Electro-optic liquid crystal device employing two-dimensional WSe 2 as the planar-alignment layers

: Two-dimensional (2D) tungsten diselenide (WSe 2 ) nanosheets were transferred onto indium tin oxide (ITO) coated glass slides. Two such 2D WSe 2 -covered ITO glass slides were placed together to fabricate an electro-optic liquid crystal (LC) cell. A nematic LC inside this WSe 2 -based device obtains uniform planar-alignment. The coherent overlay of the LC molecules along the armchair direction on the WSe 2 lattice leads to this planar-alignment at the molecular scale. This WSe 2 -based LC device exhibits the typical electro-optical eﬀect on the application of an electric ﬁeld. A sharp Fréedericksz transition of the nematic director from this electro-optical eﬀect conﬁrms that the 2D WSe 2 provides suﬃcient planar anchoring energy in the device. Finally, the WSe 2 /ITO slide exhibits more optical transparency than a standard polyimide alignment layer/ITO slide.


Introduction
Monolayer tungsten diselenide (WSe 2 ) is a highly stable two-dimensional (2D) semiconductor [1,2,3,4] whose crystal structure is shown in Fig. 1(a).Here we experimentally demonstrate that 2D WSe 2 can impose planar-alignment to a nematic liquid crystal (LC) in an electro-optic device.Optically anisotropic LC materials are vastly employed in modern electro-optical display technology.Conventionally, unidirectionally rubbed polyimide (PI) layers are used as the planar-alignment agent in standard optically transmissive liquid crystal displays (LCDs) [5], where the LC molecules align with the alkyl side chains along the rubbing direction on the PI layers, achieving a homogeneous (i.e., uniform planar) director (n) profile inside the device [6].However, this LC alignment process using the rubbed PI layers triggers some disadvantages.For example, a large distribution of pre-tilt angles of the LC developed due to the uneven mechanical rubbing process on the PI layers generates non-uniform brightness in the LCD panel [5]; free ion impurities stemming from the PI alignment layers can contaminate the LC [7]; and the residual fiber dust from the rubbing process of the PI layers increases the contaminants in the LC [5].Moreover, the organic PI layers are responsive to UV light and high temperature, and therefore, the alignment characteristics are affected when the PI-based LC devices are exposed to UV light and high temperature [8,9].Thus, there exists an important research direction to explore various LC-substrate anchoring phenomena to develop alternate LC alignment methods, such as photoalignment method [10], epitaxial alignment technique using inorganic alignment agents, e.g., graphene [11,12,13,14] and hexagonal boron nitride [15,16,17,18], oblique SiO evaporation technique [5], and microgroove grating surface fabrication method [5] to name a few.
Recent studies show that the crystallographic orientation of 2D hexagonal transition metal dichalcogenides (TMDs), such as MoSe 2 and WSe 2 , can be characterized by the alignment process of an LC on their surfaces [19,20].The LC aligns on the 2D hexagonal nanostructures, including WSe 2 , due to the epitaxial interaction between the LC's benzene rings and the honeycomb crystal structure of the 2D hexagonal nanostructures [19,20].It has been found using the density functional calculations that the alignment of the LC molecules has a distinct preferential direction along the armchair direction on the WSe 2 lattice with an adsorption energy ∼ 1.708 eV/molecule [19].Here we report that the 2D WSe 2 can function as the planar-alignment agent, without any additional PI layers, in an LC device that exhibits the required electro-optical effect on the application of a voltage.

Experiments, results, and discussion
In this section, we present (a) the fabrication of the WSe 2 -based planar LC cell, (b) the electrooptical effect of the LC in the cell, and finally, (c) the optical transmission spectroscopy of WSe 2 /ITO slide.

