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The measured frequencies and intensities of different first- and second-order Raman peaks of suspended graphene are used to show that optical phonons and different acoustic phonon polarizations are driven out of local equilibrium inside a submicron laser spot. The experimental results are correlated with a first-principles-based multiple temperature model to suggest a considerably lower equivalent local temperature of the flexural phonons than those of other phonon polarizations. The finding reveals weak coupling between the flexural modes with hot electrons and optical phonons. Since the ultrahigh intrinsic thermal conductivity of graphene has been largely attributed to contributions from the flexural phonons, the observed local nonequilibrium phenomena have important implications for understanding energy dissipation processes in graphene-based electronic and optoelectronic devices, as well as in Raman measurements of thermal transport in graphene and other two-dimensional materials.
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http://dx.doi.org/10.1021/acs.nanolett.7b00110 | DOI Listing |
J Chem Phys
September 2025
Department of Physics and Astronomy and Stewart Blusson Quantum Matter Institute, University of British Columbia, Vancouver, British Columbia V6T 1Z1, Canada.
Polymer dynamics is analyzed through the lens of linear dimensionality reduction methods, in particular principal and time-lagged independent component analysis (tICA). For a polymer undergoing ideal Rouse dynamics, the slow modes identified by these transformations coincide with the conventional Rouse modes. When applied to the Fourier modes of the segment density, we show that tICA generates dynamics equivalent to dynamic self-consistent field theory (D-SCFT) with a wavevector-dependent Onsager coefficient and a free energy functional subject to the random phase approximation.
View Article and Find Full Text PDFAdv Sci (Weinh)
September 2025
Department of Theoretical Physics and Center for Biophysics, Saarland University, 66123, Saarbrücken, Germany.
Understanding interactions between chiral active particles- self-propelling and self-rotating entities- is crucial for uncovering how chiral active matter self-organizes into dynamic structures. Although fluctuation-induced forces in nonequilibrium active systems can drive structure formation, the role of chirality remains largely unexplored. Effective fluctuation-induced forces between intruders immersed in chiral active fluids are investigated and revealing that the impact of chirality depends sensitively on particle shape.
View Article and Find Full Text PDFJ Chem Phys
September 2025
Department of Applied Chemistry, University of Seoul, Seoul 02504, Republic of Korea.
Nonequilibrium thermodynamics plays a crucial role in understanding a wide range of physical and chemical processes. While significant advances have been made through frameworks, such as the fluctuation theorem, it remains challenging to define thermodynamic quantities, such as energy, entropy, and free energy, at the local level during nonequilibrium processes. Recently, Jinwoo and Tanaka [Sci.
View Article and Find Full Text PDFJ Phys Condens Matter
September 2025
Physics, Birla Institute of Technology and Science - Pilani Campus, Department of Physics, Birla Institute of Technology and Science, Pilani, Pilani Campus, Vidya Vihar, Pilani, RJ, 333031, INDIA.
We investigate the transport properties of a two-dimensional Su-Schrieffer-Heeger (2D SSH) model in the quantum Hall regime using non-equilibrium Green's function formalism (NEGF). The device Hamiltonian, where the 2D SSH model serves as the channel, is constructed using a nearest-neighbor tight-binding model. The effect of an external perpendicular magnetic field is incorporated into the contacts via Peierls substitution.
View Article and Find Full Text PDFProc Natl Acad Sci U S A
September 2025
Istituto Nazionale di Fisica Nucleare Sezione di Trieste, Trieste 34127, Italy.
We discuss the dependence of the critical properties of the Anderson model on the dimension in the language of -function and renormalization group recently introduced in Vanoni et al. [C. Vanoni , , e2401955121 (2024)] in the context of Anderson transition on random regular graphs.
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