中国科学院数学与系统科学研究院期刊网

15 July 1952, Volume 2 Issue 4
    

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  • Acta Mathematica Sinica, Chinese Series. 1952, 2(4): 203-230. https://doi.org/10.12386/A1952sxxb0012
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    This paper gives detailed proofs of results announced in C.R.230(1950).We determine completely the squares in grassmannian manifolds.As a consequence we prove that for an(m-1)-sphere bundle the mod 2Stiefel-Whitney classes are all determined,with the aid of cup productsand squares,by those of dimensions a power of 2.
  • Acta Mathematica Sinica, Chinese Series. 1952, 2(4): 231-245. https://doi.org/10.12386/A1952sxxb0013
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    The spaces S_N considered in the present paper are of two structures,one being with an assigned K-dimensional areal metric and the other withan affine connection which depends upon the position as well as the K-pleelement,taken for the supporting element.These structures are connectedto each other such that the metric of any K-ple areal element is invariantwith respect to the parallel transport of the connection when the elementitself is taken for the supporting element.Letx~i=x~i(u~a) (i=1,...,N;α=1,...,K)be the equations of a differentiable K-dimensional variety V_K in S_N,andlet the'volume'of a certain domain R of the variety is given by a K-pleintegralA=∫_R F(x~k,p_a~i)(du)~k,where(du)~K is an abbreviation for du~1du~2...du~k and the functionF(x,p)is invariant under the transformationbut is positively homogeneous of order zero and weight unity under thetransformationSuppose that in S_N there is given a system of functions Γ_(jk)~i derivablefrom a system of generalized homogeneous functions H_(αβ)~i(x,p)by theformulaAccording to the above assumption these Γ's are related to the metricfunction F by the equations of connectionwhere Consider the infinitesimal transformationwhich carries the base variety V_K into infinitely near ones V_K and theelement(p_α~i)into the corresponding oneIt is assumed that all the V_K'S have a common boundary B_(K-1),so that(?)vanishes on B_(K-1).Denoting the Eulerian vector by E_i we obtain the first variation ofthe'volume'integral in the form whereandThe variety V_K characterized by the condition E_i=0 will be calledthe extremal variety of the space.On calculating the second variation ofthe'volume'integral for an extremal variety we are led to the result:where R_(ijz)~h denotes the affine curvature tensorandIn particular,when the coefficients of the affine connection Γ_(jk)~i arefunctions of position only the last equation takes the simple formIn this case we can put,for example,the functions H_(αβ)~i asthe space S_N then becomes the ordinary affinely connected one.Thisfurnishes a generalization of Davies'result for Riemannian spaces.
  • Acta Mathematica Sinica, Chinese Series. 1952, 2(4): 246-257. https://doi.org/10.12386/A1952sxxb0014
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    This note is a sequel to a previous one in which the geometry was as-sumed to be affine[1].Besides the notation newly introduced I shall usethe same notation.Let us assume that the space S_N is of affine connectionwhere H_(αβ)~i is a homogeneous function-system symmetric in the indicesα,β[2].Further,we need to add the condition that the function-systemconstructed at each point of a differentiable variety V_K of K dimensionsx~i=x~i(u~α)should be tensor-invariant under both sorts of transformations[3]Especially,under the latter the function-system H_(αβ)~i is transformed to(?) where we have placedConsequently,Γ_(jk)~i is transformed towith the abbreviationTherefore the function-system defined byis invariant under the parameter transformation.In the case ⊿=const.>0 we obtain the volumemary connection V_(jk)~i:Consider now the“volume integral”taken on a region R of V_K;the function F obeys the law Then follows the relationThis combined with the well-known identitysuffices to demonstrate thatIn attempting to obtain a tensor-invariant parallelism of any K-pleareal element(p_α~i)when the element itself is taken for the supporting ele-ment of the space we adopt Bortolotti's differential[4]:whereand impose the condition that the metric function F(x,p)should remainunchanged when the areal element (?) of the variety V_K is sub-jected to the parallel transportIt is easily shown that the equations of connections are the same as in theformer note,namely,or in virtue of the above relationIutroducing the covariant derivatives of vectorsξ~i(x,t)and(?)byusing the connection ccefficients V_(jk)~i,for example, (?)and adopting the notationwe are led to the second variation of the“volume integral”of an extremalvariety V_K:where B_(ijk)~h denotes the volumentary curvature tensor:
