in various embodiments , the liquid crystal composition of the invention comprises a liquid crystal and a polymer . the liquid crystal exhibits a macroscopic anisotropic property in the absence of the polymer and under a condition such as a temperature in the range of from about 0 ° c . to about 200 ° c . the polymer can stabilize the liquid crystal so that the liquid crystal exhibits a macroscopic isotropic property under the same condition such as the temperature in the range of from about 0 ° c . to about 200 ° c . it should be understood that the term “ condition ” used in this specification includes any condition which affects the liquid crystal &# 39 ; s physical , chemical , optical , and electrical properties , except that it does not include an electrical field . in various embodiments , the liquid crystal stabilized by the polymer exhibits a macroscopic anisotropic property when an electrical field is applied thereon . although there is no specific limitation on the macroscopic anisotropic property and the macroscopic isotropic property , in typical embodiments they are both an optical property . examples of the liquid crystal that can be used in the liquid crystal composition of the invention include , but are not limited to , chiral or achiral lcs ; liquid crystals with positive dielectric anisotropy in the absence of the polymer ; and liquid crystals in the anisotropic liquid crystal state , such as nematic , cholesteric , and smectic phases , when in the absence of the polymer . in exemplified embodiments , the liquid crystal is selected from a nematic liquid crystal such as e31 lv , e49 , bl036 , tl203 , or any mixture thereof . e31 lv , e49 , bl036 , and tl203 are commercially available from em industries , inc ., and their molecules comprise rigid phenyl ring ( s ) and / or cyclohexane ring ( s ), flexible hydrocarbon tail ( s ) and polar group ( s ). the liquid crystal composition of the invention may further comprise any suitable additional ingredient , such as a chiral dopant . examples of suitable chiral dopants include but are not limited to r811 , s811 , r1011 , cb15 , and any mixture thereof . r811 , s811 , r1011 , and cb15 are all commercially available from em industries , inc . the liquid crystal composition of the invention may further comprise any suitable additional ingredient such as a chiral dopant . examples of the chiral dopant may be selected from r811 , s811 , r1011 , cb15 , and any mixture thereof . r811 , s811 , r1011 , and cb15 are all commercially available from em industries , inc . in embodiments , the liquid crystal and the polymer in the composition of the invention may have a weight ratio generally in the range of from about 100 : 1 to about 1 : 1 , preferably in the range of from about 20 : 1 to about 2 : 1 , and more preferably in the range of from about 10 : 1 to about 3 : 1 . the invention also provides a liquid crystal device , such as a liquid crystal display or a phase modulator , including one or more cells , wherein at least one of the cells comprises a liquid crystal composition . the composition comprises a liquid crystal and a polymer , wherein the liquid crystal exhibits an anisotropic property in the absence of the polymer under a condition such as the operation temperature of the device , and the polymer stabilizes the liquid crystal so that the liquid crystal exhibits a macroscopic isotropic property under the same condition . typically , the liquid crystal stabilized by the polymer exhibits a macroscopic anisotropic property under an electrical field . for example , the macroscopic anisotropic property and the macroscopic isotropic property may both be an optical property . a liquid crystal display is a device that can show arbitrary pictures . a phase modulator is a device that can vary the optical length . in some exemplary embodiments , the cell comprises two substrates with transparent electrodes . the transparent electrodes are thin electric conducting layers coating on glass or plastic substrates , one example of which is ito ( indium tin oxide ). a liquid crystal display of the invention may have a viewing angle in the range of from about − 60 ° to about 60 °, and a response time shorter than 1 ms . the response time means the time intervals of the transmittance changes from low to high and from high to low when a voltage is turned on or turned off . when no electric field is applied , the display may have a low transmittance , such as lower than 1 %. when an electric field is applied , the display may have a high transmittance , such as greater than 5 %. the intensity of the electric field may range from about 0 v / micron to about 20 v / micron , and preferably range from about 2 v / micron to about 10 v / micron . when no electric field is applied , a phase modulator of the invention may have a polarization - insensitivity with an optical retardation value in a range such as from about 0 micron to about +/− 1 . 0 micron . such a phase modulator may have a polarization - insensitivity with a second optical retardation value in a range such as from about +/− 0 . 