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Nilpotent

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Inmathematics,an elementof aringis callednilpotentif there exists some positiveinteger,called theindex(or sometimes thedegree), such that.

The term, along with its sisteridempotent,was introduced byBenjamin Peircein the context of his work on the classification of algebras.[1]

Examples

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is nilpotent because.Seenilpotent matrixfor more.
  • In thefactor ring,theequivalence classof 3 is nilpotent because 32iscongruentto 0modulo9.
  • Assume that two elementsandin a ringsatisfy.Then the elementis nilpotent asAn example with matrices (fora,b):Hereand.

Properties

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No nilpotent element can be aunit(except in thetrivial ring,which has only a single element0 = 1). All nilpotent elements arezero divisors.

Anmatrixwith entries from afieldis nilpotent if and only if itscharacteristic polynomialis.

Ifis nilpotent, thenis aunit,becauseentails

More generally, the sum of a unit element and a nilpotent element is a unit when they commute.

Commutative rings

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The nilpotent elements from acommutative ringform anideal;this is a consequence of thebinomial theorem.This ideal is thenilradicalof the ring. Every nilpotent elementin a commutative ring is contained in everyprime idealof that ring, since.Sois contained in the intersection of all prime ideals.

Ifis not nilpotent, we are able tolocalizewith respect to the powers of:to get a non-zero ring.The prime ideals of the localized ring correspond exactly to those prime idealsofwith.[2]As every non-zero commutative ring has a maximal ideal, which is prime, every non-nilpotentis not contained in some prime ideal. Thusis exactly the intersection of all prime ideals.[3]

A characteristic similar to that ofJacobson radicaland annihilation of simple modules is available for nilradical: nilpotent elements of ringare precisely those that annihilate all integral domains internal to the ring(that is, of the formfor prime ideals). This follows from the fact that nilradical is the intersection of all prime ideals.

Nilpotent elements in Lie algebra

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Letbe aLie algebra.Then an elementis called nilpotent if it is inandis a nilpotent transformation. See also:Jordan decomposition in a Lie algebra.

Nilpotency in physics

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Anyladder operatorin a finite dimensional space is nilpotent. They representcreation and annihilation operators,which transform from one state to another, for example the raising and loweringPauli matrices.

Anoperandthat satisfiesis nilpotent.Grassmann numberswhich allow apath integralrepresentation for Fermionic fields are nilpotents since their squares vanish. TheBRST chargeis an important example inphysics.

As linear operators form an associative algebra and thus a ring, this is a special case of the initial definition.[4][5]More generally, in view of the above definitions, an operatoris nilpotent if there issuch that(thezero function). Thus, alinear mapis nilpotentiffit has a nilpotent matrix in some basis. Another example for this is theexterior derivative(again with). Both are linked, also throughsupersymmetryandMorse theory,[6]as shown byEdward Wittenin a celebrated article.[7]

Theelectromagnetic fieldof a plane wave without sources is nilpotent when it is expressed in terms of thealgebra of physical space.[8]More generally, the technique of microadditivity (which can used to derive theorems in physics) makes use of nilpotent or nilsquare infinitesimals and is partsmooth infinitesimal analysis.

Algebraic nilpotents

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The two-dimensionaldual numberscontain a nilpotent space. Other algebras and numbers that contain nilpotent spaces includesplit-quaternions(coquaternions),split-octonions, biquaternions,and complexoctonions.If a nilpotent infinitesimal is a variable tending to zero, it can be shown that any sum of terms for which it is the subject is an indefinitely small proportion of the first order term.

See also

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References

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  1. ^Polcino Milies & Sehgal (2002),An Introduction to Group Rings.p. 127.
  2. ^Matsumura, Hideyuki (1970). "Chapter 1: Elementary Results".Commutative Algebra.W. A. Benjamin. p. 6.ISBN978-0-805-37025-6.
  3. ^Atiyah, M. F.; MacDonald, I. G. (February 21, 1994). "Chapter 1: Rings and Ideals".Introduction to Commutative Algebra.Westview Press. p. 5.ISBN978-0-201-40751-8.
  4. ^Peirce, B.Linear Associative Algebra.1870.
  5. ^Polcino Milies, César; Sehgal, Sudarshan K.An introduction to group rings.Algebras and applications, Volume 1. Springer, 2002.ISBN978-1-4020-0238-0
  6. ^A. Rogers,The topological particle and Morse theory,Class. Quantum Grav. 17:3703–3714, 2000doi:10.1088/0264-9381/17/18/309.
  7. ^E Witten,Supersymmetry and Morse theory.J.Diff.Geom.17:661–692,1982.
  8. ^Rowlands, P.Zero to Infinity: The Foundations of Physics,London, World Scientific 2007,ISBN978-981-270-914-1