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=== Antitone Galois connection === The above definition is common in many applications today, and prominent in [[lattice (order)|lattice]] and [[domain theory]]. However the original notion in Galois theory is slightly different. In this alternative definition, a Galois connection is a pair of ''antitone'', i.e. order-reversing, functions {{math|''F'' : ''A'' β ''B''}} and {{math|''G'' : ''B'' β ''A''}} between two posets {{mvar|A}} and {{mvar|B}}, such that :{{math|''b'' β€ ''F''(''a'')}} if and only if {{math|''a'' β€ ''G''(''b'')}}. The symmetry of {{mvar|F}} and {{mvar|G}} in this version erases the distinction between upper and lower, and the two functions are then called '''polarities''' rather than adjoints.{{sfn|Galatos|Jipsen|Kowalski|Ono|2007|p= 145}} Each polarity uniquely determines the other, since :{{math|''F''(''a'')}} is the largest element {{mvar|b}} with {{math|''a'' β€ ''G''(''b'')}}, and :{{math|''G''(''b'')}} is the largest element {{mvar|a}} with {{math|''b'' β€ ''F''(''a'')}}. The compositions {{math|''GF'' : ''A'' β ''A''}} and {{math|''FG'' : ''B'' β ''B''}} are the associated closure operators; they are monotone idempotent maps with the property {{math|''a'' β€ ''GF''(''a'')}} for all {{mvar|a}} in {{mvar|A}} and {{math|''b'' β€ ''FG''(''b'')}} for all {{mvar|b}} in {{mvar|B}}. The implications of the two definitions of Galois connections are very similar, since an antitone Galois connection between {{mvar|A}} and {{mvar|B}} is just a monotone Galois connection between {{mvar|A}} and the [[duality (order theory)|order dual]] {{math|''B''<sup>op</sup>}} of {{mvar|B}}. All of the below statements on Galois connections can thus easily be converted into statements about antitone Galois connections.
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