In the presence of randomness, a relativistic semimetal undergoes a quantumtransition towards a diffusive phase. A standard approach relates thistransition to the $U(N)$ Gross-Neveu model in the limit of $N o 0$, whilerare events were argued to be relevant close to the transition. In this work wereconcile previous studies by developing a functional renormalization groupamenable to include non-perturbative effects. We show that the previouslyconsidered fixed point is indeed infinitely unstable, confirming the necessityto describe fluctuations beyond the Gaussian approximation. Furthermore, thedisorder distribution renormalizes following the so-called porous mediumequation. We find that the transition is controlled by a non-analytic fixedpoint drastically different from the fixed point of the $U(N)$ Gross-Neveumodel. We relate a self-similar solution of the porous medium equation to amechanism of generation of a finite density of states at the nodal pointresponsible for the transition.
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机译:在随机性的情况下,一个半金属相对论经历朝向扩散相的quantumtransition。的标准方法涉及thistransition到的$ N 0 $,whilerare事件被认为是相关的接近的过渡限制$ U(N)$总-奈芙模型。在这项工作中通过开发功能重整化groupamenable包括非微扰效应wereconcile以前的研究。我们表明,previouslyconsidered定点确实是无限不稳定,证实超出了高斯近似的necessityto描述波动。此外,thedisorder分布renormalizes以下的所谓的多孔mediumequation。我们发现,转型是由非解析定点从$ U(N)$格罗斯 - Neveumodel的定点截然不同的控制。我们涉及生成状态的有限密度的amechanism在过渡节点pointresponsible多孔介质方程的自相似的解决方案。
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