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Adaptation in complex systems implies a natural ability to change. In networks, adaptation may include a change in structural connectivity, which can lead to a change in collective behavior. When dihedral symmetry is present, i.e., rotations and reflections of a regular polygon, it is well-known that traveling and standing waves occur, generically, via spontaneous symmetry-breaking Hopf bifurcations. While synchronization appears via standard, symmetry-preserving, Hopf bifurcations. In these cases, the symmetries of the network equations do not change even though the bifurcating solutions may lose symmetry as parameters are varied. But when they do, possibly due to adaptation, there is, however, little knowledge of what happens to those patterns. Here, we choose to investigate the effects of forced-breaking the rotation symmetry of a network with (unperturbed) dihedral symmetry. We study, in particular, the changes in the region of existence and stability of the unperturbed patterns-traveling and standing waves and synchronization.
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http://dx.doi.org/10.1063/5.0288584 | DOI Listing |
Chaos
September 2025
Indian Institute of Science Education and Research, Tirupati, Andhra Pradesh 517507, India.
Adaptation in complex systems implies a natural ability to change. In networks, adaptation may include a change in structural connectivity, which can lead to a change in collective behavior. When dihedral symmetry is present, i.
View Article and Find Full Text PDFActa Crystallogr E Crystallogr Commun
September 2025
College of Materials Science and Opto-electronic Technology University of Chinese Academy of Sciences, Huairou Beijing 101408 People's Republic of China.
The title complex, [Fe(CHN)(CHN)]·3CH, possesses inversion symmetry with the iron(II) atom located on a center of symmetry. The metal atom is coordinated in a symmetric octa-hedral geometry by four pyrrole N atoms of the porphyrin ligand in the equatorial plane and two N atoms of 1-methyl-imidazole ligands in the axial sites; the complex crystallizes with three toluene solvent mol-ecules. The average Fe-N (N is a porphyrin N atom) bond length is 1.
View Article and Find Full Text PDFPhys Rev Lett
July 2025
University of Science and Technology of China, Interdisciplinary Center for Theoretical Study, Hefei, Anhui 230026, China.
We derive the full system of canonical differential equations for all planar two-loop massless six-particle master integrals and determine analytically the boundary conditions. This fully specifies the solutions, which may be written as Chen iterated integrals. We argue that this is sufficient information for evaluating any scattering amplitude in four dimensions up to the finite part.
View Article and Find Full Text PDFNat Mater
July 2025
Department of Biochemistry, University of Washington, Seattle, WA, USA.
Advances in computational methods have led to considerable progress in the design of protein nanomaterials. However, nearly all nanoparticles designed so far exhibit strict point group symmetry, which limits structural diversity and precludes anisotropic functionalization. Here we describe a computational strategy for designing multicomponent bifaceted protein nanomaterials with two distinctly addressable sides.
View Article and Find Full Text PDFbioRxiv
May 2025
Department of Medicine, UCLA, Los Angeles, CA 90095, USA.
We report the cryoEM structure of the protein FTN_1118, identifying it as a novel 13 kDa periplasmic protein unique to the genus, which we now designate FPM13 ( Periplasmic Metalloprotein, 13 kDa) based on its structural and biochemical properties. FPM13 was serendipitously identified during purification of type VI secretion system (T6SS) effector proteins, co-purifying with them. Its identity, initially unknown, was established using the novel cryoID method.
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