  • Acta Mathematica Sinica, Chinese Series. 1952, 2(4): 258-266. https://doi.org/10.12386/A1952sxxb0015
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    Let d_k(n)denote the number of expressions of n as a product of kfactors,and letIt is known thatIt was proved by Hardy and Littlewood[4]that by Tichmarsh[6]that β_4≦3/7.In this paper I prove thatk=4 5 6 7 8 9 10 11...;α_k≦1/2 4/7 5/8 71/107 41/59 31/43 26/35 19/25...;β_k≦23/54 1/2 35/62 11/18 149/230...;
  • Acta Mathematica Sinica, Chinese Series. 1952, 2(4): 267-274. https://doi.org/10.12386/A1952sxxb0016
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    The present note gives a reduction to E.G(?)tlind's axiom system forthe propositional calculus:(1)p∨p(?)p,(2)p(?)p∨q,(3)p(?)p,(4)(p(?)r)(?)(q∨p(?)r∨q).which he showed in a paper to be sufficient but with the independenceproblem left open.(I learn this only through a review of his paper byB.Jónsson(Math.Reviews,9(1948),p.1).)In I.it is shown that(3)is a consequence of(1),(2)and(4)(using-and ∨ as primitive junction symbols)and hence is superfluous.In Ⅱ.a proof of the mutual independence of(1),(2)and(4)is ap-pended;the proof of their sufficiency is easy(omitted);hence(1),(2)and(4)constitute a new axiom system for the propositional calculus.Finally,comparison of the new system with Hilbert's axiom systemsuggests a frequently occuring phenomenon,namely,the omission of thecommutative laws(or symmetric laws)contained in an axiom system can frequently be effected as a result of suitably permuting the variables con-tained in other axioms of the system.As another(new)example of thisphenomenon is given(ithout proof)the following result,which is asolution to Problem 64 in G.Birkhoff's Lattice Theory(revised edition,(1949)p.138):Birkhoff's axioms on a ternary operation(abc)for defin-ing a distributive lattice with O,I:(14),(15),(16)and(17)(see his bookp.137),in which(16)is a commutative law,are equivalent to the follow-ing(mutually independent.)ones:(14),(15)and(17')(d(abc)e)=((ebd)(dae)c).
  • Acta Mathematica Sinica, Chinese Series. 1952, 2(4): 275-287. https://doi.org/10.12386/A1952sxxb0017
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  • Acta Mathematica Sinica, Chinese Series. 1952, 2(4): 288-323. https://doi.org/10.12386/A1952sxxb0018
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    Let m and n be integers,n≧m≧1.Z=Z~(m,n) denotes m×n ma-trices with complex elements z_(jk)(j=1,2,...,m;k=1,2,...,n).The setof matrices Z making I~(n)-Z(?)positive definite is called the hyperbolicspace of m×n matrices.By means of the theory of representations,theauthor obtained explicitly the orthonormal system of this space.Forexample,as n=m,let A(X) and B(X) be two integral irreduciblerepresentations of dimensions a and b respectively,and A(U) and B(U)are unitary for unitary U.Consider(?)Multiplying on the left by A(U) and on the right by(?),we deduceA(U)Q=QB(U).By Schur's lemma,we obtain the orthogonalitybetween the elements of A(Z) and those of B(Z).By such a methodwe establish that the elements of all integral irreducible representationsform an orthogonal set.The comparatively more difficult part is to cal-culate the normalization factor,the kernel function being obtained directly from the orthonormal system.For m=n=2,some partial results havebeen obtained by J.Mitchell[1].For this space,Cauchy's formula has been obtained,the proceduredepending essentially on the fact that Cauchy's formula is a linear operatorcarrying the Hilbert space of functions on the characteristic manifold tothe Hilbert space of the functions,analytic in a bounded domain and onthe characteristic manifold.For m≠n,a better Cauchy's formula willbe given latter.