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In mathematics, the annihilator of a
subset In mathematics, set ''A'' is a subset of a set ''B'' if all elements of ''A'' are also elements of ''B''; ''B'' is then a superset of ''A''. It is possible for ''A'' and ''B'' to be equal; if they are unequal, then ''A'' is a proper subset o ...
of a module over a ring is the ideal formed by the elements of the ring that give always zero when multiplied by an element of . Over an
integral domain In mathematics, specifically abstract algebra, an integral domain is a nonzero commutative ring in which the product of any two nonzero elements is nonzero. Integral domains are generalizations of the ring of integers and provide a natural s ...
, a module that has a nonzero annihilator is a torsion module, and a finitely generated torsion module has a nonzero annihilator. The above definition applies also in the case noncommutative rings, where the left annihilator of a left module is a left ideal, and the right-annihilator, of a right module is a right ideal.


Definitions

Let ''R'' be a ring, and let ''M'' be a left ''R''- module. Choose a non-empty subset ''S'' of ''M''. The annihilator of ''S'', denoted Ann''R''(''S''), is the set of all elements ''r'' in ''R'' such that, for all ''s'' in ''S'', . In set notation, :\mathrm_R(S)=\ It is the set of all elements of ''R'' that "annihilate" ''S'' (the elements for which ''S'' is a torsion set). Subsets of right modules may be used as well, after the modification of "" in the definition. The annihilator of a single element ''x'' is usually written Ann''R''(''x'') instead of Ann''R''(). If the ring ''R'' can be understood from the context, the subscript ''R'' can be omitted. Since ''R'' is a module over itself, ''S'' may be taken to be a subset of ''R'' itself, and since ''R'' is both a right and a left ''R'' module, the notation must be modified slightly to indicate the left or right side. Usually \ell.\!\mathrm_R(S)\, and r.\!\mathrm_R(S)\, or some similar subscript scheme are used to distinguish the left and right annihilators, if necessary. If ''M'' is an ''R''-module and , then ''M'' is called a faithful module.


Properties

If ''S'' is a subset of a left ''R'' module ''M'', then Ann(''S'') is a left ideal of ''R''. If ''S'' is a
submodule In mathematics, a module is a generalization of the notion of vector space in which the field of scalars is replaced by a ring. The concept of ''module'' generalizes also the notion of abelian group, since the abelian groups are exactly the ...
of ''M'', then Ann''R''(''S'') is even a two-sided ideal: (''ac'')''s'' = ''a''(''cs'') = 0, since ''cs'' is another element of ''S''. If ''S'' is a subset of ''M'' and ''N'' is the submodule of ''M'' generated by ''S'', then in general Ann''R''(''N'') is a subset of Ann''R''(''S''), but they are not necessarily equal. If ''R'' is
commutative In mathematics, a binary operation is commutative if changing the order of the operands does not change the result. It is a fundamental property of many binary operations, and many mathematical proofs depend on it. Most familiar as the name o ...
, then the equality holds. ''M'' may be also viewed as a ''R''/Ann''R''(''M'')-module using the action \overlinem:=rm\,. Incidentally, it is not always possible to make an ''R'' module into an ''R''/''I'' module this way, but if the ideal ''I'' is a subset of the annihilator of ''M'', then this action is well-defined. Considered as an ''R''/Ann''R''(''M'')-module, ''M'' is automatically a faithful module.


For commutative rings

Throughout this section, let R be a commutative ring and M a finitely generated (for short, finite) R-module.


Relation to support

Recall that the support of a module is defined as :\operatornameM = \. Then, when the module is finitely generated, there is the relation :V(\operatorname_R(M)) = \operatornameM, where V(\cdot) is the set of prime ideals containing the subset.


Short exact sequences

Given a
short exact sequence An exact sequence is a sequence of morphisms between objects (for example, groups, rings, modules, and, more generally, objects of an abelian category) such that the image of one morphism equals the kernel of the next. Definition In the conte ...
of modules, :0 \to M' \to M \to M'' \to 0, the support property :\operatornameM = \operatornameM' \cup \operatornameM'', together with the relation with the annihilator implies :V(\operatorname_R(M)) = V(\operatorname_R(M')) \cup V(\operatorname_R(M'')). More specifically, we have the relations :\operatorname_R(M') \cap \operatorname_R(M'') \supseteq \operatorname_R(M) \supseteq \operatorname_R(M') \operatorname_R(M''). If the sequence splits then the inequality on the left is always an equality. In fact this holds for arbitrary direct sums of modules, as :\operatorname_R\left( \bigoplus_ M_i \right) = \bigcap_ \operatorname_R(M_i).


