Memorial Article in honor of Maurice Kleman
Liquid Crystals Reviews 10(1-2) (2022) 6-33.
The initial aim of this memorial article was to illustrate with color pictures the very first article of Maurice Kleman and Jacques Friedel devoted to dislocations in cholesterics :
Color pictures of cholesteric dislocations in a wedge made of mica sheets cholesterics :
Nets of dislocations in Grandjean wedges produced by a partial cleavage of mica sheets and filled with 5CB/CB15 cholesteric mixtures. (a–c) Single dislocations lines (SL) located in the thinnest areas of wedges. (d) Coexistence of single (SL) and double (DL) dislocations lines. In agreement with a commonly believed paradigm, the single and double lines are located respectively in thinner and thicker areas of wedges.
Wedge made of two cylindrical mica sheets
Nucleation of a loop, folded three times, made of a thick (double) dislocation inside the thinnest part of the cylinder/cylinder gap. This observation contradicts the commonly accepted paradigm.
Nucleation of a thick (double) dislocation loop triggered by a compressive strain of the cholesteric helix. Note the presence of a cusp corresponding to a kink on the dislocation loop.
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Memorial Article in honor of Gérard Toulouse
Comptes Rendus Physique, 25 (2024) 367-388
Abstract. Classification of defects in ordered systems, based on the homotopy theory, conceived by Gérard Toulouse and Maurice Kléman has a very wide range of applications. We illustrate its modus operandi with three experimental examples. We deal first with dislocations in a dissipative periodic pattern of convection rolls in a shear flow instability in nematics. As the second example we chose the captive disclination loops threaded on polymer fibers immersed in nematics. Third, we focus on objects with double topological character defined for the first time in the generic article [1] coauthored by Gérard Toulouse: the “double et tripple anneau” Hopf links made of interlaced dislocation loops in cholesterics. Finally, we report on the recent discovery of their generalised, beads necklace version made of many minimal dislocation loops threaded, like pearls, on a string-like dislocation loops.
[1] : Y. Bouligand, B. Derrida, V. Poénaru, Y. Pomeau and G. Toulouse, “Distorsions with double topological character:
the case of cholesterics”, J. Phys. France 39 (1978), pp. 863–867.
a) Microscopic picture obtained in a recent experiment with a cholesteric sample (5CB/CB15) confined in the crossed cylinders geometry. b) Geometry of the interlaced dislocation loops observed from above. c) Side view of the cholesteric texture.
“The triple ring structure” predicted in ref. [1]. a) Reproduction of Figure 1 from the ref. [1]. b) The three components Hopf link observed in our experiments. c) Perspective view showing three kinks on the cargo loop carrying the two minimal loops.
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Decay of skeins of dislocations in cholesterics:
rewiring Conway's tangles into necklaces of bangles
Abstract: Knotted and linked skeins of vortices and disclinations generated, respectively, by symmetry-breaking normal - superfluid and isotropic - nematic phase transitions are known to untie, by rewiring of their crossings, into independent unknots that finally shrink and collapse until the defect-free ground state is reached. We demonstrate that the decay of skeins of dislocations, generated by the isotropic - cholesteric phase transition within a cylinder/cylinder gap, leads to stable necklace-like states made of numerous minimal loops, called bangles, tethered to kinks of much larger loops called cargo. We analyze the topological decay of skeins of dislocations in terms of the Conway–Kauffman theory of knots, showing that the necklace state results from rewiring of crossings triggered by collisions of tangles with their numerator closure. We point out that, in general, for symmetry reasons, kinks on edge dislocations are chiral. Their handedness, right or left, directly depends on the sign of kinks on which they are localized. In cholesterics with intrinsic chirality, the energy of kinks bearing bangles depends on their handedness. For this reason, within necklaces, all bangles are tethered to kinks of the same sign.
Jun-Yong Lee et al. , Soft Matter 21 (2025) 8205
The necklace state
(a) Geometry of experiments with cholesteric droplets (5CB/CB15 mixtures) confined between cylindrical mica sheets. The upper mica sheet can be moved in the x, y and z directions. (b) Microscopy image of a necklace composed of a circular dislocation called a cargo loop bearing five small circular dislocations called minimal loops or bangles. N is the number of cholesteric pitches p E 5 mm located between the mica sheets. (c) Close-up image of a bangle tethered to a kink of the cargo loop. The radius of the bangle is about three times smaller than the cholesteric pitch: rb E p/3. It varies with the concentration cCB15 of the chiral compound CB15 in the nematic 5CB. Here, cCB15 = 0.86% and p E 25 mm. (d) Perspective view of the necklace state. As all minimal loops are tethered exclusively on the +p kinks of the cargo loop, this configuration is chiral (for details see Fig. 10).
