Abstract:
An in-plane switching mode liquid crystal display device includes a first substrate, a second substrate, ferroelectric liquid crystal layers between the first and second substrates disposed substantially at respective surfaces of the first and second substrates, the ferroelectric liquid crystal layers arranged by an exposure to one of an amphiphobic medium and an amphiphilic medium, a nematic liquid crystal layer between the ferroelectric liquid crystal layer of the first substrate and the ferroelectric liquid crystal layer of the second substrate, and electrodes disposed on surfaces of each of the first and second substrates to vertically apply an electric field to the ferroelectric liquid crystal layers and to the nematic liquid crystal layer.

Description:
This application claims the benefit of Korean Patent Application No. P2003-99337 filed in Korea on Dec. 29, 2003, which is hereby incorporated by reference. 
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates to a liquid crystal display device, more particularly, to an in plane switching mode liquid crystal display device having ferroelectric liquid crystal material and a method of fabricating the same. 
     2. Description of the Related Art 
     A liquid crystal display (LCD) device controls an electric field applied to a liquid crystal cell. The controlling of the electric field modulates light incident to the liquid crystal cell, thereby displaying a picture. A liquid crystal material injected into the liquid crystal display device is in a middle state of a solid and a liquid having both fluidity and elasticity together. 
     A twisted nematic (TN) mode uses a vertical electric field scheme and is the liquid crystal mode most commonly used in liquid crystal display devices until recently. The TN mode has the advantage of having a relatively high aperture ratio. On the other hand, the TN mode has a disadvantage of not having a wide viewing angle because of the refractive index of the liquid crystal material. Further, the response speed of the liquid crystal material using TN mode is slow. 
     An in-plane switching (IPS) mode uses an electric field that is parallel to the display panel of the liquid crystal display device. In the IPS mode, an electric field is formed between electrodes formed on a substrate, and liquid crystal molecules are driven by the horizontal electric field.  FIG. 1  is a cross-sectional view schematically illustrating schematically an in-plane switching mode liquid crystal display device according to the related art. In the IPS mode, as shown in  FIG. 1 , a pixel electrode  16  and a common electrode  15  are formed on a lower glass substrate  18 , and an electric field  20  is formed in a horizontal direction by a voltage difference applied between the electrodes  15  and  16 . Liquid crystal molecules  14  are rotated on a surface of the substrate by the electric field  20  to modulate a polarization component of light transmitting a liquid crystal layer. In  FIG. 1 , polarizers  11  and  19  are respectively attached to an upper glass substrate  12  and the lower glass substrate  18  such that the axes of the polarizers cross each other. The alignment films  13  and  17  are respectively formed on the upper glass substrate  12  and the lower glass substrate  18 . If the polarization component of the light transmitting through the liquid crystal layer is changed by 90 degrees, then the light passes through the upper polarizer  11 . On the other hand, if the polarization component of the light does not change, then the light cannot pass thorough the upper polarizer  11 . 
     The IPS mode liquid crystal display device shown in  FIG. 1  has an advantage in that it has a wide viewing angle since a refractive index change of the liquid crystal material is not large. However, in the IPS mode liquid crystal display device, the electric field applied to the liquid crystal molecules is done with opaque electrodes  15  and  16  on the lower substrate. As a result, it has the disadvantage of having a low aperture ratio. 
     A ferroelectric liquid crystal (FLC) has the advantage having a high response speed and a wide viewing angle. The ferroelectric liquid crystal has a structure the uses both electrical and magnetic properties. A ferroelectric liquid crystal can be driven within plane that rotates along a virtual cone in response to electric field. The ferroelectric liquid crystal has a permanent polarization, in other words, a spontaneous polarization without having an external electric field. Like an interaction between two magnets. If an external electric field is applied, the ferroelectric liquid crystal rotates rapidly with an interaction between the external field and the spontaneous polarization. The response speed of the ferroelectric liquid crystal is several hundred or thousand times as fast as that of other mode liquid crystal. Further, since the ferroelectric liquid crystal has an in-plane-switching property in itself, it has a wide viewing angle without having a special electrode structure or a compensation film. Ferroelectric liquid crystal is classified into a V-switching mode and a half V-switching mode according to a characteristic reacting in response to a polarity of an electric field. 
