Cantor-Schröder-Bernstein theorem Created 2026-09-24 Updated 2026-10-18
If there are injections and , then there is a bijection .
For arbitrary sets and , the precise equivalence is
The reverse direction uses the bijection and its inverse function. Neither set is assumed to be a subset of the other: the hypothesis concerns functions, rather than containments. The forward direction holds in ZF without the axiom of choice.[ref]
This makes cardinality comparison an antisymmetric relation: if each set is no larger than the other in the sense of an injection, they have equal cardinality. It also gives a practical strategy: build two convenient injections and let the theorem supply the bijection. The Injection-chain proof of the Cantor-Schröder-Bernstein theorem explains how to combine them without losing an output or pairing two inputs with the same output.
With all variables ranging over the domain of the partially ordered set, the three first-order logic formulas are
The middle formula defines an antisymmetric relation; it does not forbid for distinct , but forbids both directions simultaneously for distinct elements.
In first-order logic with equality, the three first-order sentences are
A reflexive relation relates each element to itself. An antisymmetric relation forbids distinct elements from relating in both directions. A transitive relation contains every composite of two successive related pairs. Together these axioms define a partially ordered set.
The requested examples are binary relations on sets, rather than partially ordered sets: a partially ordered set necessarily has all three properties. This corrects the wording of the source.[ref]
For an antisymmetric relation and transitive relation that is not a reflexive relation, take and . No distinct pair relates both ways, so the antisymmetric relation condition holds. There are no composable pairs, so the transitive relation condition holds vacuously. Neither nor belongs to , so the reflexive relation condition fails.
For a reflexive relation and transitive relation that is not an antisymmetric relation, take and . All diagonal pairs and all composite pairs belong to , but and both hold with .
For a reflexive relation and antisymmetric relation that is not a transitive relation, take
All diagonal pairs are present, and no off-diagonal pair has its reverse present. However and hold while fails. Thus each pair of axioms can hold without the third.
A binary relation on is a subset of . Its properties are quantified over elements of :
Thus an equivalence relation is a binary relation that is simultaneously reflexive, symmetric and transitive. The equivalence class of is the set of all elements related to it:
Antisymmetry permits diagonal pairs and does not mean that a binary relation fails to be a symmetric relation.
For a binary relation , reflexivity means for every ; a symmetric relation satisfies for every ; an antisymmetric relation satisfies for every ; transitivity means for every ; an irreflexive relation satisfies for every . In particular, failure of reflexivity means at least one missing diagonal pair, whereas irreflexivity requires every diagonal pair to be missing.
No. On take . This is an antisymmetric relation because it contains no opposite pair of distinct elements. Its reflexive transitive closure contains every ordered pair: following the directed three-cycle reaches any vertex from any other. In particular it contains both and , violating antisymmetry.
This illustrates the reachability preorder: collapsing mutually reachable vertices into strongly connected components yields a partial order, but retaining all original vertices need not.
An upper bound of is an element with for every . It need not belong to . A maximum, or greatest element, is an with that same property. A least upper bound is an upper bound satisfying for every upper bound .
A maximum belongs to ; a least upper bound need not. In a partially ordered set, an existing maximum is automatically the least upper bound, and the antisymmetric relation condition makes each unique.
The displayed relation is not a partial order on the printed . Since the empty set belongs to , vacuous truth makes
hold for every finite , including nonempty . This violates the defining condition of an antisymmetric relation. It also violates transitivity: holds, but . Consequently the usual unique-maximum and unique-least upper bound terminology for a partially ordered set does not apply as claimed.
The available inputs still determine what happens if one applies the formulas in (b) literally to this relation:
FamilyElements satisfying the maximum formulaElements satisfying the least-upper-bound formula
None
and and
None and
For , no nonempty finite set can lie above all triples of arbitrarily large numbers, while does so vacuously. Thus is its sole literal upper bound, but is not a member of . For each of the two bounded families, the literal upper bounds are and all nonempty finite sets whose elements are at least . Among these, exactly and lie below every such upper bound. Both belong to , but neither belongs to its three-element subfamily.
For comparison, a natural correction is to retain the given rule for nonempty sets and declare to be a bottom element: no nonempty set is then below . Under this explicitly corrected partial order, has neither a maximum nor a least upper bound; has maximum and least upper bound ; and has no maximum but has least upper bound . A nonempty upper bound must have every element at least as large as every element of the bounded family. These corrected answers are conditional on the stated repair, not answers obtained by silently excluding the empty set from the source.
Check each partial order axiom. For every , and , so is a reflexive relation. If both and , the first coordinates satisfy and the second coordinates satisfy . Therefore and , which proves is an antisymmetric relation.
Finally, if and , then and . Hence , making a transitive relation. All three axioms hold, so is a partial order. It is a product order, with the usual order on the first coordinate and the reversed order on the second.
Take and . Their first coordinates are equal, so both and hold, although . Thus is not an antisymmetric relation, and hence it is not a partial order. The failure arises because its comparisons ignore the second coordinate entirely.
For a counterexample to closure under union of antisymmetric relations, take , , and . Each is an antisymmetric relation: neither contains an off-diagonal pair together with its reverse. But contains both and while . Therefore is not an antisymmetric relation.
For the pointwise order on real polynomials, proves reflexivity. Two opposite inequalities imply for every real ; the polynomials are therefore equal, proving the antisymmetric relation axiom. Chaining the inequalities at every proves transitivity.
To disprove total order, take and . The inequality fails at , whereas fails at . The order is partial but non-total.
For the product order, reflexivity follows from in every coordinate. If and , the antisymmetric relation axiom for the usual real order gives for every , hence . If , transitivity in each coordinate gives , hence . Thus this is a partial order.
For , the vectors and are incomparable: each has a coordinate larger than the corresponding coordinate of the other. It is not a total order for . The dimension qualification matters: for this is the usual total order on , so the printed non-totality claim needs the implicit assumption .
A least upper bound of is an element such that for every , and such that for every other upper bound of . It need not belong to . The antisymmetric relation axiom makes it unique whenever it exists.