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        <oai_dc:dc xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"  xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
          <dc:title>Multiscale
Rheo-Optical and Scattering Signatures
of Deformation-Induced Anisotropy in Aqueous Cellulose Nanocrystal
Suspensions under Large-Amplitude Oscillatory Shear</dc:title>
          <dc:creator>Yoshifumi Yamagata (16726934)</dc:creator>
          <dc:creator>Ainaa Amirah Marzuki (25112500)</dc:creator>
          <dc:creator>Saki Otobe (20488222)</dc:creator>
          <dc:creator>Moe Araida (22447397)</dc:creator>
          <dc:creator>Taisuke Sato (1976755)</dc:creator>
          <dc:subject>Biophysics</dc:subject>
          <dc:subject>Physical Sciences not elsewhere classified</dc:subject>
          <dc:subject>Neuroscience</dc:subject>
          <dc:subject>Physiology</dc:subject>
          <dc:subject>Biotechnology</dc:subject>
          <dc:subject>Evolutionary Biology</dc:subject>
          <dc:subject>Developmental Biology</dc:subject>
          <dc:subject>Mental Health</dc:subject>
          <dc:subject>shaped lobe geometry</dc:subject>
          <dc:subject>laos ), nonphase</dc:subject>
          <dc:subject>imposed laos conditions</dc:subject>
          <dc:subject>charged cellulose nanocrystal</dc:subject>
          <dc:subject>dependent viscosity growth</dc:subject>
          <dc:subject>comparative multiscale map</dc:subject>
          <dc:subject>angle light scattering</dc:subject>
          <dc:subject>directional mesoscopic anisotropy</dc:subject>
          <dc:subject>shaped sals patterns</dc:subject>
          <dc:subject>sals readouts show</dc:subject>
          <dc:subject>larger strain amplitudes</dc:subject>
          <dc:subject>distinguish viscosity crossover</dc:subject>
          <dc:subject>amplitude oscillatory shear</dc:subject>
          <dc:subject>lower strain amplitudes</dc:subject>
          <dc:subject>directly comparable rheo</dc:subject>
          <dc:subject>annularly averaged rheo</dc:subject>
          <dc:subject>suspensions exhibit concentration</dc:subject>
          <dc:subject>anisotropic scattering signatures</dc:subject>
          <dc:subject>local optical anisotropy</dc:subject>
          <dc:subject>scattering signatures</dc:subject>
          <dc:subject>strain amplitude</dc:subject>
          <dc:subject>shear rheology</dc:subject>
          <dc:subject>rate viscosity</dc:subject>
          <dc:subject>lower concentrations</dc:subject>
          <dc:subject>empirical viscosity</dc:subject>
          <dc:subject>crossover concentration</dc:subject>
          <dc:subject>induced anisotropy</dc:subject>
          <dc:subject>amplitude ranges</dc:subject>
          <dc:subject>later sals</dc:subject>
          <dc:subject>cnc suspensions</dc:subject>
          <dc:subject>multiscale rheo</dc:subject>
          <dc:subject>results provide</dc:subject>
          <dc:subject>responses emerge</dc:subject>
          <dc:subject>polarized imaging</dc:subject>
          <dc:subject>noncoincident responses</dc:subject>
          <dc:subject>mechanical yielding</dc:subject>
          <dc:subject>linear viscoelasticity</dc:subject>
          <dc:subject>evolves continuously</dc:subject>
          <dc:subject>compare mechanical</dc:subject>
          <dc:subject>c &lt;/</dc:subject>
          <dc:subject>based signature</dc:subject>
          <dc:subject>apparent contraction</dc:subject>
          <dc:subject>anisotropic x</dc:subject>
          <dc:subject>&gt;&lt; sub</dc:subject>
          <dc:description>Aqueous surface-charged cellulose nanocrystal (CNC) suspensions
exhibit concentration-dependent viscosity growth, gelation, and deformation-induced
anisotropy, but the concentration and strain-amplitude ranges over
which these responses emerge are not necessarily the same. Here, low-shear
rheology and linear viscoelasticity are combined with rheo-polarized
imaging (Rheo-PI) and rheo-small-angle light scattering (Rheo-SALS)
to compare mechanical, optical, and scattering signatures in the same
CNC system. Analysis of the operational low-rate viscosity and the
Winter–Chambon criterion separates an empirical viscosity-crossover
concentration, &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;cross&lt;/sub&gt;, from the sol–gel
transition concentration, &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;g&lt;/sub&gt;. Under fixed-frequency
large-amplitude oscillatory shear (LAOS), nonphase-resolved but directly
comparable Rheo-PI and Rheo-SALS readouts show that annularly averaged
Rheo-PI retardation becomes detectable at lower concentrations and
lower strain amplitudes than those required for the appearance of
anisotropic X-shaped SALS patterns. The first optical transition approximately
coincides with an apparent contraction of initially circular SALS
patterns, whereas clearly directional X-shaped SALS patterns appear
only at larger strain amplitudes. The X-shaped lobe geometry then
evolves continuously with the strain amplitude, providing a later
SALS-based signature of directional mesoscopic anisotropy under the
imposed LAOS conditions. Together, these results provide a comparative
multiscale map of deformation-induced anisotropy in CNC suspensions
and distinguish viscosity crossover, gelation, local optical anisotropy,
mechanical yielding, and anisotropic scattering signatures as related
but noncoincident responses.</dc:description>
          <dc:date>2026-09-25T00:00:00Z</dc:date>
          <dc:type>Dataset</dc:type>
          <dc:type>Media</dc:type>
          <dc:identifier>10.1021/acs.langmuir.6c03702.s002</dc:identifier>
          <dc:relation>https://figshare.com/articles/media/Multiscale_Rheo-Optical_and_Scattering_Signatures_of_Deformation-Induced_Anisotropy_in_Aqueous_Cellulose_Nanocrystal_Suspensions_under_Large-Amplitude_Oscillatory_Shear/34001605</dc:relation>
          <dc:rights>CC BY-NC 4.0</dc:rights>
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