Bangle tethered to a kink of a dislocation.
(a) Bright-field image of the bangle structure. (b) Cross-sectional fluorescence confocal polarizing microscopy (FCPM) images along the dotted lines (1) and (2) in (a), showing vertical deviation of the dislocation with pitch p. The polarization direction is along the x-direction. (c) and (d) Cross-sectional FCPM images in planes (c) perpendicular and (d) parallel to the edge dislocation line far from the kink. For each slice, fluorescence intensities acquired under four linearly polarized excitations (0°, 45°, 90°, and 135°) are summed. Hence, bright regions correspond to in-plane alignment of the director, whereas dark regions indicate vertical alignment with the director, roughly along the z-axis. Images i–vi correspond to cross-sections along the lines i–vi marked in (a). (e) In-plane intensity-summed FCPM images at different heights. (f) 3D reconstruction of the dislocation kink and surrounding bangle based on experimental observations. (g) Plot of the relative height (DZd) versus the relative lateral positions (DXd) of the dislocation. Both positions are extracted from the experimental images like the ones shown in (d). For the sake of clarity, the dihedral angle of the wedge represented in the inset is exaggerated. (ZLI-3412/CB15 mixture with the cholesteric pitch p = 5 microns.)
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New concept
Topological metadefects: tangles of dislocations
Abstract: The concept of topological defects is universal. In condensed matter, it applies to disclinations, dislocations or vortices that are fingerprints of symmetry breaking during phase transitions. Using as a generic example the tangles of dislocations, we introduce the concept of topological metadefects i.e. defects made of defects. We show that in cholesterics, dextrogyre and levogyre primary tangles are generated through the D2 -> C2 symmetry breaking from the coplanar dislocation pair called Lehmann cluster submitted to a high enough tensile strain. The primary tangles can be wound up individually into double-helices. They can also annihilate in pairs or associate into tangles of higher orders following simple algebraic rules.
Published in Physical Review Letters 131 (2023) 128101
Generation of the dextrogyre primary tangle, driven by a tensile strain, from the Lehmann cluster: a) variation of the Peach-Koehler force with the gap thickness, b-e) overlapping instability of the Lehmann cluster, f) geometry of the Lehmann cluster, g-k) detailed views of the overlapping instability leading to the generation of the dextrogyre tangle.
Winding up of the primary tangle into a dextrogyre double helix by a growing tensile strain.
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Abstract: We deal here with three metastable systems: 1- the dowser texture, 2- supertwisted cholesterics and 3- hypotwisted cholesterics. We outline remarkable properties of tropisms of the dowser texture stemming from its low symmetry and we show that, using setups called Dowsons Colliders, nematic monopoles can be nucleated, set into motion and brought into collisions in the dowser texture. Subsequently we point out that nucleation of dislocation loops occurs in cholesteric layers compressed or dilated between cylindrical mica sheets. Under compression, three modes of nucleation of dislocation loops have been identied: individual, serial and continuous. The serial mode generates dislocation nets made of L circular loops connected by C radial crossing into superloops. Similar superloops can also be generated under dilation. We analyse the topology of superloops in terms of the theory of knots and point out they can be reduced into the unknot by Reidemeister moves. In other words, superloops are multiply folded loops that can be continuously unfolded.
Keynote lecture of the ILCC2022. Published online in Liquid crystals on 24 April 2023.
Single and double dislocation loops generated in the individual nucleation mode.
Four dislocation loops generated in the serial mode. They are connected by crossings into one superloop
Complex net of dislocation loops connected by crossings
Arbitrary shape of the trefoil knot.
Knotted dislocation confined inside the cylinder/cylinder wedge.
Shape of the trefoil knot confined inside the cylinder/cylinder wedge.
