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In [[mathematics]], the '''Selberg trace formula''', introduced by  {{harvtxt|Selberg|1956}}, is an expression for the character of the [[unitary representation]] of ''G'' on the space ''L''<sup>2</sup>(''G''/Γ) of [[square-integrable function]]s, where ''G'' is a [[Lie group]] and Γ a cofinite [[discrete group]]. The character is given by the trace of certain functions on ''G''.
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The simplest case is when Γ is [[cocompact]], when the representation breaks up into discrete summands. Here the trace formula is an extension of the [[Induced representation#Alternate formulations|Frobenius formula]] for the character of an [[induced representation]] of finite groups. When Γ is the cocompact subgroup '''Z''' of the real numbers ''G''='''R''', the Selberg trace formula is essentially the [[Poisson summation formula]].
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The case when ''G''/Γ is not compact is harder, because there is a [[continuous spectrum]], described using [[Eisenstein series]]. Selberg worked out the non-compact case when ''G'' is the group SL<sub>2</sub>('''R'''); the extension to higher rank groups is the [[Arthur-Selberg trace formula]].
 
When Γ is the fundamental group of a [[Riemann surface]], the Selberg trace formula describes the spectrum of differential operators such as the [[Laplacian]] in terms of geometric data involving the lengths of geodesics on the Riemann surface. In this case the Selberg trace formula is formally similar to the [[Explicit formulae (L-function)|explicit formulas]] relating the zeros of the [[Riemann zeta function]] to prime numbers, with the zeta zeros corresponding to eigenvalues of the Laplacian, and the primes corresponding to geodesics. Motivated by the analogy, Selberg introduced the [[Selberg zeta function]] of a Riemann surface, whose analytic properties are encoded by the Selberg trace formula.
 
==Early history==
Cases of particular interest include those for which the space is a [[compact Riemann surface]] ''S''. The initial publication in 1956 of [[Atle Selberg]] dealt with this case, its [[Laplacian]] differential operator and its powers. The traces of powers of a Laplacian can be used to define the [[Selberg zeta function]]. The  interest of this case was the  analogy between the formula obtained, and the [[explicit formula (L-function)|explicit formulae]] of [[prime number]] theory. Here the [[closed geodesic]]s on ''S'' play the role of prime numbers.
 
At the same time, interest in the traces of [[Hecke operator]]s was linked to the '''Eichler-Selberg trace formula''', of Selberg and [[Martin Eichler]], for a Hecke operator acting on a vector space of [[cusp form]]s of a given weight, for a given [[congruence subgroup]] of the [[modular group]]. Here the trace of the identity operator is the dimension of the vector space, i.e. the dimension of the space of modular forms of a given type: a quantity traditionally calculated by means of the [[Riemann-Roch theorem]].
 
==Applications==
The trace formula has applications to [[arithmetic geometry]] and [[number theory]].  For instance, using the trace theorem [[Eichler-Shimura theorem|Eichler and Shimura]] calculated the [[Hasse-Weil L-function]]s associated to [[modular curve]]s; [[Goro Shimura]]'s methods by-passed the analysis involved in the trace formula. The development of [[parabolic cohomology]] (from [[Eichler cohomology]]) provided a purely algebraic setting based on [[group cohomology]], taking account of the [[cusp form|cusps]] characteristic of non-compact Riemann surfaces and modular curves.
 
The trace formula also has purely [[differential geometry|differential-geometric]] applications. For instance, by a result of Buser, the [[length spectrum]] of a [[Riemann surface]] is an isospectral invariant, essentially by the trace formula.
 
==Later work==
The general theory of [[Eisenstein series]] was largely motivated by the requirement to separate out the [[continuous spectrum]], which is characteristic of the non-compact case.
 
The trace formula is often given for algebraic groups over the adeles rather than for Lie groups, because this makes the corresponding discrete subgroup &Gamma; into an algebraic group over a field which is technically easier to work with.
 
Contemporary successors of the theory are the [[Arthur-Selberg trace formula]] applying to the case of general semisimple ''G'', and the many studies of the trace formula in the [[Langlands philosophy]] (dealing with technical issues such as [[endoscopy (trace formula)|endoscopy]]). The Selberg trace formula can be derived from the Arthur-Selberg trace formula with some effort (see Palm).
 
==Selberg trace formula for compact hyperbolic surfaces==
A compact hyperbolic surface <math>X</math> can be written as
 
:<math>\Gamma \backslash \mathbb{H},</math>
 
where <math> \Gamma </math> is a subgroup of <math>PSL(2,\mathbb{R}).</math>
 
The Selberg trace formula for this case is easier than the general case because the surface is compact so there is no continuous spectrum, and the group &Gamma; has no parabolic or elliptic elements (other than the identity).
 
