Graded manifold

A graded manifold of dimension ${\displaystyle (n,m)}$ is defined as a locally ringed space ${\displaystyle (Z,A)}$ where ${\displaystyle Z}$ is an ${\displaystyle n}$-dimensional smooth manifold and ${\displaystyle A}$ is a ${\displaystyle C_{Z}^{\infty }}$-sheaf of Grassmann algebras of rank ${\displaystyle m}$ where ${\displaystyle C_{Z}^{\infty }}$ is the sheaf of smooth real functions on ${\displaystyle Z}$. The sheaf ${\displaystyle A}$ is called the structure sheaf of the graded manifold ${\displaystyle (Z,A)}$, and the manifold ${\displaystyle Z}$ is said to be the body of ${\displaystyle (Z,A)}$. Sections of the sheaf ${\displaystyle A}$ are called graded functions on a graded manifold ${\displaystyle (Z,A)}$. They make up a graded commutative ${\displaystyle C^{\infty }(Z)}$-ring ${\displaystyle A(Z)}$ called the structure ring of ${\displaystyle (Z,A)}$. The well-known Batchelor theorem and Serre–Swan theorem characterize graded manifolds as follows.

Note that above mentioned Batchelor's isomorphism fails to be canonical, but it often is fixed from the beginning. In this case, every trivialization chart ${\displaystyle (U;z^{A},y^{a})}$ of the vector bundle ${\displaystyle E\to Z}$ yields a splitting domain ${\displaystyle (U;z^{A},c^{a})}$ of a graded manifold ${\displaystyle (Z,A)}$, where ${\displaystyle \{c^{a}\}}$ is the fiber basis for ${\displaystyle E}$. Graded functions on such a chart are ${\displaystyle \Lambda (V)}$-valued functions

${\displaystyle f=\sum _{k=0}^{m}{\frac {1}{k!}}f_{a_{1}\ldots a_{k}}(z)c^{a_{1}}\cdots c^{a_{k}}}$,

where ${\displaystyle f_{a_{1}\cdots a_{k}}(z)}$ are smooth real functions on ${\displaystyle U}$ and ${\displaystyle c^{a}}$ are odd generating elements of the Grassmann algebra ${\displaystyle \Lambda (V)}$.

Given a graded manifold ${\displaystyle (Z,A)}$, graded derivations of the structure ring of graded functions ${\displaystyle A(Z)}$ are called graded vector fields on ${\displaystyle (Z,A)}$. They constitute a real Lie superalgebra ${\displaystyle \partial A(Z)}$ with respect to the superbracket

${\displaystyle [u,u']=u\cdot u'-(-1)^{[u][u']}u'\cdot u}$,

where ${\displaystyle [u]}$ denotes the Grassmann parity of ${\displaystyle u\in \partial A(Z)}$. Graded vector fields locally read

${\displaystyle u=u^{A}\partial _{A}+u^{a}{\frac {\partial }{\partial c^{a}}}}$.

They act on graded functions ${\displaystyle f}$ by the rule

${\displaystyle u(f_{a_{1}\ldots a_{k}}c^{a_{1}}\cdots c^{a_{k}})=u^{A}\partial _{A}(f_{a_{1}\ldots a_{k}})c^{a_{1}}\cdots c^{a_{k}}+\sum _{i}u^{a_{i}}(-1)^{i-1}f_{a_{1}\ldots a_{k}}c^{a_{1}}\cdots c^{a_{i-1}}c^{a_{i+1}}\cdots c^{a_{k}}}$.

The ${\displaystyle A(Z)}$-dual of the module graded vector fields ${\displaystyle \partial A(Z)}$ is called the module of graded exterior one-forms ${\displaystyle O^{1}(Z)}$. Graded exterior one-forms locally read ${\displaystyle \phi =\phi _{A}dz^{A}+\phi _{a}dc^{a}}$ so that the duality (interior) product between ${\displaystyle \partial A(Z)}$ and ${\displaystyle O^{1}(Z)}$ takes the form

${\displaystyle u\rfloor \phi =u^{A}\phi _{A}+(-1)^{[\phi _{a}]}u^{a}\phi _{a}}$.

Provided with the graded exterior product

${\displaystyle dz^{A}\wedge dc^{i}=-dc^{i}\wedge dz^{A},\qquad dc^{i}\wedge dc^{j}=dc^{j}\wedge dc^{i}}$,

graded one-forms generate the graded exterior algebra ${\displaystyle O^{*}(Z)}$ of graded exterior forms on a graded manifold. They obey the relation

${\displaystyle \phi \wedge \phi '=(-1)^{|\phi ||\phi '|+[\phi ][\phi ']}\phi '\wedge \phi }$,

where ${\displaystyle |\phi |}$ denotes the form degree of ${\displaystyle \phi }$. The graded exterior algebra ${\displaystyle O^{*}(Z)}$ is a graded differential algebra with respect to the graded exterior differential

${\displaystyle d\phi =dz^{A}\wedge \partial _{A}\phi +dc^{a}\wedge {\frac {\partial }{\partial c^{a}}}\phi }$,

where the graded derivations ${\displaystyle \partial _{A}}$, ${\displaystyle \partial /\partial c^{a}}$ are graded commutative with the graded forms ${\displaystyle dz^{A}}$ and ${\displaystyle dc^{a}}$. There are the familiar relations

${\displaystyle d(\phi \wedge \phi ')=d(\phi )\wedge \phi '+(-1)^{|\phi |}\phi \wedge d\phi '}$.

In the category of graded manifolds, one considers graded Lie groups, graded bundles and graded principal bundles. One also introduces the notion of jets of graded manifolds, but they differ from jets of graded bundles.

The differential calculus on graded manifolds is formulated as the differential calculus over graded commutative algebras similarly to the differential calculus over commutative algebras.

Due to the above-mentioned Serre–Swan theorem, odd classical fields on a smooth manifold are described in terms of graded manifolds. Extended to graded manifolds, the variational bicomplex provides the strict mathematical formulation of Lagrangian classical field theory and Lagrangian BRST theory.

• Connection (algebraic framework)
• Graded (mathematics)
• Serre–Swan theorem
• Supergeometry
• Supermanifold
• Supersymmetry

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• B. Kostant, Graded manifolds, graded Lie theory, and prequantization, in Differential Geometric Methods in Mathematical Physics, Lecture Notes in Mathematics 570 (Springer, 1977) p. 177
• A. Almorox, Supergauge theories in graded manifolds, in Differential Geometric Methods in Mathematical Physics, Lecture Notes in Mathematics 1251 (Springer, 1987) p. 114
• D. Hernandez Ruiperez, J. Munoz Masque, Global variational calculus on graded manifolds, J. Math. Pures Appl. 63 (1984) 283
• G. Giachetta, L. Mangiarotti, G. Sardanashvily, Advanced Classical Field Theory (World Scientific, 2009) ISBN 978-981-283-895-7; arXiv:math-ph/0102016; arXiv:1304.1371.

• G. Sardanashvily, Lectures on supergeometry, arXiv:0910.0092.