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Artin Conductor


The Artin conductor measures the ramification of a finite-dimensional Galois representation. Let L/K be a finite Galois extension of local fields, with Galois group G and lower ramification groups G_i, and let rho:G->GL(V) be such a representation. Its Artin conductor exponent is the nonnegative integer

 a(rho)=sum_(i>=0)(|G_i|)/(|G_0|)codimV^(G_i).

Here V^(G_i) is the subspace fixed by G_i. The term with i=0 is the contribution from tame ramification. The sum over i>=1 is the Swan conductor, which measures the contribution of wild ramification.

The local number is called a conductor exponent because, for a global representation, these exponents form the prime-power factors of its Artin conductor. The global conductor records the primes at which the representation is ramified (LMFDB). Related conductor invariants include the Swan conductor, elliptic curve conductor, and local conductor exponent.


See also

Elliptic Curve Conductor, Galois Representation, Local Conductor Exponent, Ramification Group, Swan Conductor, Tame Ramification, Wild Ramification

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References

LMFDB. "Conductor of an Artin Representation." https://www.lmfdb.org/knowledge/show/artin.conductor.Serre, J.-P. Local Fields. New York: Springer-Verlag, 1979.

Cite this as:

Weisstein, Eric W. "Artin Conductor." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/ArtinConductor.html

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