levels realizing each increase. In the resulting family, the common increase is asymptotically Gaussian, with mean and variance $\delta_\Pi\log\log X+O_g(1)$ for a positive constant $\delta_\Pi$. \end{abstract} \maketitle \section{Introduction} \label{sec:introduction} \subsection{Background and motivation} A central theme in arithmetic geometry is to understand how arithmetic invariants vary in infinite families. Iwasawa theory encodes the growth of class groups, Selmer groups and related arithmetic objects in $p$-adic towers in terms of a small collection of algebraic invariants. The theory originated in Iwasawa's study of ideal class groups in infinite towers of number fields. Let $p$ be a prime number and $K_\infty/K$ be the cyclotomic $\Zp$-extension. Let $K_n$ be the unique intermediate field satisfying $[K_n:K]=p^n$. If $A_n$ denotes the $p$-primary part of the ideal class group of $K_n$, then the inverse limit of the groups $A_n$, with respect to the norm maps, is a module over the Iwasawa algebra $\Lambda=\Zp[[T]]$. Writing $\#A_n=p^{e_n}$, Iwasawa proved that there are integers $\mu,\lambda\geq0$ and $\nu$ such that \begin{equation}\label{eq:intro-iwasawa-growth} e_n=\mu p^n+\lambda n+\nu \end{equation} for all sufficiently large $n$; see \cite{Iwasawa1959}. This essentially leverages the structure theory of finitely generated and torsion modules over $\Lambda$. The integers $\mu$ and $\lambda$ are the Iwasawa invariants of the tower. Mazur extended this point of view to elliptic curves \cite{Mazur1972}. Let $E/\Q$ be an elliptic curve and let $\Q_\infty/\Q$ be the cyclotomic $\Zp$-extension. The role of the class group is played by the $p$-primary Selmer group $\Sel_{p^\infty}(E/\Q_\infty)$. For every finite extension $F/\Q$ contained in $\Q_\infty$, the Selmer group fits into the fundamental exact sequence \[ 0\longrightarrow E(F)\otimes_{\Z}\Q_p/\Z_p \longrightarrow \Sel_{p^\infty}(E/F) \longrightarrow \Sh(E/F)[p^\infty] \longrightarrow 0. \] When its Pontryagin dual is torsion over the cyclotomic Iwasawa algebra, it has well defined invariants $\mu_p(E)$ and $\lambda_p(E)$ which arise from the structure theory of $\Lambda$-modules. These invariants describe the growth of the Selmer groups in the finite layers of $\Q_\infty/\Q$ and are closely related to the growth of Mordell--Weil groups and Tate--Shafarevich groups. The same construction applies to the Galois representation attached to a modular form. Let $h$ be a normalized newform and let $V_h$ be its $p$-adic Galois representation. A choice of stable lattice $T_h\subset V_h$ gives a discrete representation $A_h=V_h/T_h$, and one defines a Selmer group over $\Q_\infty$ by imposing suitable local conditions on $A_h$. In the ordinary case, the local condition at $p$ is obtained from the ordinary filtration of $V_h$. Kato's Euler-system shows that the Pontryagin dual of the resulting Selmer group is a finitely generated torsion module over the Iwasawa algebra \cite{Kato2004}. Its characteristic power series therefore defines the associated $\mu$- and $\lambda$-invariants. At a non-ordinary prime there is no ordinary filtration giving the required local condition. For elliptic curves with supersingular reduction, Kobayashi introduced the plus and minus Selmer groups \cite{Kobayashi2003}, while Pollack constructed the corresponding bounded $p$-adic $L$-functions when $a_p=0$ \cite{Pollack2003}. Signed Coleman maps and signed Selmer groups for modular forms were subsequently developed by Lei, Lei--Loeffler--Zerbes and Sprung \cite{Lei2011,LLZ2010,LLZ2011,Sprung2012,Sprung2017}. In the weight-two setting considered here, these constructions give two signed Selmer groups, indexed by $\natural\in\{\sharp,\flat\}$, and hence two pairs of Iwasawa invariants $\bigl(\mu^\sharp(h),\lambda^\sharp(h)\bigr)$ and $\bigl(\mu^\flat(h),\lambda^\flat(h)\bigr)$. A fundamental question is to understand how Iwasawa invariants vary with respect to congruences of Galois representations. Greenberg and Vatsal proved that, under suitable hypotheses, the vanishing of the Iwasawa $\mu$-invariant is preserved under congruences between ordinary elliptic curves. When the $\mu$-invariants vanish, they expressed the difference of the corresponding $\lambda$-invariants as a sum of explicit local correction terms \cite{GreenbergVatsal2000}. Emerton--Pollack--Weston extended this study to ordinary modular forms in Hida families \cite{EmertonPollackWeston2006}. They showed that if the algebraic or analytic $\mu$-invariant vanishes for one form, it vanishes throughout the family. They also described how the $\lambda$-invariants vary between branches and proved that they are constant along each branch. The algebraic and analytic variation formulae agree; consequently, the main conjecture for one modular form implies it for the other modular forms that are congruent to it. Kim extended the Greenberg--Vatsal comparison to the plus and minus Selmer groups of congruent supersingular elliptic curves \cite{Kim2009,Kim2013}. Pollack--Weston used congruences to prove Kida-type formulas, including one for supersingular elliptic curves \cite{PollackWeston2006}. Hatley and Lei then treated congruent non-ordinary modular forms of the same weight. For each sign, they showed that the $\mu$-invariant vanishes for one form if and only if it vanishes for the other; when it vanishes, the difference of the $\lambda$-invariants is determined by local terms at primes away from $p$ \cite{HatleyLei2019}. In \cite{Ray2024}, we combined the ordinary congruence formula with level raising results of Diamond and Taylor \cite{DiamondTaylor1994}. Starting from an ordinary weight-two newform $g$ with $\mu_p(g)=0$, we showed that, for every $n\geq0$, there are infinitely many newforms $f$ congruent to $g$ with $\mu_p(f)=0$ and $\lambda_p(f)=\lambda_p(g)+n$. The present paper extends this construction to non-ordinary modular forms and develops a probabilistic model for the variation of their signed $\lambda$-invariants as the tame level varies. In the non-ordinary setting there are two signed $\lambda$-invariants. We show that level raising increases them by the same amount, so their difference remains unchanged. We then study the distribution of the common increment as the tame level varies. \subsection{Main results} Let $p\geq 5$ be a prime number. Let \[ g=\sum_{n\geq1}a_n(g)q^n\in S_2(\Gamma_0(N_g)) \] be a normalized newform of trivial nebentypus, where $p\nmid N_g$, and suppose that $g$ is non-ordinary at $p$. Write $G_\Q=\Gal(\overline{\Q}/\Q)$ and let \[ \bar\rho_g:G_\Q\longrightarrow\operatorname{GL}_2(\mathbf{k}) \] be the residual Galois representation attached to $g$ at a fixed $p$-adic place of its coefficient field, where $\mathbf{k}$ is the corresponding residue field. Let $\overline\chi_p$ denote the mod-$p$ cyclotomic character, and let $\mu_{p^r}$ denote the group of $p^r$-th roots of unity. Put \[ H_g=\bar\rho_g(G_\Q)\subseteq\operatorname{GL}_2(\mathbf{k}). \] Let $L_g$ be the fixed field of $\ker(\bar\rho_g)$. Since $g$ has weight two and trivial nebentypus, $\det\bar\rho_g=\overline\chi_p$. In particular, $\det(H_g)=\F_p^\times$ and $\Q(\mu_p)\subseteq L_g$. For a prime $q\nmid N_gp$, we write $\Frob_q$ for an arithmetic Frobenius element at $q$. For $h\in H_g$, put $d(h)=\det(h)$ and define the conjugacy-stable subsets \begin{align*} \mathcal C_g^+ &= \{h\in H_g:d(h)\notin\{\pm1\},\ \Tr(h)=1+d(h)\},\\ \mathcal C_g^- &= \{h\in H_g:d(h)\notin\{\pm1\},\ \Tr(h)=-(1+d(h))\}. \end{align*} Thus the characteristic polynomial of an element of $\mathcal C_g^+$ is $(X-1)(X-d(h))$, whereas that of an element of $\mathcal C_g^-$ is $(X+1)(X+d(h))$. For a non-ordinary modular form $h$ and $\natural\in\{\sharp,\flat\}$, let $X^\natural(h)$ denote the Pontryagin dual of its $\natural$-signed Selmer group over the cyclotomic $\Z_p$-extension of $\Q$. When $X^\natural(h)$ is torsion, we denote its Iwasawa invariants by $\mu^\natural(h)$ and $\lambda^\natural(h)$. We impose the following hypotheses. \begin{enumerate}[label=(H\arabic*)] \item\label{H:image} The representation $\bar\rho_g$ is absolutely irreducible, both $\mathcal C_g^+$ and $\mathcal C_g^-$ are nonempty, and \[ L_g\cap\Q(\mu_{p^2})=\Q(\mu_p). \] \item\label{H:optimal} The integer $N_g$ is the prime-to-$p$ Artin conductor of $\bar\rho_g$. \item\label{H:base} For each $\natural\in\{\sharp,\flat\}$, the signed Selmer dual $X^\natural(g)$ is torsion over the cyclotomic Iwasawa algebra and $\mu^\natural(g)=0$. \end{enumerate} The residual-image hypothesis \ref{H:image} is weaker than requiring $\mathbf{k}=\Fp$ and $H_g=\operatorname{GL}_2(\Fp)$. In particular, Proposition~\ref{prop:large-image-criterion} shows that it holds whenever $\operatorname{SL}_2(\mathbf{k})\subseteq H_g$. Let $\Pi_g$ be the set of primes $q\nmid N_gp$ such that $\bar\rho_g(\Frob_q)\in\mathcal C_g^+$ and $q^{p-1}\not\equiv1\pmod{p^2}$. Let $\Omega_g$ be the set of primes $\ell\nmid N_gp$ such that $\bar\rho_g(\Frob_\ell)\in\mathcal C_g^-$.Write $\delta_\Pi$ and $\delta_\Omega$ for the natural densities of $\Pi_g$ and $\Omega_g$, respectively. These densities exist by the Chebotarev density theorem, and Proposition~\ref{prop:aux-density} gives \begin{equation}\label{eq:intro-auxiliary-densities} \delta_\Pi = \frac{p-1}{p}\frac{|\mathcal C_g^+|}{|H_g|}\quad \text{and}\quad \delta_\Omega = \frac{|\mathcal C_g^-|}{|H_g|}. \end{equation} Both are positive by \ref{H:image}. When $\mathbf{k}=\Fp$ and $H_g=\operatorname{GL}_2(\Fp)$, these become \[ \delta_\Pi=\frac{p-3}{p(p-1)}\quad \text{and}\quad \delta_\Omega=\frac{p-3}{(p-1)^2}. \] The first main result is the following signed analogue of the prescription theorem of \cite{Ray2024}. \begin{theorem}\label{thm:main} Assume \ref{H:image}--\ref{H:base}. Let $Q\subset\Pi_g$ and $R\subset\Omega_g$ be finite sets. There exists a normalized weight-two newform $f$ of trivial