     In the ferroelectric liquid crystal cell of the V-switching mode, as temperature is lowered, a thermodynamic phase transition arises like an isotropic→a smectic A phase (SA)→a chiral smectic X phase (Sm X*)→a crystal. Isotropic is a state where the liquid crystal molecules do not have direction and location order. Smectic A phase is a state where the liquid crystal molecules are divided into a virtual layer and arranged vertically on the virtual layer, and has a symmetry about up and down. The chiral smectic X phase is a middle state between the smectic A phase and the crystal phase.  FIG. 2  is a graph illustrating a voltage vs. a transmittance property of a ferroelectric liquid crystal of a V-switching mode according to the related art. The ferroelectric liquid crystal cell of the V-switching mode in which the liquid crystal molecule is phase-transited to the chiral smectic X phase, as shown in  FIG. 2 , improves a light transmittance of an incidence light by changing the arrangement state of the liquid crystal molecules in response to the external voltage of positive polarity +V and the external voltage of negative polarity −V. 
     The V-switching mode has the advantages of high-speed-response and wide viewing angle. However, the V-switching mode has the disadvantages of requiring high power for driving a liquid crystal cell to overcome a large spontaneous polarization value and a large storage capacitor to store enough charge for maintaining a data voltage. Accordingly, if the V-switching mode is used in a liquid crystal display device, power consumption of the liquid crystal display device is high, and an aperture ratio is reduced because of a large electrode area for a capacitor. 
     In contrast, the half V-switching mode has the advantages of high-speed-response, wide viewing angle, and further, it is well suited for displaying moving picture and representing liquid crystal display device because the capacitance is low comparatively.  FIG. 3  is a diagram illustrating a phase transition process of the ferroelectric liquid crystal of a half V-switching mode according to the related art. As shown in  FIG. 3 , the phase transition from the isotropic to the chiral nematic phase (N*) occurs below the transition temperature (Tni), the phase transition from the chiral nematic phase (N*) to the chiral smectic C phase (Sm C*) occurs below the transition temperature (Tsn), and the phase transition from the chiral smectic C phase to the crystal occurs as the temperature is lowered below the transition temperature (Tcs) causing. The thermodynamic phase transitions that can be attained are isotropic→the chiral nematic (N*)→the chiral smectic C phase (Sm C*)→the crystal. 
       FIG. 4  is a diagram illustrating a change of molecule arrangement depending on whether or not an alignment under an electric field is applied to the ferroelectric liquid crystal of the half V-switching mode according to the related art. A method of manufacturing the liquid crystal cell of a half V-switching mode will be described as follows with reference to  FIG. 4 . The ferroelectric liquid crystal is injected into the cells arranged in parallel at an incipient temperature of the isotropic phase that does not have direction and location order. If the temperature of the isotropic is lowered to a designated temperature, the ferroelectric liquid crystal becomes chiral nematic phase (N*) arranged in parallel with respect to the rubbing direction. In the chiral nematic phase (N*), if the temperature is gradually reduced and a sufficient electric field is applied to the inside of the liquid crystal cell, then the ferroelectric liquid crystal of the chiral nematic phase (N*) transits to the chiral smectic phase (SmC*) and the spontaneous polarization direction of the ferroelectric liquid crystal is arranged coincidentally with a direction of an electric field formed inside the cell. As a result, the spontaneous polarization direction of the ferroelectric liquid crystal coincides with the direction of electric field applied upon electric field alignment among two arrangement directions of the molecules depending on the alignment process of an upper plate and a lower plate when the parallel alignment is disposed, and the ferroelectric liquid crystal has a uniform alignment condition entirely by virtue of the electric field alignment, as shown in  FIG. 4 . 
