Chirality is one of the most intriguing fundamental phenomena in nature. Materials composed of chiral molecules find broad applications in areas ranging from nonlinear optics and spintronics to biology and pharmaceuticals. However, chirality is usually an invariable inherent property of a given material that cannot be easily changed at will. Very recently we discovered that chiral structure emerges as a basic configuration of polarization field in ferroelectric nanoparticles and nanodots in a form of stable fundamental topological excitations of polarization, Hopfions, and skyrmions, and, importantly, can be controlled and switched by cleverly devised field-temperature protocols. The key idea of the project is to reveal how this discovered emerging topological chirality will be identified, measured, explored, and put in practice.
- To optimize fabrication parameters enabling the engineering of ferroelectric nanostructures with desirable chiral properties.
- To develop research approaches for revealing and exploring the topological structures of the ferroelectric nanostructures.
- To devise efficient enantioselective procedures and elaborate effective methods for chirality revealing and operation.
The new skills in nanomaterial fabrication and operation, and in building the academia-industry links will be developed for further career pursuit. Also, the project will cluster the FerroChiral action with the complementary European networks in view of prospective development of long-lasting collaborations.
Physics Reports 1110, 1-56 (2025).
The 21st century has witnessed a revolutionary shift in the understanding of properties of matter driven by the application of topological principles. While the traditional approach to material science has been focusing on local interactions, topology introduces a global, non-local description in which the geometry of a material profoundly influences its properties. Ferroelectric materials, with their spontaneous electric polarization, have long been essential for understanding fundamental physical phenomena, which have led to numerous practical applications. Recent discoveries have revealed that nanostructured ferroelectrics host a wealth of fundamental topological states, which effectively enrich the landscape of ferroelectric research. This Review explores the topological foundation of ferroelectricity, rooted in the electrostatic essence of these materials. Drawing upon the analogy between the hydrodynamics of incompressible fluids and the electrostatics of polarization fields, we establish a comprehensive framework for classifying the complex topological states observed in ferroelectrics. We demonstrate that the rich diversity of polarization structures can be exhaustively described using the advanced topological approach. By extending fundamental topological concepts such as helicity, fibration, foliation, and ergodicity, we offer a systematic analysis of the topological textures in ferroelectrics. This work provides a coherent framework for understanding and manipulating topological structures in nanostructured ferroelectrics, paving the way for innovations in materials science and technology.
Chirality
Chirality, an inherent property of most objects of the universe, is a dynamic research topic in material science, physics, chemistry, and biology. The fundamental appeal of this extensive study is supported by the technological quest to manufacture materials with configurable chiralities for emerging applications ranging from optoelectronics and photonics to pharmaceutics and medicine. Recent advances put forth ferroelectrics as a host of chiral topological states in the form of Bloch domain walls, skyrmions, merons, and Hopfions, offering thus a unique ground for making chirality switchable and tunable. Here we review current developments, milestones achieved, and future routes of chiral ferroelectric materials. We focus on insights into the topological origin of the chirality in the nanostructured ferroelectrics, bringing new controllable functionalities. We pay special attention to novel developments enabling tunability and manipulating the chiroptical response and enantioselectivity, leading to new applications in nano-optoelectronics, plasmonics, pharmaceutics, and biomedical industries. Read more...Topological ferroelectric chirality, 2024
Chirality is a property of objects that cannot be superimposed on their mirror image. The most common example used to explain chirality is our left and right hands: they are mirror images of each other (fig. a), but it is impossible to align them perfectly by rotation or reflection.
Chirality is widespread in nature and appears in various forms. For instance, in living organisms, the shells of sea snails, such as the Neptunia species (fig. b), exhibit left- and right-handed symmetry. Chirality is also fundamental to organic molecules, such as DNA (fig. e), which demonstrates a helical structure with a distinct handedness.
In material science, chirality is observed at multiple levels:
Geometric chirality arises from the shape of objects (fig. c), like plasmonic nanoparticles with asymmetric geometries (fig. g).
Structural chirality is determined by the arrangement of atoms in molecules or crystals, as seen in amino acids (fig. f). This type of chirality is described by the crystallographic groups, known as the Sohncke groups. The relation of the Sohncke point symmetry groups with other functional symmetry groups in materials is illustrated by the diagram suggested by Halasyamani and Poeppelmeier (fig. i).
