Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals

Summary

In this report, we present a protocol to examine direct magnetoelectric effects, i.e., induction of ferroelectric polarization by applying magnetic fields, in liquid crystals. This protocol provides a unique approach, supported by the softness of liquid crystals, to achieve room-temperature magnetoelectrics.

Abstract

Materials showing coupling phenomena between magnetism and (ferro)electricity, i.e., magnetoelectric effects, have attracted a great deal of attention due to their potential applications for future device technologies such as sensors and storage. However, conventional approaches, which usually utilize materials containing magnetic metal ions (or radicals), have a major problem: only a few materials have been found to show the coupling phenomena at room temperature. Recently, we proposed a new approach to achieve room-temperature magnetoelectrics. In contrast to conventional approaches, our alternative proposal focuses on a completely different material, a "liquid crystal", free from magnetic metal ions. In such liquid crystals, a magnetic field can be utilized to control the orientational state of constituent molecules and the corresponding electric polarization through magnetic anisotropy of the molecules; it is an unprecedented mechanism of the magnetoelectric effect. In this context, this paper provides a protocol to measure ferroelectric properties induced by a magnetic field, that is, the direct magnetoelectric effect, in a liquid crystal. With the method detailed here, we successfully detected magnetically-tuned electric polarization in the chiral smectic C phase of a liquid crystal at room temperature. Taken together with the flexibility of constituent molecules, which directly affects the magnetoelectric responses, the introduced method will serve to allow liquid crystal cells to acquire more functions as room-temperature magnetoelectrics and associated optical materials.

Introduction

Research on the magnetoelectric (ME) effect, the induction of electric polarization (magnetization) by a magnetic (electric) field, has been focused towards the novel types of applications such as sensors and storage technologies. With recent studies on ME multiferroics^1,2,3,4, the target systems in the field of ME study are extended to various types of solid-state materials, including inorganic, organic, and metal-organic frameworks, by utilizing spin-lattice couplings dexterously^5,6,7,8,9. However, room-temperature operation, which must be accomplished for practical utilization of ME materials with their ME couplings, is still a challenging issue, and a very limited number of single-phase materials have been reported as room-temperature magnetoelectrics to date¹⁰.

Liquid crystals, which possess an orientational order, sometimes with a partial positional one, have also been examined with respect to ME materials in recent years^{11,12,13,14,15}. One of the advantages of liquid crystals as ME materials is their operation temperature, as liquid-crystal phases are typically stabilized around room temperature. An example of ME liquid crystals reported so far is a composite between magnetic nano-platelets with perpendicular magnetic anisotropy and liquid crystals showing the nematic phase, known as the simplest liquid-crystal phase possessing only one-dimensional orientational order¹⁵. It shows the converse ME effect, the induction of magnetization by an electric field, through the electric-field manipulation of the coupled platelet and molecular orientations.

More recently, another unique strategy to establish the ME effect in liquid crystals was proposed¹⁶. The focus of this strategy is to create a chiral smectic C (SmC*) phase with one-dimensional positional order, resulting in a diffused layer structure called the smectic layer. One characteristic of the SmC* phase is that a molecular orientation vector n is coupled with a local electric dipole moment p. This correlation is provided by the combination of tilted orientation of the rod-like constituent molecules with respect to the smectic layer normal n₀ and the chirality-induced mirror (and inversion) symmetry breaking in the molecules. From the viewpoint of symmetries, the former changes the symmetry from D_∞h (the so-called SmA phase, Figure 1A) into C_2h (the so-called SmC phase, Figure 1B), and the latter breaks the mirror symmetry of C_2h so that the symmetry is reduced into C₂ (the SmC* phase, see each layer in Figure 1C). In each SmC* layer, the presence of finite polarization is allowed along the C₂ axis, which is normal to both n₀ and n. The strong coupling between n and p is essential for ferroelectricity in liquid crystals. In the SmC* phase, n aligns in the helicoidal manner through layer by layer (Figure 1C), and thus there is no macroscopic polarization. Ferroelectricity in such liquid crystals is achieved by using strong surface effects, which stabilize the homogeneously oriented state of n known as a surface-stabilized ferroelectric liquid-crystal (SSFLC) state (Figure 1D). It should be noted that ferroelectric polarization reversal always accompanies a switching of the bi-stable orientation states through the coupling between n and p¹⁷. As the inverse effect, a change in molecular orientation of the SmC* phase is expected to give rise to a change in electric polarization. Through magnetic anisotropy caused by spins on magnetic elements and/or aromatic rings in liquid-crystal molecules and the flexibility of n in a liquid-crystal state due to weaker molecular interactions than in a solid crystal state, n is also tunable by a magnetic field. Thus, the SmC* phase can be transformed into a magnetic-field-induced homogeneously oriented state similar to an SSFLC state. Therefore, the direct ME effect, the induction of electric polarization by a magnetic field, is achieved as the development of macroscopic electric polarization is induced by a homogeneous alignment of n coupled with p, in all the layers.