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The Geilo School 2022
Collisions of monopoles disclinations and dislocations
Proceedings of the Geilo School 2022, EPJST 233 (2024) 2711-2731
Abstract: Motions and collisions of topological defects produced during symmetry breaking transitions is a crucial issue in cosmology and in condensed matter physics. Here, we deal with topological defects in nematics and cholesterics. Nematics may contain linear defects i.e. disclinations and point defects i.e. monopoles while cholesterics may contain linear defects of their 1D periodic order parameter, i.e. dislocations. The dowser texture appears as a natural universe of the nematic monopoles. They can be generated in it, set into motion and brought to collisions that may result in annihilation of pairs of monopoles. We show how to generate pairs of disclinations in twisted nematic cells by the isotropic-nematic transition in the presence of magnetic fields. When two such disclinations collide, i.e. enter into a contact at one point, an intercommutation or rewiring into a new pair of disclination can occur. We show how to bring these disclinations to collisions by means of an electric field and how to steer the rewiring by magnetic fields. For generation of dislocations in cholesteric we use a Grandjean-Cano wedge made of crossed cylindrical mica sheets. After their nucleation upon dilation, dislocation loops are growing along the meniscus and their lateral segments collide. Such a selfcollision of a dislocation can result in a trivial crossing or may produce a stable configuration called Lehman cluster.
Intercommutations of colliding disclinations.
Generation, motions and collision of monopoles.
Energy landscape of the cholesteric conned between the cylindrical mica sheets.
Selfcollision of an open dislocation loop.
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Publication de la version française du livre collectif sur les cristaux liquides
Table des matières :
Chapitre 1: Optique singulière des défauts de cristaux liquides par Etienne Brasselet
Chapitre 2: Contrôle des microparticules avec des cristaux liquides par Chenhui Peng et Oleg Lavrentovich
Chapitre 3: Les effets thermomécaniques dans les cristaux liquides par Patrick Oswald, Alain Dequidt et Guilhem Poy
Chapitre 4: La physique de la texture furcelle par Pawel Pieranski et Maria Helena Godinho
Chapitre 5: L’émergence spontanée de la chiralité par Mohan Sinivasarao
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Collective book on liquid crystals
Françoise Brochard - Wyart
Two years ago, Mme Françoise Brochard-Wyart, director of the field "Physics of Soft Matter" at ISTE Editions, proposed us to write a book on recent advances in Liquid Crystals. The team of contributing authors and the content of the book were set thanks to Tigran Galstian who invited six of the authors to the 18th Conference on Optics of liquid Crystals in Quebec City.
We are glad to announce today that the book is available.
Contents :
Chapter 1: Singular optics of liquid crystals defects by Etienne Brasselet
Chapter 2: Control of microparticles with liquid crystals by Chenhui Peng and Oleg Lavrentovich
Chapter 3: Thermomechanical effects in liquid crystals by Patrick Oswald, Alain Dequidt and Guilhem Poy
Chapter 4: Physics of the dowser texture by Pawel Pieranski and Maria Helena Godinho
Chapter 5: Spontaneous emergence of chirality by Mohan Sinivasarao
E. Brasselet
M.H. Godinho
P. Pieranski
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Article published in AJP
In November 2019 three students from Ecole Normale Supérieure Paris-Cachan - Juliette Plo, Dihya Sadi and Elio Thellier - came to our lab for a two months internship untitled "From liquid crystals to displays". During the internship they worked simultaneously on two projects: 1°- detection of the isotropic - nematic phase transition and the measure of the quadropolar order parameter by means of RMN. 2° - detection of the magnetic and dielectric anisotropies of nematics by means of a new setup, built during the internship, inspired by the method invented by Mieczyslaw Jezewski and Wilhelm Kast about 100 years ago. Results of the internship were reported in an article untitled "Fréedericksz transition on air" published in American Journal Physics - well known bulletin of the American Association of Physics Teachers.
Abstract: The operational principle of twisted nematic displays involves the dielectric anisotropy of nematics. This crucial property was discovered about a hundred years ago by Jezewski and Kast who used a so-called resonance method in which the frequency of an LC tank circuit was set by the capacitance of a capacitor filled with a nematic liquid crystal. Jezewski and Kast observed that the resonance frequency changed upon application of a magnetic field to the capacitor. They interpreted the corresponding change in the dielectric permittivity as being due to reorientation of molecules by the magnetic field. Here, we describe a modern, simple, and low-cost version of this experiment. Instead of the LC oscillator working with vacuum lamps, we use an op-amp RC oscillator in which a twisted nematic display plays the role of the capacitor. For the purpose of classroom demonstrations, the oscillator frequency f is detected by a software-defined radio operating in the double-side band mode (DSB). Upon an appropriate tuning of the reception frequency f, even small changes of f become audible. This setup is very convenient for demonstration and measurements of all characteristics of the Freedericksz transition driven by magnetic or electric fields.
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