Chaotic percolation in the random geometry of maximum-density dimer packings
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| Format: | Preprint |
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2023
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| _version_ | 1866913848244568064 |
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| author | Bhola, Ritesh Damle, Kedar |
| author_facet | Bhola, Ritesh Damle, Kedar |
| contents | Maximum-density dimer packings (maximum matchings) of non-bipartite site-diluted lattices, such as the triangular and Shastry-Sutherland lattices in $d=2$ dimensions and the stacked-triangular and corner-sharing octahedral lattices in $d=3$, generically exhibit a nonzero density of monomers (unmatched vertices). Following a construction in the recent literature, we use the structure theory of Gallai and Edmonds to decompose the disordered lattice into ``${\mathcal R}$-type'' regions which host the monomers of any maximum matching, and perfectly matched ``${\mathcal P}$-type'' regions from which such monomers are excluded. When the density $n_v$ of quenched vacancies lies well within the low-$n_v$ geometrically percolated phase of the disordered lattice, we find that the random geometry of these regions exhibits unusual {\em Gallai-Edmonds percolation} phenomena. In $d=2$, we find two phases separated by a critical point, namely a phase in which all ${\mathcal R}$-type and ${\mathcal P}$-type regions are small, and a percolated phase that displays a striking lack of self-averaging in the thermodynamic limit: Each sample has a single percolating region which is of type ${\mathcal R}$ with probability $f_{\mathcal R}$ and type ${\mathcal P}$ with probability $1-f_{\mathcal R}$, where $f_{\mathcal R} \approx 0.50(2)$ is independent of $n_v$ (away from the critical region). In this regime, microscopic changes in the vacancy configuration lead to chaotic changes in the large-scale structure of ${\mathcal R}$-type and ${\mathcal P}$-type regions. In $d=3$, apart from a phase with small ${\mathcal R}$-type and ${\mathcal P}$-type regions, the thermodynamic limit exhibits {\em four} distinct percolated phases separated by critical points at successively lower $n_v$, two of which again display unusual violations of self-averaging. Physical consequences are also discussed. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2311_05634 |
| institution | arXiv |
| publishDate | 2023 |
| record_format | arxiv |
| spellingShingle | Chaotic percolation in the random geometry of maximum-density dimer packings Bhola, Ritesh Damle, Kedar Disordered Systems and Neural Networks Strongly Correlated Electrons Maximum-density dimer packings (maximum matchings) of non-bipartite site-diluted lattices, such as the triangular and Shastry-Sutherland lattices in $d=2$ dimensions and the stacked-triangular and corner-sharing octahedral lattices in $d=3$, generically exhibit a nonzero density of monomers (unmatched vertices). Following a construction in the recent literature, we use the structure theory of Gallai and Edmonds to decompose the disordered lattice into ``${\mathcal R}$-type'' regions which host the monomers of any maximum matching, and perfectly matched ``${\mathcal P}$-type'' regions from which such monomers are excluded. When the density $n_v$ of quenched vacancies lies well within the low-$n_v$ geometrically percolated phase of the disordered lattice, we find that the random geometry of these regions exhibits unusual {\em Gallai-Edmonds percolation} phenomena. In $d=2$, we find two phases separated by a critical point, namely a phase in which all ${\mathcal R}$-type and ${\mathcal P}$-type regions are small, and a percolated phase that displays a striking lack of self-averaging in the thermodynamic limit: Each sample has a single percolating region which is of type ${\mathcal R}$ with probability $f_{\mathcal R}$ and type ${\mathcal P}$ with probability $1-f_{\mathcal R}$, where $f_{\mathcal R} \approx 0.50(2)$ is independent of $n_v$ (away from the critical region). In this regime, microscopic changes in the vacancy configuration lead to chaotic changes in the large-scale structure of ${\mathcal R}$-type and ${\mathcal P}$-type regions. In $d=3$, apart from a phase with small ${\mathcal R}$-type and ${\mathcal P}$-type regions, the thermodynamic limit exhibits {\em four} distinct percolated phases separated by critical points at successively lower $n_v$, two of which again display unusual violations of self-averaging. Physical consequences are also discussed. |
| title | Chaotic percolation in the random geometry of maximum-density dimer packings |
| topic | Disordered Systems and Neural Networks Strongly Correlated Electrons |
| url | https://arxiv.org/abs/2311.05634 |