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Related papers: Line of fixed points in a bosonic tensor model

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A general mechanism for the loss of conformal invariance is the merger and disappearance of an infrared fixed point and an ultraviolet fixed point of a renormalization group flow. We show explicitly how this mechanism works in the case of…

Quantum Gases · Physics 2018-08-08 Abhishek Mohapatra , Eric Braaten

We study the renormalization group flow of the Lagrangian for statistical and quantum systems by representing their path integral in terms of a tensor network. Using a tensor-entanglement-filtering renormalization (TEFR) approach that…

Strongly Correlated Electrons · Physics 2010-11-02 Zheng-Cheng Gu , Xiao-Gang Wen

We study the two-dimensional N-component Landau-Ginzburg Hamiltonian with cubic anisotropy. We compute and analyze the fixed-dimension perturbative expansion of the renormalization-group functions to four loops. The relations of these…

Statistical Mechanics · Physics 2009-11-07 Pasquale Calabrese , Alessio Celi

We show that non-perturbative fixed points of the exact renormalization group, their perturbations and corresponding massive field theories can all be determined directly in the continuum -- without using bare actions or any tuning…

High Energy Physics - Theory · Physics 2009-10-30 Tim R. Morris

Classifying perturbative fixed points near upper critical dimensions plays an important role in understanding the space of conformal field theories and critical phases of matter. In this work, we consider perturbative fixed points of $N=5$…

High Energy Physics - Theory · Physics 2024-02-07 Junchen Rong , Slava Rychkov

The noncommutative selfdual \phi^3 model in 6 dimensions is quantized and essentially solved, by mapping it to the Kontsevich model. The model is shown to be renormalizable and asymptotically free, and solvable genus by genus. It requires…

High Energy Physics - Theory · Physics 2009-03-16 Harald Grosse , Harold Steinacker

We study the double scaling limit of the $O(N)^3$-invariant tensor model, initially introduced in Carrozza and Tanasa, Lett. Math. Phys. (2016). This model has an interacting part containing two types of quartic invariants, the tetrahedric…

High Energy Physics - Theory · Physics 2022-08-15 Valentin Bonzom , Victor Nador , Adrian Tanasa

We search for infrared fixed points of Gross-Neveu Yukawa models with matrix degrees of freedom in $d=4-\varepsilon$. We consider three models -- a model with $SU(N)$ symmetry in which the scalar and fermionic fields both transform in the…

High Energy Physics - Theory · Physics 2024-01-15 Shiroman Prakash , Shubham Kumar Sinha

We calculate the static critical behavior of systems of $O(n_\|)\oplus O(n_\perp)$ symmetry by renormalization group method within the minimal subtraction scheme in two loop order. Summation methods lead to fixed points describing…

Statistical Mechanics · Physics 2009-11-13 R. Folk , Yu. Holovatch , G. Moser

We study $T\bar{T}$-deformed $O(N)$ scalar field theory in two-dimensional spacetime using the functional renormalization group. We derive the $\beta$ functions for the couplings in the system and explore the fixed points. In addition to…

High Energy Physics - Theory · Physics 2024-03-15 Jie Liu , Junichi Haruna , Masatoshi Yamada

We apply the functional renormalization group to an Abelian Group Field Theory extended beyond the branched-polymer (melonic) sector by including interactions that are subdominant from a power-counting perspective but enhanced by derivative…

High Energy Physics - Theory · Physics 2026-05-05 Seke Fawaaz Zime Yerima , Vincent Lahoche , Dine Ousmane Samary

The Regge-Gribov model of the pomeron and odderon in the non-trivial transverse space is studied by the renormalization group technique. The single loop approximation is adopted. Five real fixed points are found and the high-energy…

High Energy Physics - Theory · Physics 2024-06-28 M. A. Braun , E. M. Kuzminskii , M. I. Vyazovsky

We study three dimensional O(N)_k and U(N)_k Chern-Simons theories coupled to a scalar field in the fundamental representation, in the large N limit. For infinite k this is just the singlet sector of the O(N) (U(N)) vector model, which is…

High Energy Physics - Theory · Physics 2015-05-30 Ofer Aharony , Guy Gur-Ari , Ran Yacoby

The SU(3) gauge theory with fermions in the sextet representation is one of several theories of interest for technicolor models. We have carried out a Schrodinger functional (SF) calculation for the lattice theory with two flavors of Wilson…

High Energy Physics - Lattice · Physics 2010-01-15 Benjamin Svetitsky , Yigal Shamir , Thomas DeGrand

A renormalization group flow of Hamiltonians for two-dimensional classical partition functions is constructed using tensor networks. Similar to tensor network renormalization ([G. Evenbly and G. Vidal, Phys. Rev. Lett. 115, 180405 (2015)],…

Statistical Mechanics · Physics 2017-06-29 Matthias Bal , Michaël Mariën , Jutho Haegeman , Frank Verstraete

We propose new methods to extend the renormalization group transformation to complex coupling spaces. We argue that the Fisher's zeros are located at the boundary of the complex basin of attraction of infra-red fixed points. We support this…

High Energy Physics - Lattice · Physics 2015-03-17 A. Denbleyker , Daping Du , Yuzhi Liu , Y. Meurice , Haiyuan Zou

We renormalize the six dimensional cubic theory with an $O(N)$ $\times$ $O(m)$ symmetry at three loops in the modified minimal subtraction (MSbar) scheme. The theory lies in the same universality class as the four dimensional…

High Energy Physics - Theory · Physics 2017-03-08 J. A. Gracey , R. M. Simms

We investigate the UV fixed-point structure of the three-dimensional Thirring model by means of the functional renormalization group (RG). We classify all possible 4-fermi interactions compatible with the present chiral and discrete…

High Energy Physics - Theory · Physics 2010-10-27 Holger Gies , Lukas Janssen

We study large charge sectors in the $O(N)$ model in $6-\epsilon $ dimensions. For $4<d<6$, in perturbation theory, the quartic $O(N)$ theory has a UV stable fixed point at large $N$. It was recently argued that this fixed point can be…

High Energy Physics - Theory · Physics 2020-04-13 Guillermo Arias-Tamargo , Diego Rodriguez-Gomez , Jorge G. Russo

We study the flow equation of the O($N$) $\varphi^4$ model in $d$ dimensions at the next-to-leading order (NLO) in the $1/N$ expansion. Using the Schwinger-Dyson equation, we derive 2-pt and 4-pt functions of flowed fields. As the first…

High Energy Physics - Theory · Physics 2019-12-06 Sinya Aoki , Janos Balog , Tetsuya Onogi , Peter Weisz