95,709 research outputs found

    A simple proof of the Gauss-Bonnet-Chern formula for Finsler manifolds

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    From the point of view of index theory, we give a simple proof of a Gauss-Bonnet-Chern formula for all Finsler manifolds by the Cartan connection. Based on this, we establish a Gauss-Bonnet-Chern formula for any metric-compatible connection and also derive the Gauss-Bonnet-Chern formula of Lackey

    A Gauss-Bonnet-Chern theorem for Finsler vector bundles

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    In this paper, we give a simple proof of the Gauss-Bonnet-Chern theorem for a real oriented Finsler vector bundle with rank equal to the dimension of the base manifold. As an application, a Gauss-Bonnet-Chern formula for any metric-compatible connection is established on Finsler manifolds

    A comparison theorem for Finsler submanifolds and its applications

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    In this paper, we consider the conormal bundle over a submanifold in a Finsler manifold and establish a volume comparison theorem. As an application, we derive a lower estimate for length of closed geodesics in a Finsler manifold. In the reversible case, a lower bound of injective radius is also obtained

    Integral curvature bounds and diameter estimates on Finsler manifolds

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    In this paper, we study the integral curvatures of Finsler manifolds and prove several Myers type theorems

    A Gauss-Bonnet-Chern theorem for complex Finsler manifolds

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    In this paper, we establish a Gauss-Bonnet-Chern theorem for general closed complex Finsler manifolds

    The 2-adic valuations of differences of Stirling numbers of the second kind

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    Let m,n,km, n, k and cc be positive integers. Let ν2(k)\nu_2(k) be the 2-adic valuation of kk. By S(n,k)S(n,k) we denote the Stirling numbers of the second kind. In this paper, we first establish a convolution identity of the Stirling numbers of the second kind and provide a detailed 2-adic analysis to the Stirling numbers of the second kind. Consequently, we show that if 2mn2\le m\le n and cc is odd, then ν2(S(c2n+1,2m1)S(c2n,2m1))=n+1\nu_2(S(c2^{n+1},2^m-1)-S(c2^n, 2^m-1))=n+1 except when n=m=2n=m=2 and c=1c=1, in which case ν2(S(8,3)S(4,3))=6\nu_2(S(8,3)-S(4,3))=6. This solves a conjecture of Lengyel proposed in 2009.Comment: 20 page

    Divisibility by 2 of Stirling numbers of the second kind and their differences

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    Let n,k,an,k,a and cc be positive integers and bb be a nonnegative integer. Let ν2(k)\nu_2(k) and s2(k)s_2(k) be the 2-adic valuation of kk and the sum of binary digits of kk, respectively. Let S(n,k)S(n,k) be the Stirling number of the second kind. It is shown that ν2(S(c2n,b2n+1+a))s2(a)1,\nu_2(S(c2^n,b2^{n+1}+a))\geq s_2(a)-1, where 0<a<2n+10<a<2^{n+1} and 2c2\nmid c. Furthermore, one gets that ν2(S(c2n,(c1)2n+a))=s2(a)1\nu_2(S(c2^{n},(c-1)2^{n}+a))=s_2(a)-1, where n2n\geq 2, 1a2n1\leq a\leq 2^n and 2c2\nmid c. Finally, it is proved that if 3k2n3\leq k\leq 2^n and kk is not a power of 2 minus 1, then ν2(S(a2n,k)S(b2n,k))=n+ν2(ab)log2k+s2(k)+δ(k),\nu_2(S(a2^{n},k)-S(b2^{n},k))=n+\nu_2(a-b)-\lceil\log_2k\rceil +s_2(k)+\delta(k), where δ(4)=2\delta(4)=2, δ(k)=1\delta(k)=1 if k>4k>4 is a power of 2, and δ(k)=0\delta(k)=0 otherwise. This confirms a conjecture of Lengyel raised in 2009 except when kk is a power of 2 minus 1.Comment: 23 pages. To appear in Journal of Number Theor

    Revised Iterative Solution of Ground State of Double-Well Potential

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    A revised new iterative method based on Green function defined by quadratures along a single trajectory is developed and applied to solve the ground state of the double-well potential. The result is compared to the one based on the original iterative method. The limitation of the asymptotic expansion is also discussed.Comment: 19 page

    Revised Iterative Solution for Groundstate of Schroedinger Equation

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    A revised iterative method based on Green function defined by quadratures along a single trajectory is proposed to solve the low-lying quantum wave function for Schroedinger equation. Specially a new expression of the perturbed energy is obtained, which is much simpler than the traditional one. The method is applied to solve the unharmonic oscillator potential. The revised iteration procedure gives exactly the same result as those based on the single trajectory quadrature method. A comparison of the revised iteration method to the old one is made using the example of Stark effect. The obtained results are consistent to each other after making power expansion

    The universal Kummer congruences

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    Let pp be a prime. In this paper, we present a detailed pp-adic analysis to factorials and double factorials and their congruences. We give good bounds for the pp-adic sizes of the coefficients of the divided universal Bernoulli number B^nn{{\hat B_n}\over n} when nn is divisible by p1p-1. Using these we then establish the universal Kummer congruences modulo powers of a prime pp for the divided universal Bernoulli numbers B^nn{{\hat B_n}\over n} when nn is divisible by p1p-1.Comment: 20 pages. To appear in Journal of the Australian Mathematical Societ
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