2021
DOI: 10.48550/arxiv.2103.14325
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Invariant subspaces of elliptic systems I: pseudodifferential projections

Matteo Capoferri,
Dmitri Vassiliev

Abstract: Consider an elliptic self-adjoint pseudodifferential operator A acting on m-columns of half-densities on a closed manifold M , whose principal symbol is assumed to have simple eigenvalues. We show existence and uniqueness of m orthonormal pseudodifferential projections commuting with the operator A and provide an algorithm for the computation of their full symbols, as well as explicit closed formulae for their subprincipal symbols. Pseudodifferential projections yield a decomposition of L 2 (M ) into invariant… Show more

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Cited by 3 publications
(12 citation statements)
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“…Another important special case is that of nonnegative second order operators. For example, the operator of linear elasticity (Lamé operator) falls into this category, see [10,Subsection 8.2] for details. For such operators we have m = m + and the propagator is defined as…”
Section: Resultsmentioning
confidence: 99%
“…Another important special case is that of nonnegative second order operators. For example, the operator of linear elasticity (Lamé operator) falls into this category, see [10,Subsection 8.2] for details. For such operators we have m = m + and the propagator is defined as…”
Section: Resultsmentioning
confidence: 99%
“…We believe that the self-contained explicit construction presented here will prove useful in applications -see, for example, [4,15,5] and [24,25,26,43] -and be more accessible for the wider mathematical physics community. From a theoretical perspective, this paper complements the analysis of invariant subspaces of elliptic systems carried out in [12,13], and the spectral results therein.…”
mentioning
confidence: 76%
“…The operators P j from the above theorem form an orthonormal basis of pseudodifferential projections commuting with A, and an explicit algorithm for the construction of their full symbols was given in [12]. Pseudodifferential projections were exploited in [13] to partition the spectrum of A into precisely m infinite series of eigenvalues, singling out the contribution to the spectrum of A of individual eigenvalues of A prin (more details about this will be recalled later on).…”
Section: Statement Of the Problemmentioning
confidence: 99%
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