Universal scaling function ansatz for finite-temperature jamming
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arXiv
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| Format: | Preprint |
| Publié: |
2023
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| _version_ | 1866914928551526400 |
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| author | Ridout, Sean A. Liu, Andrea J. Sethna, James P. |
| author_facet | Ridout, Sean A. Liu, Andrea J. Sethna, James P. |
| contents | We cast a nonzero-temperature analysis of the jamming transition into the framework of a scaling ansatz. We show that four distinct regimes for scaling exponents of thermodynamic derivatives of the free energy such as pressure, bulk and shear moduli, can be consolidated by introducing a universal scaling function with two branches. Both the original analysis and the scaling theory assume that the system always resides in a single basis in the energy landscape. The two branches are separated by a line $T^*(Δϕ)$ in the $T-Δϕ$ plane, where $Δϕ=ϕ-ϕ_c^Λ$ is the deviation of the packing fraction from its critical, jamming value, $ϕ_c^Λ$, for that basin. The branch for $T<T^*(Δϕ)$ reduces at $T=0$ to an earlier scaling ansatz that is restricted to $T=0$, $Δϕ\ge 0$, while the branch for $T>T^*(Δϕ)$ reproduces exponents observed for thermal hard spheres. In contrast to the usual scenario for critical phenomena, the two branches are characterized by different exponents. We suggest that this unusual feature can be resolved by the existence of a dangerous irrelevant variable $u$, which can appear to modify exponents if the leading $u=0$ term is sufficiently small in the regime described by one of the two branches of the scaling function. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2304_11152 |
| institution | arXiv |
| publishDate | 2023 |
| record_format | arxiv |
| spellingShingle | Universal scaling function ansatz for finite-temperature jamming Ridout, Sean A. Liu, Andrea J. Sethna, James P. Soft Condensed Matter Statistical Mechanics We cast a nonzero-temperature analysis of the jamming transition into the framework of a scaling ansatz. We show that four distinct regimes for scaling exponents of thermodynamic derivatives of the free energy such as pressure, bulk and shear moduli, can be consolidated by introducing a universal scaling function with two branches. Both the original analysis and the scaling theory assume that the system always resides in a single basis in the energy landscape. The two branches are separated by a line $T^*(Δϕ)$ in the $T-Δϕ$ plane, where $Δϕ=ϕ-ϕ_c^Λ$ is the deviation of the packing fraction from its critical, jamming value, $ϕ_c^Λ$, for that basin. The branch for $T<T^*(Δϕ)$ reduces at $T=0$ to an earlier scaling ansatz that is restricted to $T=0$, $Δϕ\ge 0$, while the branch for $T>T^*(Δϕ)$ reproduces exponents observed for thermal hard spheres. In contrast to the usual scenario for critical phenomena, the two branches are characterized by different exponents. We suggest that this unusual feature can be resolved by the existence of a dangerous irrelevant variable $u$, which can appear to modify exponents if the leading $u=0$ term is sufficiently small in the regime described by one of the two branches of the scaling function. |
| title | Universal scaling function ansatz for finite-temperature jamming |
| topic | Soft Condensed Matter Statistical Mechanics |
| url | https://arxiv.org/abs/2304.11152 |