Then the spectrum for the [[Laplace-Beltrami operator]] on <math>X</math> is discrete and real, since the Laplace operator is self adjoint with compact [[resolvent formalism|resolvent]]; that is
 
:<math> 0 = \mu_0 < \mu_1 \leq \mu_2 \leq \cdots </math>
where the eigenvalues <math> \mu_n </math> correspond to &Gamma;-invariant eigenfunctions <math> u \in C^{\infty}(\mathbb{H}) </math>  of the Laplacian; in other words
 
:<math>
\begin{cases}
u(\gamma z)=u(z), \ \ \forall \gamma \in \Gamma \\
y^2 \left (u_{xx} + u_{yy} \right) + \mu_{n} u = 0.
\end{cases}
</math>
 
Using the variable substitution
 
:<math> \mu = s(1-s), s=\frac{1}{2}+ir </math>
the eigenvalues are labeled
 
:<math> r_{n}, n \geq 0. </math>
 
Then the '''Selberg trace formula''' is given by
 
:<math>
\sum_{n=0}^{\infty} h(r_n) =  \frac{\mu(F)}{4 \pi } \int_{-\infty}^{\infty} r \, h(r) \tanh(\pi r) dr  +  \sum_{ \{T\} } \frac{ \log N(T_0) }{ N(T)^{1/2} - N(T)^{-1/2} } g \left ( \log N(T) \right ).
</math>
 
The right hand side is a sum over conjugacy classes of the group &Gamma;, with the first term corresponding to the identity element and the remaining terms forming a sum over the other conjugacy classes<math> \lbrace T \rbrace </math> (which are all hyperbolic in this case).
The function <math> h </math> has to be an analytic function on <math> \vert \Im(r) \vert \leq 1/2+\delta </math>, satisfy
 
:<math> h(-r)=h(r), \  \vert h(r) \vert \leq M \left( 1+\vert \Re(r) \vert^{-2-\delta} \right ),</math>
 
where the numbers <math> \delta </math> and <math> M </math> are positive constants. The function <math> g </math> is the Fourier transform of <math> h </math>, that is,
 
<math> h(r) = \int_{-\infty}^{\infty} g(u) e^{iru} du. </math>
 
==References==
*{{Citation | last1=Fischer | first1=Jürgen | title=An approach to the Selberg trace formula via the Selberg zeta-function | publisher=[[Springer-Verlag]] | location=Berlin, New York | series=Lecture Notes in Mathematics | isbn=978-3-540-15208-8 | doi=10.1007/BFb0077696 | id={{MathSciNet | id = 892317}} | year=1987 | volume=1253}}
*{{Citation | author1-link=Israel Gelfand|last1=Gel'fand | first1=I. M. | last2=Graev | first2=M. I. | last3=Pyatetskii-Shapiro | first3=I. I. | title=Representation theory and automorphic functions | publisher=[[Academic Press]] | location=Boston, MA | series=Generalized Functions | isbn=978-0-12-279506-0 | id={{MathSciNet | id = 1071179}} | year=1990 | volume=6}}
*{{Citation | author=[[Dennis Hejhal|Hejhal, Dennis A.]] | title=The Selberg trace formula and the Riemann zeta function | url=http://projecteuclid.org/euclid.dmj/1077311789 | id={{MathSciNet | id = 0414490}} | year=1976 | journal=[[Duke Mathematical Journal]] | issn=0012-7094 | volume=43 | issue=3 | pages=441–482 | doi=10.1215/S0012-7094-76-04338-6}}
*{{Citation | last1=Hejhal | first1=Dennis A. | title=The Selberg trace formula for PSL(2,R). Vol. I | publisher=Springer-Verlag | location=Berlin, New York | series=Lecture Notes in Mathematics, Vol. 548 | doi=10.1007/BFb0079608 | id={{MathSciNet | id = 0439755}} | year=1976 | volume=548 | isbn=978-3-540-07988-0}}
*{{Citation | last1=Hejhal | first1=Dennis A. | title=The Selberg trace formula for  PSL(2,R). Vol. 2 | publisher=Springer-Verlag | location=Berlin, New York | series=Lecture Notes in Mathematics | isbn=978-3-540-12323-1 | doi=10.1007/BFb0061302 | id={{MathSciNet | id = 711197}} | year=1983 | volume=1001}}
*{{Citation | last1=McKean | first1=H. P. | title=Selberg's trace formula as applied to a compact Riemann surface | doi=10.1002/cpa.3160250302  | id={{MathSciNet | id = 0473166}} | year=1972 | journal=[[Communications on Pure and Applied Mathematics]] | issn=0010-3640 | volume=25 | pages=225–246 | issue=3}}
*{{Citation | last1=Palm | first1=Marc | title=Explicit GL(2) trace formulas and uniform, mixed Weyl laws | url=http://webdoc.sub.gwdg.de/diss/2012/palm/palm.pdf | year=2012 | journal=PhD thesis}}
*{{Citation | last1=Selberg | first1=Atle | authorlink=Atle Selberg|title=Harmonic analysis and discontinuous groups in weakly symmetric Riemannian spaces with applications to Dirichlet series | id={{MathSciNet | id = 0088511}} | year=1956 | journal=J. Indian Math. Soc. (N.S.) | volume=20 | pages=47–87}}
 
==External links==
*[http://www.maths.ex.ac.uk/~mwatkins/zeta/physics4.htm Selberg trace formula resource page]
 
[[Category:Automorphic forms]]

Revision as of 20:54, 3 March 2014

Sacs Longchamps Xxl

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