Topological chirality is seen in complex organic molecules (fig. h) or complex systems like nanostructured ferroelectrics, where knotted or linked polarization streamlines create unique chiral states. This type of chirality is provided by the nontrivial linking of the molecular chains. On the mathematical level, this type of chirality is described by the knots theory, similar to that describing the mathematical knots (fig. d).
These different types of chirality play a critical role in various applications, from optoelectronics and photonics to medicine and nanotechnology. Understanding and controlling chirality opens pathways to innovative technologies and advancements across multiple scientific fields. Read more...Topological ferroelectric chirality, 2024
Chirality switching in ferroelectric nanoparticles
Chiral ferroelectric materials, in which the structural polar ordering is directly coupled to the electric field, appear to be the unique choice of materials for exploring field-tunable chirality. They offer a remarkable operational platform for controlled optical activity manipulation by the electric field. Notably, yet underexplored kinds of ferroelectrics are the structurally chiral ferroelectrics in which the chirality emerges together with the polarization via the spontaneous symmetry breaking from the non-chiral paraelectric state as a ferroelectric with polarization-induced chirality. The handedness of such materials is related to the orientation of polarization and is switchable by reversing the polarization by the applied field. The switching of chirality in nanoparticles is of special interest because of its high technological potential. In particular, it offers remarkable perspectives for tunable chiral optoelectronics.
Here we show the possibility of chirality switching in topological states of ferroelectrics. Note that when the polarization topological state possesses definite handedness, the chirality cannot be inversed just by the field-induced reversion of polarity in each point of the structure since the structure of the streamlines will remain the same. Therefore, the efficient changing handedness of the system requires reconstruction of the topological polarization ordering, occurring via passing through a series of intermediate metastable states via the pathway, guided by an electric field.
The figures illustrate the geometry of the switching device and switching hysteresis loops.
The bottom panels (movie and figure) demonstrate polarization distribution (arrows) and chirality (color map) of the initial states, intermediate states through which the switching occurs, and the final chiral states. Yellow arrows indicate the direction of the average polarization flux in the Hopfion core.
The movie shows how the polarizing-depolarizing cycle for the Hopfion-hosting nanoparticle inverses its chirality. For illustrative purposes, we simulated the isotropic case using the phase-field method, in which the strain-renormalized coefficients in the Ginzburg-Landau functional are close to those in PbZr0.6Ti0.4O3 (PZT) with the spherical symmetry. The switching pathway using the full Ginzburg-Landau functional for PZT is described in (Luk’yanchuk et al., 2020). We consider a nanoparticle with the left-handed Hopfion (state 1 in the bottom figure). The combination of the directed-down counterclockwise helix-like central flux and directed-up counterclockwise peripheral helix-like fluxes constitutes a Hopfion’s structure. The total chirality is defined by the dominating contribution of the central part. Application of the electric field in the up direction, i.e., against the polarization direction at the core, favors the peripheral helix and suppresses the central helix. With the increasing absolute value of the field, the topological phase transition occurs, at which the new topological states abruptly emerge inside the nanoparticles. The outer part of the upcoming helical streamlines unlink in the nanoparticle pole regions from the downstream central flux and pierces the nanoparticle, enveloping, thus, the shrinking Hopfion (states 2,3). Another topological phase transition occurs when the Hopfion completely disappears, and the up-directed helical stream occupies all the space of the nanoparticle (state 4). Then, the helix continues the unwinding, leading finally to a complete poling of the nanoparticle. Notably, the chirality of the final upcoming helix is a succession of the chirality of the peripheral upcoming flux of the Hopfion, hence is opposite to the initial total Hopfion chirality. This chirality conserves on the way back to the zero-field state, where another sequence of topological phase transitions occurs. Upon decreasing the absolute value of the applied field, the new Hopfion appears in the nanoparticle. However, unlike in the field-increasing case, this Hopfion emerges at the periphery of the nanoparticle and embraces the upcoming polarization helix (state 5). Upon decreasing the field, it propagates to the nanoparticle center and finally occupies the full nanoparticle when the field vanishes (final state 6). The right-handed chirality and polarity of the newly-formed Hopfion (state 6), dominated by its central part of the counterclockwise-swirled flux, is inherited from the upcoming helix that remained from the high field configuration.
