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首页> 外文期刊>Journal of Physics Communications >Quantum field theory, Feynman-, Wheeler propagators, dimensional regularization in configuration space and convolution of Lorentz Invariant Tempered Distributions
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Quantum field theory, Feynman-, Wheeler propagators, dimensional regularization in configuration space and convolution of Lorentz Invariant Tempered Distributions

机译:量子场论,Feynman-,Wheeler传播子,构型空间中的尺寸正则化和Lorentz不变回火分布的卷积

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The Dimensional Regularization (DR) of Bollini and Giambiagi (BG) can not be defined for all Schwartz Tempered Distributions Explicitly Lorentz Invariant (STDELI) S'_L. In this paper we overcome such limitation and show that it can be generalized to all aforementioned STDELI and obtain a product in a ring with zero divisors. For this purpose, we resort to a formula obtained by Bollini and Rocca and demonstrate the existence of the convolution (in Minkowskian space) of such distributions. This is done by following a procedure similar to that used so as to define a general convolution between the Ultradistributions of J Sebastiao e Silva (JSS), also known as Ultrahyperfunctions, obtained by Bollini et al. Using the Inverse Fourier Transform we get the ring with zero divisors S'_(LA), defined as S'_(LA) = F~(-1){S'_L}, where F~(-1) denotes the Inverse Fourier Transform. In this manner we effect a dimensional regularization inmomentum space (the ring S'_L) via convolution, and a product of distributions in the corresponding configuration space (the ring S'_(LA)). This generalizes the results obtained by BG for Euclidean space. We provide several examples of the application of our new results in Quantum Field Theory (QFT). In particular, the convolution of nmassless Feynman’s propagators and the convolution of nmassless Wheeler’s propagators in Minkowskian space. The results obtained in this work have already allowed us to calculate the classical partition function of Newtonian gravity, for the first time ever, in the Gibbs’ formulation and in the Tsallis’ one. It is our hope that this convolution will allow one to quantize non-renormalizable Quantum Field Theories (QFT’s).
机译:Bollini和Giambiagi(BG)的尺寸正则化(DR)不能为所有Schwartz钢化分布明确地定义为Lorentz不变(STDELI)S'_L。在本文中,我们克服了这种局限性,并表明可以将其推广到所有上述STDELI,并获得零除数成环的乘积。为此,我们求助于Bollini和Rocca获得的公式,并证明这种分布的卷积(在Minkowskian空间中)存在。这是通过遵循与用来定义Bollini等人获得的J Sebastiao e Silva(JSS)的超分布(也称为超超函数)之间的一般卷积相似的过程完成的。使用逆傅立叶变换,我们得到零除数为S'_(LA)的环,定义为S'_(LA)= F〜(-1){S'_L},其中F〜(-1)表示逆傅里叶变换。通过这种方式,我们通过卷积实现尺寸正则化动量空间(环S'_L),以及相应配置空间(环S'_(LA))中分布的乘积。这归纳了BG对于欧几里得空间获得的结果。我们提供了一些新结果在量子场论(QFT)中的应用实例。特别是在Minkowskian空间中无奈费恩曼传播子的卷积和无奈惠勒的传播器的卷积。这项工作中获得的结果已经使我们能够首次使用Gibbs公式和Tsallis公式计算牛顿引力的经典分配函数。我们希望这一卷积将使人们能够量化不可重归一化的量子场论(QFT)。

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