Quotient modules and annihilators

Given an ideal I \subseteq R and let M be a finite module, then there is the relation :\text(M/IM) = \operatornameM \cap V(I) on the support. Using the relation to support, this gives the relation with the annihilator :V(\text_R(M/IM)) = V(\text_R(M)) \cap V(I).


Examples


Over the integers

Over \mathbb any finitely generated module is completely classified as the direct sum of its free part with its torsion part from the fundamental theorem of abelian groups. Then, the annihilator of a finite module is non-trivial only if it is entirely torsion. This is because :\text_(\mathbb^) = \ = (0) since the only element killing each of the \mathbb is 0. For example, the annihilator of \mathbb/2 \oplus \mathbb/3 is :\text_\mathbb(\mathbb/2 \oplus \mathbb/3) = (6) = (\text(2,3)), the ideal generated by (6). In fact the annihilator of a torsion module :M \cong \bigoplus_^n (\mathbb/a_i)^ is isomorphic to the ideal generated by their
least common multiple In arithmetic and number theory, the least common multiple, lowest common multiple, or smallest common multiple of two integers ''a'' and ''b'', usually denoted by lcm(''a'', ''b''), is the smallest positive integer that is divisible by bo ...
, (\operatorname(a_1, \ldots, a_n)). This shows the annihilators can be easily be classified over the integers.


Over a commutative ring ''R''

In fact, there is a similar computation that can be done for any finite module over a commutative ring R. Recall that the definition of finiteness of M implies there exists a right-exact sequence, called a presentation, given by :R^ \xrightarrow R^ \to M \to 0 where \phi is in \text_(R). Writing \phi explicitly as a
matrix Matrix most commonly refers to: * ''The Matrix'' (franchise), an American media franchise ** '' The Matrix'', a 1999 science-fiction action film ** "The Matrix", a fictional setting, a virtual reality environment, within ''The Matrix'' (franchi ...
gives it as :\phi = \begin \phi_ & \cdots & \phi_ \\ \vdots & & \vdots \\ \phi_ & \cdots & \phi_ \end hence M has the direct sum decomposition :M = \bigoplus_^k \frac If we write each of these ideals as :I_i = (\phi_(1), \ldots, \phi_(1)) then the ideal I given by :V(I) = \bigcup^_V(I_i) presents the annihilator.


Over ''k'' 'x'',''y''

Over the commutative ring k ,y/math> for a field k, the annihilator of the module :M = \frac \oplus \frac is given by the ideal :\text_(M) = ((x^2 - y)(y - 3)).


Chain conditions on annihilator ideals

The lattice of ideals of the form \ell.\!\mathrm_R(S) where ''S'' is a subset of ''R'' comprise a
complete lattice In mathematics, a complete lattice is a partially ordered set in which ''all'' subsets have both a supremum (join) and an infimum (meet). A lattice which satisfies at least one of these properties is known as a ''conditionally complete lattice.'' S ...
when partially ordered by inclusion. It is interesting to study rings for which this lattice (or its right counterpart) satisfy the
ascending chain condition In mathematics, the ascending chain condition (ACC) and descending chain condition (DCC) are finiteness properties satisfied by some algebraic structures, most importantly ideals in certain commutative rings.Jacobson (2009), p. 142 and 147 These ...
or
descending chain condition In mathematics, the ascending chain condition (ACC) and descending chain condition (DCC) are finiteness properties satisfied by some algebraic structures, most importantly ideals in certain commutative rings.Jacobson (2009), p. 142 and 147 These ...
. Denote the lattice of left annihilator ideals of ''R'' as \mathcal\, and the lattice of right annihilator ideals of ''R'' as \mathcal\,. It is known that \mathcal\, satisfies the A.C.C.
if and only if In logic and related fields such as mathematics and philosophy, "if and only if" (shortened as "iff") is a biconditional logical connective between statements, where either both statements are true or both are false. The connective is bi ...
\mathcal\, satisfies the D.C.C., and symmetrically \mathcal\, satisfies the A.C.C. if and only if \mathcal\, satisfies the D.C.C. If either lattice has either of these chain conditions, then ''R'' has no infinite orthogonal sets of idempotents. If ''R'' is a ring for which \mathcal\, satisfies the A.C.C. and ''R''''R'' has finite uniform dimension, then ''R'' is called a left Goldie ring.