       FIGS. 5A and 5B  are graphs illustrating the changes of light transmittance according to the voltage in the ferroelectric liquid crystal cell of the half V-switching mode, respectively. Referring to  FIG. 5A , in case of the liquid crystals being aligned under electric field by a negative polarity voltage −V, the ferroelectric liquid crystal cell of the half V-switching mode makes incident light transmit by changing the polarization direction of the incident light 90° only when a positive voltage +V is applied thereto, and makes most of the incident light cut-off by maintaining the polarization direction of the incident light when the negative voltage −V is applied thereto. The ratio of the light transmittance increases in proportion to the positive electric field intensity and maintains the maximum value if the positive electric field intensity increases to more than the designated threshold value. In contrast, if the ferroelectric liquid crystal of the half V-switching mode cell is aligned under electric field by the positive polarity voltage +V, the ferroelectric liquid crystal cell of the half V-switching mode, as illustrated in  FIG. 5B , makes the incident light transmit only when the negative voltage −V is applied thereto and makes most of the incident light cut-off when the positive voltage +V is applied. 
       FIG. 6  represents a change of the ferroelectric liquid crystal arrangement when applying the alignment electric field of a negative polarity E(−) to the ferroelectric liquid crystal cell of the half V-switching mode, and a change of the ferroelectric liquid crystal arrangement when respective external electric fields E(+) and E(−) of a positive polarity and a negative polarity are applied thereto. Referring to  FIG. 6 , if the ferroelectric liquid crystal cell of the half V-switching mode is aligned under the external electric field of the negative polarity E(−), then the spontaneous polarization direction Ps of the ferroelectric liquid crystal is aligned uniformly in a direction coinciding with the external electric field of the negative polarity (E−). 
     After the electric field is aligned as described above, if the external electric field of the positive polarity (E(+)) is applied to the ferroelectric liquid crystal cell of the half V-switching mode, an arrangement of the liquid crystal molecules is changed and a direction of spontaneous polarization Ps coincides with the external electric field of the positive polarity E(+). The polarization direction of the light incident to the liquid crystal layer via a lower plate polarizer is changed to the polarization direction of an upper plate polarizer by the liquid crystal molecules in which the arrangement is changed and the incident light transmits through the polarizer installed in the upper plate. If the external electric field of the negative polarity E(−) is applied or the external electric field is not applied to the ferroelectric liquid crystal cell of the half V-switching mode, then the arrangement of the liquid crystal molecules maintains an incipient arrangement state as it is and the incident light maintains the polarization direction. Thus, the incident light cannot pass through the polarizer in the upper plate. 
       FIG. 7  is a configuration illustrating two sub-regions existing in one liquid crystal cell in a case that an alignment under an electric field is not performed according to the related art. Without performing the electric field alignment process, the two states of molecule arrangements of which the layers are randomly vent appear while phase-transiting from the chiral nematic phase (N*) to the chiral smectic C phase (SmC*). If a random bi-stable state in which the molecule arrangement of the ferroelectric liquid crystal is random becomes, then it is difficult to uniformly control the ferroelectric liquid crystal. If the two states of molecule arrangements of which the layers are different from each other randomly exist in one ferroelectric liquid crystal cell, then the liquid crystal cell, in response to the electric field having polarities different from each other, becomes divided into two regions that are separately driven. More specifically, as shown in  FIG. 7 , if two molecule arrangements exist with the layers are randomly bent in the same ferroelectric liquid crystal cell, then the direction of the spontaneous polarization Ps of ferroelectric liquid crystal molecule becomes different in the two regions. 
       FIG. 8  is a configuration illustrating a liquid crystal molecule reacting by an exterior electric field in two sub-regions shown in  FIG. 7  according to the related art. In  FIG. 7 , it is assumed that a symbol ⊙ represents a spontaneous polarization direction of the ferroelectric liquid crystal molecule identical to an electric field direction of a positive polarity and a symbol             represents a spontaneous polarization direction of the ferroelectric liquid crystal molecule identical to an electric field direction of a negative polarity. If the electric field of the negative polarity is applied to the ferroelectric liquid crystal cell including two molecule arrangements of which the layers, having the direction of the spontaneous polarization Ps different from each other, are different from each other, then the liquid crystal molecules having the direction of the spontaneous polarization Ps in running parallel to the electric field direction           of the negative polarity included in a molecular arrangement, as in the right region of  FIG. 7 , does not react to the electric field of the negative polarity and maintains the spontaneous polarization direction as it is. In contrast, the liquid crystal molecules included in a molecular arrangement, as in a left region in  FIG. 7 , reacts to the electric field of the negative polarity to rotate along the virtual cone, and, at the same time, the direction of the spontaneous polarization Ps is changed in the           direction in running parallel to the electric field of the negative polarity, as shown in  FIG. 8 . At this time, while an incident light passes through the left region of  FIG. 7 , the polarization direction is changed forward in a direction of a light outgoing side (that is, a polarization direction of the polarizer in the upper plate) to pass through the polarizer in the upper plate. In contrast, an incident light entered to the right region of in  FIG. 7  maintains its polarization direction to enter the polarizer in the upper plate, whereby the incident light cannot transmit the polarizer in the upper plate.
