Taras Turiv
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Taras Turiv has a total of 51 co-authors. Here are the top co-authors by number of shared publications:
- Oleg D. Lavrentovich
Kent State University
15 shared publications Qi-Huo Wei
Advanced Materials and Liquid Crystal Institute, Materials Science Graduate Program, Kent State University, Kent, Ohio 44242, USA
6 shared publicationsSergij V. Shiyanovskii
Advanced Materials and Liquid Crystal Institute, Kent State University, Kent, OH 44242, USA
5 shared publications- Greta Babakhanova
Advanced Materials and Liquid Crystal Institute, Kent State University
4 shared publications - Yubing Guo
School of Medical Science and Engineering Beijing Institute of Technology Beijing China
4 shared publications Bing-Xiang Li
Advanced Materials and Liquid Crystal Institute, Kent State University, Kent, Ohio 44242, USA
3 shared publications
Latest Publications
- Open Access
- 1 December 2025
- Published by Royal Society of Chemistry (RSC) in Soft Matter
- Vol. 22 (6) , 1297-1313
Bend instabilities and topological turbulence in shear-aligned living liquid crystal
Shear-aligned living liquid crystals exhibit a cascade of bend instabilities followed by defect nucleation and proliferation after shear cessation.
- 1 December 2025
- Published by Royal Society of Chemistry (RSC) in Soft Matter
- Vol. 22 (6) , 1297-1313
Open AccessBend instabilities and topological turbulence in shear-aligned living liquid crystal
Shear-aligned living liquid crystals exhibit a cascade of bend instabilities followed by defect nucleation and proliferation after shear cessation.
- 11 April 2024
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 132 (15) , 158102
High-Order Nonlinear Electrophoresis in a Nematic Liquid Crystal
Electrophoresis is the motion of particles relative to a surrounding fluid driven by a uniform electric field. In conventional electrophoresis, the electrophoretic velocity grows linearly with the applied field. Nonlinear effects with a quadratic speed vs field dependence are gaining research interest since an alternating current field could drive them. Here, we report on the giant nonlinearity of electrophoresis in a nematic liquid crystal in which the speed grows with the fourth and sixth powers of the electric field. The mechanism is attributed to the shear thinning of the nematic environment induced by the moving colloid. The observed giant nonlinear effect dramatically enhances the efficiency of electrophoretic transport.
- 11 April 2024
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 132 (15) , 158102
High-Order Nonlinear Electrophoresis in a Nematic Liquid Crystal
Electrophoresis is the motion of particles relative to a surrounding fluid driven by a uniform electric field. In conventional electrophoresis, the electrophoretic velocity grows linearly with the applied field. Nonlinear effects with a quadratic speed vs field dependence are gaining research interest since an alternating current field could drive them. Here, we report on the giant nonlinearity of electrophoresis in a nematic liquid crystal in which the speed grows with the fourth and sixth powers of the electric field. The mechanism is attributed to the shear thinning of the nematic environment induced by the moving colloid. The observed giant nonlinear effect dramatically enhances the efficiency of electrophoretic transport.
- 12 October 2020
- Published by Springer Nature in Nature Physics
- Vol. 17 (2) , 260-266
Directional self-locomotion of active droplets enabled by nematic environment
- 12 October 2020
- Published by Springer Nature in Nature Physics
- Vol. 17 (2) , 260-266
Directional self-locomotion of active droplets enabled by nematic environment
- 6 August 2020
- Published by Royal Society of Chemistry (RSC) in Soft Matter
- Vol. 16 (37) , 8565-8576
Shear-induced polydomain structures of nematic lyotropic chromonic liquid crystal disodium cromoglycate
Lyotropic chromonic liquid crystals (LCLCs) represent aqueous dispersions of organic disk-like molecules that form cylindrical aggregates. Despite the growing interest in these materials, their flow behavior is poorly understood. Here, we explore the effect of shear on dynamic structures of the nematic LCLC, formed by 14 wt% water dispersion of disodium cromoglycate (DSCG). We employ in situ polarizing optical microscopy (POM) and small-angle and wide-angle X-ray scattering (SAXS/WAXS) to obtain independent and complementary information on the director structures over a wide range of shear rates. The DSCG nematic shows a shear-thinning behavior with two shear-thinning regions (Region I at < 1 s−1 and Region III at > 10 s−1) separated by a pseudo-Newtonian Region II (1 s−1 < < 10 s−1). The material is of a tumbling type. In Region I, < 1 s−1, the director realigns along the vorticity axis. An increase of above 1 s−1 triggers nucleation of disclination loops. The disclinations introduce patches of the director that deviates from the vorticity direction and form a polydomain texture. Extension of the domains along the flow and along the vorticity direction decreases with the increase of the shear rate to 10 s−1. Above 10 s−1, the domains begin to elongate along the flow. At > 100 s−1, the texture evolves into periodic stripes in which the director is predominantly along the flow with left and right tilts. The period of stripes decreases with an increase of . The shear-induced transformations are explained by the balance of the elastic and viscous energies. In particular, nucleation of disclinations is associated with an increase of the elastic energy at the walls separating nonsingular domains with different director tilts. The uncovered shear-induced structural effects would be of importance in the further development of LCLC applications.