Fabrication of the electro-optic LC cell employing 2D WSe 2 as the planar-alignment agent
In a WSe 2 lattice, each selenium (Se) atom is bonded to three tungsten (W) atoms in a pyramidal geometry, as shown in Fig. 1(a).The top-view hexagonal lattice structure of WSe 2 is shown in Fig. 1(b).According to Ref. [19], the LC molecules align better along the armchair direction due to the epitaxial interaction-which is illustrated in Fig. 1(b).This spontaneous planar-alignment mechanism of the LC molecules along the armchair direction on this 2D WSe 2 lattice is the fundamental principle in our experiment for employing the monolayer WSe 2 as the planaralignment agent in this electro-optic LC device.In [19], the WSe 2 was deposited on a silicon substrate, and no electro-optic LC device was designed to see any electric field-induced switching effect.In our experiment, we have transferred the monolayer WSe 2 on ITO substrates, and two such WSe 2 /ITO slides were utilized to design an electro-optic LC cell where an electric field was applied.
We have first conducted the following experiments to investigate the 2D WSe 2 lattice-induced planar-alignment of the LC.High-quality chemical vapor deposition (CVD) grown monolayer WSe 2 film covered across c-cut sapphire was obtained from 2Dsemiconductors Inc.The transmission electron microscopy (TEM) image of 2D WSe 2 on a TEM grid in Fig. 1(c) confirms the highly crystalline nature of the monolayer WSe 2 samples.The monolayer WSe 2 films from the sapphire substrates were then transferred onto several indium tin oxide (ITO) coated glass substrate employing the standard polymethyl-methacrylate (PMMA) aided wet transfer method [21,22].Only 1 × 1 cm 2 area was covered with the transferred monolayer WSe 2 on the 2.5 × 2.5 cm 2 ITO coated glass substrates.We reached this size limit because only 1 × 1 cm 2 monolayer WSe 2 could be produced by 2Dsemiconductors Inc.After the transfer process, the Raman spectroscopy in Fig. 1(d) and the photoluminescence (PL) emission in the inset in Fig. 1(d) confirm the presence of monolayer WSe 2 on the ITO slide [23,24].A Raman microscope (IDRaman micro, Ocean Optics, Inc.) with a 532 nm excitation laser was used to study the Raman spectroscopy.The PL emission was studied using a QEPRO-FL spectrometer (Ocean Optics, Inc.) with a 2.5 mW and 532 nm excitation laser.
Figure 2(a) shows the picture of an ITO glass substrate with monolayer WSe 2 on it.A thin layer of LC was produced by putting down a small droplet of LC E7 (T NI = 60.5°C,EMD Millipore Corporation) on the WSe 2 /ITO slide, which was pre-heated at 70°C to bring the LC droplet in the isotropic phase.The LC droplet was then gently blowing away by a dust blower and slowly cooled down in the nematic phase.The thin LC layer was present on the monolayer WSe 2 as well as on the bare ITO area.A crossed-polarized optical microscope (Olympus BX61) was used to study the alignment of the LC on the monolayer WSe 2 film.Figure 2(b) shows the LC texture on the bare ITO substrate.The presence of multiple colors in this micrograph reveals that the LC does not achieve a uniform planar-aligned state on the bare ITO substrate.The micrograph in Fig. 2(c) exhibits the LC texture both on the monolayer WSe 2 film and on the bare ITO substrate.The white dashed line presents the edge of the monolayer WSe 2 film on the ITO substrate.The right side of the white dashed line shows that the LC achieves a uniform planar-aligned state on the WSe 2 film-where n is oriented at 45°with the crossed polarizers, producing a bright uniform texture with a maximum transmitted intensity.The small dark spots on the aligned LC texture are PMMA residues from the WSe 2 transfer process.These tiny PMMA-induced defects do not affect the overall LC alignment on the WSe 2 film.The left side of the white dashed line shows the randomly oriented LC domains on the bare ITO substrate.After the slide is rotated clockwise through 45°under the crossed-polarized microscope, the uniform planar-aligned LC on the WSe 2 film exhibits a dark uniform texture since n is now oriented parallel to the analyzer, as shown in the micrograph in Fig. 2(d).Figure 2(e) shows the LC texture at a different edge of the monolayer WSe 2 film on the ITO substrate.Similar to the previous one, a 45°rotated state is shown in the micrograph in Fig. 2(f).This experiment establishes that the monolayer WSe 2 film imposes uniaxial planar-alignment (i.e., homogeneous alignment) on the LC due to the epitaxial interaction.It is important to note here that on a single WSe 2 2D crystal, the LC molecules can assume three different orientations separated by 60 degrees due to the hexagonal symmetry.However, the micrographs shown in Figs.2(c), 2(d), 2(e), and 2(f) clearly demonstrate that it is possible to get a reasonably large uniform LC domain with unidirectional planar-alignment (without any three-fold alignment degeneracy) on the WSe 2 film.We have not seen any misalignment.We believe this was achieved because of our LC coating technique-where a dust blower was used to gently blow the LC droplet in one direction from one side to the other on the t WSe 2 /ITO slide.
A WSe 2 -based cell (with a cell-gap d = 16.8 µm) was prepared by placing together two WSe 2 /ITO glass substrates with the WSe 2 sides facing each other.The cell was filled with LC E7 in the isotropic phase by capillary injection from one opening and gentle vacuum suction from the other opening to maintain the average LC-flow in one direction during the filling process.Then the LC was slowly cooled down in the nematic phase.The micrograph in Fig. 3(a) shows that LC gains a uniformed planar-aligned state, with n at 45°with the crossed polarizers, in-between the two WSe 2 monolayers in the WSe 2 -based cell.Also, as expected, the LC does not achieve homogeneous alignment where there are two bare ITO layers are present in the cell.After the cell is rotated counterclockwise through 45°under the crossed-polarized microscope, the uniform planar-aligned LC in-between the two WSe 2 monolayers exhibits a dark uniform texture with n at 0°with respect to the polarizer, as shown in the micrograph in Fig. 3(b).
To realize the LC's planar-alignment quality in this WSe 2 -based cell, the cell was rotated under the crossed-polarized microscope, and the change in the transmitted intensity only through the WSe 2 region of the cell was recorded at every 2°rotation-step.The results are presented in Figs.3(c

