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首页> 外文期刊>The European physical journal, C. Particles and fields >A new numerical method for inverse Laplace transforms used to obtain gluon distributions from the proton structure function
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A new numerical method for inverse Laplace transforms used to obtain gluon distributions from the proton structure function

机译:拉普拉斯逆变换的新数值方法,用于从质子结构函数获得胶子分布

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摘要

We recently derived a very accurate and fast new algorithm for numerically inverting the Laplace transforms needed to obtain gluon distributions from the proton structure function F_2~(γp)(x, Q~2). We numerically inverted the function g (s), s being the variable in Laplace space, to G (v), where v is the variable in ordinary space. We have since discovered that the algorithm does not work if g (s)→0 less rapidly than 1/ s as s →∞, e.g., as 1/ s ~β for 0< β <1. In this note, we derive a new numerical algorithm for such cases, which holds for all positive and non-integer negative values of β. The new algorithm is exact if the original function G (v) is given by the product of a power v ~(β ?1) and a polynomial in v. We test the algorithm numerically for very small positive β, β =10 ~(?6) obtaining numerical results that imitate the Dirac delta function δ (v). We also devolve the published MSTW2008LO gluon distribution at virtuality Q ~2 =5 GeV ~2 down to the lower virtuality Q ~2 =1.69 GeV ~2. For devolution, β is negative, giving rise to inverse Laplace transforms that are distributions and not proper functions. This requires us to introduce the concept of Hadamard Finite Part integrals, which we discuss in detail.
机译:最近,我们导出了一种非常准确,快速的新算法,用于对从质子结构函数F_2〜(γp)(x,Q〜2)获得胶子分布所需的拉普拉斯变换进行数值求逆。我们将函数g(s)(s是拉普拉斯空间中的变量)从数值上反转为G(v),其中v是普通空间中的变量。此后,我们发现,如果g(s)→0的速度不如s→∞的1 / s快,例如,对于0 <β<1,则为1 / s〜β,则该算法无效。在本说明中,我们为这种情况导出了一种新的数值算法,该算法适用于所有β的正值和非整数负值。如果原始函数G(v)由幂v〜(β?1)与v的多项式的乘积给出,则新算法是精确的。我们对算法进行数值测试,以求非常小的正β,β= 10〜( Δ6)获得了模仿狄拉克δ函数δ(v)的数值结果。我们还将已发布的MSTW2008LO胶子分布从虚拟度Q〜2 = 5 GeV〜2降低到较低的虚拟度Q〜2 = 1.69 GeV〜2。对于下放,β为负,从而产生拉普拉斯逆变换,该逆拉普拉斯变换是分布而不是适当的函数。这要求我们引入Hadamard有限零件积分的概念,我们将对其进行详细讨论。

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