Perturbation of harmonic structures and an index-zero theorem

Bertram Walsh

Annales de l'institut Fourier (1970)

  • Volume: 20, Issue: 1, page 317-359
  • ISSN: 0373-0956

Abstract

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In the framework of an axiomatic theory of sheaves of “harmonic” functions, a notion of perturbation of these sheaves is introduced which corresponds to the replacement of the operator Δ by an operator Δ + f , in the classical situation. The “harmonic” functions with which the paper is concerned are assumed to satisfy certain hypotheses (weaker than the axioms of Bauer); it is shown that the perturbed harmonic functions also satisfy these hypotheses. Moreover, the results obtained imply that the dimensions of the spaces H 0 ( W , H ) and H 1 ( W , H ) are (finite and) equal whenever the base space W of a sheaf H satisfying these hypotheses is compact. That fact generalizes the classical theorem that the index of any second order elliptic operator on a (trivial bundle over a ) compact manifold is zero. Further, it implies that whenever H satisfies the Brelot axioms and its adjoint sheaf H * exists, the spaces H W and H W * (where W is again compact) have the same (finite) dimension.

How to cite

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Walsh, Bertram. "Perturbation of harmonic structures and an index-zero theorem." Annales de l'institut Fourier 20.1 (1970): 317-359. <http://eudml.org/doc/74005>.

@article{Walsh1970,
abstract = {In the framework of an axiomatic theory of sheaves of “harmonic” functions, a notion of perturbation of these sheaves is introduced which corresponds to the replacement of the operator $\Delta $ by an operator $\Delta +f$, in the classical situation. The “harmonic” functions with which the paper is concerned are assumed to satisfy certain hypotheses (weaker than the axioms of Bauer); it is shown that the perturbed harmonic functions also satisfy these hypotheses. Moreover, the results obtained imply that the dimensions of the spaces $H^0(W,\{\bf H\})$ and $H^1(W,\{\bf H\})$ are (finite and) equal whenever the base space $W$ of a sheaf $\{\bf H\}$ satisfying these hypotheses is compact. That fact generalizes the classical theorem that the index of any second order elliptic operator on a (trivial bundle over $a$) compact manifold is zero. Further, it implies that whenever $\{\bf H\}$ satisfies the Brelot axioms and its adjoint sheaf $\{\bf H\}^*$ exists, the spaces $\{\bf H\}_W$ and $\{\bf H\}^*_W$ (where $W$ is again compact) have the same (finite) dimension.},
author = {Walsh, Bertram},
journal = {Annales de l'institut Fourier},
keywords = {partial differential equations},
language = {eng},
number = {1},
pages = {317-359},
publisher = {Association des Annales de l'Institut Fourier},
title = {Perturbation of harmonic structures and an index-zero theorem},
url = {http://eudml.org/doc/74005},
volume = {20},
year = {1970},
}

TY - JOUR
AU - Walsh, Bertram
TI - Perturbation of harmonic structures and an index-zero theorem
JO - Annales de l'institut Fourier
PY - 1970
PB - Association des Annales de l'Institut Fourier
VL - 20
IS - 1
SP - 317
EP - 359
AB - In the framework of an axiomatic theory of sheaves of “harmonic” functions, a notion of perturbation of these sheaves is introduced which corresponds to the replacement of the operator $\Delta $ by an operator $\Delta +f$, in the classical situation. The “harmonic” functions with which the paper is concerned are assumed to satisfy certain hypotheses (weaker than the axioms of Bauer); it is shown that the perturbed harmonic functions also satisfy these hypotheses. Moreover, the results obtained imply that the dimensions of the spaces $H^0(W,{\bf H})$ and $H^1(W,{\bf H})$ are (finite and) equal whenever the base space $W$ of a sheaf ${\bf H}$ satisfying these hypotheses is compact. That fact generalizes the classical theorem that the index of any second order elliptic operator on a (trivial bundle over $a$) compact manifold is zero. Further, it implies that whenever ${\bf H}$ satisfies the Brelot axioms and its adjoint sheaf ${\bf H}^*$ exists, the spaces ${\bf H}_W$ and ${\bf H}^*_W$ (where $W$ is again compact) have the same (finite) dimension.
LA - eng
KW - partial differential equations
UR - http://eudml.org/doc/74005
ER -

References

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  1. [1] H. BAUER, Harmonische Räume und ihre Potentialtheorie, Springer Lecture Notes in Mathematics 22 (1966). Zbl0142.38402
  2. [2] N. BOBOC, C. CONSTANTINESCU and A. CORNEA, Axiomatic theory of harmonic functions. Nonnegative superharmonic functions, Ann. Inst. Fourier (Grenoble), 15 (1965), 283-312. Zbl0139.06604MR33 #1476
  3. [3] M. BRELOT, Lectures on Potential Theory, Tata Institute, Bombay, 1960. Zbl0098.06903MR22 #9749
  4. [4] C.H. DOWKER, Lectures on Sheaf Theory, Tata Institute, Bombay, 1957. 
  5. [5] N. DUNFORD and J.T. SCHWARTZ, Linear Operators I, Interscience, New York, 1958. Zbl0084.10402MR22 #8302
  6. [6] R.C. GUNNING and H. ROSSI, Analytic Functions of Several Complex Variables, Prentice-Hall, Englewood Cliffs, 1965. Zbl0141.08601MR31 #4927
  7. [7] R.M. HERVÉ, Recherches axiomatiques sur la théorie des fonctions surharmoniques et du potentiel, Ann. Inst. Fourier (Grenoble), 12 (1962), 415-571. Zbl0101.08103MR25 #3186
  8. [8] T. KATO, Perturbation Theory for Linear Operators, Springer, Berlin-Göttingen-Heidelberg, 1966. Zbl0148.12601MR34 #3324
  9. [9] P.A. MEYER, Brelot's axiomatic theory of the Dirichlet problem and Hunt's theory, Ann. Inst. Fourier (Grenoble), 13 (1963), 357-372. Zbl0116.30404MR29 #260
  10. [10] H. SCHAEFER, Topological Vector Spaces, Macmillan, New York, 1966. Zbl0141.30503MR33 #1689
  11. [11] B. WALSH, Flux in axiomatic potential theory. I : Cohomology, Inventiones Math. 8 (1969), 175-221. Zbl0179.15203MR42 #532
  12. [12] B. WALSH, Flux in axiomatic potential theory. II : Duality, Ann. Inst. Fourier, (Grenoble), 19 (1969). Zbl0181.11703MR42 #2023

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