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Hochschild Cohomology Group

Updated 26 November 2025
  • Hochschild Cohomology Group is defined via a cochain complex that captures deformation and symmetry aspects of associative algebras.
  • It features a graded-commutative cup product and a Gerstenhaber bracket, which formalize the algebra's multiplicative and derivational properties.
  • Applications extend to noncommutative geometry, representation theory, and topological field theory through explicit combinatorial and categorical frameworks.

The Hochschild cohomology group, denoted HHn(A,M)HH^n(A, M) for an associative algebra AA and an AA-bimodule MM, is a central invariant in the cohomology theory of associative algebras and more generally in noncommutative geometry, representation theory, and homological algebra. It encodes deformation, structural, and symmetry data via its algebraic, functorial, and higher categorical constructions.

1. Definition, Construction, and First Properties

Let AA be an associative KK-algebra, MM an AA-bimodule, and n0n \geq 0. The nn-th Hochschild cohomology group is defined via the cochain complex

Cn(A,M):=HomK(An,M),C^n(A, M) := \operatorname{Hom}_K(A^{\otimes n}, M),

with C0(A,M)=MC^0(A, M) = M and Ck(A,M)=0C^{-k}(A, M) = 0 for k>0k>0, equipped with the differentials

(dnf)(a1,...,an+1)=a1f(a2,...,an+1)+i=1n(1)if(a1,...,aiai+1,...,an+1)+(1)n+1f(a1,...,an)an+1.(d^n f)(a_1, ..., a_{n+1}) = a_1 \cdot f(a_2, ..., a_{n+1}) + \sum_{i=1}^n (-1)^i f(a_1, ..., a_i a_{i+1}, ..., a_{n+1}) + (-1)^{n+1} f(a_1, ..., a_n) \cdot a_{n+1}.

The cohomology groups are then

HHn(A,M):=Hn(C(A,M),d).HH^n(A, M) := H^n(C^\bullet(A, M), d).

In particular, for M=AM = A (the regular bimodule), HH0(A)=Z(A)HH^0(A) = Z(A) is the center of AA, and HH1(A)HH^1(A) is the space of outer derivations modulo inner derivations. This construction also generalizes to the setting of ring objects in monoidal categories, where the same model persists and the central interpretations in degree $0$ and derivations in degree $1$ remain valid (Hellstrøm-Finnsen, 2016).

2. Algebraic Structures: Cup Product, Gerstenhaber Bracket, and Graded-Commutativity

The Hochschild cohomology HH(A,A)=nHHn(A,A)HH^*(A, A) = \bigoplus_n HH^n(A, A) is naturally endowed with a graded-commutative algebra structure via the cup product

(fg)(a1,...,am+n)=f(a1,...,am)g(am+1,...,am+n).(f \smile g)(a_1, ..., a_{m+n}) = f(a_1, ..., a_m) \cdot g(a_{m+1}, ..., a_{m+n}).

This product is graded-commutative: [f][g]=(1)mn[g][f],[f] \smile [g] = (-1)^{mn} [g] \smile [f], and HH(A,A)HH^*(A, A) is a Gerstenhaber algebra. Explicitly, the Gerstenhaber bracket is the degree 1-1 graded Lie bracket

[f,g]=fg(1)(m1)(n1)gf,[f, g] = f \circ g - (-1)^{(m-1)(n-1)} g \circ f,

where circle denotes insertion of one cochain into another. This bracket measures the failure of strict associativity in the cup product and governs the deformation theory of AA (Wang, 2015).

In symmetric algebras, Δ\Delta-type operators further promote HH(A,A)HH^*(A,A) or singular HHsg(A,A)HH^*_{sg}(A,A) to a Batalin–Vilkovisky (BV) algebra, with the bracket generated by the BV operator reflecting string topology phenomena (Wang, 2015).

3. Hochschild Cohomology for Structured Algebras and Categories

3.1. Hopf Algebras and Modular Group Action

For finite-dimensional factorizable ribbon Hopf algebras AA, the modular group SL(2,Z)SL(2, \mathbb{Z}) acts projectively on Z(A)=HH0(A)Z(A) = HH^0(A) and, via explicit functorial lifts of Drinfel’d and Radford maps, this action extends up to homotopy to the entire Hochschild cochain complex and the cohomology groups HHn(A)HH^n(A) (Lentner et al., 2017). Generators of SL(2,Z)SL(2,\mathbb{Z}) map to projective automorphisms [Gn],[In]PGL(HHn(A))[G_n], [I_n] \in PGL(HH^n(A)) satisfying the modular relations up to prescribed scalars.