nebentypus and exact level \[ N_f=N_g\prod_{q\in Q}q\prod_{\ell\in R}\ell \] such that $\bar\rho_f\simeq\bar\rho_g$ and $f$ is non-ordinary at $p$. For each $\natural\in\{\sharp,\flat\}$, the signed Selmer dual $X^\natural(f)$ is torsion over the cyclotomic Iwasawa algebra and \[ \mu^\natural(f)=0\quad \text{and}\quad \lambda^\natural(f) = \lambda^\natural(g)+|Q|. \] \end{theorem} The distinction between the two sets of auxiliary primes is local. A prime in $\Pi_g$ contributes one to each signed $\lambda$-invariant, whereas a prime in $\Omega_g$ contributes zero. At the primes dividing $N_g$, the optimal-level hypothesis implies that the local correction terms for $f$ and $g$ agree. Since these tame corrections do not depend on the signed label, Theorem~\ref{thm:main} also gives \[ \lambda^\sharp(f)-\lambda^\flat(f) = \lambda^\sharp(g)-\lambda^\flat(g). \] As both auxiliary sets are infinite, we obtain the following consequence. \begin{corollary}\label{cor:realization} Assume \ref{H:image}--\ref{H:base}. For every $n\geq0$, there are infinitely many normalized newforms $f$, of pairwise distinct exact levels, such that $\bar\rho_f\simeq\bar\rho_g$ and the following assertions hold: \begin{enumerate} \item $\mu^\sharp(f)=\mu^\flat(f)=0$, \item $\bigl(\lambda^\sharp(f),\lambda^\flat(f)\bigr) = \bigl(\lambda^\sharp(g)+n,\lambda^\flat(g)+n\bigr)$. \end{enumerate} \end{corollary} Theorem~\ref{thm:main} determines the signed $\lambda$-invariants for each choice of level-raising primes. We now let these choices vary and bound the product of the primes. If the level is raised at $Q\subset\Pi_g$ and $R\subset\Omega_g$, both signed $\lambda$-invariants increase by $|Q|$. Their common increment is therefore the number of prime factors of the new level belonging to $\Pi_g$. For comparison, let $\omega(m)$ denote the number of distinct prime divisors of a positive integer $m$. Hardy and Ramanujan proved that the normal order of $\omega(m)$ is $\log\log m$ \cite{HardyRamanujan1917}, and Tur\'an gave a proof using the second moment \cite{Turan1934}. Erd\H{o}s and Kac showed that the fluctuations about this normal order have a Gaussian limiting distribution \cite{ErdosKac1940}. More precisely, for every $x\in\mathbb R$, \[ \lim_{Y\to\infty} \frac{1}{Y} \# \left\{ m\leq Y: \frac{\omega(m)-\log\log Y}{\sqrt{\log\log Y}}\leq x \right\} = \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{x}e^{-t^2/2}\,dt. \] We prove the corresponding limit law for the common signed $\lambda$-increment, with $\delta_\Pi\log\log Y$ in place of $\log\log Y$. Call a positive integer $D$ \emph{admissible} if it is squarefree and every prime divisor of $D$ belongs to $\Pi_g\cup\Omega_g$. Since the two sets are disjoint, we may write $D=D_\Pi D_\Omega$, where $D_\Pi$ is supported on $\Pi_g$ and $D_\Omega$ is supported on $\Omega_g$. Put \[ \omega_\Pi(D)=\#\{q:q\mid D_\Pi\}. \] For every admissible $D$, choose one form $f_D$ supplied by Theorem~\ref{thm:main}. It has exact level $N_gD$, and \begin{equation}\label{eq:intro-common-increment} \lambda^\sharp(f_D)-\lambda^\sharp(g) = \lambda^\flat(f_D)-\lambda^\flat(g) = \omega_\Pi(D). \end{equation} Thus the variation of the signed Iwasawa invariants is governed by an additive arithmetic function supported on the Frobenian set $\Pi_g$. Let \[ \mathscr D(Y) = \{D\leq Y:D\text{ is admissible}\}\quad \text{and}\quad \mathscr F(Y) = \{f_D:D\in\mathscr D(Y)\}. \] Since $f_D$ has exact level $N_gD$, different admissible integers give different members of $\mathscr F(Y)$. For $\natural\in\{\sharp,\flat\}$ and $f\in\mathscr F(Y)$, set \[ \Delta^\natural(f) = \lambda^\natural(f)-\lambda^\natural(g). \] If $X$ is a real-valued function on $\mathscr F(Y)$, we write $\mathbb E_Y[X]$ and $\operatorname{Var}_Y(X)$ for its expectation and variance with respect to the uniform probability measure on $\mathscr F(Y)$. The second main result is the following. \begin{theorem}[Analogue of Erd\H{o}s--Kac theorem] \label{thm:erdos-kac} Let $\natural\in\{\sharp,\flat\}$. Then for every real number $x$, \begin{equation}\label{eq:EK-limit} \begin{aligned} &\lim_{Y\to\infty} \frac{1}{\#\mathscr F(Y)} \#\Biggl\{ f\in\mathscr F(Y):\\[-2pt] &\hspace{5em} \frac{ \lambda^\natural(f)-\lambda^\natural(g) -\delta_\Pi\log\log Y} {\sqrt{\delta_\Pi\log\log Y}} \leq x \Biggr\} = \frac{1}{\sqrt{2\pi}} \int_{-\infty}^x e^{-t^2/2}\,dt. \end{aligned} \end{equation} Moreover, \begin{align} \mathbb E_Y[\Delta^\natural] &= \delta_\Pi\log\log Y+O_g(1), \label{eq:EK-mean}\\ \operatorname{Var}_Y(\Delta^\natural) &= \delta_\Pi\log\log Y+O_g(1). \label{eq:EK-variance} \end{align} The two signed increments agree for every member of the family. Consequently, \[ \lambda^\sharp(f)-\lambda^\flat(f) = \lambda^\sharp(g)-\lambda^\flat(g) \] for every $f\in\mathscr F(Y)$. \end{theorem} The Gaussian law describes the typical size of the common increase in the two signed $\lambda$-invariants. We also count the forms for which this increase has a prescribed value. For $n\geq0$, let $\mathscr F_n(X)$ consist of the chosen forms $f_D$ of level at most $X$ for which \[\lambda^\sharp(f_D)-\lambda^\sharp(g) =\lambda^\flat(f_D)-\lambda^\flat(g)=n.\] For each fixed $n$, we prove that \[ \#\mathscr F_n(X) \sim \frac{C_{g,n}}{N_g} X(\log X)^{\delta_\Omega-1}(\log\log X)^n, \] where $C_{g,n}>0$. \subsection{Organization of the paper} Including the introduction, the article consists of five sections. Section~\ref{sec:signed} recalls the signed Selmer groups and the congruence results we use. In Section~\ref{sec:level-raising}, we construct the auxiliary primes and the level-raised forms. Section~\ref{sec:local} computes the local contributions to the signed $\lambda$-invariants and proves Theorem~\ref{thm:main}. Finally, Section~\ref{sec:quantitative} counts the levels realizing each fixed increase and proves the Erd\H{o}s--Kac theorem. \section*{Statements and Declarations} \noindent\textbf{Funding.} The author received no funding for this work. \noindent\textbf{Ethical approval.} Not applicable. \noindent\textbf{Consent to participate.} Not applicable. \noindent\textbf{Consent for publication.} Not applicable. \noindent\textbf{Conflict of interest.} The author declares no conflict of interest. \noindent\textbf{Data availability.} No datasets were generated or analyzed during the current study. \section{Signed Selmer groups and their congruences} \label{sec:signed} Fix a prime number $p\geq 5$. Let $\chi_p$ be the $p$-adic cyclotomic character and $\bar{\chi}_p$ be its mod-$p$ reduction. Let $\Q(\mu_{p^\infty})$ be the infinite cyclotomic field generated by the $p$-power roots of unity $\mu_{p^\infty}$. Let $\Q_\infty/\Q$ be the cyclotomic $\Zp$-extension and set $\Gamma:=\Gal(\Q_\infty/\Q)$. Let $E/\Q_p$ be a finite extension with valuation ring $\cO$, uniformizer $\varpi$ and $\mathbf k=\cO/(\varpi)$. The Iwasawa algebra (with coefficients in $\cO$) is defined as the completed group algebra: \[\Lambda_{\cO}:=\cO[[\Gamma]]=\varprojlim_n \cO[\Gamma/\Gamma^{p^n}].\] We choose a topological generator $\gamma$ of $\Gamma$ and identify $\Lambda_{\cO}$ with $\cO[[T]]$ by setting $T:=\gamma-1$. \subsection{Iwasawa modules} We first describe the properties of modules over the Iwasawa algebra $\Lambda_{\cO}$. Here, if $M$ and $M'$ are two modules over $\Lambda_{\cO}$, then a pseudoisomorphism is a $\Lambda_{\cO}$-module homomorphism $\varphi: M\rightarrow M'$ whose kernel and cokernel both have finite cardinality. If $M$ is a finitely generated and torsion $\Lambda_{\cO}$-module, there is a pseudo-isomorphism \begin{equation}\label{eq:structure-module} M\longrightarrow \bigoplus_{i=1}^{r}\Lambda_{\cO}/(\varpi^{\mu_i}) \oplus \bigoplus_{j=1}^{s}\Lambda_{\cO}/(F_j(T)^{e_j}), \end{equation} where $\mu_i,e_j\geq1$ and the $F_j(T)$ are irreducible distinguished polynomials. We then set \[ \mu(M)=\sum_{i=1}^{r}\mu_i\quad \text{and}\quad \lambda(M)=\sum_{j=1}^{s}e_j\deg F_j. \] \begin{lemma}\label{lem:modpi-criterion} Let $M$ be a compact $\Lambda_{\cO}$-module, where $\Lambda_{\cO}=\cO[[T]]$. The following conditions are equivalent. \begin{enumerate}[label=(\roman*)] \item The quotient $M/\varpi M$ is finite-dimensional over $\mathbf{k}$. \item The module $M$ is finitely generated and torsion over $\Lambda_{\cO}$, and $\mu(M)=0$. \end{enumerate} If these conditions hold and $M$ has no nonzero finite $\Lambda_{\cO}$-submodule, then \[ \lambda(M)=\dim_{\mathbf{k}}(M/\varpi M). \] \end{lemma} \begin{proof} We first assume that $M/\varpi M$ is finite-dimensional over $\mathbf{k}$. Let \[ \mathfrak n=(\varpi,T) \] be the maximal ideal of $\Lambda_{\cO}$. Since \[ M/\mathfrak nM = (M/\varpi M)/T(M/\varpi M), \] the quotient $M/\mathfrak nM$ is finite-dimensional over $\mathbf{k}$. Choose elements $m_1,\ldots,m_r\in M$ whose images generate $M/\mathfrak nM$, and let $N$ be the $\Lambda_{\cO}$-submodule of $M$ generated by these elements. Then $M=N+\mathfrak nM$. Since $M$ is compact and $\Lambda_{\cO}$ is a complete local ring, the topological Nakayama lemma gives $M=N$. Thus $M$ is finitely generated over $\Lambda_{\cO}$; see \cite[Section~3, Corollary following the first theorem]{BalisterHowson1997}. We may now apply the structure theorem for finitely generated $\Lambda_{\cO}$-modules. There is a homomorphism \[ \phi:M\longrightarrow M' \] with finite kernel and finite cokernel, where \[ M'= \Lambda_{\cO}^{\,r_0} \oplus \bigoplus_{i=1}^{u} \Lambda_{\cO}/(\varpi^{a_i}) \oplus \bigoplus_{j=1}^{v} \Lambda_{\cO}/(F_j(T)^{e_j}). \] Here $a_i,e_j\geq1$, and each $F_j(T)$ is a distinguished irreducible polynomial which is not divisible by $\varpi$. It is easy to see that $M'/\varpi M'$ is finite-dimensional over $\mathbf{k}$. This rules out the first two types of elementary factors. Indeed, a free summand $\Lambda_{\cO}$ contributes $\mathbf{k}[[T]]$ to $M'/\varpi M'$, which is infinite-dimensional over $\mathbf{k}$. Likewise, \[ \bigl(\Lambda_{\cO}/(\varpi^{a_i})\bigr) \big/ \varpi\bigl(\Lambda_{\cO}/(\varpi^{a_i})\bigr) \simeq \mathbf{k}[[T]], \] so the presence of a factor $\Lambda_{\cO}/(\varpi^{a_i})$ would again make $M'/\varpi M'$ infinite-dimensional. It follows that $r_0=u=0$. Therefore $M$ is torsion and $\mu(M)=0$. We now prove the converse. Suppose that $M$ is finitely generated and torsion over $\Lambda_{\cO}$ and that $\mu(M)=0$. The structure theorem then gives a pseudo-isomorphism \[ \varphi: M\longrightarrow M':=\bigoplus_{j=1}^{v} \Lambda_{\cO}/(F_j(T)^{e_j}), \] with finite kernel and cokernel. If $d_j=\deg F_j$, then, since $F_j$ is distinguished, \[ F_j(T)\equiv T^{d_j}\pmod{\varpi}. \] It follows that $M'/\varpi M'$ is finite-dimensional. Since $M$ is pseudoisomorphic to $M'$, it is easy to see that $M/\varpi M$ is finite-dimensional. It remains to prove the formula for the $\lambda$-invariant. Assume in addition that $M$ has no nonzero finite $\Lambda_{\cO}$-submodule. In the pseudo-isomorphism $\varphi$ above, the kernel is finite and is a submodule of $M$. Hence $K=0$. We therefore have an exact sequence \[ 0\longrightarrow M\longrightarrow M'\longrightarrow C \longrightarrow0 \] with $C$ finite. Each module $\Lambda_{\cO}/(F_j(T)^{e_j})$ is finite free over $\cO$ of rank $e_jd_j$. Thus $M'$ is a finitely generated and free $\cO$-module of rank \[ \sum_{j=1}^{v}e_jd_j=\lambda(M). \] Since $M$ is an $\cO$-submodule of the finite free module $M'$, it is finitely generated and torsion-free over the discrete valuation ring $\cO$, and hence is itself free over $\cO$. The quotient $M'/M=C$ is finite, so $M$ and $M'$ have the same $\cO$-rank. Therefore \[ \operatorname{rank}_{\cO}M=\lambda(M). \] Finally, if a finite free $\cO$-module has rank $r$, then its reduction modulo $\varpi$ has dimension $r$ over $\mathbf{k}$. Hence \[ \dim_{\mathbf{k}}(M/\varpi M) = \operatorname{rank}_{\cO}M = \lambda(M), \] as required. \end{proof} \subsection{Signed local conditions} Let $h=\sum_{n\geq1}a_n(h)q^n$ be a normalized newform of weight $2$, level prime to $p$, and trivial nebentypus. Choose an embedding $\overline{\Q}\hookrightarrow\overline{\Q}_p$ and let $E/\Q_p$ be a finite extension containing the image of the coefficient field of $h$. Associated to $h$ is a $2$-dimensional Galois representation over $E$; let $V_h$ denote the underlying vector space. Our convention is that the Hodge--Tate weights of $V_h$ are $\{0,-1\}$. Let $T_h\subset V_h$ be Kato's Galois stable $\cO$-lattice, cf. \cite[Section~8.3]{Kato2004}. We then set \[ A_h=(V_h/T_h)(1)\quad \text{and}\quad \mathscr T_h=T_h(1). \] The lattice $\mathscr T_h$ is crystalline at $p$, with Hodge--Tate weights $\{0,1\}$. For $n\geq 0$, put $K_n=\Qp(\mu_{p^{n+1}})$ and let $K_\infty=\bigcup_{n\geq0}K_n$. Thus \[ G_\infty:=\Gal(K_\infty/\Qp) \simeq \Delta\times\Gamma. \] The completion $\Q_{\infty,p}$ of $\Q_\infty$ at the prime above $p$ is $K_\infty^\Delta$. Thus passage to the trivial $\Delta$-component identifies the local conditions below with the corresponding local conditions over $\Q_{\infty,p}$. If $T$ is a $\cO$-lattice equipped with a continuous action of $G_{\Qp}$, its local Iwasawa cohomology is defined by \begin{equation}\label{eq:iw-cohomology} H^1_{\Iw}(\Qp,T) := \varprojlim_n H^1(K_n,T), \end{equation} where the inverse limit is taken with respect to the corestriction maps. It is naturally a module over \[ \cO[[G_\infty]] \simeq \Lambda_{\cO}(\Delta) := \cO[\Delta]\widehat\otimes_{\cO}\Lambda_{\cO}. \] We apply this construction to the positive crystalline lattice $\mathscr T_h$. The construction of Lei--Loeffler--Zerbes \cite{LLZ2010} gives, after fixing a suitable basis, two Coleman maps \[ \operatorname{Col}_{h,1},\operatorname{Col}_{h,2}: H^1_{\Iw}(\Qp,\mathscr T_h)\longrightarrow \Lambda_{\cO}(\Delta). \] We use the notation $\sharp,\flat$ for the signed Coleman maps in the normalization customary in the weight-two non-ordinary setting; see \cite{Sprung2012,Sprung2017}. For a character $\eta:\Delta\rightarrow\cO^\times$, projection to the $\eta$-isotypical component gives \[ \operatorname{Col}_{h,\natural}^{\eta}: H^1_{\Iw}(\Qp,\mathscr T_h)^\eta \longrightarrow \Lambda_{\cO}, \] where $\natural\in\{\sharp,\flat\}$. In this article we work throughout in the trivial $\Delta$-component, so $\eta=\mathbf 1$. We shall therefore suppress $\eta$ from the notation and regard the signed Coleman maps as $\Lambda_{\cO}$-valued maps. We next recall the local Tate pairing used to define the signed local condition. The representation $A_h$ is the Cartier dual of $\mathscr T_h$ in our normalization. Thus there is a perfect $G_{\Qp}$-equivariant pairing \[ \mathscr T_h\times A_h \longrightarrow E/\cO(1). \] For every finite extension $K/\Qp$, cup product followed by the local invariant map gives Tate's local pairing \[ H^1(K,\mathscr T_h)\times H^1(K,A_h) \longrightarrow H^2(K,E/\cO(1)) \xrightarrow{\operatorname{inv}_K} E/\cO. \] If $L/K$ is a finite extension, then \[ \langle\operatorname{cores}_{L/K}(x),y\rangle_K = \langle x,\operatorname{res}_{L/K}(y)\rangle_L. \] Passing to the inverse limit in the first variable and the direct limit in the second gives a pairing \begin{equation}\label{eq:iw-local-tate-pairing} \langle\ ,\ \rangle_p: H^1_{\Iw}(\Qp,\mathscr T_h) \times H^1(K_\infty,A_h) \longrightarrow E/\cO. \end{equation} If $\natural\in\{\sharp,\flat\}$, the signed local condition at $p$ is defined to be the orthogonal complement of the kernel of the corresponding Coleman map: \[ H^1_{\natural}(K_\infty,A_h) = \bigl(\ker(\operatorname{Col}_{h}^{\natural})\bigr)^\perp. \] This is the local condition at $p$ used in the definition of the signed Selmer group. For a prime $\ell\neq p$, the local condition is the unramified subgroup \[ H^1_{\ur}(\Q_{\infty,v},A_h) =\ker\bigl(H^1(\Q_{\infty,v},A_h) \longrightarrow H^1(I_v,A_h)\bigr), \] where $v$ is a prime of $\Q_\infty$ above $\ell$. If $\Sigma$ contains $p$, $\infty$ and all primes at which $A_h$ is ramified, we define \begin{equation}\label{eq:signed-selmer-definition} \Sel^\natural(A_h/\Q_\infty) =\ker\left( H^1(G_{\Q,\Sigma}/\Q_\infty,A_h) \longrightarrow \frac{H^1(\Q_{\infty,p},A_h)}{H^1_\natural(\Q_{\infty,p},A_h)} \oplus \bigoplus_{\substack{ v\mid\ell\\ \ell\in\Sigma\setminus\{p\}}} \frac{H^1(\Q_{\infty,v},A_h)}{H^1_{\ur}(\Q_{\infty,v},A_h)} \right). \end{equation} Its Pontryagin dual is denoted \[ X^\natural(h)=\Sel^\natural(A_h/\Q_\infty)^\vee. \] Whenever $X^\natural(h)$ is torsion, its Iwasawa invariants are written $\mu^\natural(h)$ and $\lambda^\natural(h)$. Let $\Sigma_0\subseteq\Sigma\setminus\{p,\infty\}$. The non-primitive signed Selmer group $\Sel^{\natural,\Sigma_0}(A_h/\Q_\infty)$ is obtained from \eqref{eq:signed-selmer-definition} by imposing no local condition at the primes above $\Sigma_0$. Set \[ Y_h^{\natural,\Sigma_0} =\Sel^{\natural,\Sigma_0}(A_h/\Q_\infty)^\vee. \] For $\ell\in\Sigma_0$, put \[ \mathcal H_{\ell}(A_h) =\prod_{v\mid\ell} \frac{H^1(\Q_{\infty,v},A_h)}{H^1_{\ur}(\Q_{\infty,v},A_h)}. \] Under the torsion hypothesis, the Poitou--Tate argument of \cite[Corollary~2.10]{HatleyLei2019} gives an exact sequence \begin{equation}\label{eq:primitive-nonprimitive-exact} 0\longrightarrow \Sel^\natural(A_h/\Q_\infty) \longrightarrow \Sel^{\natural,\Sigma_0}(A_h/\Q_\infty) \longrightarrow \bigoplus_{\ell\in\Sigma_0}\mathcal H_{\ell}(A_h) \longrightarrow0. \end{equation} The local modules on the right are cotorsion and have vanishing $\mu$-invariant; see \cite[Remark~2.11]{HatleyLei2019}. If \[ \delta_{\ell,h}:=\lambda\bigl(\mathcal H_{\ell}(A_h)^\vee\bigr), \] then \eqref{eq:primitive-nonprimitive-exact} gives \begin{equation}\label{eq:primitive-nonprimitive} \lambda^{\natural,\Sigma_0}(h) =\lambda^\natural(h)+\sum_{\ell\in\Sigma_0}\delta_{\ell,h}. \end{equation} \subsection{Residual comparison} We next compare the residual signed Selmer groups for two congruent modular forms. Let $f$ and $g$ be $p$-non-ordinary modular forms of the same even weight $k$, and let $T_f$ and $T_g$ be the corresponding $G_{\Q}$-stable $\cO$-lattices. We assume that the hypotheses \textup{(irred)}, \textup{(inv)}, \textup{(BLZ)} and \textup{(Cong)} of Hatley--Lei hold. We recall these conditions explicitly; they are summarized in \cite[p.~1289]{HatleyLei2019}. The hypothesis \textup{(irred)} requires that $T_f/\varpi T_f$ be irreducible as a $G_{\Q}$-representation. Since we assume that $T_f/\varpi T_f\simeq T_g/\varpi T_g$, this is equivalent to the corresponding assertion for $g$. The hypothesis \textup{(Cong)} is precisely the residual congruence \begin{equation}\label{eq:HL-cong} T_f/\varpi T_f \simeq T_g/\varpi T_g \end{equation} as $G_{\Q}$-representations. The hypothesis \textup{(inv)} is the vanishing \begin{equation}\label{eq:HL-inv} A_h(m)^{G_{\Q_{\infty,p}}}=0 \end{equation} for every $m\geq0$. Finally, the hypothesis \textup{(BLZ)} requires that \begin{equation}\label{eq:HL-BLZ} \ord_p(a_p(f)), \ord_p(a_p(g)) > \left\lfloor\frac{k-2}{p-1}\right\rfloor; \end{equation} cf. \cite[p.~1289]{HatleyLei2019} and \cite[pp.