Category-theoretic description for commutative rings

When ''R'' is commutative and ''M'' is an ''R''-module, we may describe Ann''R''(''M'') as the
kernel Kernel may refer to: Computing * Kernel (operating system), the central component of most operating systems * Kernel (image processing), a matrix used for image convolution * Compute kernel, in GPGPU programming * Kernel method, in machine lea ...
of the action map determined by the adjunct map of the identity along the
Hom-tensor adjunction In mathematics, the tensor-hom adjunction is that the tensor product - \otimes X and hom-functor \operatorname(X,-) form an adjoint pair: :\operatorname(Y \otimes X, Z) \cong \operatorname(Y,\operatorname(X,Z)). This is made more precise below. T ...
. More generally, given a
bilinear map In mathematics, a bilinear map is a function combining elements of two vector spaces to yield an element of a third vector space, and is linear in each of its arguments. Matrix multiplication is an example. Definition Vector spaces Let V, ...
of modules F\colon M \times N \to P, the annihilator of a subset S \subseteq M is the set of all elements in N that annihilate S: :\operatorname(S) := \ . Conversely, given T \subseteq N, one can define an annihilator as a subset of M. The annihilator gives a
Galois connection In mathematics, especially in order theory, a Galois connection is a particular correspondence (typically) between two partially ordered sets (posets). Galois connections find applications in various mathematical theories. They generalize the fu ...
between subsets of M and N, and the associated
closure operator In mathematics, a closure operator on a set ''S'' is a function \operatorname: \mathcal(S)\rightarrow \mathcal(S) from the power set of ''S'' to itself that satisfies the following conditions for all sets X,Y\subseteq S : Closure operators are d ...
is stronger than the span. In particular: * annihilators are submodules * \operatornameS \leq \operatorname(\operatorname(S)) * \operatorname(\operatorname(\operatorname(S))) = \operatorname(S) An important special case is in the presence of a nondegenerate form on a
vector space In mathematics and physics, a vector space (also called a linear space) is a set whose elements, often called '' vectors'', may be added together and multiplied ("scaled") by numbers called '' scalars''. Scalars are often real numbers, but ...
, particularly an
inner product In mathematics, an inner product space (or, rarely, a Hausdorff pre-Hilbert space) is a real vector space or a complex vector space with an operation called an inner product. The inner product of two vectors in the space is a scalar, often ...
: then the annihilator associated to the map V \times V \to K is called the
orthogonal complement In the mathematical fields of linear algebra and functional analysis, the orthogonal complement of a subspace ''W'' of a vector space ''V'' equipped with a bilinear form ''B'' is the set ''W''⊥ of all vectors in ''V'' that are orthogonal to every ...
.


Relations to other properties of rings

Given a module ''M'' over a Noetherian commutative ring ''R'', a prime ideal of ''R'' that is an annihilator of a nonzero element of ''M'' is called an
associated prime In abstract algebra, an associated prime of a module ''M'' over a ring ''R'' is a type of prime ideal of ''R'' that arises as an annihilator of a (prime) submodule of ''M''. The set of associated primes is usually denoted by \operatorname_R(M ...
of ''M''. *Annihilators are used to define left Rickart rings and Baer rings. *The set of (left)
zero divisor In abstract algebra, an element of a ring is called a left zero divisor if there exists a nonzero in such that , or equivalently if the map from to that sends to is not injective. Similarly, an element of a ring is called a right zero ...
s ''D''''S'' of ''S'' can be written as ::D_S = \bigcup_. :(Here we allow zero to be a zero divisor.) :In particular ''DR'' is the set of (left) zero divisors of ''R'' taking ''S'' = ''R'' and ''R'' acting on itself as a left ''R''-module. *When ''R'' is commutative and Noetherian, the set D_R is precisely equal to the union of the
associated prime In abstract algebra, an associated prime of a module ''M'' over a ring ''R'' is a type of prime ideal of ''R'' that arises as an annihilator of a (prime) submodule of ''M''. The set of associated primes is usually denoted by \operatorname_R(M ...
s of the ''R''-module ''R''.


See also

* Socle * Support of a module *
Faltings' annihilator theorem In abstract algebra (specifically commutative ring theory Commutative algebra, first known as ideal theory, is the branch of algebra that studies commutative rings, their ideals, and modules over such rings. Both algebraic geometry and a ...


Notes


References

* * Israel Nathan Herstein (1968) ''Noncommutative Rings'', Carus Mathematical Monographs #15, Mathematical Association of America, page 3. * * Richard S. Pierce. ''Associative algebras''. Graduate texts in mathematics, Vol. 88, Springer-Verlag, 1982, {{ISBN, 978-0-387-90693-5 Ideals (ring theory) Module theory Ring theory