250
MATHEMATICS: J. W. ALEXANDER
PRoc. N. A. S.
of (3.4) and (4.1) Hence equations (6.1) admit solutions involving ""...
6 downloads
503 Views
190KB Size
Report
This content was uploaded by our users and we assume good faith they have the permission to share this book. If you own the copyright to this book and it is wrongfully on our website, we offer a simple DMCA procedure to remove your content from our site. Start by pressing the button below!
Report copyright / DMCA form
250
MATHEMATICS: J. W. ALEXANDER
PRoc. N. A. S.
of (3.4) and (4.1) Hence equations (6.1) admit solutions involving ""(i + 1) n(n + 1)/2 arbitrary constants, and consequently there are 2o2 Riemannian manifolds admitting a given simply transitive group as a group of motions, a result due to Bianchi.8 1 Space, Time, Matter, p. 112. The Mathematical Theory of Relativity, Chapter 7. 3These PROCEEDINGS, 8 and 9; Trans. Amer. Soc., 25 and 26; Annals, 24. 4Der Ricci-Kalkul, pp. 64, 65. 6 Invariantentheorie, pp. 318, 319. 6 Lie, Vorlesungen uber Continuerliche Gruppen, pp. 391, 396. 7 Crelle, 109, 1892, p. 121. 8 Lezioni Sulla Teoria dei Gruppi Continue Finiti, p. 517. 2
NOTE ON A THEOREM B Y H. KNESER By J. W. ALuXANDPR DEPARTMENT OF MATHEMATICS, PRINCETON UNIVERSITY
Communicated March 30, 1925
In a recent number of the Proceedings of the Royal Academy oj Amsterdam,' H. Kneser proves the following theorem: I. A necessary and szfficient condition that a connected n-dimensional manifold M? (n > 1) be separated into two and only two regions by every connected (n-1)-dimensional manifold M"-1 contained in MA is that the first Betti number Pl oJ M" be equal to unity and that there be no even coeffi-
cients of torsion of the lowest order. Kneser's proof is combinatorial and presupposes that M"1- always belongs to a cellular subdivision of M". It is perhaps worth noticing that the meaning of this theorem becomes very transparent in the light of the simplified, modulo 2 theory of connectivity, in which no distinction is made between positively and negatively oriented cells. Let us say that an n-complex is completely connected if it is possible to pass from anv n-cell of the complex to any other by a series of steps at each of which we go from an n-cell E" to an n-cell F" incident to the same (n- 1)-cell as En. Then, in the language of the modulo 2 theory, we have the following basic theorem which is almost self-evident. II. Let C" be any closed, irreducible n-complex and C-' any closed irreducible (n - 1)-complex made up of cells of Cn. Then, if C"-1 is bounding, it decomposes the complex C" into exactly two completely connected complexes C1 and C2, but if Cn-I is non-bounding, it leaves C" completely connected. The complexes C1 and C: which touch along C"' may also touch in certain cells of dimensionalities less than n-1.
VoL. 11, 1925
MA THEMA TICS: J. W. ALEXA NDER
251
For suppose an irreducible sub-complex C- 1 of C" decomposes C' into two or more completely connected complexes Ci'. Evidently the boundary of each of the regions C' is made up of cells of C"- ' Therefore, since C"is irreducible, it must be the complete boundary of each complex C'. It follows that if C"l is non-bounding, it has to leave Cn completely connected. On the other hand, if the irreducible complex C"-' bounds a complex Clr, it also bounds the complex C2 = C" - Cl. It cannot bound more than twice, otherwise Cn would contain Cr + C2' as a proper closed sub-complex, contrary to the assumption about the irreducibility of Cn. This proves the theorem. As a corollary we have at once: III. A necessary and sufficient condition that every closed irreducible (n - 1)-complex C"- 1 decompose the closed, irreducible n-complex C" into exactly two completely connected complexes Cj' and C: is that the (n-1) - th connectivity number R"1 be equal to unity. The condition R"- = 1 is the essential thing. If the complex C" happens to determine a manifold, then, by the well known duality theorem, Rn-l = Rly where R1 is the first connectivity number of the manifold. Moreover, since we have the simple general relation. R' = P1 + h, where PI is the first Betti number of the manifold and h the number of even coefficients of torsion of lowest order, we may replace the condition R"-1 = 1 by Kneser's condition that pI be equal to unity and that there be no even coefficients of torsion of lowest order. To prove Theorem I, we now have only to prove (1) that if C" of Theorem II determines a manifold, the completely connected complexes C', and C2 can touch in points of C"'- only, otherwise C" would possess a singular point, and (2) that if the irreducible complex C"' fails to determine a manifold M"- because of singularities, there is always a neighboring irreducible complex Co"1 without singularities and homologous to c"'. This may be proved in the manner indicated by Kneser.2 1 Proc. Amsterdam, 27, Nos. 7 and 8, Sept. 27, 1924, pp. 1-156. A detailed exposition of the theory at connectivity mod 2 is given in Veblen's Cambridge Colloquium Lectures. See also Veblen, Decomposition of N-Space by a Polyhedron, Trans. Amer. Math. Soc., 14, 65-72 (1913). 2