~374--376]{BergerLiZhu2004}. When $k=2$, the right-hand side of \eqref{eq:HL-BLZ} is zero. Consequently \textup{(BLZ)} becomes $\ord_p(a_p(f))>0$ and $\ord_p(a_p(g))>0$, i.e., both forms are non-ordinary at $p$. \begin{proposition}\label{prop:residual-comparison} Let $\Sigma$ contain $p$, $\infty$, and all primes at which either $f$ or $g$ is ramified, and set $\Sigma_0=\Sigma\setminus\{p,\infty\}$. For either signed label $\natural$, there is an isomorphism \[ \Sel^{\natural,\Sigma_0}(A_f/\Q_\infty)[\varpi] \simeq \Sel^{\natural,\Sigma_0}(A_g/\Q_\infty)[\varpi]. \] \end{proposition} \begin{proof} This is a standard result and the method goes back to Greenberg--Vatsal \cite[Section~2]{GreenbergVatsal2000}. The same argument in the ordinary modular-form setting is recalled and used in \cite[Section~4]{Ray2024}. In the non-ordinary setting, Hatley--Lei \cite[Propositions~4.3 and~4.5]{HatleyLei2019} identify the $\varpi$-torsion of the non-primitive signed Selmer group with the residual Selmer group. \end{proof} \begin{proposition} \label{prop:one-sided} Let $f$ and $g$ be as in Proposition~\ref{prop:residual-comparison}. Fix $\natural\in\{\sharp,\flat\}$. If $X^\natural(g)$ is torsion and $\mu^\natural(g)=0$, then $X^\natural(f)$ is torsion and $\mu^\natural(f)=0$. \end{proposition} \begin{proof} Take $\Sigma_0$ as in Proposition~\ref{prop:residual-comparison} and write $Y_h=Y_h^{\natural,\Sigma_0}$. Since $X^\natural(g)$ is torsion, \eqref{eq:primitive-nonprimitive-exact} is an exact sequence for $g$. The local terms are torsion with vanishing $\mu$-invariant, so $Y_g$ is torsion with $\mu(Y_g)=0$. Lemma~\ref{lem:modpi-criterion} gives $\dim_{\mathbf k}Y_g/\varpi Y_g<\infty$. Pontryagin duality identifies \[ (\Sel^{\natural,\Sigma_0}(A_h/\Q_\infty)[\varpi])^\vee \simeq Y_h/\varpi Y_h \] for $h=g$ or $f$. Therefore Proposition~\ref{prop:residual-comparison} gives \[ Y_f/\varpi Y_f\simeq Y_g/\varpi Y_g. \] It follows that $Y_f/\varpi Y_f$ is finite dimensional. Applying Lemma~\ref{lem:modpi-criterion} to $Y_f$ shows that $Y_f$ is finitely generated and torsion over $\Lambda_{\cO}$ with $\mu(Y_f)=0$. The primitive signed Selmer group is a subgroup of the non-primitive group; after dualizing, $X^\natural(f)$ is a quotient of $Y_f$. Hence $X^\natural(f)$ is torsion over $\Lambda_{\cO}$ with $\mu(X^\natural(f))=0$. \end{proof} \begin{lemma} \label{lem:weight-two-finite-index} Let $h$ be a weight-two $p$-non-ordinary newform of level prime to $p$ and trivial nebentypus. Assume \textup{(irred)}, \textup{(inv)}, \textup{(BLZ)} and \textup{(tor)} in the notation of Hatley--Lei. For each $\natural\in\{\sharp,\flat\}$, we have that $\Sel^\natural(A_h/\Q_\infty)$ has no proper $\Lambda_{\cO}$-submodule of finite index. \end{lemma} \begin{proof} The result follows from \cite[Theorem~3.1]{HatleyLei2019}. \end{proof} \begin{proposition}[Signed congruence formula] \label{prop:signed-congruence} Let $f$ and $g$ satisfy the hypotheses of Proposition~\ref{prop:residual-comparison}. If $X^\natural(g)$ is torsion and $\mu^\natural(g)=0$, then $X^\natural(f)$ is torsion, $\mu^\natural(f)=0$, and \begin{equation}\label{eq:transition} \lambda^\natural(f)-\lambda^\natural(g) =\sum_{\ell\in\Sigma_0} \bigl(\delta_{\ell,g}-\delta_{\ell,f}\bigr). \end{equation} \end{proposition} \begin{proof} Proposition~\ref{prop:one-sided} first supplies the torsion and $\mu=0$ hypotheses for $f$. Thus the running hypothesis \textup{(tor)} of Hatley--Lei is satisfied for both $f$ and $g$. By Lemma~\ref{lem:weight-two-finite-index}, both signed Selmer groups have no proper finite-index submodule. By Proposition~\ref{prop:residual-comparison}, the residual non-primitive Selmer groups are isomorphic. It follows then from the \cite[Proof of Theorem~4.6]{HatleyLei2019} and \cite[Lemma~12]{Kim2009} that \[ \lambda^{\natural,\Sigma_0}(f) =\lambda^{\natural,\Sigma_0}(g). \] Applying \eqref{eq:primitive-nonprimitive} to $f$ and $g$ and subtracting gives \eqref{eq:transition}. \end{proof} \begin{theorem} \label{thm:rigidity} Let $f$ and $g$ be as in Proposition~\ref{prop:signed-congruence}. Assume that $X^\sharp(g)$ and $X^\flat(g)$ are torsion and that $\mu^\sharp(g)=\mu^\flat(g)=0$. Then \[ \lambda^\sharp(f)-\lambda^\flat(f) =\lambda^\sharp(g)-\lambda^\flat(g). \] More precisely, there is an integer $c(f,g)$ determined by the tame local correction terms such that \[ (\lambda^\sharp(f),\lambda^\flat(f)) =(\lambda^\sharp(g)+c(f,g),\lambda^\flat(g)+c(f,g)). \] \end{theorem} \begin{proof} Apply Proposition~\ref{prop:signed-congruence} for $\sharp$ and $\flat$. Every term on the right-hand side of \eqref{eq:transition} is attached to a prime $\ell\neq p$ and is therefore the same for the two signed Selmer structures. On subtracting the two identities, we obtain the result. \end{proof} \section{Residual images, non-optimal levels and auxiliary primes} \label{sec:level-raising} In this section, we carry out the global construction of the forms that will be used in the proof of Theorem~\ref{thm:main}. There are three ingredients. We first recall the part of the non-optimal-level theorem of Carayol and Diamond--Taylor that allows one to raise the tame level at several primes simultaneously. We then isolate two conjugacy-stable subsets of the residual image and use the Chebotarev density theorem to produce two corresponding sets of auxiliary primes. Finally, we show that level raising at any finite collection of these primes preserves the residual representation and forces the required local Steinberg signs. The argument is a refinement of the construction in \cite[Sections~2, 4--5]{Ray2024}. \subsection{Artin conductors and non-optimal levels} Fix an algebraic closure $\overline\Q$ of $\Q$. For every prime $\ell$, choose an embedding $\overline\Q\hookrightarrow \overline\Q_\ell$. This identifies the absolute Galois group $G_\ell=\Gal(\overline\Q_\ell/\Q_\ell)$ with a decomposition subgroup of $G_\Q=\Gal(\overline\Q/\Q)$. We write $I_\ell\subseteq G_\ell$ for the inertia subgroup and choose an arithmetic Frobenius element $\Frob_\ell\in G_\ell/I_\ell$. Let \[ \bar\rho:G_\Q\longrightarrow\operatorname{GL}_2(\mathbf k) \] be a continuous, odd and absolutely irreducible representation of characteristic $p$. If $\ell\neq p$, let $a_\ell(\bar\rho)$ denote the Artin-conductor exponent of the local representation $\bar\rho|_{G_\ell}$. The prime-to-$p$ Artin conductor of $\bar\rho$ is \begin{equation}\label{eq:residual-artin-conductor} N(\bar\rho)=\prod_{\ell\neq p}\ell^{a_\ell(\bar\rho)}. \end{equation} If $h$ is a modular lift of $\bar\rho$ whose tame level is $N_h$, then $N(\bar\rho)$ divides $N_h$; see \cite{Ribet1994Report,Carayol1989}. We say that $h$ has \emph{optimal level} if $N_h=N(\bar\rho)$. In this terminology, a prime dividing $N_h/N(\bar\rho)$ records ramification that is present in the characteristic-zero representation but disappears after reduction modulo the maximal ideal. Suppose that $\ell\nmid pN(\bar\rho)$. The residual representation is then unramified at $\ell$, and Carayol's condition for introducing conductor exponent one at $\ell$ is \begin{equation}\label{eq:carayol-condition} \ell\,\Tr\bigl(\bar\rho(\Frob_\ell)\bigr)^2 = (1+\ell)^2\det\bigl(\bar\rho(\Frob_\ell)\bigr) \quad\text{in }\mathbf k. \end{equation} Since $\det(\bar\rho(\Frob_\ell))=\ell$, condition \eqref{eq:carayol-condition} is equivalent to \begin{equation}\label{eq:levelraising-trace} \Tr\bigl(\bar\rho(\Frob_\ell)\bigr)^2=(1+\ell)^2. \end{equation} Let $f$ be a weight-two newform with trivial nebentypus, and let $\ell\neq p$ be a prime such that $\ell\Vert N_f$. We say that $f$ is \emph{Steinberg at $\ell$} if its local automorphic representation has the form $\pi_{f,\ell}\simeq \operatorname{St}\otimes\xi_\ell$, where $\xi_\ell$ is an unramified character. Since the nebentypus of $f$ is trivial, one has $\xi_\ell(\Frob_\ell)=\varepsilon_\ell$. The semisimplification of the local representation at $\ell$ has unramified characters $\xi_\ell$ and $\xi_\ell\chi_p$. Consequently, after reduction modulo $\varpi$, the Frobenius eigenvalues are $\varepsilon_\ell$ and $\varepsilon_\ell\ell$. \begin{theorem} \label{thm:carayol-DT} Let $p\geq5$, and let $\bar\rho:G_\Q\rightarrow\operatorname{GL}_2(\mathbf k)$ be odd and absolutely irreducible, with determinant $\overline\chi_p$. Suppose that $\bar\rho$ arises from a normalized newform of weight two, trivial nebentypus and optimal tame level $N(\bar\rho)$. Let $S$ be a finite set of primes such that every $\ell\in S$ satisfies \begin{itemize} \item $\ell\nmid pN(\bar\rho)$, \item $\ell\not\equiv\pm1\pmod p$, \item $\Tr\bigl(\bar\rho(\Frob_\ell)\bigr)^2=(1+\ell)^2.$ \end{itemize} Then there is a normalized weight-two newform $h$ of trivial nebentypus, lifting $\bar\rho$, whose tame level is \begin{equation}\label{eq:CDT-raised-level} N_h=N(\bar\rho)\prod_{\ell\in S}\ell. \end{equation} The form $h$ is new at every prime in $S$. More precisely, its local representation at such a prime is a Steinberg representation of sign $\varepsilon_\ell\in\{\pm1\}$, and the residual Frobenius eigenvalues are $\varepsilon_\ell$ and $\varepsilon_\ell\ell$. \end{theorem} \begin{proof} This is the same non-optimal level argument as \cite[Proposition~4.7]{Ray2024}. Indeed, for every $\ell\in S$, condition \eqref{eq:carayol-condition} is case~(1) of Carayol's criterion, so adjoining $\ell$ increases the conductor exponent by one. Hence \[ M=N(\bar\rho)\prod_{\ell\in S}\ell \] is an admissible non-optimal level for $\bar\rho$. Since $p\geq5$ and the weight is $2$, the fixed-nebentypus form of the Diamond--Taylor level-raising theorem applies in the trivial-character Hecke algebra and produces a weight-two newform $f$ of trivial nebentypus lifting $\bar\rho$ of level $M$; see \cite[Theorem~2.3]{Ray2024}, which recalls \cite{DiamondTaylor1994}. Equivalently, one may apply the usual level-raising theorem successively at the primes in $S$; at each step the nebentypus remains trivial. This is precisely the argument used in \cite[Proposition~4.7]{Ray2024}. At every $\ell\in S$, the form $f$ is ramified at $\ell$ and $\bar\rho_f(\Frob_\ell)$ has eigenvalues $\epsilon_\ell\ell$ and $\epsilon_\ell$, with $\epsilon_\ell\in\{\pm1\}$. The local calculation of \cite[Lemma~4.4]{Ray2024} therefore applies. It shows that, after a change of basis, \[ \rho_f(\Frob_\ell)= \begin{pmatrix} \ell x_\ell&0\\ 0&x_\ell \end{pmatrix}\quad \text{and}\quad \rho_f(\tau_\ell)= \begin{pmatrix} 1&y_\ell\\ 0&1 \end{pmatrix}, \] where $x_\ell\equiv\epsilon_\ell\pmod{\varpi}$. Since $f$ has weight two and trivial nebentypus, $\det\rho_f=\chi_p$, and hence $x_\ell^2=1$. As $p$ is odd, it follows that $x_\ell=\epsilon_\ell$. Thus the local representation is of Steinberg type