Electro-optical effect of LC in WSe 2 -based cell
The electro-optical effect of LC E7 in the WSe 2 -based cell was studied using an optical setup where the cell was mounted between two crossed polarizers, and n in the cell was oriented at 45°with respect to the crossed polarizers.A 5-mW He-Ne laser beam of wavelength 633 nm was sent through the polarizer, the WSe 2 -based LC cell, the crossed analyzer, and into a photodetector, which was fed into a dc voltmeter to measure the transmitted intensity.The applied ac voltage at f = 1000 Hz across the cell was gradually ramped up, and the change in the transmitted intensity was detected from the dc voltmeter.The same experiment was also carried out under the crossed polarized microscope with a white light source, and several micrographs of the WSe 2 -based LC cell at different applied voltages were taken.When the applied voltage across the cell exceeds Fréedericksz threshold value, n rotates from the initial planar orientation to homeotropic orientation, and the LC's effective birefringence, <∆n > changes as a function of the applied voltage.In our optical setup, n is initially oriented at 45°with the crossed polarizers.Therefore, if I o is the intensity of the plane-polarized light incident on the WSe 2 -based LC cell, then the transmitted optical intensity, I at the exit of the analyzer shows an oscillatory behavior according to the equation [25] where λ is the wavelength of the laser beam and d is the cell-gap.The number of maxima appearing in the transmittance curve in Fig. 4(a) is given by (d ∆n/λ) [25].Using ∆n = 0.225 for LC E7, λ = 633 nm for the He-Ne laser and, the WSe 2 -based LC cell-gap, d = 16.8 µm, we obtain (d ∆n/λ) ≈ 6.The transmittance curve in a smaller voltage range in the inset in Fig. 4(a) shows six maxima-which confirms a complete director rotation from the planar state to the homeotropic state in the WSe 2 -based LC cell.The inset also shows a sharp Fréedericksz transition (V th = 0.88 V), indicating that the 2D WSe 2 is able to supply the required amount of planar-anchoring strength as the alignment agent in the cell.Figure 4(b) shows the micrographs of the LC texture in the WSe 2 -based LC cell under the crossed-polarized microscope at different applied voltages.The results indicate that the WSe 2 -based LC cell exhibits the essential electro-optical effect for a transmissive LC device-where the 2D WSe 2 is employed as the planner-alignment agent.

Optical transmission spectroscopy of the WSe 2 /ITO slide
The optical transmission spectra of a standard PI/ITO substrate and the WSe 2 /ITO substrate were studied using FLAME-S-XR1-ES (Ocean Optics, Inc.) spectrometer in the wavelength range from 300 nm to 1000 nm.A standard planar PI material, KPI-300B (60 nm thick layer on an ITO slide) was used for the PI/ITO slide.The transmission spectra for these two slides are shown in Fig. 5.The thickness of monolayer WSe 2 is ∼ 0.6 nm.Replacing the PI layer by monolayer WSe 2 reduces the alignment layer thickness from 60 nm to well below 1 nm.Recent studies using density functional theory calculations suggest that various monolayer 2D materials, including WSe 2 , show low absorbance, low reflectance, and high transmittance in the visible spectrum [26].Therefore, as expected, the WSe 2 /ITO substrate shows more optical transparency than the standard PI/ITO substrate.Thus, replacing the PI alignment agent by 2D WSe 2 should minimize the transmissive losses over a wide spectral range in the LC device.

