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arXiv 1401.3299hep-thhep-lat
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具有非平凡测度项的欧氏动态三角剖分研究

Exploring Euclidean Dynamical Triangulations with a Non-trivial Measure Term

Daniel Coumbe, John Laiho

摘要:

研究了在路径积分中引入非平凡测度项的欧氏动力学三角剖分(EDT)下的量子引力的非微扰形式。我们的动机是重新审视这个老配方的动力学三角形的暗示,从重整化群的方法,重力可能是渐近安全的,并出现了一个半经典阶段的因果动力学三角形(CDT)。我们研究了这个模型的相图,并确定了两个阶段,这是众所周知的从以前的工作:支化聚合物相和塌陷相。我们验证的相变划分支化的聚合物相从塌陷相的顺序几乎肯定是一阶的。非平凡测度项扩大了相图,使我们能够探索相图中被称为褶皱区的区域。尽管在文献中已经广泛地研究了塌陷和支化的聚合物相,但是褶皱区域没有受到相同的仔细检查。我们发现,起皱的区域可能是特别大的有限尺寸效应的崩溃阶段的一部分。有趣的是,在小体积下,卷曲区域的光谱维数的行为与CDT的相似,正如arXiv:1104.5505中首次报道的那样,但对于足够大的体积,卷曲区域似乎没有4维半经典特征。因此,我们发现EDT配方的褶皱区域不具有CDT延长相的良好特征,正如我们在arXiv:1104.5505中首次提出的那样。这与arXiv:1307.2270的最新结果一致,其中作者使用了与本文所述略有不同的EDT离散化。

英文摘要:

We investigate a nonperturbative formulation of quantum gravity defined via Euclidean dynamical triangulations (EDT) with a non-trivial measure term in the path integral. We are motivated to revisit this older formulation of dynamical triangulations by hints from renormalization group approaches that gravity may be asymptotically safe and by the emergence of a semiclassical phase in causal dynamical triangulations (CDT). We study the phase diagram of this model and identify the two phases that are well known from previous work: the branched polymer phase and the collapsed phase. We verify that the order of the phase transition dividing the branched polymer phase from the collapsed phase is almost certainly first-order. The nontrivial measure term enlarges the phase diagram, allowing us to explore a region of the phase diagram that has been dubbed the crinkled region. Although the collapsed and branched polymer phases have been studied extensively in the literature, the crinkled region has not received the same scrutiny. We find that the crinkled region is likely a part of the collapsed phase with particularly large finite-size effects. Intriguingly, the behavior of the spectral dimension in the crinkled region at small volumes is similar to that of CDT, as first reported in arXiv:1104.5505, but for sufficiently large volumes the crinkled region does not appear to have 4-dimensional semiclassical features. Thus, we find that the crinkled region of the EDT formulation does not share the good features of the extended phase of CDT, as we first suggested in arXiv:1104.5505. This agrees with the recent results of arXiv:1307.2270, in which the authors used a somewhat different discretization of EDT from the one presented here.

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