     Accordingly, the two regions exist with the layers are vent randomly and the direction of the spontaneous polarization Ps is different in the two regions in one ferroelectric liquid crystal cell, then it is impossible to accurately control the half V-switching mode. Further, as shown in  FIG. 7 , if there are exist the two regions different from each other in the same ferroelectric liquid crystal cell, then a brightness difference can be appeared every frame period because the liquid crystal molecules react to the electric fields having polarities different from each other depending on the respective regions. 
     SUMMARY OF THE INVENTION 
     Accordingly, the present invention is directed to an in-plane-switching mode liquid crystal display device of and a method of fabricating the same that substantially obviates one or more of the problems due to limitations and disadvantages of the related art. 
     An object of the present invention to provide a liquid crystal display device of in-plane switching mode and a method of fabricating the same capable of aligning a ferroelectric liquid crystal and representing a wide viewing angle without requiring an exterior electric field. 
     Additional features and advantages of the invention will be set forth in the description which follows, and in part will be apparent from the description, or may be learned by practice of the invention. The objectives and other advantages of the invention will be realized and attained by the structure particularly pointed out in the written description and claims hereof as well as the appended drawings. 
     To achieve these and other advantages and in accordance with the purpose of the present invention, as embodied and broadly described, an in-plane switching mode liquid crystal display device includes a first substrate, a second substrate, ferroelectric liquid crystal layers between the first and second substrates disposed substantially at respective surfaces of the first and second substrates, the ferroelectric liquid crystal layers arranged by an exposure to one of an amphiphobic medium and an amphiphilic medium, a nematic liquid crystal layer between the ferroelectric liquid crystal layer of the first substrate and the ferroelectric liquid crystal layer of the second substrate, and electrodes disposed on surfaces of each of the first and second substrates to vertically apply an electric field to the ferroelectric liquid crystal layers and to the nematic liquid crystal layer. 
     In another aspect of the present invention, a method of fabricating an in-plane switching mode liquid crystal display device includes forming an electrode on each of first and second substrates, forming ferroelectric liquid crystal layers at respective surfaces of the first and second substrates, deriving a phase transition of the ferroelectric liquid crystal layers in a state exposed to one of an amphiphilic medium and an amphiphobic medium to stabilize the ferroelectric liquid crystal layers, and forming a nematic liquid crystal layer between the ferroelectric liquid crystal layer of the first substrate and the ferroelectric liquid crystal layer of the second substrate. 
     It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory and are intended to provide further explanation of the invention as claimed. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       The accompanying drawings, which are included to provide a further understanding of the invention and are incorporated in and constitute a part of this specification, illustrate embodiments of the invention and together with the description serve to explain the principles of the invention. 
         FIG. 1  is a cross-sectional view illustrating schematically an in-plane switching mode liquid crystal display device according to the related art. 
         FIG. 2  is a graph illustrating a voltage vs. a transmittance property of a ferroelectric liquid crystal of a V-switching mode according to the related art. 
         FIG. 3  is a diagram illustrating a phase transition process of the ferroelectric liquid crystal of a half V-switching mode according to the related art. 
         FIG. 4  is a diagram illustrating a change of molecule arrangement depending on whether or not an alignment under an electric field is applied to the ferroelectric liquid crystal of the half V-switching mode according to the related art. 
         FIGS. 5A and 5B  are graphs illustrating a voltage vs. a transmittance property of the half V-switching mode according to the related art. 
         FIG. 6  is a diagram illustrating the ferroelectric liquid crystal of the half V-switching mode reacting to an electric field upon aligning under an electric field and to an electric field applied upon driving according to the related art. 
