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TECHNICAL ANNEX B: QUANTUM INFORMATION & CONDENSED MATTER SIMULATIONS IN STRONGLY CORRELATED ELECTRON SYSTEMS The definitive empirical test for HIGM's scale-invariance at the microscale is the phenomenon of **Sub-Kelvin Horizon Matching**. As the temperature of heavy-fermion or cuprate lattices drops toward absolute zero, the thermal noise drops below the microscopic information threshold

Samir A Hamouda

Published Jan 1, 2026• 0 citations
Publisher
DOI
10.13140/rg.2.2.34125.19687

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We discuss the momentum-space topology of 3+1 and 2+1 strongly correlated fermionic systems. For the 3+1 systems the important universality class is determined by the topologically stable Fermi points in momentum space. In the extreme limit of low energy the condensed matter system of this universality class acquires all the symmetries, which we know today in high energy physics: Lorentz invariance, gauge invariance, general covariance, etc. The chiral fermions as well as gauge bosons and gravity field arise as fermionic and bosonic collective modes of the system. This introduces the conceptual similarity between such condensed matter and the quantum vacuum of Standard Model, which also contains the Fermi point. For the 2+1 fermionic systems the momentum space topology gives rise to the quantization of different physical parameters, such as Hall conducivity and spin-Hall conductivity, and to quantum phase transitions with the abrupt change of the momentum-space topology. The combined p-space and r-space topology determines in particular the topology of the energy spectrum of fermion zero modes living within the topological defects; fermionic charges of the topologically nontrivial extended objects; axial anomaly; etc.

arXiv:cond-mat/0012195•Topology of Strongly Correlated Systems•Aug 1, 2001•1 citation
Magnetic properties of the two-dimensional t-J model are reviewed. Some of these properties are close to those observed in cuprate perovskites. In particular, the magnetic response of the model is characterized by the intensive peak at the antiferromagnetic wave vector and at some transfer frequency. The peak splits into several incommensurate maxima for lower and higher frequencies. We discuss mechanisms which are responsible for these peculiarities in the model, which might also refer to cuprates.
We discuss the momentum-space topology of 3+1 and 2+1 strongly correlated fermionic systems. For the 3+1 systems the important universality class is determined by the topologically stable Fermi points in momentum space. In the extreme limit of low energy the condensed matter system of this universality class acquires all the symmetries, which we know today in high energy physics: Lorentz invariance, gauge invariance, general covariance, etc. The chiral fermions as well as gauge bosons and gravity field arise as fermionic and bosonic collective modes of the system. This introduces the conceptual similarity between such condensed matter and the quantum vacuum of Standard Model, which also contains the Fermi point. For the 2+1 fermionic systems the momentum space topology gives rise to the quantization of different physical parameters, such as Hall conducivity and spin-Hall conductivity, and to quantum phase transitions with the abrupt change of the momentum-space topology. The combined p-space and r-space topology determines in particular the topology of the energy spectrum of fermion zero modes living within the topological defects; fermionic charges of the topologically nontrivial extended objects; axial anomaly; etc.