with sign $\epsilon_\ell$. This proves the final assertion. \end{proof} \subsection{The residual image} We study the residual representation of the fixed form $g$ in more detail. Set \[ H_g=\bar\rho_g(G_\Q)\subseteq\operatorname{GL}_2(\mathbf k), \] where $L_g=\overline\Q^{\ker\bar\rho_g}$ is the field cut out by $\bar \rho_g$. The representation $\bar\rho_g$ identifies $H_g$ with $\Gal(L_g/\Q)$. Since $g$ has weight two and trivial nebentypus, one has $\det\bar\rho_g=\overline\chi_p$. In particular, $\det(H_g)=\Fp^\times$, where $\Fp^\times$ is viewed as a subgroup of $\mathbf k^\times$. Moreover, $\ker\bar\rho_g$ is contained in $\ker\overline\chi_p$, and hence $\Q(\mu_p)\subseteq L_g$. \begin{proposition}[Dickson] \label{prop:dickson-zywina} Let $G$ be a subgroup of $\operatorname{GL}_2(\mathbb F_{p^r})$, and let $\overline G$ denote its image in $\operatorname{PGL}_2(\mathbb F_{p^r})$. Up to conjugacy, one of the following possibilities occurs: \begin{enumerate}[label=(\roman*)] \item $G$ is contained in a Borel subgroup; \item $G$ is contained in the normalizer of a Cartan subgroup; \item $\overline G$ is isomorphic to $A_4$, $S_4$, or $A_5$; \item there is a subfield $\mathbb F_{p^s}\subseteq\mathbb F_{p^r}$ such that $\overline G$ is conjugate to $\operatorname{PSL}_2(\mathbb F_{p^s})$ or $\operatorname{PGL}_2(\mathbb F_{p^s})$. \end{enumerate} \end{proposition} \begin{proof} This is Dickson's classification in the form recalled in \cite[Lemma~5.1]{Zywina2023}. \end{proof} For $u\in H_g$, write $d(u)=\det(u)$ and define \begin{align} \mathcal C_g^+ &=\bigl\{u\in H_g:d(u)\notin\{\pm1\},\ \Tr(u)=1+d(u)\bigr\},\label{eq:Cplus}\\ \mathcal C_g^- &=\bigl\{u\in H_g:d(u)\notin\{\pm1\},\ \Tr(u)=-(1+d(u))\bigr\}.\label{eq:Cminus} \end{align} Both conditions depend only on the trace and determinant, so the two sets are stable under conjugation in $H_g$. If $u\in\mathcal C_g^+$, then its characteristic polynomial factors as \[ X^2-(1+d(u))X+d(u)=(X-1)(X-d(u)). \] Similarly, if $u\in\mathcal C_g^-$, its characteristic polynomial is $(X+1)(X+d(u))$. Since $d(u)\notin\{\pm1\}$, the two roots in either factorization are distinct. The following proposition shows, in particular, that hypothesis \ref{H:image} is automatic under a large-image condition. It also gives explicit densities in that case. \begin{proposition} \label{prop:large-image-criterion} Suppose that $\operatorname{SL}_2(\mathbf k)\subseteq H_g$, and put $q_0=|\mathbf k|$. Then $\mathcal C_g^+$ and $\mathcal C_g^-$ are nonempty and \begin{equation}\label{eq:large-image-disjointness} L_g\cap\Q(\mu_{p^2})=\Q(\mu_p). \end{equation} Moreover, \begin{equation}\label{eq:large-image-C-density} \frac{|\mathcal C_g^+|}{|H_g|} =\frac{|\mathcal C_g^-|}{|H_g|} =\frac{p-3}{(p-1)(q_0-1)}. \end{equation} \end{proposition} \begin{proof} The determinant map on $H_g$ is surjective onto $\Fp^\times$. It is easy to see that \begin{equation}\label{eq:H-large} H_g=\bigl\{A\in\operatorname{GL}_2(\mathbf k): \det(A)\in\Fp^\times\bigr\}. \end{equation} For $a\in\Fp^\times\setminus\{\pm1\}$, the two matrices $\operatorname{diag}(a,1)$ and $\operatorname{diag}(-a,-1)$ both belong to $H_g$. They belong to $\mathcal C_g^+$ and $\mathcal C_g^-$, respectively. Since $p\geq5$, there is at least one such $a$, proving that both sets are nonempty. We next prove \eqref{eq:large-image-disjointness}. We already know that $\Q(\mu_p)$ is contained in $L_g$. Since $[\Q(\mu_{p^2}):\Q(\mu_p)]=p$, there is no proper intermediate field between these two cyclotomic fields. Thus, if the intersection in \eqref{eq:large-image-disjointness} were larger than $\Q(\mu_p)$, it would contain all of $\Q(\mu_{p^2})$. Restriction would then exhibit the cyclic group $\Gal(\Q(\mu_{p^2})/\Q(\mu_p))$, which has order $p$, as a quotient of \[ \Gal(L_g/\Q(\mu_p)) =\ker\bigl(\det:H_g\longrightarrow\Fp^\times\bigr). \] By \eqref{eq:H-large}, this kernel is $\operatorname{SL}_2(\mathbf k)$. For $p\geq5$, the group $\operatorname{SL}_2(\mathbf k)$ is perfect. It has no nontrivial abelian quotient and, in particular, no quotient of order $p$. It remains to count the two conjugacy-stable subsets. Fix $a\in\Fp^\times\setminus\{\pm1\}$. Every element of $\mathcal C_g^+$ with determinant $a$ has distinct eigenvalues $1$ and $a$, and is therefore conjugate in $\operatorname{GL}_2(\mathbf k)$ to $\operatorname{diag}(a,1)$. Its centralizer is the split diagonal torus, of order $(q_0-1)^2$. Hence this conjugacy class has cardinality \[ \frac{|\operatorname{GL}_2(\mathbf k)|}{(q_0-1)^2} =q_0(q_0+1). \] The classes obtained from distinct values of $a$ are disjoint because their determinants are distinct. There are $p-3$ possible values of $a$, and consequently $|\mathcal C_g^+|=(p-3)q_0(q_0+1)$. The same argument, using $\operatorname{diag}(-a,-1)$, gives the identical formula for $|\mathcal C_g^-|$. Finally, \eqref{eq:H-large} gives $|H_g|=(p-1)|\operatorname{SL}_2(\mathbf k)| =(p-1)q_0(q_0^2-1)$. Dividing the preceding cardinalities by this order proves \eqref{eq:large-image-C-density}. \end{proof} \subsection{The two Frobenian sets} We now define the auxiliary primes. Let $\Pi_g$ be the set of primes $q\nmid N_gp$ such that $\bar\rho_g(\Frob_q)\in\mathcal C_g^+$ and $ q^{p-1}\not\equiv1\pmod{p^2}$. Let $\Omega_g$ be the set of primes $\ell\nmid N_gp$ such that $\bar\rho_g(\Frob_\ell)\in\mathcal C_g^-$. The determinant of $\bar\rho_g(\Frob_v)$ is the reduction of $v$ modulo $p$. Since the determinant of an element of either $\mathcal C_g^+$ or $\mathcal C_g^-$ is different from $\pm1$, every prime in $\Pi_g\cup\Omega_g$ satisfies $v\not\equiv\pm1\pmod p$. Thus the congruence restriction required by Theorem~\ref{thm:carayol-DT} is already built into the definitions. \begin{proposition}[Densities of the auxiliary primes] \label{prop:aux-density} Assume \ref{H:image}. The sets $\Pi_g$ and $\Omega_g$ are Frobenian, and their densities are \begin{equation}\label{eq:aux-densities} \delta(\Pi_g)=\frac{p-1}{p}\frac{|\mathcal C_g^+|}{|H_g|} \quad\text{and}\quad \delta(\Omega_g)=\frac{|\mathcal C_g^-|}{|H_g|}. \end{equation} In particular, both sets have positive density and are infinite. \end{proposition} \begin{proof} The set $\Omega_g$ is the Chebotarev set in the finite Galois extension $L_g/\Q$ associated with the union of conjugacy classes $\mathcal C_g^-$. Removing the finitely many primes that divide $N_gp$ does not change its density. The Chebotarev density theorem therefore gives $\delta(\Omega_g)=|\mathcal C_g^-|/|H_g|$. The additional congruence $ q^{p-1}\not\equiv1\pmod{p^2}$ in the definition of $\Pi_g$ requires us to adjoin the $p^2$-th roots of unity. Setting $M=\Q(\mu_{p^2})$, we find that both $L_g$ and $M$ contain $\Q(\mu_p)$. Hypothesis \ref{H:image} states that their intersection is $\Q(\mu_p)$. Consequently, the Galois group of the compositum can be identified with the fibered product \begin{equation}\label{eq:fiber-product} \Gal(L_gM/\Q) \simeq H_g\times_{\Fp^\times}(\Z/p^2\Z)^\times. \end{equation} Here the maps to $\Fp^\times$ are the determinant on $H_g$ and reduction modulo $p$ on $(\Z/p^2\Z)^\times$. Every element of $\Fp^\times$ has exactly $p$ lifts to $(\Z/p^2\Z)^\times$, so the group in \eqref{eq:fiber-product} has order $p|H_g|$. Fix $u\in\mathcal C_g^+$ and set $a=d(u)$. Among the $p$ elements of $(\Z/p^2\Z)^\times$ which reduce to $a$, exactly one has $(p-1)$-st power equal to $1$ modulo $p^2$. Indeed, reduction modulo $p$ induces an isomorphism from the subgroup of $(p-1)$-st roots of unity in $(\Z/p^2\Z)^\times$ onto $\Fp^\times$, and the unique lift in that subgroup is the Teichmuller lift of $a$. The remaining $p-1$ lifts have $(p-1)$-st power different from $1$ modulo $p^2$. It follows that the conjugacy-stable subset of $\Gal(L_gM/\Q)$ defining $\Pi_g$ has cardinality $(p-1)|\mathcal C_g^+|$. The Chebotarev density theorem therefore gives \[ \delta(\Pi_g) =\frac{(p-1)|\mathcal C_g^+|}{p|H_g|}. \] This proves \eqref{eq:aux-densities}. Positivity follows from the nonemptiness of $\mathcal C_g^+$ and $\mathcal C_g^-$ in hypothesis \ref{H:image}. \end{proof} If $v\nmid N_gp$, the characteristic polynomial of $\bar\rho_g(\Frob_v)$ is the reduction of $X^2-a_v(g)X+v$. Hence, for $q\in\Pi_g$, the factorization attached to $\mathcal C_g^+$ gives $a_q(g)\equiv1+q\pmod\varpi$. Likewise, if $\ell\in\Omega_g$, then $a_\ell(g)\equiv-(1+\ell)\pmod\varpi$. In either case, \eqref{eq:levelraising-trace} holds. Every prime in $\Pi_g\cup\Omega_g$ is therefore a level-raising prime. \subsection{Simultaneous level raising} We may now apply the preceding construction to any finite collection of auxiliary primes. \begin{proposition} \label{prop:level-raising} Let $Q\subset\Pi_g$ and $R\subset\Omega_g$ be finite sets. Under hypotheses \ref{H:image} and \ref{H:optimal}, there is a normalized newform $f$ of weight two and trivial nebentypus such that $\bar\rho_f\simeq\bar\rho_g$ and \begin{equation}\label{eq:simultaneous-raised-level} N_f=N_g\prod_{q\in Q}q\prod_{\ell\in R}\ell. \end{equation} Further, $f$ is new at every prime in $Q\cup R$. Its Steinberg sign is $+1$ at every $q\in Q$ and $-1$ at every $\ell\in R$. \end{proposition} \begin{proof} The two auxiliary sets are disjoint. Indeed, an element of $\mathcal C_g^+$ has trace $1+d$, while an element of $\mathcal C_g^-$ has trace $-(1+d)$; these values cannot be equal when $d\neq-1$. Thus $Q\cap R=\varnothing$. If both sets are empty, we may simply take $f=g$. Suppose otherwise and put $S=Q\cup R$. Every prime in $S$ is prime to $pN_g$, is not congruent to $\pm1$ modulo $p$, and satisfies the trace condition \eqref{eq:levelraising-trace}. Hypothesis \ref{H:optimal} identifies $N_g$ with $N(\bar\rho_g)$. Theorem~\ref{thm:carayol-DT} therefore produces a normalized newform $f$ of trivial nebentypus whose residual representation is isomorphic to $\bar\rho_g$ and whose level is the integer in \eqref{eq:simultaneous-raised-level}. The