         FIG. 7  is a configuration illustrating two sub-regions existing in one liquid crystal cell in a case that an alignment under an electric field is not performed according to the related art. 
         FIG. 8  is a configuration illustrating a liquid crystal molecule reacting by an exterior electric field in two sub-regions shown in  FIG. 7  according to the related art. 
         FIGS. 9A to 9D  are cross-sectional views sequentially illustrating a method of fabricating a liquid crystal display device of an in-plane switching mode according to an exemplary embodiment of the present invention. 
         FIG. 10  is a configuration schematically illustrating a ferroelectric liquid crystal being stabilized into a mono-stable state in the phase transition process of  FIGS. 9C and 9D . 
         FIGS. 11A to 11D  are sectional views sequentially illustrating a method of fabricating a liquid crystal display device of an in-plane switching mode according to another exemplary embodiment of the present invention. 
         FIG. 12  is a configuration schematically illustrating a ferroelectric liquid crystal being stabilized to a mono-stable state in the phase transition process of  FIGS. 11C and 11D . 
         FIG. 13  is a cross-sectional view illustrating a liquid crystal display device of an in-plane switching mode according to an exemplary embodiment of the present invention. 
         FIG. 14  is a configuration illustrating a movement of the in-plane switching mode of the ferroelectric liquid crystal shown in  FIG. 13  and of a nematic system liquid crystal. 
         FIGS. 15 and 16  are sectional views illustrating a liquid crystal display device of an in-plane switching mode according to additional embodiments of the present invention. 
     
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     Reference will now be made in detail to the preferred embodiments of the present invention, examples of which are illustrated in the accompanying drawing. Hereinafter, the preferred embodiments of the present invention will be described in detail with reference to  FIGS. 9 to 16 . 
       FIGS. 9A to 9D  are cross-sectional views sequentially illustrating a method of fabricating a liquid crystal display device of an in-plane switching mode according to an exemplary embodiment of the present invention. First, an electrode  32  and a polarity alignment film  33  are formed on a glass substrate  31 , as shown in  FIG. 9A . The electrode  32  is formed of a transparent conductive material, such as an indium-tin-oxide (ITO). Since the polarity alignment film  33  has an electric negativity such as a polyamic acid, the polarity alignment film  33  electrically represents a polarity and is formed of an organic alignment material capable of aligning a liquid crystal material. The polarity alignment film  33  is rubbed to determine an alignment direction of ferroelectric liquid crystal molecules. 
     Subsequently, a mixture in which the ferroelectric liquid crystal and an organic solvent are uniformly mixed is applied to the glass substrate  31  while in a state that the glass substrate  31  is exposed to an amphiphobic medium almost not representing electric polarity, and then the glass substrate  31  is increased up to the temperature between about 140° C. to 160° C. to vaporize the organic solvent. As a result, a ferroelectric liquid crystal layer  34  of an isotropic phase is formed on the glass substrate  31 . The amphiphobic medium may be selected from an atmosphere of air or nitrogen N 2 , for example. 
     To make a phase transition from the ferroelectric liquid crystal layer  34  to the chiral nematic phase (N*) as shown in  FIG. 9C , the temperature of the glass substrate  31  is lowered to the temperature for the phase transition between 110° C. to 85° C. Further, to make a phase transition from the ferroelectric liquid crystal layer  34  to the chiral nematic phase (N*) as shown in  FIG. 9C  to the chiral smectic C phase (Sm C*) as shown in  FIG. 9D , the temperature of the glass substrate  31  is lowered to the temperature for the phase transition between about 80° C. to 50° C. At this time, as shown in  FIG. 10 , a spontaneous polarization Ps is generated in the liquid crystal molecules  40  of the ferroelectric liquid crystal layer  34  during the transition process to the chiral smectic C phase (Sm C*), and the direction of the spontaneous polarization Ps directs to the polarity alignment film  33 . In other words, while the liquid crystal molecules  40  of the ferroelectric liquid crystal layer  34  is subjected to the phase transition to the chiral smectic C phase (Sm C*), the direction of the spontaneous polarization Ps is uniformly arranged to a mono-stable state without having an external electric field. Alternatively, the liquid crystal molecules  40  of the ferroelectric liquid crystal layer  34  may go though phase transitions from an isotropic phase to a chiral smectic A phase (Sm A*) and from the chiral smectic A phase (Sm A*) to a chiral smectic C phase (Sm C*). Also, the liquid crystal molecules  40  of the ferroelectric liquid crystal layer  34  may go though phase transitions from an isotropic phase to a chiral smectic C phase (Sm C*). 