3.2. Group Algebras and Topological Field Theory

For A=k[G]A = k[G] a group algebra, HH(A)HH^*(A) can be interpreted via the classifying space of the adjoint groupoid of GG, encoding geometric and representation theoretic information (Mishchenko, 2018). The Hochschild cochains admit a natural Frobenius algebra structure extending the (1,2)(1,2)-TQFT on HH0HH^0 and a homotopy-commutative Gerstenhaber product, with the group cohomology complex embedded canonically as a DG subalgebra (Lodder, 2014). This perspective underlies both the topological field theory quantization of finite group data and the structure of modular functors in quantum algebra.

3.3. Algebras with Finiteness and Representation-Theoretic Constraints

In gentle, special biserial, and string algebras, Hochschild cohomology displays strong combinatorial control, often admitting closed formulas for dimensions and explicit vanishing or degeneracy of the multiplicative structure (Ladkani, 2012, Furuya, 2014, Redondo et al., 2013). In many such classes (e.g., triangular string algebras), the cup product on positive-degree elements is trivial, rendering HH>0HH^{>0} a square-zero ideal.

3.4. Gluing, Extensions, and Derived Categories

The behavior of HHnHH^n under gluing of idempotents in monomial algebras or extensions by bimodules has been described precisely: dimensions of HH1HH^1 differ by explicit combinatorial invariants associated to special paths and pairs, and higher degrees are controlled by path-length arguments (Liu et al., 2022). In cluster-tilted and related algebras, the first Hochschild cohomology admits a direct sum decomposition reflecting the trivial extension structure, splitting derivations into those inherited from the base algebra and those detecting the extension data (Assem et al., 2012).

4. Geometric and Categorical Generalizations

Hochschild cohomology generalizes to schemes and (triangulated, DG, or stable \infty-) categories, with central roles in homological algebra, deformation theory, and noncommutative geometry.

  • On smooth schemes XX, Hochschild–Kostant–Rosenberg (HKR) theory gives

HHn(X)p+q=nHp(X,qTX),HH^n(X) \cong \bigoplus_{p+q = n} H^p(X, \wedge^q T_X),

and this decomposition characterizes smoothness in large classes (e.g., projective hypersurfaces) (Liu et al., 2015).

  • For kk-linear enhanced categories, the Hochschild cohomology is computed as Ext\operatorname{Ext}^* of the identity functor, with group actions decomposing HHHH^* into invariant and twisted summands reflecting the category's autoequivalences (Perry, 2018).

In singular settings or for algebras of infinite global dimension, "singular Hochschild cohomology" replaces Ext\operatorname{Ext} in Db(A)D^b(A) by its singular quotient Dsg(Ae)D_{sg}(A^e), thus extending the Gerstenhaber and (for symmetric algebras) BV structures to the negative and Tate-theoretic region (Wang, 2015).

5. Applications in Deformation Theory and Algebraic Geometry

The space HH2(A)HH^2(A) controls infinitesimal deformations of the algebra AA (Gerstenhaber), classifies deformations of presheaf/multiplication structures (in the geometric context), and detects obstructions. Explicit descriptions associate summands of HH2HH^2 to "local multiplicative", "restriction map", or "twist" deformations for schemes, or to extension classes, as in the cluster-tilted context. In several important classes, dimension formulas for HH2HH^2 are related to the existence or absence of nontrivial deformations, reflecting rigidity or moduli phenomena (e.g., standard one-parametric self-injective algebras have HH2HH^2 of dimension one, yielding a unique nontrivial deformation direction) (Al-Kadi, 2011).

6. Further Structures and Invariants

Tables and structural theorems provide formulas for HHnHH^n in various algebraic classes:

Algebra/Class dimHH1\dim HH^1 dimHH2\dim HH^2 Cup Product Structure
Triangular string Combinatorial (Theorem 4.3) Combinatorial All cup products vanish for n,m>0n,m>0
Gentle Derived from ϕA\phi_A invariant Derived from ϕA\phi_A All higher products trivial
Self-injective biserial Closed form in n (mod 4)n\ (\bmod\ 4) Closed form, linear growth Multiplicative structure governed by periodicity in Koszul case

Hochschild cohomology is thus a highly structured, functorial, and categorically robust invariant, reflecting deformation theory, algebraic and topological symmetries, representation-theoretic data, and the deeper homotopy-theoretic properties of associative and ring-like objects across classical and higher contexts.

References:

(Lentner et al., 2017, Lodder, 2014, Wang, 2015, Mishchenko, 2018, Hellstrøm-Finnsen, 2016, Assem et al., 2012, Redondo et al., 2013, Liu et al., 2022, Al-Kadi, 2011, Liu et al., 2015, Furuya, 2014, Ladkani, 2012, Perry, 2018, Itaba et al., 2019)

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