same theorem shows that $f$ is new at every prime in $S$. It remains to determine the local signs. Let $v\in S$, and let $\varepsilon_v\in\{\pm1\}$ be the Steinberg sign of $f$ at $v$. The residual Frobenius eigenvalues of a Steinberg representation of sign $\varepsilon_v$ are $\{\varepsilon_v,\varepsilon_vv\}$, and hence its residual trace is $\varepsilon_v(1+v)$. If $q\in Q$, the definition of $\mathcal C_g^+$ gives residual trace $1+q$. Since $q\not\equiv-1\pmod p$, the element $1+q$ is nonzero in $\mathbf k$, and therefore $\varepsilon_q=+1$. If $\ell\in R$, the definition of $\mathcal C_g^-$ gives residual trace $-(1+\ell)$, and the same argument gives $\varepsilon_\ell=-1$. \end{proof} \begin{lemma}[Preservation of non-ordinarity] \label{lem:nonordinary-preserved} The newform $f$ furnished by Proposition~\ref{prop:level-raising} is non-ordinary at $p$. \end{lemma} \begin{proof} After enlarging the coefficient field if necessary, choose stable lattices for $f$ and $g$ whose reductions realize the fixed isomorphism $\bar\rho_f\simeq\bar\rho_g$. Restricting this isomorphism to a decomposition group at $p$ gives \begin{equation}\label{eq:local-residual-isomorphism-at-p} \bar\rho_f|_{G_{\Q_p}}\simeq\bar\rho_g|_{G_{\Q_p}}. \end{equation} Since $g$ has weight two, level prime to $p$, and is non-ordinary, its $p$-th Fourier coefficient is zero modulo $\varpi$. The local description of the residual representation in the Fontaine--Laffaille range shows that $\bar\rho_g|_{G_{\Q_p}}$ is of niveau two and is irreducible; see \cite[Theorem~2.6]{Edixhoven1992}. More explicitly, after extending scalars to an algebraic closure of the residue field, the semisimplification of its restriction to inertia has characters $\omega_2$ and $\omega_2^p$, where $\omega_2$ is a fundamental character of niveau two. These two characters are interchanged by Frobenius, so neither inertia eigenspace is stable under the full group $G_{\Q_p}$. This is precisely the irreducible niveau-two case. Suppose, to the contrary, that $f$ were ordinary at $p$. The $p$-adic representation attached to an ordinary weight-two form has a $G_{\Q_p}$-stable one-dimensional subspace and an unramified one-dimensional quotient. This gives a rank-one direct summand whose reduction modulo $\varpi$ is a nonzero proper $G_{\Q_p}$-stable subspace. Thus the residual local representation of $f$ would be reducible. This contradicts \eqref{eq:local-residual-isomorphism-at-p} and the irreducibility of the residual local representation of $g$. Hence $f$ is non-ordinary at $p$. \end{proof} \section{The local correction terms and proof of the main theorem} \label{sec:local} Let $h$ be a weight-two newform and let $\ell\neq p$. With respect to the notation of \cite[Section~5]{HatleyLei2019}, set \begin{equation}\label{eq:local-polynomial-def} P_{\ell,h}(X) =\det\left(1-\Frob_\ell X\mid V_h^{I_\ell}\right)\in\cO[X] \end{equation} and write $\widetilde P_{\ell,h}(X)$ for its reduction modulo $\varpi$. Let $d_{\ell,h}$ be the multiplicity of $X=\ell^{-1}$ as a root of $\widetilde P_{\ell,h}(X)$. If $r_\ell$ denotes the number of primes of $\Q_\infty$ above $\ell$, then Proposition~5.1 and Corollary~5.2 of \cite{HatleyLei2019} give \begin{equation}\label{eq:delta-rd} \delta_{\ell,h}=r_\ell d_{\ell,h}. \end{equation} Indeed, the local $\lambda$-invariant at each prime $v\mid\ell$ is $d_{\ell,h}$, and there are $r_\ell$ such primes. Let $q\in\Pi_g$. Since $q\nmid N_gp$, the representation $V_g$ is unramified at $q$. The residual Frobenius eigenvalues are $1$ and $q$, hence \begin{equation}\label{eq:local-Pi-g} \widetilde P_{q,g}(X)=(1-X)(1-qX). \end{equation} Note that $X=q^{-1}$ is a root of the second factor. It is not a root of the first factor because $q\not\equiv1\pmod p$, and thus \begin{equation}\label{eq:d-Pi-g} d_{q,g}=1. \end{equation} Let $f$ be the form given by Proposition~\ref{prop:level-raising}. Since $f$ is new of exponent one at $q$, its local automorphic representation is Steinberg up to an unramified twist. Consequently $V_f^{I_q}$ is one-dimensional. The positive sign in Proposition~\ref{prop:level-raising} gives \begin{equation}\label{eq:local-Pi-f} \widetilde P_{q,f}(X)=1-X. \end{equation} At $X=q^{-1}$ this is nonzero because $q\not\equiv1\pmod p$, and hence \begin{equation}\label{eq:d-Pi-f} d_{q,f}=0. \end{equation} The factor $r_q$ is controlled by the additional congruence modulo $p^2$. We spell this out. The cyclotomic character gives an identification $\Gamma\simeq1+p\Zp$. The decomposition subgroup of a prime $q\neq p$ is the closed subgroup generated by the pro-$p$ part of $q$. Equivalently it is generated by $q^{p-1}\in1+p\Zp$. The condition \[ q^{p-1}\not\equiv1\pmod{p^2} \] is equivalent to $v_p(q^{p-1}-1)=1$, and an element of $1+p\Zp$ with this property is a topological generator. Hence the decomposition subgroup is all of $\Gamma$, and therefore \begin{equation}\label{eq:r-q-one} r_q=[\Gamma:\Gamma_q]=1. \end{equation} Combining \eqref{eq:delta-rd}, \eqref{eq:d-Pi-g}, \eqref{eq:d-Pi-f} and \eqref{eq:r-q-one} yields \begin{equation}\label{eq:Pi-correction} \delta_{q,g}-\delta_{q,f}=1. \end{equation} Now let $\ell\in\Omega_g$. The residual Frobenius eigenvalues of $g$ are $-1$ and $-\ell$, so \begin{equation}\label{eq:local-Omega-g} \widetilde P_{\ell,g}(X)=(1+X)(1+\ell X). \end{equation} At $X=\ell^{-1}$ the two factors are $1+\ell^{-1}$ and $2$, both nonzero because $p\geq5$ and $\ell\not\equiv-1\pmod p$. Therefore $d_{\ell,g}=0$. The level-raised form has negative Steinberg sign and \begin{equation}\label{eq:local-Omega-f} \widetilde P_{\ell,f}(X)=1+X, \end{equation} which is again nonzero at $X=\ell^{-1}$. Hence $d_{\ell,f}=0$, and \eqref{eq:delta-rd} gives \begin{equation}\label{eq:Omega-correction} \delta_{\ell,g}-\delta_{\ell,f}=0 \end{equation} without any condition on the number of primes above $\ell$ in $\Q_\infty$. \begin{lemma} \label{lem:old-prime-lattice} Assume that $h$ is congruent to $g$ and let $\ell\neq p$ be a prime such that the exponent of $\ell$ in the level of $h$ equals the exponent of $\ell$ in the Artin conductor of $\bar\rho_g$. Setting $\bar T_h:=T_h/\varpi T_h$, we find that the natural inclusion map \begin{equation}\label{eq:invariants-inclusion} T_h^{I_\ell}/\varpi T_h^{I_\ell} \longrightarrow (\bar T_h)^{I_\ell} \end{equation} is an isomorphism. Consequently \begin{equation}\label{eq:old-euler-reduction} \widetilde P_{\ell,h}(X) =\det\left(1-\Frob_\ell X\mid(\bar T_h)^{I_\ell}\right). \end{equation} \end{lemma} \begin{proof} This is precisely the argument of \cite[Lemma~4.8]{Ray2024}, applied to the inertia-invariant lattice and its Frobenius characteristic polynomial. \end{proof} \begin{lemma}\label{lem:old-prime-cancellation} Let $f$ be as in Proposition~\ref{prop:level-raising} and let $\ell\mid N_g$. Then, we have that \begin{enumerate} \item $\widetilde P_{\ell,f}(X)=\widetilde P_{\ell,g}(X)$, \item $d_{\ell,f}=d_{\ell,g}$, \item $\delta_{\ell,f}=\delta_{\ell,g}$. \end{enumerate} \end{lemma} \begin{proof} The forms $f$ and $g$ have the same $\ell$-adic level exponent, which equals the residual Artin-conductor exponent by Hypothesis~\ref{H:optimal}. Lemma~\ref{lem:old-prime-lattice}, together with $\bar T_f\simeq\bar T_g$, therefore gives $\widetilde P_{\ell,f}(X)=\widetilde P_{\ell,g}(X)$. Equality of the multiplicities at $X=\widetilde\ell^{-1}$ gives $d_{\ell,f}=d_{\ell,g}$, and then \eqref{eq:delta-rd} gives $\delta_{\ell,f}=\delta_{\ell,g}$. \end{proof} \begin{proposition} \label{prop:local-variation} Let $f$ be as in Proposition~\ref{prop:level-raising}. Then the following assertions hold: \begin{enumerate}[label=(\roman*)] \item if $q\in Q\subset\Pi_g$, then $\delta_{q,g}-\delta_{q,f}=1$; \item if $\ell\in R\subset\Omega_g$, then $\delta_{\ell,g}-\delta_{\ell,f}=0$; \item if $\ell\mid N_g$, then $\delta_{\ell,g}=\delta_{\ell,f}$; \item at every other tame prime the two reduced local Euler polynomials agree, and hence there is no contribution to the transition formula. \end{enumerate} \end{proposition} \begin{proof} Assertions (i) and (ii) are \eqref{eq:Pi-correction} and \eqref{eq:Omega-correction}. Assertion (iii) is Lemma~\ref{lem:old-prime-cancellation}. Finally, if $\ell\nmid pN_f$, both characteristic-zero representations are unramified at $\ell$ and the congruence $\bar\rho_f\simeq\bar\rho_g$ identifies the reduced Frobenius polynomials. Thus $d_{\ell,f}=d_{\ell,g}$ and the corresponding term is zero. \end{proof} We can now prove the main theorem. \begin{proof}[Proof of Theorem~\ref{thm:main}] Choose finite disjoint sets $Q\subset\Pi_g$ and $R\subset\Omega_g$. Proposition~\ref{prop:level-raising} produces a newform $f$ of the asserted level with $\bar\rho_f\simeq\bar\rho_g$. By Lemma~\ref{lem:nonordinary-preserved}, the form $f$ is again non-ordinary at $p$. The hypotheses needed for the signed congruence results hold for $f$ and $g$: \textup{(irred)} and \textup{(Cong)} follow from \ref{H:image} and $\bar\rho_f\simeq\bar\rho_g$, \textup{(BLZ)} follows from non-ordinarity in weight two, and \textup{(inv)} follows from \cite[Lemma~4.4]{Lei2011} since $2\leq p$. Fix a signed label $\natural\in\{\sharp,\flat\}$. Proposition~\ref{prop:one-sided} implies that $X^\natural(f)$ is torsion and $\mu^\natural(f)=0$. Let $\Sigma$ contain $p$, $\infty$, and every prime dividing $N_f$, and put $\Sigma_0=\Sigma\setminus\{p,\infty\}$. Proposition~\ref{prop:signed-congruence} then gives \[ \lambda^\natural(f)-\lambda^\natural(g) = \sum_{\ell\in\Sigma_0} \bigl(\delta_{\ell,g}-\delta_{\ell,f}\bigr). \] By Proposition~\ref{prop:local-variation}, every prime of $Q$ contributes one, every prime of $R$ contributes zero, and the contributions at the old primes cancel. The right-hand side is therefore $|Q|$. The calculation is independent of $\natural$, and hence it holds simultaneously for $\sharp$ and $\flat$. \end{proof} \begin{proof}[Proof