00001 micron to about +/− 5 micron when an electric field is applied . the polarization - insensitivity is used to characterize that the optical phase change when light propagates through the device is independent of the polarization of the incident light . the invention provides a method of modifying the property of a liquid crystal comprising : ( i ) providing a liquid crystal that alone exhibits a macroscopic anisotropic property such as an optical property under a condition ; and wherein the polymer stabilizes the liquid crystal so that the liquid crystal exhibits a macroscopic isotropic property such as an optical property under the same condition . the method of the invention may further include a step of applying an electrical field to the liquid crystal stabilized by the polymer so that the liquid crystal exhibits a macroscopic anisotropic property . according to the invention , one process for combining the liquid crystal with the polymer comprises : ( a ) mixing the liquid crystal with monomers and / or oligomers at a first temperature , wherein the liquid crystal exhibits an anisotropic property at the first temperature ; ( b ) heating the mixture from step ( a ) to a second temperature , wherein the liquid crystal alone exhibits an isotropic property at the second temperature ; and ( c ) polymerizing the monomers and / or oligomers into a polymer at the second temperature ; wherein the polymer stabilizes the liquid crystal so that the liquid crystal exhibits a macroscopic isotropic property at the first temperature . polymerizing the monomers and / or oligomers into the polymer may be accomplished by free radical polymerization , cationic polymerization , anionic polymerization , and photo - polymerization , among others . in an embodiment , a chiral or achiral liquid crystal is mixed with monomers and / or oligomers . in either case , the liquid crystal has a positive dielectric anisotropy and tends to be aligned parallel to an applied electric field . in this embodiment , the lc / polymer mixture is filled into the display or modulator cell , which generally consists of two substrates with transparent electrodes . once filled , the cell is heated to an elevated temperature such that the mixture is in the isotropic phase . under the heated condition , the monomers ( oligomers ) are polymerized in the isotropic phase to form an isotropic polymer network . when the cell is cooled to the operation temperature of the display , the liquid crystal retains the isotropic state , rendering a cell substantially in the macroscopic isotropic optical state . without the intention to be bound by any particular theory , it is believed that , on the sub - micron or smaller scale , the liquid crystal may be in an anisotropic liquid crystal state , i . e ., in a nematic , cholesteric or smectic phase . when light propagates through the material at any angle with respect to the cell normal , the net optical retardation of the material is substantially zero . the material also has a very small scattering effect on the light , and further does not change the polarization of the light . when an electric field is applied to the material , the liquid crystal molecules are tilted toward the field direction . fig1 schematically illustrates the basic structure of a polymer stabilized isotropic liquid crystal display . with reference to fig1 , a composition including a polymer network 102 and macroscopic isotropic liquid crystals 103 stabilized by network 102 is shown . the composition is sandwiched between two substrates 104 and 105 . on one of the substrates such as substrate 105 there are inter - digitated electrodes 106 , as in an in - plane - switch ( ips ) display or a bump display , through which electrical field with field direction 101 can be applied to the material . the transmission axes ( denoted as two - way straight arrows ) of the polarizer 107 and analyzer 108 ( as shown on 107 and 108 ) are orthogonal to each other . the electrodes make the angle about 45 ° with respect to the transmission axes of the polarizer and analyzer . in a pixel where no voltage is applied , the liquid crystal is in a random orientation state . when linearly polarized light goes through it , the polarization state does not change , because the material is optically isotropic . the light is absorbed by the analyzer , and the pixel is dark . in contrast , in the same pixel where voltage is applied , the liquid crystal is tilted toward the electric field direction and therefore exhibits birefringence . when linearly polarized light goes through it , the polarization is rotated toward the transmission axis of the analyzer . the light passes the analyzer and the pixel is bright . nematic liquid crystal e31lv ( 68 %), monomer rm 25 ( 20 %), chiral dopant r811 ( 10 %) and photo - initiator bme from polyscience inc . ( 2 %) were mixed . the mixture was filled into an ips cell with a thickness of 4 microns . the width of the electrode was also 4 microns , and the distance between any two consecutive electrodes was 10 microns . once filled , the cell was heated to 100 ° c . and the monomer was photo - polymerized for 30 minutes . after curing , the electro - optical properties of the cell were measured at room temperature ( 22 ° c .) by standard electro - optical equipment . fig2 shows the transmittance of the cell containing psi lc as a function of the applied electrical filed . the legend “ lc : mo (+ m2 ): ch = 70 : 20 : 10 ” in fig2 denotes that the psi lc was prepared from a mixture of the nematic lc , the monomers and the chiral dopant , in the weight ratio of 70 : 20 : 10 . similar to example 2 , nematic liquid crystal e31 lv ( 58 %), monomer rm 257 ( 20 %), chiral dopant r811 ( 20 %) and photo - initiator bme ( 2 %) were mixed . the mixture was filled into an ips cell with a thickness of 4 microns . the width of the electrode was 4 microns and the distance between any two consecutive electrodes was 10 microns . the cell was heated to 100 ° c . and the monomer was photo - polymerized for 30 minutes . after curing the electro - optical properties of the cell were measured at room temperature ( 22 ° c .) by standard electro - optical equipment . fig3 shows the transmittance of the cell containing psi lc as a function of the applied electrical filed . the legend “ lc : mo (+ m2 ): ch = 60 : 20 : 20 ” in fig3 denotes that the psi lc was prepared from a mixture of the nematic lc , the monomers and the chiral dopant , in the weight ratio of 60 : 20 : 20 . similar to example 2 , nematic liquid crystal e31lv ( 63 . 5 %), monomer rm 257 ( 15 %), chiral dopant r811 ( 20 %) and photo - initiator bme ( 1 . 5 %) were mixed . the mixture was filled into an ips cell with a thickness of 4 microns . the width of the electrode was 4 microns and the distance between any two consecutive electrodes was 10 microns . the cell was heated to 100 ° c . and the monomer was photo - polymerized for 30 minutes . after curing , the electro - optical properties of the cell were measured at room temperature ( 22 ° c .) by standard electro - optical equipment . fig4 shows the transmittance of the cell containing psi lc as a function of the applied electrical filed . the legend “ lc : mo (+ m2 ): ch = 65 : 15 : 20 ” in fig4 denotes that the psi lc was prepared from a mixture of the nematic lc , the monomers and the chiral dopant , in the weight ratio of 65 : 15 : 20 . similar to example 2 , nematic liquid crystal e31lv ( 63 %), monomer rm 257 ( 20 %), chiral dopant r811 ( 15 %) and photo - initiator bme ( 2 %) were mixed . the mixture was filled into an ips cell with a thickness of 4 microns . the width of the electrode was 4 microns and the distance between any two consecutive electrodes was 10 microns . the cell was heated to 100 ° c . and the monomer was photo - polymerized for 30 minutes . after curing , the electro - optical properties of the cell were measured at room temperature ( 22 ° c .) by standard electro - optical equipment . fig5 shows the transmittance of the cell containing psi lc as a function of the applied electrical filed . the legend “ lc : mo (+ m2 ): ch = 65 : 20 : 15 ” in fig5 denotes that the psi lc was prepared from a mixture of the nematic lc , the monomers and the chiral dopant , in the weight ratio of 65 : 20 : 15 . the material used in this example can be prepared in the same way as for a polymer stabilized isotropic liquid crystal display . fig6 schematically illustrates the basic structure of a polymer stabilized isotropic liquid crystal phase modulator . with reference to fig6 , a composition including a polymer network 602 and macroscopic isotropic liquid crystal 603 stabilized by network 602 is shown . the composition is sandwiched between two substrates 604 and 605 . electrodes 606 and 607 are on the inner surface of both substrates 604 and 605 and the electric field is in the cell normal direction 601 . when no voltage is applied , the liquid crystal is in the random oriented state . when normal incident light goes through it , the refractive index of the material is n iso =[( n e 2 + 2n o 2 )/ 3 ] 1 / 2 , where n e and n o are the extraordinary and ordinary refractive indices of the liquid crystal in the absence of the polymer , respectively . the optical phase retardation is 2πn iso d / λ , where d is the cell thickness and λ is the wavelength of the light . when a voltage is applied across the cell , the liquid crystal is tilted toward the electric field direction , and the refractive index of the material changes to a value n eff which is smaller than n iso . the optical phase retardation becomes 2πn eff d / λ . the higher the applied voltage , the smaller the effective refractive index . therefore , by varying the applied voltage , the optical phase retardation can be modulated . for example , this material can be used to make an electrically tunable fabry - perot interferometer . the invention has been described with reference to the exemplary embodiments . obviously , modifications and alterations will occur to others upon reading and understanding the preceding detailed description . it is intended that the invention be construed as including all such modifications and alterations insofar as they come within the scope of the appended claims or the equivalents thereof .