\documentclass[11pt]{article} \usepackage[T1]{fontenc} \usepackage[utf8]{inputenc} \usepackage{lmodern} \usepackage[a4paper,margin=28mm]{geometry} \usepackage{amsmath,amssymb,amsthm,mathtools} \usepackage{enumitem,booktabs,array,microtype} \usepackage{tikz-cd} \usepackage{xcolor} \usepackage[unicode,pdfencoding=auto,psdextra,hyperfootnotes=false]{hyperref} \usepackage[nameinlink,capitalise,noabbrev]{cleveref} \hypersetup{colorlinks=true,linkcolor=blue,citecolor=blue, urlcolor=blue, pdftitle={A note of refinements to an algebra of infinite little finitistic dimension}, pdfauthor={Qiyue Tang},pdfsubject={A finite-dimensional algebra of infinite little finitistic dimension}} \urlstyle{same} \pdfgentounicode=1 \pdfinfoomitdate=1 \pdftrailerid{} \pdfsuppressptexinfo=15 \newtheorem{theorem}{Theorem}[section] \numberwithin{equation}{section} \newtheorem{proposition}[theorem]{Proposition} \newtheorem{lemma}[theorem]{Lemma} \newtheorem{corollary}[theorem]{Corollary} \theoremstyle{definition} \newtheorem{definition}[theorem]{Definition} \theoremstyle{remark} \newtheorem{remark}[theorem]{Remark} \AddToHook{env/theorem/begin}{\crefalias{theorem}{theorem}} \AddToHook{env/proposition/begin}{\crefalias{theorem}{proposition}} \AddToHook{env/lemma/begin}{\crefalias{theorem}{lemma}} \AddToHook{env/corollary/begin}{\crefalias{theorem}{corollary}} \AddToHook{env/definition/begin}{\crefalias{theorem}{definition}} \AddToHook{env/remark/begin}{\crefalias{theorem}{remark}} \crefname{theorem}{Theorem}{Theorems} \Crefname{theorem}{Theorem}{Theorems} \crefname{proposition}{Proposition}{Propositions} \Crefname{proposition}{Proposition}{Propositions} \crefname{lemma}{Lemma}{Lemmas} \Crefname{lemma}{Lemma}{Lemmas} \crefname{corollary}{Corollary}{Corollaries} \Crefname{corollary}{Corollary}{Corollaries} \newcommand{\C}{\mathbb C} \newcommand{\F}{\mathbb F} \newcommand{\Z}{\mathbb Z} \newcommand{\N}{\mathbb N} \newcommand{\D}{\mathsf D} \newcommand{\K}{\mathsf K} \newcommand{\otL}{\otimes^{\mathbf L}} \DeclareMathOperator{\Hom}{Hom} \DeclareMathOperator{\End}{End} \DeclareMathOperator{\Ext}{Ext} \DeclareMathOperator{\Tor}{Tor} \DeclareMathOperator{\pd}{pd} \DeclareMathOperator{\gldim}{gl.dim} \DeclareMathOperator{\findim}{fin.dim} \DeclareMathOperator{\Findim}{Fin.dim} \DeclareMathOperator{\rad}{rad} \DeclareMathOperator{\id}{id} \DeclareMathOperator{\Cone}{Cone} \DeclareMathOperator{\Kar}{Kar} \DeclareMathOperator{\supp}{supp} \DeclareMathOperator{\thick}{thick} \DeclareMathOperator{\perf}{perf} \DeclareMathOperator{\proj}{proj} \DeclareMathOperator{\Mod}{Mod} \DeclareMathOperator{\modu}{mod} \setlist[enumerate]{label=\textup{(\roman*)},leftmargin=2em} \setlength{\emergencystretch}{1.5em} \allowdisplaybreaks[1] \usepackage{indentfirst} \setlength{\parindent}{1.5em} \title{A note of refinements to an algebra of infinite little finitistic dimension} \author{Qiyue Tang} \date{\small Generated by GPT-6-Astra\\[6pt] October 7, 2026\\[3pt]\small This paper is not intended for journal submission.} \begin{document} \maketitle \begingroup\renewcommand{\thefootnote}{}\footnotetext{\textit{2020 Mathematics Subject Classification.} Primary 16E10; Secondary 16G20. \textit{Keywords.} Finitistic dimension, trivial extension, derived tensor product, brick.