To summarize here, the described process of the re-polarization of the ferroelectric nanoparticle results in deterministic chirality switching.
Movie: Chirality switching in nanoparticles hosting Hopfions
Field-induced topological states in PZT nanoparticle
These codes provide visualization of chirality switching in ideal spherical PZT nanoparticles by an electric field. One should gather the simulation results in HDF5 format in some directory and launch the script driver.py to obtain the series of PNG files, which can be combined into the movie by any suitable means (FFMPEG...). User also need to record ParaView traces with desirable camera angles and color parameters. The code to the programmable filter from the template is injected automatically into the ParaView state.
#Template_programmable_filter:
class Input:
def __init__(self, source):
self._source = source
self._accessor = None
def set_accessor(self, accessor):
self._accessor = accessor
def clean_accessor(self):
self._accessor = None
def __getitem__(self, property_name):
if not self._accessor:
return self._source[property_name]
else:
return self._source.__getattribute__(self._accessor)[property_name]
def get_coordinates(self):
return self._source.Points
class IndexedInput(Input):
def __init__(self, source, index):
super().__init__(source[index])
class Output:
def __init__(self, sink):
self._sink = sink
self._accessor = None
def set_accessor(self, accessor):
self._accessor = accessor
def clean_accessor(self):
self._accessor = None
def write(self, characterictic):
if not self._accessor:
self._sink.append(characterictic.value, characterictic.name)
else:
self._sink.__getattribute__(self._accessor).append(characterictic.value, characterictic.name)
class Accessor:
def __init__(self, connection, accessor):
self._connection = connection
self._accessor = accessor
def __enter__(self):
self._connection.set_accessor(self._accessor)
return self
def __exit__(self, exc_type, exc_value, exc_traceback):
self._connection.clean_accessor()
def __getitem__(self, property_name):
return self._connection[property_name]
@property
def connection(self):
return self._connection
class Characteristic:
def __init__(self, name, value):
self._name = name
self._value = value
@property
def name(self):
return self._name
@property
def value(self):
return self._value
class PolarizationCharacteristics:
def __init__(self, P):
self._P = P
def bound_charge(self):
return Characteristic('Bound charge', -divergence(self._P))
def chirality(self):
return Characteristic('Chirality', dot(self._P, curl(self._P)))
def toroidal_moment(self):
return Characteristic('Toroidal moment', curl(self._P))
def main():
data = IndexedInput(inputs, 0)
with Accessor(data, "PointData") as point_data:
polarization = point_data["polar"]
polar_characteristics = PolarizationCharacteristics(polarization)
chirality = polar_characteristics.chirality()
sink = Output(output)
with Accessor(sink, "PointData") as point_data:
point_data.connection.write(chirality)
main()
#Driver:
from subprocess import run
def subs(string):
mapper = {
'\n': '
',
'\'': ''',
'\"': '"',
}
new_string = string
for k in mapper.keys():
new_string = new_string.replace(k, mapper[k])
return new_string
def main():
#Set proper path to paraview pvbatch
command = 'path/to/ParaView/bin/pvbatch'
#Prepare pvsm paraview state for proper screenshot
#Check the line where the source of programmable filter is located
template_pvsm = './template.pvsm'
substitution_line_number = 38777
with open(template_pvsm) as inp:
template_lines = inp.readlines()
with open("./template_programmable_filter.py") as inp:
pr_filter_lines = inp.readlines()
pr_filter_line = ''.join([ subs(s) for s in pr_filter_lines ])
template_lines[substitution_line_number] = f'<Element index="0" value="{pr_filter_line}"/>'
with open('./state.pvsm', 'w') as out:
out.writelines(template_lines)
#Write short trace using template.pvsm to take a screenshot with state.pvsm
#Or loop through the xdmf files in some directory
#Recorded trace should use state.pvsm
i = 0
res = run(f'{command} trace.py {i:0>10}.png', shell=True)
if __name__ == '__main__':
main()