of Corollary~\ref{cor:realization}] Fix $n\geq0$. Choose a set $Q\subset\Pi_g$ with $|Q|=n$. If $n>0$, there are already infinitely many possible choices for $Q$. If $n=0$, take $Q=\varnothing$ and vary finite nonempty sets $R\subset\Omega_g$. Since both auxiliary sets are infinite, this gives infinitely many distinct tame levels. The result then follows from Theorem~\ref{thm:main}. \end{proof} \section{Quantitative and probabilistic realization} \label{sec:quantitative} Throughout this section we retain the hypotheses and notation of Theorem~\ref{thm:main}. Thus $g$ is a weight-two newform which is non-ordinary at $p$, both $X^\sharp(g)$ and $X^\flat(g)$ are torsion over the cyclotomic Iwasawa algebra, and $\mu^\sharp(g)=\mu^\flat(g)=0$. Recall also that a prime in $\Pi_g$ contributes one to each signed $\lambda$-invariant, whereas a prime in $\Omega_g$ changes the exact tame level without changing either signed $\lambda$-invariant. Write $\delta_\Pi$ and $\delta_\Omega$ for the positive densities of $\Pi_g$ and $\Omega_g$, respectively, as in Proposition~\ref{prop:aux-density}. Thus \[ \delta_\Pi = \frac{p-1}{p}\frac{|\mathcal C_g^+|}{|H_g|} \qquad\text{and}\qquad \delta_\Omega = \frac{|\mathcal C_g^-|}{|H_g|}. \] When $\mathbf{k}=\mathbf F_p$ and $H_g=\operatorname{GL}_2(\mathbf F_p)$, these specialize to \[ \delta_\Pi=\frac{p-3}{p(p-1)}, \qquad \delta_\Omega=\frac{p-3}{(p-1)^2}. \] Since the two sets of primes are disjoint, an admissible integer has a unique factorization $D=D_\Pi D_\Omega$, where $D_\Pi$ is supported on $\Pi_g$ and $D_\Omega$ is supported on $\Omega_g$. Put \[ \omega_\Pi(D)=\#\{q:q\mid D_\Pi\}. \] For every admissible $D$, choose one newform $f_D$ supplied by Theorem~\ref{thm:main}, using the prime divisors of $D_\Pi$ as the set $Q$ and the prime divisors of $D_\Omega$ as the set $R$. The next proposition records the arithmetic content which will be counted below. \begin{proposition} \label{prop:iwasawa-family} For every admissible $D$, the form $f_D$ is a normalized weight-two newform of trivial nebentypus and exact level $N_gD$. It is non-ordinary at $p$ and satisfies $\bar\rho_{f_D}\simeq\bar\rho_g$. Moreover, for each $\natural\in\{\sharp,\flat\}$, the signed Selmer dual $X^\natural(f_D)$ is torsion over the cyclotomic Iwasawa algebra, \begin{equation}\label{eq:iwasawa-family} \mu^\natural(f_D)=0 \quad\text{and}\quad \lambda^\natural(f_D) =\lambda^\natural(g)+\omega_\Pi(D). \end{equation} In particular, \begin{equation}\label{eq:signed-difference-rigid-family} \lambda^\sharp(f_D)-\lambda^\flat(f_D) = \lambda^\sharp(g)-\lambda^\flat(g) \end{equation} for every admissible $D$. \end{proposition} \begin{proof} Apply Proposition~\ref{prop:level-raising} with $Q$ and $R$ equal to the sets of prime divisors of $D_\Pi$ and $D_\Omega$, respectively. This gives all the assertions concerning $f_D$. Theorem~\ref{thm:main} then gives, for each $\natural\in\{\sharp,\flat\}$, \[\mu^\natural(f_D)=0\] and \[ \lambda^\natural(f_D) =\lambda^\natural(g)+|Q| =\lambda^\natural(g)+\omega_\Pi(D). \] Subtracting the formulas for $\sharp$ and $\flat$ proves \eqref{eq:signed-difference-rigid-family}. \end{proof} We next recall the analytic input in the form needed here. Recall that a set of rational primes $\mathcal P$ is called Frobenian if there exists a finite Galois extension $L/\mathbb Q$ and a union $C$ of conjugacy classes in $\operatorname{Gal}(L/\mathbb Q)$ such that, apart from finitely many primes, a prime $p$ belongs to $\mathcal P$ precisely when the Frobenius conjugacy class $\operatorname{Frob}_p$ lies in $C$. \begin{lemma} \label{lem:frobenian-prime-sum} Let $\mathcal P$ be a Frobenian set of density $\delta$. There is a constant $c>0$ and a function $G_{\mathcal P}(s)$, holomorphic in the dented zero-free region \[ \mathcal R_c= \left\{s=\sigma+it: \sigma\geq1-\frac{c}{1+\log(2+|t|)}\right\}\setminus(-\infty,1], \] and continuous at $1$, such that \begin{equation}\label{eq:frobenian-prime-sum} \sum_{\ell\in\mathcal P}\ell^{-s} = \delta\log\frac{1}{s-1}+G_{\mathcal P}(s). \end{equation} The constant $c$ may be chosen so that $\exp(G_{\mathcal P}(s))$ has at most polynomial growth in $|t|$ on $\mathcal R_c$. In particular, $\sum_{\ell\leq Y,\,\ell\in\mathcal P}\ell^{-1} =\delta\log\log Y+O_{\mathcal P}(1)$. \end{lemma} \begin{proof} This is the Frobenian Dirichlet-series theorem of Serre \cite{Serre1981}, together with the standard zero-free region for the finite collection of Artin--Hecke $L$-functions occurring in its proof. Brauer induction reduces the required continuation and growth bound to Hecke $L$-functions. Since the extension defining $\mathcal P$ is fixed, the region may be chosen uniformly for these finitely many factors. \end{proof} We define for $z\in \mathbb C$ and $\Re(s)>1$, \begin{equation}\label{eq:marked-euler-product} F(s,z) = \prod_{\ell\in\Omega_g}(1+\ell^{-s}) \prod_{q\in\Pi_g}(1+zq^{-s}). \end{equation} Expanding the product gives \begin{equation}\label{eq:marked-dirichlet-series} F(s,z) = \sum_{D\ \mathrm{admissible}} \frac{z^{\omega_\Pi(D)}}{D^s}. \end{equation} We set $\alpha(z):=\delta_\Omega+z\delta_\Pi$. \begin{lemma} \label{lem:SD-factorization} There is an open set of $z$-values containing the closed interval $[0,1]$ and a constant $c>0$ such that \begin{equation}\label{eq:SD-factorization} F(s,z)=(s-1)^{-\alpha(z)}H(s,z), \end{equation} where $H(s,z)$ is holomorphic in both variables for $s\in\mathcal R_c$. For every compact set $K$ of $z$-values in this open set, $H(s,z)$ has at most polynomial growth in $|\Im(s)|$, uniformly for $z\in K$. Moreover the open set can be chosen so that $H(1,z)$ is nonzero there. Moreover, $H(1,x)>0$ for $0\leq x\leq1$. \end{lemma} \begin{proof} For $\Re(s)>1$, the expansion $\log(1+w)=w+O(w^2)$ gives \[ \log F(s,z) = \sum_{\ell\in\Omega_g}\ell^{-s} +z\sum_{q\in\Pi_g}q^{-s}+R(s,z), \] where $R(s,z)$ is holomorphic for $\Re(s)>1/2$ and locally uniformly holomorphic in $z$. Lemma~\ref{lem:frobenian-prime-sum} identifies the singular part with $\alpha(z)\log(1/(s-1))$. After shrinking $c$ if necessary, exponentiating the remaining holomorphic terms gives \eqref{eq:SD-factorization} throughout $\mathcal R_c$, with the stated polynomial growth uniformly on compact sets of $z$-values. For real $s>1$ and real $x\geq0$, all Euler factors in $F(s,x)$ are positive. Taking $s\to1^+$ proves positivity of the resulting nonzero limiting factor. \end{proof} For $Y\geq2$, write \[ S(Y,z)= \sum_{\substack{D\leq Y\\D\ \mathrm{admissible}}} z^{\omega_\Pi(D)}. \] The Selberg--Delange theorem allows us to deduce an asymptotic formula for $S(Y,z)$ from the behavior of $F(s,z)$ near $s=1$. \begin{proposition} \label{prop:uniform-SD} Let $K$ be a compact set of $z$-values contained in the open set from Lemma~\ref{lem:SD-factorization}, and suppose that $\inf_{z\in K}\Re\alpha(z)>0$. Then, uniformly for $z\in K$, \begin{equation}\label{eq:uniform-SD} S(Y,z) = Y(\log Y)^{\alpha(z)-1} \left( \frac{H(1,z)}{\Gamma(\alpha(z))} +O_K\left(\frac{1}{\log Y}\right) \right). \end{equation} On a slightly smaller compact set, this estimate may be differentiated a fixed number of times with respect to $z$. \end{proposition} \begin{proof} Put \[ G(s,z)=F(s,z)\zeta(s)^{-\alpha(z)}. \] Since $(s-1)\zeta(s)$ is holomorphic and nonzero in a sufficiently small region of the form $\mathcal R_c$, Lemma~\ref{lem:SD-factorization} shows that $G(s,z)$ is holomorphic there and has at most polynomial growth, uniformly for $z\in K$. If $A=\max(1,\sup_{z\in K}|z|)$, then the coefficients of $F(s,z)$ are bounded in absolute value by the nonnegative coefficients of $F(s,A)$. Thus the type hypotheses in the uniform Selberg--Delange theorem are satisfied uniformly for $z\in K$. Theorem~II.5.2 of \cite[Chapter~II.5]{Tenenbaum2015} gives \eqref{eq:uniform-SD}. Applying the same uniform estimate on a slightly larger compact set and using Cauchy's integral formula gives the asserted fixed number of $z$-derivatives. \end{proof} For a fixed integer $n\geq0$, let \[ \mathscr D_n(Y) = \{D\leq Y:D\text{ is admissible and }\omega_\Pi(D)=n\}, \] and let $\mathscr F_n(X)$ be the family consisting of the chosen forms $f_D$ with $D\in\mathscr D_n(X/N_g)$. Thus every member of $\mathscr F_n(X)$ has level at most $X$. \begin{theorem} \label{thm:quantitative} For every fixed $n\geq0$, \begin{equation}\label{eq:Dn-asymptotic} \#\mathscr D_n(Y) \sim C_{g,n}Y(\log Y)^{\delta_\Omega-1}(\log\log Y)^n, \end{equation} where \begin{equation}\label{eq:Cgn} C_{g,n} = \frac{H(1,0)}{\Gamma(\delta_\Omega)} \frac{\delta_\Pi^n}{n!}>0. \end{equation} Consequently, \begin{equation}\label{eq:Fn-asymptotic} \#\mathscr F_n(X) \sim \frac{C_{g,n}}{N_g} X(\log X)^{\delta_\Omega-1}(\log\log X)^n. \end{equation} Every $f\in\mathscr F_n(X)$ is non-ordinary at $p$, satisfies $\bar\rho_f\simeq\bar\rho_g$, and has torsion signed Selmer duals with \begin{equation}\label{eq:quantitative-iwasawa-conclusion} \mu^\sharp(f)=\mu^\flat(f)=0 \quad \text{and}\quad (\lambda^\sharp(f),\lambda^\flat(f)) = (\lambda^\sharp(g)+n,\lambda^\flat(g)+n). \end{equation} \end{theorem} \begin{proof} For a power series $F(z)$, we write $[z^m]F(z)$ for the coefficient of $z^m$ in its expansion. By definition, the coefficient of $z^n$ in $S(Y,z)$ counts precisely those admissible integers having exactly $n$ prime divisors in $\Pi_g$. Thus \[ [z^n]S(Y,z)=\#\mathscr D_n(Y). \] We may therefore recover the required asymptotic by extracting the coefficient of $z^n$ from the uniform Selberg--Delange estimate \eqref{eq:uniform-SD}. Choose $\rho>0$ sufficiently small that $\rho\delta_\Pi<\min\{\delta_\Omega,1\}$. The first inequality ensures that $\Re(\delta_\Omega+z\delta_\Pi)>0$ throughout the closed disc $|z|\leq\rho$, so Proposition~\ref{prop:uniform-SD} applies uniformly on this disc. Put \[ B(z)=\frac{H(1,z)} {\Gamma(\delta_\Omega+z\delta_\Pi)}. \] This is holomorphic near the origin, and the Selberg--Delange estimate takes the form \[ S(Y,z) = Y(\log Y)^{\delta_\Omega-1} e^{z\delta_\Pi\log\log Y}B(z)+E(Y,z), \] where, uniformly for $|z|=\rho$, \[ E(Y,z) \ll_\rho Y(\log Y)^{\delta_\Omega-2+\rho\delta_\Pi}. \] The additional factor $(\log Y)^{\rho\delta_\Pi}$ in this bound comes from taking the maximum of $|(\log Y)^{z\delta_\Pi}|$ on the circle $|z|=\rho$. Let $L=\log\log Y$ and write $B(z)=\sum_{j\geq0}b_jz^j$. Since \[ e^{z\delta_\Pi L} = \sum_{m\geq0}\frac{(\delta_\Pi L)^m}{m!