2004
DOI: 10.1007/bf02829439
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Conductors and newforms for U(1,1)

Abstract: Abstract.Let F be a non-Archimedean local field whose residue characteristic is odd. In this paper we develop a theory of newforms for U(1, 1)(F), building on previous work on SL 2 (F). This theory is analogous to the results of Casselman for GL 2 (F) and Jacquet, Piatetski-Shapiro, and Shalika for GL n (F). To a representation π of U(1, 1)(F), we attach an integer c(π) called the conductor of π, which depends only on the L-packet Π containing π. A newform is a vector in π which is essentially fixed by a congr… Show more

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Cited by 10 publications
(11 citation statements)
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“…Therefore we need to consider only non-supercuspidal representations. Similar results are obtained by Lansky and Raguram for unramified U(1, 1) and for SL(2)( [8] and [9]), and by Roberts and Schmidt for PGSp(4) ( [14]).…”
Section: Introductionsupporting
confidence: 88%
See 1 more Smart Citation
“…Therefore we need to consider only non-supercuspidal representations. Similar results are obtained by Lansky and Raguram for unramified U(1, 1) and for SL(2)( [8] and [9]), and by Roberts and Schmidt for PGSp(4) ( [14]).…”
Section: Introductionsupporting
confidence: 88%
“…After Casselman [3], similar results are obtained by Jacquet, Piatetski-Shapiro and Shalika [6] and Reeder [13] for GL n (F ) and by Roberts and Schmidt [14] for PGSp (4). For unitary groups, there is a result by Lansky and Raguram [8]. They computed the dimensions of the spaces of vectors fixed by certain open compact subgroups of unramified U (1,1).…”
Section: Introductionmentioning
confidence: 99%
“…A companion to this article [Lansky and Raghuram 2004] deals with newforms for the quasisplit unramified unitary group U (1, 1). It would be of interest to generalize these results to other groups, namely, to SL n for higher n and for unitary groups in three variables (for instance the quasisplit unramified unitary group U (2, 1)).…”
Section: Introductionmentioning
confidence: 99%
“…Thus under the assumption that BC(π) = (ψ, Π) with JL(Π) cuspidal, we have attached a continuous 2-dimensional p-adic representation R 1 (π) to π (note that we have implicitly used the theory of the conductor for U (1, 1) developed in section 5 of [LR04]).…”
Section: Base Changementioning
confidence: 99%