Quantum differential calculus

In quantum geometry or noncommutative geometry a quantum differential calculus or noncommutative differential structure on an algebra $A$ over a field $k$ means the specification of a space of differential forms over the algebra. The algebra $A$ here is regarded as a coordinate ring but it is important that it may be noncommutative and hence not an actual algebra of coordinate functions on any actual space, so this represents a point of view replacing the specification of a differentiable structure for an actual space. In ordinary differential geometry one can multiply differential 1-forms by functions from the left and from the right, and there exists an exterior derivative. Correspondingly, a first order quantum differential calculus means at least the following:

1. An $A$-$A$-bimodule $\Omega^1$ over $A$, i.e. one can multiply elements of $\Omega^1$ by elements of $A$ in an associative way:

: $a(\omega b)=(a\omega)b,\ \forall a,b\in A,\ \omega\in\Omega^1$.

2. A linear map $:A\to\Omega^1$ obeying the Leibniz rule
: $(ab)=a(b)+(a)b,\ \forall a,b\in A$

3. $\Omega^1=\$

4. (optional connectedness condition) $\ker\ =k1$

The last condition is not always imposed but holds in ordinary geometry when the manifold is connected. It says that the only functions killed by $$ are constant functions.

An ''exterior algebra'' or ''differential graded algebra'' structure over $A$ means a compatible extension of $\Omega^1$ to include analogues of higher order differential forms

: $\Omega=\oplus_n\Omega^n,\ :\Omega^n\to\Omega^$

obeying a graded-Leibniz rule with respect to an associative product on $\Omega$ and obeying $^2=0$. Here $\Omega^0=A$ and it is usually required that $\Omega$ is generated by $A,\Omega^1$. The product of differential forms is called the exterior or wedge product and often denoted $\wedge$. The noncommutative or quantum de Rham cohomology is defined as the cohomology of this complex.

A higher order differential calculus can mean an exterior algebra, or it can mean the partial specification of one, up to some highest degree, and with products that would result in a degree beyond the highest being unspecified.

The above definition lies at the crossroads of two approaches to noncommutative geometry. In the Connes approach a more fundamental object is a replacement for the Dirac operator in the form of a spectral triple, and an exterior algebra can be constructed from this data. In the quantum groups approach to noncommutative geometry one starts with the algebra and a choice of first order calculus but constrained by covariance under a quantum group symmetry.

Note

The above definition is minimal and gives something more general than classical differential calculus even when the algebra $A$ is commutative or functions on an actual space. This is because we do ''not'' demand that

: $a(b)=(b)a,\ \forall a,b\in A$

since this would imply that $(ab-ba)=0,\ \forall a,b\in A$, which would violate axiom 4 when the algebra was noncommutative. As a byproduct, this enlarged definition includes finite difference calculi and quantum differential calculi on finite sets and finite groups (finite group Lie algebra theory).

Examples

1. For A= /math> the algebra of polynomials in one variable the translation-covariant quantum differential calculi are parametrized by $\lambda\in \mathbb C$ and take the form

: $\Omega^1=.x,\quad (x)f(x)=f(x+\lambda)(x),\quad f=x$

This shows how finite differences arise naturally in quantum geometry. Only the limit $\lambda\to 0$ has functions commuting with 1-forms, which is the special case of high school differential calculus.

2. For A= ,t^/math> the algebra of functions on an algebraic circle, the translation (i.e. circle-rotation)-covariant differential calculi are parametrized by $q\ne 0\in \mathbb C$ and take the form

: $\Omega^1=.t,\quad (t)f(t)=f(qt)(t),\quad f=\,$

This shows how $q$-differentials arise naturally in quantum geometry.

3. For any algebra $A$ one has a universal differential calculus defined by

: $\Omega^1=\ker(m:A\otimes A\to A),\quad a=1\otimes a-a\otimes 1,\quad\forall a\in A$

where $m$ is the algebra product. By axiom 3., any first order calculus is a quotient of this.

See also

*Quantum geometry
*Noncommutative geometry
*Quantum calculus
*Quantum group
*Quantum spacetime

Further reading

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Noncommutative geometry
Algebraic structures
{{Quantum mechanics topics