371,209 research outputs found

    A Diophantine approximation problem with two primes and one k-power of a prime

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    We refine a result of the last two Authors on a Diophantine approximation problem with two primes and a k-th power of a prime which was only proved to hold for 1<k<4/3. We improve the k-range to 1<k 643 by combining Harman's technique on the minor arc with a suitable estimate for the L4-norm of the relevant exponential sum over primes Sk. In the common range we also give a stronger bound for the approximation

    A Diophantine problem with prime variables

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    We study the distribution of the values of the form λ1p1+λ2p2+λ3p3k\lambda_1 p_1 + \lambda_2 p_2 + \lambda_3 p_3^k, where λ1\lambda_1, λ2\lambda_2 and λ3\lambda_3 are non-zero real number not all of the same sign, with λ1/λ2\lambda_1 / \lambda_2 irrational, and p1p_1, p2p_2 and p3p_3 are prime numbers. We prove that, when 1<k<4/31 < k < 4 / 3, these value approximate rather closely any prescribed real number.Comment: submitte

    The number of Goldbach representations of an integer

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    We prove the following result: Let N2N \geq 2 and assume the Riemann Hypothesis (RH) holds. Then n=1NR(n)=N222ρNρ+1ρ(ρ+1)+O(Nlog3N), \sum_{n=1}^{N} R(n) =\frac{N^{2}}{2} -2 \sum_{\rho} \frac{N^{\rho + 1}}{\rho (\rho + 1)} + O(N \log^{3}N), where ρ=1/2+iγ\rho=1/2+i\gamma runs over the non-trivial zeros of the Riemann zeta function ζ(s)\zeta(s)

    Effective non-linear spinor dynamics in a spin-1 Bose-Einstein condensate

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    We derive from first principles the experimentally observed effective dynamics of a spinor Bose gas initially prepared as a Bose-Einstein condensate and then left free to expand ballistically. In spinor condensates, which represent one of the recent frontiers in the manipulation of ultra-cold atoms, particles interact with a two-body spatial interaction and a spin-spin interaction. The effective dynamics is governed by a system of coupled semi-linear Schr\"odinger equations: we recover this system, in the sense of marginals in the limit of infinitely many particles, with a mean-field re-scaling of the many-body Hamiltonian. When the resulting control of the dynamical persistence of condensation is quantified with the parameters of modern observations, we obtain a bound that remains quite accurate for the whole typical duration of the experiment.Comment: To appear on "Journal of Physics A: Mathematical and Theoretical" (2018

    A Vietoris-Smale mapping theorem for the homotopy of hyperdefinable sets

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    Results of Smale (1957) and Dugundji (1969) allow to compare the homotopy groups of two topological spaces XX and YY whenever a map f:XYf:X\to Y with strong connectivity conditions on the fibers is given. We apply similar techniques in o-minimal expansions of fields to compare the o-minimal homotopy of a definable set XX with the homotopy of some of its bounded hyperdefinable quotients X/EX/E. Under suitable assumption, we show that πn(X)defπn(X/E)\pi_{n}(X)^{\rm def}\cong\pi_{n}(X/E) and dim(X)=dimR(X/E)\dim(X)=\dim_{\mathbb R}(X/E). As a special case, given a definably compact group, we obtain a new proof of Pillay's group conjecture "dim(G)=dimR(G/G00\dim(G)=\dim_{\mathbb R}(G/G^{00})" largely independent of the group structure of GG. We also obtain different proofs of various comparison results between classical and o-minimal homotopy.Comment: 24 page

    On the constant in the Mertens product for arithmetic progressions. I. Identities

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    The aim of the paper is the proof of new identities for the constant in the Mertens product for arithmetic progressions. We deal with the problem of the numerical computation of these constants in another paper.Comment: References added, misprints corrected. 9 page

    A Ces\`aro Average of Goldbach numbers

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    Let Λ\Lambda be the von Mangoldt function and (rG(n)=m1+m2=nΛ(m1)Λ(m2))(r_G(n) = \sum_{m_1 + m_2 = n} \Lambda(m_1) \Lambda(m_2)) be the counting function for the Goldbach numbers. Let N2N \geq 2 be an integer. We prove that nNrG(n)(1n/N)kΓ(k+1)=N2Γ(k+3)2ρΓ(ρ)Γ(ρ+k+2)Nρ+1+ρ1ρ2Γ(ρ1)Γ(ρ2)Γ(ρ1+ρ2+k+1)Nρ1+ρ2+Ok(N1/2),\begin{align} &\sum_{n \le N} r_G(n) \frac{(1 - n/N)^k}{\Gamma(k + 1)} = \frac{N^2}{\Gamma(k + 3)} - 2 \sum_\rho \frac{\Gamma(\rho)}{\Gamma(\rho + k + 2)} N^{\rho+1}\\ &\qquad+ \sum_{\rho_1} \sum_{\rho_2} \frac{\Gamma(\rho_1) \Gamma(\rho_2)}{\Gamma(\rho_1 + \rho_2 + k + 1)} N^{\rho_1 + \rho_2} + \mathcal{O}_k(N^{1/2}), \end{align} for k>1k > 1, where ρ\rho, with or without subscripts, runs over the non-trivial zeros of the Riemann zeta-function ζ(s)\zeta(s).Comment: submitte

    Ghost imaging with the human eye

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    Computational ghost imaging relies on the decomposition of an image into patterns that are summed together with weights that measure the overlap of each pattern with the scene being imaged. These tasks rely on a computer. Here we demonstrate that the computational integration can be performed directly with the human eye. We use this human ghost imaging technique to evaluate the temporal response of the eye and establish the image persistence time to be around 20 ms followed by a further 20 ms exponential decay. These persistence times are in agreement with previous studies but can now potentially be extended to include a more precise characterisation of visual stimuli and provide a new experimental tool for the study of visual perception
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