• Source: Connection (algebraic framework)
  • Geometry of quantum systems (e.g.,
    noncommutative geometry and supergeometry) is mainly
    phrased in algebraic terms of modules and
    algebras. Connections on modules are
    generalization of a linear connection on a smooth vector bundle



    E

    X


    {\displaystyle E\to X}

    written as a Koszul connection on the





    C




    (
    X
    )


    {\displaystyle C^{\infty }(X)}

    -module of sections of



    E

    X


    {\displaystyle E\to X}

    .


    Commutative algebra


    Let



    A


    {\displaystyle A}

    be a commutative ring
    and



    M


    {\displaystyle M}

    an A-module. There are different equivalent definitions
    of a connection on



    M


    {\displaystyle M}

    .


    = First definition

    =
    If



    k

    A


    {\displaystyle k\to A}

    is a ring homomorphism, a



    k


    {\displaystyle k}

    -linear connection is a



    k


    {\displaystyle k}

    -linear morphism





    :
    M


    Ω

    A

    /

    k


    1





    A


    M


    {\displaystyle \nabla :M\to \Omega _{A/k}^{1}\otimes _{A}M}


    which satisfies the identity





    (
    a
    m
    )
    =
    d
    a

    m
    +
    a

    m


    {\displaystyle \nabla (am)=da\otimes m+a\nabla m}


    A connection extends, for all



    p

    0


    {\displaystyle p\geq 0}

    to a unique map





    :

    Ω

    A

    /

    k


    p





    A


    M


    Ω

    A

    /

    k


    p
    +
    1





    A


    M


    {\displaystyle \nabla :\Omega _{A/k}^{p}\otimes _{A}M\to \Omega _{A/k}^{p+1}\otimes _{A}M}


    satisfying




    (
    ω

    f
    )
    =
    d
    ω

    f
    +
    (

    1

    )

    p


    ω


    f


    {\displaystyle \nabla (\omega \otimes f)=d\omega \otimes f+(-1)^{p}\omega \wedge \nabla f}

    . A connection is said to be integrable if






    =
    0


    {\displaystyle \nabla \circ \nabla =0}

    , or equivalently, if the curvature






    2


    :
    M


    Ω

    A

    /

    k


    2



    M


    {\displaystyle \nabla ^{2}:M\to \Omega _{A/k}^{2}\otimes M}

    vanishes.


    = Second definition

    =
    Let



    D
    (
    A
    )


    {\displaystyle D(A)}

    be the module of derivations of a ring



    A


    {\displaystyle A}

    . A
    connection on an A-module



    M


    {\displaystyle M}

    is defined
    as an A-module morphism





    :
    D
    (
    A
    )



    D
    i
    f
    f


    1


    (
    M
    ,
    M
    )
    ;
    u




    u




    {\displaystyle \nabla :D(A)\to \mathrm {Diff} _{1}(M,M);u\mapsto \nabla _{u}}


    such that the first order differential operators






    u




    {\displaystyle \nabla _{u}}

    on




    M


    {\displaystyle M}

    obey the Leibniz rule







    u


    (
    a
    p
    )
    =
    u
    (
    a
    )
    p
    +
    a



    u


    (
    p
    )
    ,

    a

    A
    ,

    p

    M
    .


    {\displaystyle \nabla _{u}(ap)=u(a)p+a\nabla _{u}(p),\quad a\in A,\quad p\in M.}


    Connections on a module over a commutative ring always exist.
    The curvature of the connection






    {\displaystyle \nabla }

    is defined as
    the zero-order differential operator




    R
    (
    u
    ,

    u


    )
    =
    [



    u


    ,




    u




    ]




    [
    u
    ,

    u


    ]





    {\displaystyle R(u,u')=[\nabla _{u},\nabla _{u'}]-\nabla _{[u,u']}\,}


    on the module



    M


    {\displaystyle M}

    for all



    u
    ,

    u



    D
    (
    A
    )


    {\displaystyle u,u'\in D(A)}

    .
    If



    E

    X


    {\displaystyle E\to X}

    is a vector bundle, there is one-to-one
    correspondence between linear
    connections



    Γ


    {\displaystyle \Gamma }

    on



    E

    X


    {\displaystyle E\to X}

    and the
    connections






    {\displaystyle \nabla }

    on the





    C




    (
    X
    )


    {\displaystyle C^{\infty }(X)}

    -module of sections of



    E

    X


    {\displaystyle E\to X}

    . Strictly speaking,






    {\displaystyle \nabla }

    corresponds to
    the covariant differential of a
    connection on



    E

    X


    {\displaystyle E\to X}

    .


    Graded commutative algebra


    The notion of a connection on modules over commutative rings is
    straightforwardly extended to modules over a graded
    commutative algebra. This is the case of
    superconnections in supergeometry of
    graded manifolds and supervector bundles.
    Superconnections always exist.


    Noncommutative algebra


    If



    A


    {\displaystyle A}

    is a noncommutative ring, connections on left
    and right A-modules are defined similarly to those on
    modules over commutative rings. However
    these connections need not exist.
    In contrast with connections on left and right modules, there is a
    problem how to define a connection on an
    R-S-bimodule over noncommutative rings
    R and S. There are different definitions
    of such a connection. Let us mention one of them. A connection on an
    R-S-bimodule



    P


    {\displaystyle P}

    is defined as a bimodule
    morphism





    :
    D
    (
    A
    )

    u




    u





    D
    i
    f
    f


    1


    (
    P
    ,
    P
    )


    {\displaystyle \nabla :D(A)\ni u\to \nabla _{u}\in \mathrm {Diff} _{1}(P,P)}


    which obeys the Leibniz rule







    u


    (
    a
    p
    b
    )
    =
    u
    (
    a
    )
    p
    b
    +
    a



    u


    (
    p
    )
    b
    +
    a
    p
    u
    (
    b
    )
    ,

    a

    R
    ,

    b

    S
    ,

    p

    P
    .


    {\displaystyle \nabla _{u}(apb)=u(a)pb+a\nabla _{u}(p)b+apu(b),\quad a\in R,\quad b\in S,\quad p\in P.}



    See also


    Connection (vector bundle)
    Connection (mathematics)
    Noncommutative geometry
    Supergeometry
    Differential calculus over commutative algebras


    Notes




    References




    External links


    Sardanashvily, G. (2009). "Lectures on Differential Geometry of Modules and Rings". arXiv:0910.1515 [math-ph].

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