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Defects&TLSs and glass transition

theory

2022 Theory of melting of glasses Chandra M. Varma

motivation - specific heat peak at melting temperature is closely connected with the density of LEEs see also as linear-in-temperature specific heat at VERY low temperatures. Therefore LEAKING (with or without tunneling). Both phenomena, peak at $T_g$ and $\gamma*T$ of specific heat at glass temperature and low tempreatures correspondingly, occur concurrently

already topological-KT transition

Third, the measured $T^3$ specific heat is larger than that given by the elastic constants - the original TLM has nothing to say about this.
The change in the so called excess $T^3$ specific heat with density is identical to that of the linear in T heat capacity

HUGE peak for crystal but noticeable peak for glass - features of the specific heat

open questions

  • a) since $T_G \sim 100-1000K$, for defect-freezing-out transition the defect size needs to be $\xi_G \sim 10A=10^{-7}cm$

    1-order of magnitude ---BPeak energy scale of defect is (30k), but glass temperature (300k)

crossover temparature $T_Q \sim 10K$ is by KT relation $T_Q \approx \frac{1}{2} \rho_s \sim \frac{\gamma^2}{\rho c_t^2 \xi^3}$

$10K \sim 10^{-15} erg \sim 10^{-3} eV \sim \frac{\hbar c}{R_0}$
$10^{-15} erg = \frac{10^{-27} erg*s *4*10^5 cm/s}{50 A}$, so $R_0 \sim 50A$

IF $\gamma \sim 6.3eV$ and $\rho c_t^2 \xi^3 \approx 2(g/cm^3) 4^2 10^{10} (cm/s)^2 125*10^{-21} cm^3 \approx 4*10^{-8} erg=40,000eV$,
so $T_Q \sim 10^{-3} eV \sim 10K$

  • b) RG equations to be checked/reproduced?

2022 Anomalous Elasticity and Emergent Dipole Screening in Three-Dimensional Amorphous Solids

experimental links - forcing out of "universal"/natural regime

2021 Decoupling between propagating acoustic waves and two-level systems in hydrogenated amorphous silicon

experiments around "universal regime"

How Universal are the Low Temperature Acoustic Properties of Glasses? - 1988 - Berret-Meissner