       FIGS. 11A to 11D  are sectional views sequentially illustrating a method of fabricating a liquid crystal display device of an in-plane switching mode according to another exemplary embodiment of the present invention. 
     First, an electrode  22  and a polarity alignment film  23  are formed on a glass substrate  21  as shown in  FIG. 11A . The electrode  22  is formed of a transparent conductive material such as an indium tin oxide (ITO). The polarity alignment film  23  is formed of an organic alignment material such as a polyamic acid, and the polarity alignment film is rubbed to define an alignment direction of ferroelectric liquid crystal molecules. 
     Subsequently, a mixture in which the ferroelectric liquid crystal and an organic solvent are uniformly mixed is applied to the glass substrate  11  with the glass substrate  11  being exposed under an amphiphilic medium, e.g., under an atmosphere of H 2 O or O 2 , having a high electric negativity (i.e., a high polarity) as compared with the alignment film  23  as shown in  FIG. 11B , and with the glass substrate  11  being at a temperature of the glass substrate  21  is increased to a temperature between about 140° C. to 160° C. to vaporize the organic solvent. As a result, a ferroelectric liquid crystal layer  24  of an isotropic phase is formed on the glass substrate  21 . 
     In order to make a phase transition from the ferroelectric liquid crystal layer  24  to the chiral nematic phase (N*) as shown in  FIG. 11C , the temperature of the glass substrate  21  is lowered to the temperature for the phase transition between about 110° C. to 85° C. Further, to make a phase transition from the ferroelectric liquid crystal layer  24  to the chiral nematic phase (N*) as shown in  FIG. 11C  to the chiral smectic C phase (Sm C*) as shown in  FIG. 11D , the temperature of the glass substrate  21  is lowered to the temperature for the phase transition between about 80° C. to 50° C. At this time, as shown in  FIG. 12 , a spontaneous polarization Ps is generated in the liquid crystal molecules  40  of the ferroelectric liquid crystal layer  24  during the transition process to the chiral smectic C phase (Sm C*), and the direction of the spontaneous polarization Ps directs toward the polarity medium on the opposite side to the alignment film  23 . This is because the polarity medium on the opposite side to the alignment film  23  has a higher electrical negativity as compared with the alignment film  23 . In other words, while the liquid crystal molecules  40  of the ferroelectric liquid crystal layer  24  is subject to the phase transition to the chiral smectic C phase (Sm C*), the direction of the spontaneous polarization Ps is uniformly arranged to a mono-stable state without having an external electric field. 
     The ferroelectric liquid crystal layers  24  and  34 , uniformly aligned to the mono-stable state through the processes as in  FIGS. 9A to 9D  and  FIGS. 11A to 11D , are operated in the half V-switching mode shown in  FIG. 5A  or  5 B. The liquid crystal display device of the in-plane switching mode implemented by using the ferroelectric liquid crystal of the half V-switching mode and the method of fabricating the same will be described in conjunction with  FIGS. 13 and 14 . The upper plate of the liquid crystal display device of the in-plane switching mode according to the present invention is manufactured by the method as in  FIGS. 9A to 9D , and the lower plate is manufactured by the method as in  FIGS. 11A to 11D . 
       FIG. 13  is a cross-sectional view illustrating a liquid crystal display device of an in-plane switching mode according to an exemplary embodiment of the present invention. Referring to  FIG. 13 , the exemplary liquid crystal display device of the in-plane switching mode according to the present invention includes an upper plate  100  and a lower plate  110  combined by a sealant (not shown), and a nematic liquid crystal  50  injected between the upper plate  100  and the lower plate  110 . The ferroelectric liquid crystal layers  24  and  34  respectively formed in the upper glass substrate  21  of the upper plate  100  and the lower glass substrate  31  of the lower plate  110  forms an interface with the nematic liquid crystal. Polarizers (not shown) whose light transmitting axes are vertically crossed with each other are attached on a light incident surface of the lower glass substrate  31  and on a light outgoing surface of the upper glass substrate  21 , respectively. 