- 6 August 2020
- Published by Royal Society of Chemistry (RSC) in Soft Matter
- Vol. 16 (37) , 8565-8576
Shear-induced polydomain structures of nematic lyotropic chromonic liquid crystal disodium cromoglycate
Lyotropic chromonic liquid crystals (LCLCs) represent aqueous dispersions of organic disk-like molecules that form cylindrical aggregates. Despite the growing interest in these materials, their flow behavior is poorly understood. Here, we explore the effect of shear on dynamic structures of the nematic LCLC, formed by 14 wt% water dispersion of disodium cromoglycate (DSCG). We employ in situ polarizing optical microscopy (POM) and small-angle and wide-angle X-ray scattering (SAXS/WAXS) to obtain independent and complementary information on the director structures over a wide range of shear rates. The DSCG nematic shows a shear-thinning behavior with two shear-thinning regions (Region I at < 1 s−1 and Region III at > 10 s−1) separated by a pseudo-Newtonian Region II (1 s−1 < < 10 s−1). The material is of a tumbling type. In Region I, < 1 s−1, the director realigns along the vorticity axis. An increase of above 1 s−1 triggers nucleation of disclination loops. The disclinations introduce patches of the director that deviates from the vorticity direction and form a polydomain texture. Extension of the domains along the flow and along the vorticity direction decreases with the increase of the shear rate to 10 s−1. Above 10 s−1, the domains begin to elongate along the flow. At > 100 s−1, the texture evolves into periodic stripes in which the director is predominantly along the flow with left and right tilts. The period of stripes decreases with an increase of . The shear-induced transformations are explained by the balance of the elastic and viscous energies. In particular, nucleation of disclinations is associated with an increase of the elastic energy at the walls separating nonsingular domains with different director tilts. The uncovered shear-induced structural effects would be of importance in the further development of LCLC applications.
- Open Access
- 13 July 2020
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 2 (3) , 033060
Control of microswimmers by spiral nematic vortices: Transition from individual to collective motion and contraction, expansion, and stable circulation of bacterial swirls
Active systems composed of self-propelled units show fascinating transitions from Brownian-like dynamics to collective coherent motion. Swirling of swimming bacteria is a spectacular example. This study demonstrates that a nematic liquid crystal environment patterned as a spiral vortex controls individual-to-collective transition in bacterial swirls and defines whether they expand or shrink. In dilute dispersions, the bacteria swim along open spiral trajectories, following the preimposed molecular orientation. The trajectories are nonpolar. As their concentration exceeds some threshold, the bacteria condense into unipolar circular swirls resembling stable limit cycles. This collective circular motion is controlled by the spiral angle that defines the splay-to-bend ratio of the background director. Vortices with dominating splay shrink the swirls toward the center, while vortices with dominating bend expand them to the periphery. Spiraling vortices of with splay-bend parity produce the most stable swirls. All the dynamic scenarios are explained by hydrodynamic interactions of bacteria mediated by the patterned passive nematic environment and by the coupling between the concentration and orientation. The acquired knowledge of how to control individual and collective motion of microswimmers by a nematic environment can help in the development of microscopic mechanical systems.- 13 July 2020
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 2 (3) , 033060
Open AccessControl of microswimmers by spiral nematic vortices: Transition from individual to collective motion and contraction, expansion, and stable circulation of bacterial swirls
Active systems composed of self-propelled units show fascinating transitions from Brownian-like dynamics to collective coherent motion. Swirling of swimming bacteria is a spectacular example. This study demonstrates that a nematic liquid crystal environment patterned as a spiral vortex controls individual-to-collective transition in bacterial swirls and defines whether they expand or shrink. In dilute dispersions, the bacteria swim along open spiral trajectories, following the preimposed molecular orientation. The trajectories are nonpolar. As their concentration exceeds some threshold, the bacteria condense into unipolar circular swirls resembling stable limit cycles. This collective circular motion is controlled by the spiral angle that defines the splay-to-bend ratio of the background director. Vortices with dominating splay shrink the swirls toward the center, while vortices with dominating bend expand them to the periphery. Spiraling vortices of with splay-bend parity produce the most stable swirls. All the dynamic scenarios are explained by hydrodynamic interactions of bacteria mediated by the patterned passive nematic environment and by the coupling between the concentration and orientation. The acquired knowledge of how to control individual and collective motion of microswimmers by a nematic environment can help in the development of microscopic mechanical systems. - Open Access
- 15 May 2020
- Published by American Association for the Advancement of Science (AAAS) in Science Advances
- Vol. 6 (20) , eaaz6485
Topology control of human fibroblast cells monolayer by liquid crystal elastomer
Photopatterned liquid crystal elastomer templates living tissue with predesigned alignment patterns and topological defects.
- 15 May 2020
- Published by American Association for the Advancement of Science (AAAS) in Science Advances
- Vol. 6 (20) , eaaz6485
Open AccessTopology control of human fibroblast cells monolayer by liquid crystal elastomer
Photopatterned liquid crystal elastomer templates living tissue with predesigned alignment patterns and topological defects.