Conclusion
The appearance of the homogeneous alignment of the LC on the WSe 2 film and its absence on bare ITO substrate is a clear indication that 2D WSe 2 can serve as the planar-alignment agent in an LC cell.This WSe 2 -based LC cell shows a sharp Fréedericksz transition with the standard electro-optical effect when an electric field is applied across the cell.The higher optical transparency of 2D WSe 2 has potential applications in modern transmissive electro-optic LC devices.Future studies will involve measurements of polar anchoring energy, azimuthal anchoring energy, voltage holding ratio, and residual dc charge of the WSe 2 -based LC cell.

Fig. 1 .
Fig. 1.(a) Schematic representation of the monolayer WSe 2 crystal structure.(b) Schematic representation of the planar alignment of the LC along the armchair direction the monolayer WSe 2 nanostructure.(c) The transmission electron microscopy (TEM) of WSe 2 on a TEM grid.(d) Raman spectroscopy of monolayer WSe 2 on ITO; inset: photoluminescence (PL) emission of monolayer WSe 2 on ITO.

Fig. 2 .
Fig. 2. (a) Picture of the monolayer WSe 2 on an ITO substrate.(b) Crossed-polarized micrograph of unaligned LC on the bare ITO substrate.(c), (d) Crossed-polarized micrograph and its 45°rotated state, respectively, of the LC on the WSe 2 /ITO substrate revealing uniform planar-alignment of the LC on the monolayer WSe 2 film and unaligned LC on the bare ITO region.(e), (f) Crossed-polarized micrograph and its 45°rotated state, respectively, of the same LC sample at a different edge of the monolayer WSe 2 film on the ITO substrate.
), 3(d), 3(e), and 3(f).The angle between the average LC director, n and the analyzer is defined by θ.Figures 3(c), 3(d), and 3(e) are the micrographs of the LC texture in the WSe 2 -based cell, where θ = 0°, 22.5°, and 45°, respectively.The graph in Fig. 3(f) shows the normalized transmitted intensity of the WSe 2 -based LC cell under the crossed-polarized microscope as a function of θ.This transition of the transmitted intensity from a uniform dark texture to a uniform bright texture at every 45°rotation confirms that the two WSe 2 monolayers can impose homogeneous alignment on the LC inside the device.

Figure 3 (
g) shows the picture of the WSe 2 -based LC cell.

Fig. 3 .
Fig. 3. (a), (b) Crossed-polarized micrograph and its 45°rotated state, respectively, of the WSe 2 -based LC cell showing uniform planar-alignment of the LC in the WSe 2 region and unaligned LC in the bare ITO region.(c), (d), and (e) Micrographs of the dark, intermediate, and bright states, respectively, as the WSe 2 -based LC cell was rotated under the crossed-polarized optical microscope.(f) Normalized transmitted intensity through the WSe 2 -based LC cell as a function of angle θ.(g) The picture of the WSe 2 -based LC cell.

Figure 4
Figure 4 represents the electro-optical effect of LC E7 in the WSe 2 -based LC cell.Figure 4(a) exhibits the oscillatory response of the transmittance, I/I o of LC E7 in the WSe 2 -based LC cell as a function of the applied ac voltage according to Eq. (1).

Fig. 4 .
Fig. 4. (a) The transmittance, I/I o of LC E7 (T = 22°C) in the WSe 2 -based LC device as a function of applied ac voltage (f = 1000 Hz).A smaller voltage range of the same transmittance curve is shown in the inset, where six maxima can be clearly counted.(b) Twelve separate micrographs of the WSe 2 -based LC cell under the crossed-polarized optical microscope at different applied voltages.

Fig. 5 .
Fig. 5. Optical transmission spectroscopy for WSe 2 /ITO slide and PI/ITO slide.The color band on the x-axis shows the visible wavelength range.