}z^m, \] the coefficient of $z^n$ in $B(z)e^{z\delta_\Pi L}$ is \[ \sum_{j=0}^n b_j\frac{(\delta_\Pi L)^{n-j}}{(n-j)!}. \] Here $n$ is fixed. The term with $j=0$ is the only term containing $L^n$; all the remaining terms contain at most $L^{n-1}$. Consequently, \[ [z^n]\bigl(B(z)e^{z\delta_\Pi L}\bigr) = B(0)\frac{\delta_\Pi^n}{n!}L^n +O_{g,n}(L^{n-1}). \] It remains to verify that the error term remains negligible after coefficient extraction. By Cauchy's coefficient formula, \[ |[z^n]E(Y,z)| \leq \rho^{-n}\max_{|z|=\rho}|E(Y,z)| \ll_{\rho,n} Y(\log Y)^{\delta_\Omega-2+\rho\delta_\Pi}. \] Relative to $Y(\log Y)^{\delta_\Omega-1}(\log\log Y)^n$, this is bounded by a constant multiple of \[ \frac{(\log Y)^{-1+\rho\delta_\Pi}} {(\log\log Y)^n}, \] which tends to zero because $\rho\delta_\Pi<1$. We therefore obtain \[ \#\mathscr D_n(Y) \sim B(0)\frac{\delta_\Pi^n}{n!} Y(\log Y)^{\delta_\Omega-1}(\log\log Y)^n. \] Finally, \[ B(0)=\frac{H(1,0)}{\Gamma(\delta_\Omega)}>0, \] so this is precisely \eqref{eq:Dn-asymptotic}, with the constant given in \eqref{eq:Cgn}. To pass from admissible integers to modular forms, take $Y=X/N_g$. The form $f_D$ has exact level $N_gD$, so two different admissible integers give forms of different exact levels. Hence \[ \#\mathscr F_n(X)=\#\mathscr D_n(X/N_g). \] Since $N_g$ is fixed, replacing $Y$ by $X/N_g$ does not change the powers of $\log X$ or $\log\log X$ in the asymptotic. This proves \eqref{eq:Fn-asymptotic}. The assertion \eqref{eq:quantitative-iwasawa-conclusion} now follows directly from Proposition~\ref{prop:iwasawa-family}. \end{proof} We now allow the number of primes from $\Pi_g$ to vary. Let $\mathscr D(Y)$ denote the set of all admissible integers $D\leq Y$, and consider the corresponding family \[ \mathscr F(Y)=\{f_D:D\in\mathscr D(Y)\}. \] Since $f_D$ has exact level $N_gD$, different values of $D$ give different members of $\mathscr F(Y)$. In particular, $\#\mathscr F(Y)=\#\mathscr D(Y)$. We regard $\mathscr F(Y)$ as a finite probability space by giving each of its members equal weight. Thus, if $\mathscr A\subseteq\mathscr F(Y)$, then \[ \mathbb P_Y(\mathscr A) = \frac{\#\mathscr A}{\#\mathscr F(Y)}. \] If $X:\mathscr F(Y)\rightarrow\mathbb R$ is a real-valued function, we define its expectation and variance by \[ \mathbb E_Y[X] = \frac{1}{\#\mathscr F(Y)} \sum_{f\in\mathscr F(Y)}X(f) \] and \[ \operatorname{Var}_Y(X) = \frac{1}{\#\mathscr F(Y)} \sum_{f\in\mathscr F(Y)} \bigl(X(f)-\mathbb E_Y[X]\bigr)^2. \] Equivalently, $\operatorname{Var}_Y(X)=\mathbb E_Y[X^2]-\mathbb E_Y[X]^2$. For $\natural\in\{\sharp,\flat\}$, define the signed increment by \[ \Delta^\natural(f_D) = \lambda^\natural(f_D)-\lambda^\natural(g). \] Proposition~\ref{prop:iwasawa-family} gives the pointwise identity \begin{equation}\label{eq:increment-identity} \Delta^\sharp(f_D) = \Delta^\flat(f_D) = \omega_\Pi(D). \end{equation} Thus the variation of either signed $\lambda$-invariant is governed by the elementary arithmetic function $\omega_\Pi(D)$. The probabilistic statements below are consequently distribution theorems for the signed Iwasawa invariants in the family $\mathscr F(Y)$. We first record the size of the underlying family. Setting $z=1$ in Proposition~\ref{prop:uniform-SD} removes the weight which records the number of prime divisors in $\Pi_g$. We obtain \begin{equation}\label{eq:total-admissible} \#\mathscr F(Y) = \#\mathscr D(Y) \sim \frac{H(1,1)} {\Gamma(\delta_\Pi+\delta_\Omega)} Y(\log Y)^{\delta_\Pi+\delta_\Omega-1}. \end{equation} \begin{proposition} \label{prop:mod-poisson} There is a function \[ \Phi_g(z) = \frac{H(1,z)}{H(1,1)} \frac{\Gamma(\delta_\Pi+\delta_\Omega)} {\Gamma(\delta_\Omega+z\delta_\Pi)}, \] which is holomorphic and nonzero in a neighborhood of $z=1$ and satisfies $\Phi_g(1)=1$, such that, locally uniformly for $z$ near $1$ and for either signed label $\natural$, \begin{equation}\label{eq:mod-poisson} \frac{1}{\#\mathscr F(Y)} \sum_{f\in\mathscr F(Y)}z^{\Delta^\natural(f)} = \Phi_g(z) \exp\!\bigl(\delta_\Pi(z-1)\log\log Y\bigr) \left( 1+O_g\left(\frac{1}{\log Y}\right) \right). \end{equation} The error term may be differentiated twice with respect to $z$ on a neighborhood of $1$. \end{proposition} \begin{proof} By \eqref{eq:increment-identity}, the numerator on the left-hand side of \eqref{eq:mod-poisson} is \[ \sum_{D\in\mathscr D(Y)}z^{\omega_\Pi(D)} = S(Y,z). \] The denominator is $S(Y,1)$. Choose a closed disc centered at $1$ on which $\Re(\delta_\Omega+z\delta_\Pi)>0$. Proposition~\ref{prop:uniform-SD} applies uniformly on this disc and gives \[ S(Y,z) = Y(\log Y)^{\delta_\Omega+z\delta_\Pi-1} \left( \frac{H(1,z)} {\Gamma(\delta_\Omega+z\delta_\Pi)} +O_g\left(\frac{1}{\log Y}\right) \right). \] At $z=1$, the same formula gives \eqref{eq:total-admissible}. Dividing the two asymptotic formulae, and using the positivity of $H(1,1)$, we find that \[ \frac{S(Y,z)}{S(Y,1)} = \frac{H(1,z)}{H(1,1)} \frac{\Gamma(\delta_\Pi+\delta_\Omega)} {\Gamma(\delta_\Omega+z\delta_\Pi)} (\log Y)^{\delta_\Pi(z-1)} \left( 1+O_g\left(\frac{1}{\log Y}\right) \right). \] Since \[ (\log Y)^{\delta_\Pi(z-1)} = \exp\!\bigl(\delta_\Pi(z-1)\log\log Y\bigr), \] this is precisely \eqref{eq:mod-poisson}. The function $\Phi_g$ is holomorphic near $1$. It is also nonzero after the neighborhood is made sufficiently small, since $H(1,1)>0$ and the Gamma function is finite and nonzero at $\delta_\Pi+\delta_\Omega>0$. Finally, the Selberg--Delange estimate is uniform and holomorphic in $z$. Cauchy's integral formula therefore allows its error term to be differentiated twice on a slightly smaller disc. \end{proof} \begin{theorem} \label{thm:levy-continuity} Let $(Y_m)_{m\geq1}$ be a sequence tending to infinity, and let \[ X_m:\mathscr F(Y_m)\longrightarrow\mathbb R \] be a sequence of real-valued functions. Suppose that, for every $t\in\mathbb R$, \[ \frac{1}{\#\mathscr F(Y_m)} \sum_{f\in\mathscr F(Y_m)}e^{itX_m(f)} \longrightarrow e^{-t^2/2}. \] Then, for every $x\in\mathbb R$, \[ \frac{1}{\#\mathscr F(Y_m)} \# \{f\in\mathscr F(Y_m):X_m(f)\leq x\} \longrightarrow \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{x}e^{-u^2/2}\,du. \] \end{theorem} \begin{proof} Let \[ \nu_m = \frac{1}{\#\mathscr F(Y_m)} \sum_{f\in\mathscr F(Y_m)}\delta_{X_m(f)} \] be the probability distribution of $X_m$. Its characteristic function is the expression on the left-hand side of the hypothesis. Since this converges pointwise to $e^{-t^2/2}$, L\'evy's continuity theorem \cite[Theorem~26.3, p.~349]{Billingsley1995} shows that $\nu_m$ converges weakly to the standard normal distribution and the asserted formula follows. \end{proof} \begin{proof}[Proof of Theorem \ref{thm:erdos-kac}] We set $L_Y=\delta_\Pi\log\log Y$ and define \[Z_Y = \frac{\Delta^\natural-L_Y}{\sqrt{L_Y}}. \] Since $\delta_\Pi>0$, we have $L_Y\to\infty$. We shall prove the limiting distribution by showing that the characteristic functions of the variables $Z_Y$ converge to that of a standard Gaussian. Fix $t\in\mathbb R$ and set \[ z_Y=\exp\!\left(\frac{it}{\sqrt{L_Y}}\right). \] Then $z_Y\to1$, and hence Proposition~\ref{prop:mod-poisson} applies for all sufficiently large $Y$. We find that $z_Y^{\Delta^\natural} =\exp(it\Delta^\natural/\sqrt{L_Y})$. We arrive at \[ \mathbb E_Y[e^{itZ_Y}] = \Phi_g(z_Y) \exp\!\left( L_Y\left( z_Y-1-\frac{it}{\sqrt{L_Y}} \right) \right) (1+o(1)). \] The first factor tends to one because $\Phi_g$ is continuous at $1$ and $\Phi_g(1)=1$. On the other hand, Taylor's formula gives \[ z_Y = 1+\frac{it}{\sqrt{L_Y}} -\frac{t^2}{2L_Y} +O_t(L_Y^{-3/2}). \] It follows that \[ L_Y\left( z_Y-1-\frac{it}{\sqrt{L_Y}} \right) = -\frac{t^2}{2}+O_t(L_Y^{-1/2}). \] Consequently, we find that \[ \lim_{Y\rightarrow \infty} \mathbb E_Y[e^{itZ_Y}] = e^{-t^2/2}. \] The function $e^{-t^2/2}$ is the characteristic function of the standard normal distribution. Theorem \ref{thm:levy-continuity} now gives \eqref{eq:EK-limit}. It remains to prove \eqref{eq:EK-mean} and \eqref{eq:EK-variance}. We do this by computing the first two moments. Let \[ G_Y(z)=\mathbb E_Y[z^{\Delta^\natural}] \] be the probability generating function of the signed increment. Taking logarithms in \eqref{eq:mod-poisson} gives, locally uniformly near $z=1$, \[ \log G_Y(z) = L_Y(z-1)+\log\Phi_g(z) +O_g\left(\frac{1}{\log Y}\right). \] The differentiated assertion in Proposition~\ref{prop:mod-poisson} allows us to differentiate this identity twice at $z=1$. Since $G_Y(1)=1$, we have \[ \mathbb E_Y[\Delta^\natural] = G_Y'(1) = (\log G_Y)'(1) = L_Y+(\log\Phi_g)'(1) +O_g\left(\frac{1}{\log Y}\right). \] This proves \eqref{eq:EK-mean}. For the variance, the usual identities for a probability generating function give \[ \operatorname{Var}_Y(\Delta^\natural) = G_Y''(1)+G_Y'(1)-G_Y'(1)^2 = (\log G_Y)''(1)+(\log G_Y)'(1). \] Differentiating the logarithmic asymptotic once more, we obtain \[ \operatorname{Var}_Y(\Delta^\natural) = L_Y +(\log\Phi_g)'(1) +(\log\Phi_g)''(1) +O_g\left(\frac{1}{\log Y}\right), \] which proves \eqref{eq:EK-variance}. Finally, \eqref{eq:increment-identity} shows that the two signed increments agree for every $D$, rather than merely having the same limiting distribution. Subtracting the two identities gives \[ \lambda^\sharp(f_D)-\lambda^\flat(f_D) = \lambda^\sharp(g)-\lambda^\flat(g); \] see \eqref{eq:signed-difference-rigid-family}. This completes the proof. \end{proof} \printbibliography \end{document}