- Open Access
Topology control of human cells monolayer by liquid crystal elastomer
Biological cells in living tissues form dynamic patterns with local orientational order and topological defects. Here we demonstrate an approach to produce cell monolayer with the predesigned orientational patterns using human dermal fibroblast cells (HDF) placed onto a photoaligned liquid crystal elastomer (LCE). The alignment of cells is caused by anisotropic swelling of the substrates in contact with the aqueous cell growth medium. The patterns predesigned in the LCE cause a strong spatial variation of cell phenotype (evidenced by shape variations), their surface density and number density fluctuations. The concentration of cells is significantly higher near the cores of positive-strength defects as compared to negative-strength defects. Unbinding of defect pairs intrinsic to active matter is suppressed by anisotropic surface anchoring. The geometry of arrays allows one to estimate the elastic and surface anchoring characteristics of the tissues. The demonstrated patterned LCE approach could be used to control the collective behavior of cells in living tissues, cell differentiation, and tissue morphogenesis.
Open AccessTopology control of human cells monolayer by liquid crystal elastomer
Biological cells in living tissues form dynamic patterns with local orientational order and topological defects. Here we demonstrate an approach to produce cell monolayer with the predesigned orientational patterns using human dermal fibroblast cells (HDF) placed onto a photoaligned liquid crystal elastomer (LCE). The alignment of cells is caused by anisotropic swelling of the substrates in contact with the aqueous cell growth medium. The patterns predesigned in the LCE cause a strong spatial variation of cell phenotype (evidenced by shape variations), their surface density and number density fluctuations. The concentration of cells is significantly higher near the cores of positive-strength defects as compared to negative-strength defects. Unbinding of defect pairs intrinsic to active matter is suppressed by anisotropic surface anchoring. The geometry of arrays allows one to estimate the elastic and surface anchoring characteristics of the tissues. The demonstrated patterned LCE approach could be used to control the collective behavior of cells in living tissues, cell differentiation, and tissue morphogenesis.
- 2 March 2020
- Published by Springer Nature in Nature Physics
- Vol. 16 (4) , 481-487
Polar jets of swimming bacteria condensed by a patterned liquid crystal
- 2 March 2020
- Published by Springer Nature in Nature Physics
- Vol. 16 (4) , 481-487
Polar jets of swimming bacteria condensed by a patterned liquid crystal
- Open Access
- 20 May 2019
- Published by Royal Society of Chemistry (RSC) in Physical Chemistry Chemical Physics
- Vol. 21 (24) , 13078-13089
Pretransitional behavior of viscoelastic parameters at the nematic to twist-bend nematic phase transition in flexiblen-mers
We report dynamic light scattering measurements of the orientational (Frank) elastic constants and associated viscosities among a homologous series of a liquid crystalline dimer, trimer, and tetramer exhibiting a uniaxial nematic (N) to twist-bend nematic (NTB) phase transition.
- 20 May 2019
- Published by Royal Society of Chemistry (RSC) in Physical Chemistry Chemical Physics
- Vol. 21 (24) , 13078-13089
Open AccessPretransitional behavior of viscoelastic parameters at the nematic to twist-bend nematic phase transition in flexiblen-mers
We report dynamic light scattering measurements of the orientational (Frank) elastic constants and associated viscosities among a homologous series of a liquid crystalline dimer, trimer, and tetramer exhibiting a uniaxial nematic (N) to twist-bend nematic (NTB) phase transition.
- Open Access
- 30 August 2018
- Published by Springer Nature in Nature Communications
- Vol. 9 (1) , 3528
Publisher Correction: Electrically driven three-dimensional solitary waves as director bullets in nematic liquid crystals
The original version of this article contained an error in the description of Supplementary Movie 7, which incorrectly read ‘Collision resulting in annihilation of two solitons. U = 45.1 V, f = 600 Hz, T = 50 °C, d = 8.0 μm. The original movie is taken at the frame rate of 91 fps. The playback speed is 7 fps.’ The correct version reads ‘Death of a soliton at a dust particle. U = 65.6 V, f = 800 Hz, T = 50 °C, d = 7.7 µm. The original movie is taken at the frame rate of 92 fps. The playback speed is 7 fps.’ The HTML has been updated to include a corrected version of the ‘Description of Additional Supplementary Files’ file.
- 30 August 2018
- Published by Springer Nature in Nature Communications
- Vol. 9 (1) , 3528
Open AccessPublisher Correction: Electrically driven three-dimensional solitary waves as director bullets in nematic liquid crystals
The original version of this article contained an error in the description of Supplementary Movie 7, which incorrectly read ‘Collision resulting in annihilation of two solitons. U = 45.1 V, f = 600 Hz, T = 50 °C, d = 8.0 μm. The original movie is taken at the frame rate of 91 fps. The playback speed is 7 fps.’ The correct version reads ‘Death of a soliton at a dust particle. U = 65.6 V, f = 800 Hz, T = 50 °C, d = 7.7 µm. The original movie is taken at the frame rate of 92 fps. The playback speed is 7 fps.’ The HTML has been updated to include a corrected version of the ‘Description of Additional Supplementary Files’ file.