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    Diophantine approximation by special primes

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    We show that whenever δ>0\delta>0, η\eta is real and constants λi\lambda_i satisfy some necessary conditions, there are infinitely many prime triples p1,p2,p3p_1,\, p_2,\, p_3 satisfying the inequality λ1p1+λ2p2+λ3p3+η<(maxpj)1/12+δ|\lambda_1p_1 + \lambda_2p_2 + \lambda_3p_3+\eta|<(\max p_j)^{-1/12+\delta} and such that, for each i{1,2,3}i\in\{1,2,3\}, pi+2p_i+2 has at most 2828 prime factors

    Left-handed nuclei

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    The orientation of the angular momentum vector with respect to the triaxial density distribution selects a left-handed or right-handed system principal axes. This breaking of chiral symmetry manifests itself as pairs of nearly identical ΔI=1\Delta I=1-bands. The chiral structures combine high-j particles and high-j holes with a triaxial rotor. Tilted axis cranking calculations predict the existence of such configurations in different mass regions. There is experimental evidence in odd-odd nuclei around mass 134. The quantized motion of the angular momentum vector between the left- and right-handed configurations, which causes the splitting between the chiral sister bands, can be classified as tunneling (chiral rotors) or oscillation (chiral vibrators).Comment: Invited lecture at the Conference on Frontiers of Nuclear Structure, Berkeley, 200
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