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Updated: Apr 4, 2026

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level
Published on: September 26, 2016
Coupling of Caged Molecule Dynamics to JG β-Relaxation II: Polymers
K L Ngai1,2, S Capaccioli1,3, D Prevosto1
1CNR-IPCF , Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy.
The fast dynamics of glass-forming materials, known as the nearly constant loss (NCL), change their temperature dependence near the secondary glass transition temperature (Tgβ). This newly identified property, observed across various materials, links fast caged dynamics to the Johari-Goldstein β-relaxation.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Physical Chemistry
Background:
- At high frequencies (above 1 GHz), structural α-relaxation and Johari-Goldstein (JG) β-relaxation are too slow to be observed in glass-forming materials.
- The fast dynamics at these frequencies are attributed to molecular vibrations and caged molecule dynamics, manifesting as nearly constant loss (NCL).
- The secondary glass transition temperature (Tgβ) is a key parameter characterizing the JG β-relaxation.
Purpose of the Study:
- To investigate the high-frequency dynamics (100 MHz to THz) in the glassy state of various glass-formers, including polymers and small molecules.
- To identify and characterize the temperature at which the NCL's temperature dependence changes (THF).
- To establish the relationship between THF and the secondary glass transition temperature (Tgβ).
Main Methods:
- Analysis of existing and new experimental data from quasielastic light scattering, Brillouin scattering, quasielastic neutron scattering, and GHz-THz dielectric relaxation.
- Comparison of the temperature dependence of NCL, elastic scattering intensity (I(Q, T)), and mean-square-displacement (⟨u(2)(T)⟩) with Tgβ.
- Independent determination of Tgβ using positronium annihilation lifetime spectroscopy (PALS) and adiabatic calorimetry.
Main Results:
- A consistent change in the temperature dependence of NCL, I(Q, T), or ⟨u(2)(T)⟩ was observed at a temperature THF in the glassy state of diverse glass-formers.
- This temperature THF was found to be approximately equal to the independently determined secondary glass transition temperature (Tgβ) (THF ≈ Tgβ).
- This THF ≈ Tgβ relationship was not previously recognized in scattering studies of polymers and small molecular glass-formers.
Conclusions:
- The observed property (THF ≈ Tgβ) arises from the coupled nature of JG β-relaxation and caged dynamics, both influenced by density and entropy.
- The JG β-relaxation acts as a terminator for caged dynamics, making these processes inseparable.
- The universality of the THF ≈ Tgβ relationship provides crucial insights into the glass transition problem, necessitating its consideration in future research.
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