}\endgroup \begin{abstract} Building on OpenAI's \emph{An algebra of infinite little finitistic dimension}, we refine the construction and extend it to every field. \end{abstract} \section{Introduction}\label{sec:introduction} For a finite-dimensional algebra $A$ over a field $k$, write $\pd_A N$ for the projective dimension of a left $A$-module $N$, and set \[ \findim A=\sup\{\pd_A N:N\text{ is a finite-dimensional left }A\text{-module},\ \pd_A N<\infty\}. \] The finitistic-dimension problem asks whether this supremum is finite for every finite-dimensional algebra; see \cite{Bass1960,HuisgenZimmermann1995}. OpenAI's construction \cite{OpenAI198} gives a complex algebra for which the supremum is infinite. We retain its group, localization, tensor realization, and square-zero extension constructions, and refine their field of definition, test modules, and dimension estimates. For an algebra $A$, let $J_A=\rad A$ denote its Jacobson radical. The Loewy length of a nonzero module $N$ is the least $h\ge1$ with $J_A^hN=0$. An algebra is split basic if $A/J_A$ is a finite product of copies of $k$. We call a module a brick when its endomorphism ring is a division ring; the complex bricks below have endomorphism ring $\C$. \begin{theorem}\label{thm:main} For every field $k$ there are a finite-dimensional split basic $k$-algebra $A$ with $J_A^7=0$, integers $b_*\ge0$ and $l\ge0$, and finite-dimensional left $A$-modules $N_m$, $m\ge1$, such that \[ (b_*+5)(m-1)+1\le\pd_A N_m\le(b_*+5)(m-1)+l+3. \] The modules have Loewy length three, their endomorphism rings are division rings, and $\Hom_A(N_m,N_n)=0$ for $m\ne n$. In particular, $\findim A=\infty$. For $k=\C$ they can be chosen with \[ \dim_{\C}N_m=3\cdot2^{3m},\qquad \End_A(N_m)=\C. \] Every primitive vertex idempotent $\varepsilon$ in this construction satisfies $\varepsilon A\varepsilon=k\varepsilon$. \end{theorem} The proof follows the original construction in \cite{OpenAI198}. A finitely presented group supplies a group algebra $R$, a central idempotent $e$, and an automorphism $\alpha$. For a left $R$-module $Y$, the operation $H(Y)={}_{\alpha}(eY)$ takes the summand $eY$ and lets $r\in R$ act by $\alpha(r)$. We construct simple modules that vanish under precisely the $m$th iteration of $H$. A three-vertex algebra $B$ encodes $R$, and a bounded bimodule complex $P$ realizes $H$ together with a shift by three. A chain algebra records the differential of $P$ in an ordinary bimodule $X$ over an algebra $D$ of finite global dimension. The square-zero extension of $D$ by $X$ converts finite tensor extinction into finite projective dimension. All algebras are associative and unital, and algebra homomorphisms preserve $k$ and the unit. Modules are left modules unless designated right. The notation $\D^b(A\text{-}\modu)$ means the bounded derived category of finite-dimensional left $A$-modules; $\K^b(\proj\text{-}A)$ means the homotopy category of bounded finitely generated projective right $A$-module complexes. The symbol $\otL$ denotes derived tensor product. For a complex $K$ and an integer $n$, write $d_K^n:K^n\to K^{n+1}$ for its differential and $H^n(K)=\ker d_K^n/\operatorname{im}d_K^{n-1}$ for its cohomology. For integers $n,s$, the shift convention is \[ K[s]^n=K^{n+s},\qquad d_{K[s]}^n=(-1)^s d_K^{n+s}. \] A module is regarded as a complex concentrated in degree zero, so its shift by $s$ has cohomology in degree $-s$. Path products and endomorphism products are composed from right to left. \section{A selection process with unbounded extinction} \label{sec:selection} Let $R$ be a unital $k$-algebra, let $e\in R$ be a central idempotent, and let $\alpha:R\to R$ be a unital $k$-algebra endomorphism. For a left $R$-module $Y$, define \begin{equation} H(Y)={}_{\alpha}(eY). \label{eq:selection-functor} \end{equation} Here $eY$ is an $R$-submodule, and the subscript denotes restriction of scalars along $\alpha$: on the vector space $eY$, an element $r\in R$ acts by the original operator $\alpha(r)$. On a module map $f:Y\to Z$, the functor acts by the restriction $f|_{eY}:eY\to eZ$, with both actions twisted by $\alpha$. It is additive and preserves finite dimensionality. For $j\ge0$, write $H^{\circ j}$ for its $j$-fold iterate, with $H^{\circ 0}$ the identity functor; superscripts without a circle on $H$ will denote cohomology of a complex. \begin{proposition} \label{prop:selection} For every field $k$, there exist a finitely presented unital $k$-algebra $R$, a central idempotent $e\in R$, and an automorphism $\alpha$ of $R$ such that, for every integer $m\geq 1$, a finite-dimensional simple left $R$-module $Y_m$ satisfies \begin{equation} H^{\circ j}(Y_m)\neq 0\quad(0\leq j0\), the right projective \(\varepsilon_iC\) has basis \(\varepsilon_i,c_i\), and its radical is the right simple at \(i-1\). Left multiplication by \(c_i\) maps \(\varepsilon_{i-1}\) to \(c_i\) and, when \(i>1\), maps \(c_{i-1}\) to zero. This proves exactness, including injectivity at the first term. For \(l=0\), the resolution consists of the isomorphism \(\varepsilon_0C\to W\). Define a \((B\otimes_k C,B)\)-bimodule \(O\) by \[ \varepsilon_iO=P^{a_*+i}, \qquad c_i\big|_{\varepsilon_{i-1}O}=d_P^{a_*+i-1}. \] Here the two \(B\)-actions are those on the terms of \(P\). The relation \(d_P^2=0\) makes this a representation of \(C\), and the bimodule linearity of \(d_P\) makes the \(C\)-action commute with both \(B\)-actions. Thus \(O\) is an ordinary finite-dimensional bimodule. Set \[ D=B\times(B\otimes_k C),\qquad T=B\otimes_k W,\qquad X=O\oplus T. \] Regard \(O\) as having its left action from the second factor of \(D\) and its right action from the first. Regard \(T\) as having its left action from the first factor and its right action from the second, with the regular \(B\)-actions on its \(B\)-factor. These prescriptions define an ordinary finite-dimensional \(D\)-bimodule \(X\). The two summands of \(X\) move complexes between the factors of \(D\), as shown in \Cref{fig:simulation}. Thus two tensor steps return to the first factor; the next proposition identifies their composite. \begin{figure}[htbp] \centering \begin{tikzcd}[column sep=huge] \D^b(B\text{-}\modu) \arrow[r,bend left=22,"O\otL_B-"] & \D^b((B\otimes_k C)\text{-}\modu) \arrow[l,bend left=22,"T\otL_{B\otimes_k C}-"] \end{tikzcd} \caption{The two factors of \(D\) and the tensor functors supplied by the off-diagonal summands of \(X\). Starting on the left, the composite is \(P[b_*]\otL_B-\) by \Cref{prop:ordinary-simulation}.} \label{fig:simulation} \end{figure} \begin{proposition} \label{prop:ordinary-simulation} The algebra \(D\) has finite global dimension on both sides. Let \(F=X\otL_D-\). For every complex \(Z\) of left \(B\)-modules, regarded as a complex on the first factor of \(D\), there is an isomorphism \begin{equation} \label{eq:compression} F^2(Z)\simeq P[b_*]\otL_B Z, \qquad T\otL_{B\otimes_k C}O\simeq P[b_*]. \end{equation} The second isomorphism is an isomorphism of complexes of \(B\)-bimodules, and the first is supported on the first factor of \(D\). \end{proposition} \begin{proof} The vertices of \(B\otimes_k C\) are pairs \((i,j)\), where \(0\le i\le2\) and \(0\le j\le l\). Its diagonal vertex corners are \(k\). A nonzero component between distinct vertices moves in the product of the two directed orders. Assign height $i+j$ to vertex $(i,j)$. Every nonzero off-diagonal component increases height; the algebra on each height layer is a product of copies of $k$. The proof of \Cref{lem:directed-bound}, applied one layer at a time, gives \[ \gldim(B\otimes_k C),\quad \gldim\bigl((B\otimes_k C)^{\mathrm{op}}\bigr)\le l+2. \] The same bound holds for $D$ and $D^{\mathrm{op}}$, since $\gldim B,\gldim B^{\mathrm{op}}\le2$. Tensor \eqref{eq:right-chain-resolution} over \(k\) with the regular \(B\)-bimodule, placing its last projective term in degree zero. This gives a bounded resolution \(Q_T\to T\) by right \(B\otimes_k C\)-projectives, preserving the left \(B\)-action. Also, \(O\) is projective as a right \(B\)-module, being the finite direct sum of the terms of \(P\). Thus \(Q_X=O\oplus Q_T\), with the prescribed block actions, is a bounded right-\(D\)-projective resolution of \(X\) retaining its left \(D\)-action. Ordinary tensor with \(Q_X\) computes \(F\) on every complex. On the first factor, the block supports therefore give \[ F^2(Z)\simeq Q_T\otimes_{B\otimes_k C}(O\otimes_B Z) \cong \bigl(Q_T\otimes_{B\otimes_k C}O\bigr)\otimes_B Z. \] In degree \(n\), for \(-l\le n\le0\), tensoring \(Q_T\) with \(O\) gives \[ \bigl(B\otimes_k\varepsilon_{l+n}C\bigr) \otimes_{B\otimes_k C}O \cong\varepsilon_{l+n}O =P^{a_*+l+n}=P^{b_*+n}. \] The induced differential is \(d_P\). In comparison, the standard differential of \(P[b_*]\) is \((-1)^{b_*}d_P\). Multiplication by \((-1)^{b_*n}\) in degree \(n\) defines a chain isomorphism to \(P[b_*]\); it respects both \(B\)-actions. Since this complex is termwise right-\(B\)-projective, its ordinary tensor with any \(Z\) computes the derived tensor. This proves the second isomorphism in \eqref{eq:compression}, and hence the first. \end{proof} \section{A square-zero extension and projective dimension} \label{sec:square-zero} For a $D$-bimodule $X$, the square-zero extension $D\ltimes X$ is the vector space $D\oplus X$ with multiplication $(d,x)(d',x')=(dd',dx'+xd')$. A derived bar decomposition relates tensor extinction to projective dimension. \subsection{The derived bar decomposition} The splitting below also follows from the graded-component decomposition of Minamoto and Yamaura \cite[Lemma~4.13(4) and the proof of Theorem~4.17]{MinamotoYamaura}, after forgetting the grading and passing to opposite algebras. The direct proof identifies each derived tensor factor and its shift. \begin{proposition} \label{prop:bar-splitting} Let \(D\) be a finite-dimensional \(k\)-algebra, let \(X\) be a finite-dimensional \(D\)-bimodule, and let \(A=D\ltimes X\). Let \(N\) be a left \(D\)-module, inflated to \(A\) through the projection \(A\to D\), and put \(F=X\otL_D-\). In the derived category of left \(D\)-modules there is an isomorphism \begin{equation} \label{eq:bar-splitting} D\otL_A N \simeq \bigoplus_{r\ge0}(F^rN)[r]. \end{equation} Here \(F^0N=N\), and every \(F^r\) denotes an iteration of the derived tensor functor. \end{proposition} \begin{proof} Use the ordinary unnormalized bar resolution of \(N\) over the field \(k\). It is a free left \(A\)-resolution with degree \(-n\) term \(A\otimes_k A^{\otimes_k n}\otimes_k N\). Its augmentation is a quasi-isomorphism: the augmented bar complex has the usual \(k\)-linear contraction