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\newcommand{\coproduct}{\coprod} \newcommand{\product}{\prod} \newcommand{\closure}{\overline} \newcommand{\integral}{\int} \newcommand{\doubleintegral}{\iint} \newcommand{\tripleintegral}{\iiint} \newcommand{\quadrupleintegral}{\iiiint} \newcommand{\conint}{\oint} \newcommand{\contourintegral}{\oint} \newcommand{\infinity}{\infty} \newcommand{\bottom}{\bot} \newcommand{\minusb}{\boxminus} \newcommand{\plusb}{\boxplus} \newcommand{\timesb}{\boxtimes} \newcommand{\intersection}{\cap} \newcommand{\union}{\cup} \newcommand{\Del}{\nabla} \newcommand{\odash}{\circleddash} \newcommand{\negspace}{\!} \newcommand{\widebar}{\overline} \newcommand{\textsize}{\normalsize} \renewcommand{\scriptsize}{\scriptstyle} \newcommand{\scriptscriptsize}{\scriptscriptstyle} \newcommand{\mathfr}{\mathfrak} \newcommand{\statusline}[2]{#2} \newcommand{\tooltip}[2]{#2} \newcommand{\toggle}[2]{#2} % Theorem Environments \theoremstyle{plain} \newtheorem{theorem}{Theorem} \newtheorem{lemma}{Lemma} \newtheorem{prop}{Proposition} \newtheorem{cor}{Corollary} \newtheorem*{utheorem}{Theorem} \newtheorem*{ulemma}{Lemma} \newtheorem*{uprop}{Proposition} \newtheorem*{ucor}{Corollary} \theoremstyle{definition} \newtheorem{defn}{Definition} \newtheorem{example}{Example} \newtheorem*{udefn}{Definition} \newtheorem*{uexample}{Example} \theoremstyle{remark} \newtheorem{remark}{Remark} \newtheorem{note}{Note} \newtheorem*{uremark}{Remark} \newtheorem*{unote}{Note} %------------------------------------------------------------------- \begin{document} %------------------------------------------------------------------- \section*{Loday-Pirashvili category} \hypertarget{overview}{}\subsection*{{Overview}}\label{overview} Given any category $C$, one can define the [[arrow category]] $\Arr(C)$ of $C$, whose objects are morphisms in $C$ and whose morphisms are commutative squares. If $C$ is the category of [[vector space]]s (or some other $k$-linear [[closed monoidal category|closed]] [[symmetric monoidal category]] with [[equalizer]]s) one can define the \emph{infinitesimal} or \emph{Loday--Pirashvili} (LP) tensor product on the category of arrows, as well as an inner hom, equipping the category $\mathrm{Arr} C$ with a structure of a $k$-linear closed symmetric monoidal category. The LP-tensor product is \begin{displaymath} (f:V_1\to V_0)\otimes (g:W_1\to W_0):= (V_0\otimes g + f\otimes W_0: V_0\otimes W_1 \oplus V_1\otimes W_0\to V_0\otimes W_0). \end{displaymath} This is a truncation of the tensor product of [[chain complex]]es where $V_1\otimes W_1$ is dropped. The inner hom is rather interesting: $\mathbf{Hom}(f,g) = (p:\mathrm{Hom}_1(f,g)\to\mathrm{Hom}_0(f,g))$, where $\mathrm{Hom}_0(f,g)$ is the equalizer of two morphisms \begin{displaymath} \mathrm{hom}(V_0,W_0)\oplus\mathrm{hom}(V_1,W_1)\to\mathrm{hom}(V_1,W_0), \end{displaymath} namely precomposing the first summand with $f$ and postcomposing the second summand with $g$ (where $\mathrm{hom}$ is the ordinary [[hom-set|inner hom]] in $C$), and where $\mathrm{Hom}_1(f,g)$ is the equalizer of two morphisms \begin{displaymath} \mathrm{Hom}_0(f,g)\oplus\mathrm{hom}(V_0,W_1)\to \mathrm{Hom}_0(f,g), \end{displaymath} namely the identity and the map which replaces the lower component with the postcomposition by $g$ applied on $\mathrm{hom}(V_0,W_1)$ and keeps the upper component. Finally, $p$ is the natural projection. In the case of vector spaces this means that we have diagonal lifts in squares such that the lower square commutes but not necessarily the upper, i.e. $\mathrm{Hom}(f,g)$ is the space consisting of all triples $(u_1,u_0,\phi)$ where $u_1:V_1\to W_1$, $u_0:V_0\to W_0$ and $\phi:V_0\to W_1$ such that $g\circ u_1= u_0\circ f$ and $u_0=g\circ\phi$ while one does \emph{not} require $\phi\circ f=u_1$. There are a number of remarkable functors relating [[internalization|internal]] algebras in LP, [[Lie algebra]]s in LP etc., to or from some other categories of algebras. For example the categories of left [[Leibniz algebra]]s and of right Leibniz algebras embed as full subcategories into the category of internal Lie algebras in LP. This embedding has an [[adjoint functor|adjoint]]. Notice that because of truncation, being a Lie algebra in LP is a bit less than a (strict) $2$-[[n-Lie algebra|Lie algebra]] (a requirement in degree $2$ is dropped). \hypertarget{literature_and_discussions}{}\subsection*{{Literature and discussions}}\label{literature_and_discussions} \begin{itemize}% \item [[Jean-Louis Loday]], [[Teimuraz Pirashvili]], \emph{The tensor category of linear maps}, Georg. Math. J. vol. 5, n.3 (1998) 263--276. \item \href{http://golem.ph.utexas.edu/category/2007/10/loday_and_pirashvili_on_lie_2a.html}{nlab} \end{itemize} [[Tim Porter|Tim]]: Methinks that we need some comment on the evident connection with [[Baez–Crans 2-vector space]]. I think I remember seeing some paper on 2-vector spaces that mentions the connection. Whether or not it exploited that connection has slipped my memory. Can Zoran say something on this? [[Zoran Škoda|Zoran]] Surely in char 0, internal categories to vector spaces are the same as 2-term chain complexes, but if one translates strict associative algebra, Lie algebra etc. internal to the categories of internal categories in $Vec_k$ then one has more on the internal category side then on LP side because of the truncation of the tensor product. So every strict Lie algebra in Baez-Crans 2-vector spaces gives an examples of an internal Lie algebra in LP but not other way around. Eventually I will put some treatment of this, but it is not that simple to write it clearly, so it will wait a bit for now. [[!redirects Loday–Pirashvili category]] [[!redirects Loday--Pirashvili category]] [[!redirects Loday-Pirashvili tensor category]] [[!redirects Loday–Pirashvili tensor category]] [[!redirects Loday--Pirashvili tensor category]] \end{document}