We introduce procedures to prepare liquid-crystal cells for the investigation of ME couplings and methodologies to detect the ME effect. A method for the preparation of liquid-crystal cells was reported in detail previously¹⁸. Here, we modified this method for dielectric and ME measurements. With the method detailed here, we detected magnetically-tuned electric polarization, that is, the direct ME effect, in a liquid crystal showing the SmC* phase at room temperature.

Protocol

1. Preparation of Liquid-Crystal Cells and the Determination of the Cell Gap

1. Preparation of liquid-crystal cells
   1. Cut glass substrates coated with indium/tin-oxide (ITO) on one side into the desired size (typical size: 10 x 10 x 1.1 mm, Figure 2A). To cut the substrates, scratch a line on their face with a glass cutter and break off excess glass manually.
   2. Wash the cut glass substrates using a detergent in an ultrasonic bath at 35 kHz for 30 min. Rinse them with deionized water in the ultrasonic bath for 10 min. Replace deionized water and rinse the substrates 5 times to remove contaminants (Figure 2B). Blow off remaining water with an air-duster-gun with care not to touch the widest faces of the substrates.
   3. Drip polyimide solutions (alignment layer planer in Table of Materials) onto the ITO-coated side of the washed substrates, and spin-coat the solutions at 5000 rpm for 30 s (Figure 2C). Bake the substrates at 200 °C for 1 h to remove the solvent and cure the polyimide thin films.
   4. Put the substrates on an XZ stage so that the ITO- and polyimide-coated side of the substrates faces upwards. Place the substrates under a roller covered with a velvet cloth and fix the substrates by air suctioning (Figure 2D). Apply a uniform and soft pressure on the substrates with the roller by adjusting the height of the stage.
      Note: Here, the XZ stage was made by a machine shop at Osaka University.
   5. Rotate the roller and move the stage back and forth under the roller 5 times along the horizontal direction to rub the substrates by the velvet cloth. Dip the rubbed substrates into isopropyl alcohol in a 10 – 50 mL glass container for 1 min to remove contaminants, and dry them at 80 °C for a few minutes.
   6. Glue the two substrates together with 12 μm thickness flat resin films as spacers. Note that adhesive points are placed only at the edge of the substrates and the inner sides of the glued substrates are coated with the ITO and polyimide. Make sure that the opposite substrates have been rubbed antiparallel and are slightly shifted (about 2 mm) to provide enough spaces for electrical terminals on both of the substrates (Figure 2E).
   7. Glue the conducting wires on the above-mentioned spaces for terminals by using silver conducting paste (Figure 2F). Bake the substrates with conductive wires at 150 °C for 1 h to remove the solvent in the silver conductive paste.
2. Determination of cell gap¹⁹
   1. Irradiate the blank cells prepared in 1.1.7 with white light propagating normal to their widest face. Measure the transmission spectra using an optical spectrometer, and observe pseudo-sinusoidal oscillation (Figure 3), which appears due to the Fabry-Pérot effect²⁰.
   2. Estimate the cell gap d by using the relationship d = λ₁λ₂/2(λ₂-λ₁), where the wavelengths λ₁ and λ₂ denote a pair of adjacent peak-wavelengths in the transmission spectra.

2. Preparation of the Liquid-crystal Mixture and Introduction into the Cells

1. Mix two compounds, 5-octyl-2-(4-octyloxyphenyl) pyrimidine (compound 1: Figure 4A) and (S)-5-decyl-2-[4(2-fluorodecyloxy) phenyl] pyrimidine (compound 2: Figure 4B) with a mass ratio of 3:1 in a glass vial. Prepare 100 mg of the solution in total (75 mg of compound 1 and 25 mg of compound 2).
2. Put the prepared blank cell from step 1.1.7 on a hot stage, keeping the temperature at 80 °C, a temperature at which the mixture from 2.1 is in the isotropic liquid phase (Figure 5). Introduce the mixture from step 2.1 into the cell by using a spatula and capillary action. Keep the cell temperature at 80 °C for 30 min, then cool down to room temperature at a rate of about 5 °C/min.