obtained by inserting the unit. After tensoring with the right \(A\)-module \(D\), it yields a model \(\mathcal B\) for \(D\otL_AN\), with \[ \mathcal B^{-n}=D\otimes_k A^{\otimes_k n}\otimes_k N \qquad(n\ge0). \] The differential is the alternating sum of the faces that multiply adjacent algebra entries or apply the two endpoint actions. Expand each internal copy of \(A\) as \(D\oplus X\). Every nonzero face preserves the number of entries from \(X\). Indeed, a product involving exactly one \(X\)-entry remains in \(X\), a product of two \(X\)-entries is zero, and an endpoint action by \(X\) is zero on both \(D\) and \(N\). Thus there is a decomposition of complexes \[ \mathcal B=\bigoplus_{r\ge0}\mathcal B_r, \] where \(\mathcal B_r\) consists of words with precisely \(r\) entries from \(X\). For fixed \(r\), write \(i_0,\ldots,i_r\) for the lengths of the blocks of \(D\)-entries before, between, and after the \(X\)-entries. The corresponding tensor is \begin{equation} \label{eq:bar-block} D\otimes_kD^{\otimes_k i_0}\otimes_k X \otimes_kD^{\otimes_k i_1}\otimes_k\cdots \otimes_k X\otimes_kD^{\otimes_k i_r}\otimes_k N, \end{equation} in degree \(-r-\sum_{j=0}^r i_j\). We identify this with the multiple two-sided bar complex for \begin{equation} \label{eq:derived-multibar} D\otL_D \underbrace{X\otL_D\cdots\otL_D X}_{r\ \text{factors}} \otL_D N, \end{equation} shifted by \(r\). First consider the signs. Within block \(j\), a bar face has alternating-sign offset \[ j+\sum_{hg\). Applying this observation to successive truncation triangles shows inductively that \[ H^q(F^rN)=0\quad\text{unless}\quad -rg\le q\le0. \] For the first assertion, vanishing at \(t\) implies vanishing at every \(r\ge t\). By \eqref{eq:bar-splitting}, \(D\otL_AN\) then has bounded cohomology. Since \(X\) is a nilpotent ideal, it is contained in \(\rad A\), and \[ \rad A=(\rad D)\oplus X, \qquad A/\rad A\cong D/\rad D=:S. \] Derived associativity gives \[ S\otL_A N \simeq S\otL_D(D\otL_A N). \] The right \(D\)-module \(S\) has a finite projective resolution, so this complex also has bounded cohomology. Choose a minimal projective resolution of \(N\) over the finite-dimensional algebra \(A\), using successive projective covers. Its terms are finitely generated, and every differential has image in the radical of its target. Tensoring with \(S=A/\rad A\) therefore annihilates every differential. If \(Q\) is a nonzero finitely generated projective \(A\)-module, then \[ S\otimes_A Q\cong Q/(\rad A)Q\ne0 \] by Nakayama's Lemma. Consequently bounded cohomology of \(S\otL_AN\) forces the minimal resolution to have only finitely many nonzero terms. This proves \(\pd_A N<\infty\). For the second assertion, choose \(q\le0\) with \(H^q(F^rN)\ne0\). Its direct summand in \eqref{eq:bar-splitting} gives \[ H^{q-r}(D\otL_A N)\ne0,\qquad q-r\le-r. \] A projective \(A\)-resolution of \(N\) of length strictly less than \(r\) would make the derived tensor zero in this degree. Hence \(\pd_A N\ge r\), as asserted. \end{proof} With $D$ of finite global dimension, for a bounded complex $Z$ of left $D$-modules with finite-dimensional cohomology, $\pd_D Z$ is the least integer $d$ such that $Z$ is represented by a bounded projective complex zero below degree $-d$; set $\pd_D0=-\infty$. In particular $\pd_D(Z[s])=\pd_D Z+s$. \begin{proposition}\label{prop:exact-pd} Under the hypotheses of \Cref{cor:pd-detection}, if $F^tN=0$ for some $t\ge1$, then \[ \pd_A N=\max_{0\le r