     In liquid crystal display device according to the present invention, a voltage is applied to the upper electrode  22  and the lower electrode  32  to drive the nematic liquid crystal  50  under in-plane, to thereby modulate light. At this time, when applying an electric field (E) having a polarity different from the polarity having been aligned during the transition process to the chiral smectic C phase (Sm C*), the ferroelectric liquid crystal  40  is driven in a direction of the in-plane as the direction of the spontaneous polarization Ps is changed, and induces the namatic liquid crystal molecules  50  adjacent to the ferroelectric liquid crystal  40  to drive under in-plane. 
     The liquid crystal display device of the in-plane switching mode assures that a wide viewing angle is implemented by virtue of the in-plane driving of the nematic liquid crystal  50  and that a deterioration of an aperture ratio is minimized by applying an electric field to the liquid crystal  50  under a vertical electric field scheme. Further, since the nematic liquid crystal  50  is rapidly moved by the ferroelectric liquid crystal  40 , it is possible to improve a response speed of the nematic liquid crystal  50 . 
       FIGS. 15 and 16  are cross-sectional views illustrating a liquid crystal display device of an in-plane switching mode according to further another embodiment of the present invention. Referring to  FIGS. 15 and 16 , in the liquid crystal display device of the in-plane switching mode according to the present invention, directions of spontaneous polarizations Ps of ferroelectric liquid crystals  80  and  90  in ferroelectric liquid crystal layers  60 ,  61 ; and  70 ,  71  formed on the upper plate  110  and the lower plate  100  are made differently from each other. 
     The liquid crystal display device shown in  FIG. 13  reacts to only an electric field with any one of polarities in accordance with a half V-switching mode to drive the nematic liquid crystal  50  under the in-plane switching since the spontaneous polarization directions of the ferroelectric liquid crystals on the upper plate  100  and the lower plate  110  are same with each other. 
     In contrast, if the spontaneous polarization directions of the ferroelectric liquid crystal on the upper plate  100  and the lower plate  110  are made differently from each other, then the ferroelectric liquid crystal  80  or  90  formed on any one of the upper and the lower glass substrates  21  and  31  derives the driving of the nematic liquid crystal under the in-plane switching when an electric field with a positive polarity or a negative polarity is applied, and simultaneously, the ferroelectric liquid crystal  80  or  90  formed on the other substrate  21  or  31  do not react to the electric field and maintain an incipient arrangement state as it is. At this time, as the nematic liquid crystal  50  is switched in plane only by the ferroelectric liquid crystal resided in one hand, the nematic liquid crystal  50  becomes a structure twisted in a vertical direction. As a result, the liquid crystal display device of the in-plane switching mode in  FIGS. 15 and 16  reacts to both electric fields with the positive polarity and the negative polarity and thus, is capable of displaying images under the in-plane switching of the nematic liquid crystal  50 . 
     In the liquid crystal display device in  FIGS. 15 and 16 , the direction of the spontaneous polarization of the ferroelectric liquid crystal may be arranged in a desired direction, through the methods illustrated in  FIGS. 9A to 9D  and  FIGS. 11A to 11D . As described above, the ferroelectric liquid crystal is transited from the isotropic phase to the smectic phase while the ferroelectric liquid crystal  31  is exposed to a medium having an electric polarity. Therefore, it is possible to uniformly arrange the spontaneous polarization of the liquid crystal material without having the exterior electric field as well as to implement the wide viewing angle by using the in-plane driving of the ferroelectric liquid crystal. 
     It will be apparent to those skilled in the art that various modifications and variations can be made in the in plane switching mode liquid crystal display device and method of fabricating the same the present invention without departing from the spirit or scope of the invention. Thus, it is intended that the present invention cover the modifications and variations of this invention provided they come within the scope of the appended claims and their equivalents. 
     It will be apparent to those skilled in the art that various modifications and variations can be made in the present invention without departing from the spirit or scope of the invention. Thus, it is intended that the present invention cover the modifications and variations of this invention provided they come within the scope of the appended claims and their equivalents.