3. Sample Characterization

1. Place a cell filled with the mixture from step 2.2 on a hot stage between two crossed polarizers and irradiate it with light. Observe textures of the mixture with changing temperature from room temperature to 80 °C at a rate of 5 °C/min by using a microscope (and a short-pass filter with tuning range of ~600 nm to enhance the visibility, as necessary), and identify liquid-crystal phases from polarization micrographs²¹ (Figure 6).
2. Determine the phase transition sequence and transition temperatures from the observed textures (Figure 5). For the SmC* phase, estimate the helicoidal pitch as double the stripe width.
3. Confirm the first-order phase transition temperatures of the mixture prepared in 2.1 by differential thermal analysis (DTA; see Table of Materials and manufacturer’s instructions), which provides a peak (or dip) anomaly at a first-order phase transition (Figure 7).

4. Dielectric and Magnetoelectric Measurements

1. Prepare a commercial superconducting magnet (see Table of Materials) equipped with temperature controllers (2 - 400 K) and magnetic field (up to 9 T).
2. Prepare a homemade insert for the superconducting magnet, which consists of three major parts: sample space, a rod including four coaxial cables, and a connector terminal (Figure 8A).
3. Glue the cell prepared in 2.2 on the sample space of the insert (Figure 8B). Connect the two conductive wires of the cell to the terminals (high and low) of the sample space by soldering. Make sure of the cell orientation so as to apply a magnetic field in the direction parallel to the substrates of the cell. Place a thermometer on the widest plane of the cell in order to measure the sample temperature accurately and introduce the insert into the superconducting magnet.
4. Connect the connecter terminals to an LCR meter (see Table of Materials) with coaxial cables. Measure the dielectric constant as a function of temperature and magnetic field by means of quasi-four terminal methods with the LCR meter (see manufacturer’s instructions and our previous work¹⁶).
5. Connect the connecter terminals to an electrometer (see Table of Materials) with coaxial cables. Measure the magnetic-field and temperature dependence of displacement current with the electrometer while sweeping a magnetic field and temperature at a constant rate (1.0 T/min for sweeping magnetic field and 5 K/min for sweeping temperature; see manufacturer’s instructions and our previous work¹⁶). Obtain electric polarization by integrating the displacement current as a function of time.

Results

The protocol is deemed a success only if the ME effect in liquid-crystal samples is observed. Here we measured the direct ME effect in a liquid-crystal sample prepared by the aforementioned procedures. For the measurements, an in-plane magnetic field was applied with the angle tilted by about 45° from the rubbing direction (normal to smectic layers), because the largest magnetic-field-induced polarization was detected in this configuration¹⁶.

Discussion

The experimental results showed that the methods described here successfully demonstrated the ME coupling in the liquid crystal. The observed ME and magneto-dielectric effects can be associated with the orientational transition of molecular orientation in a fixed smectic layer structure. However, the layer normal direction n₀ in the layer structure can be also changed by applying a magnetic field through magnetic anisotropy. This is because the molecules prefer to have a parallel arra...

Materials

List of materials used in this article

Name	Company	Catalog Number	Comments
Material
Compound 1: Figure 4(A)	DIC Co., Ltd.	–N/A	PYP-8O8
Compound 2: Figure 4(B)	DIC Co., Ltd.	N/A	PYP-10O10F
ITO-coated glass substrates	Sigma-Aldrich Inc.	703192-10PK
Detergent	Wako Pure Chemical Industries, Ltd.	031-10401
Alignment layer planer	JSR Co., Ltd.	AL1254
Spacer	Teijin Film Solutions Co., Ltd.	Q51-12
Glue	Huntsman Inc.	ARALDITE RT30	For gluing two substrates
Glue	M&I Materials ltd.	Apiezon H Grease	For gluing a cell and homemade insert
Silver paste	Fujikura Kasei Co., Ltd.	D-753
Equipment
Ultrasonic cleaner	AS ONE Corp.	AS52GTU
Spin coater	Mikasa Co. Ltd.	1H-D7
Polarized optical microscope	Nikon Co., Ltd.	ECLIPSE LV100N POL
Short-pass filter	Thorlabs Inc.	FB600-40
Optical spectrometer	Ocean Optics Inc.	USB2000+UV-VIS
Differential thermal analyzer	Rigaku Co., Ltd.	Thermo plus EVO2
Superconducting magnet	Quantum Design Inc.	PPMS
LCR meter	Keysight Technologies Ltd.	E4980A
Electrometer	Keithley Instruments Inc.	6517A