activity
20212025
collaborators

6 papers

cond-mat.stat-mech2025

Ferromagnetic and Spin-Glass Finite-Temperature Order but no Antiferromagnetic Order in the d=1 Ising Model with Long-Range Power-Law Interactions

E. Can Artun, A. Nihat Berker

The d=1 Ising ferromagnet and spin glass with long-range power-law interactions J r^-a is studied for all interaction range exponents a by a renormalization-group transformation th…

cond-mat.dis-nn2024

Axial, Planar-Diagonal, Body-Diagonal Fields on the Cubic-Spin Spin Glass in d=3: A Plethora of Ordered Phases under Finite Fields

E. Can Artun, Deniz Sarman, A. Nihat Berker

A nematic phase, previously seen in the d=3 classical Heisenberg spin-glass system, occurs in the n-component cubic-spin spin-glass system, between the low-temperature spin-glass p…

cond-mat.dis-nn2023

Nematic Phase of the n-Component Cubic-Spin Spin Glass in d=3: Liquid-Crystal Phase in a Dirty Magnet

E. Can Artun, Deniz Sarman, A. Nihat Berker

A nematic phase, previously seen in the d=3 classical Heisenberg spin-glass system, occurs in the n-component cubic-spin spin-glass system, between the low-temperature spin-glass p…

cond-mat.dis-nn2023

Driven and Non-Driven Surface Chaos in Spin-Glass Sponges

Yiğit Ertaç Pektaş, E. Can Artun, A. Nihat Berker

A spin-glass system with a smooth or fractal outer surface is studied by renormalization-group theory, in bulk spatial dimension d=3. Independently varying the surface and bulk ran…

cond-mat.stat-mech2023

The Merged Potts-Clock Model: Algebraic and Conventional Multistructured Multicritical Orderings in Two and Three Dimensions

E. Can Artun, A. Nihat Berker

A spin system is studied, with simultaneous permutation-symmetric Potts and spin-rotation-symmetric clock interactions, in spatial dimensions d=2 and 3. The global phase diagram is…

cond-mat.dis-nn2021

Spin-s Spin-Glass Phases in the d=3 Ising Model

E. Can Artun, A. Nihat Berker

All higher-spin s >= 1/2 Ising spin glasses are studied by renormalization-group theory in spatial dimension d=3. The s-sequence of global phase diagrams, the chaos Lyapunov expone…