TWI551917B - Liquid crystal panel module and liquid crystal display - Google Patents

Description

Liquid crystal panel module and liquid crystal display device

The present invention relates to a panel module and a display device, and more particularly to a liquid crystal panel module and a liquid crystal display device.

At present, the market performance requirements for liquid crystal display devices are toward high contrast, no grayscale inversion, small color shift, high brightness, high color richness, high color saturation, fast response and wide viewing angle. The liquid crystal material is a highly efficient refractive index modulation material. The liquid crystal layer in the liquid crystal display device has a difference in optical path length between the ortho-beam and oblique-penetrating light up to half a wavelength, so that the liquid crystal display device has a problem of color shift, brightness reduction, and even gray-scale inversion at a large viewing angle. At present, technologies capable of achieving wide viewing angles include twisted nematic (TN) liquid crystals, wide viewing angle films, and multi-domain vertical alignment (MVA) liquid crystal display devices. . However, the wide viewing angle film used in the twisted nematic liquid crystal display device is expensive. The multi-domain vertical alignment liquid crystal display device has complicated process, high process time and cost, low aperture ratio, and low process yield.

In addition, the backlight module used in the liquid crystal display device does not have a light-emitting direction. Consistent, there is a disadvantage of low light utilization. In particular, the backlight provided by the side-into-light design provides a large portion of the light that cannot enter the liquid crystal panel.

In addition, since the electronic device is easy to carry, the consumer often frequently uses the liquid crystal display device of the electronic device in a public place. When a consumer reads a private letter or material in a public place by means of a liquid crystal display device, it is inevitable that private information may be leaked by an outsider.

The invention provides a liquid crystal panel module, which can solve the problems of color shift, brightness reduction and even gray scale inversion.

The invention provides a liquid crystal display device, which can solve the problems of color shift, brightness reduction and even gray scale inversion of the liquid crystal panel module, or solve the problem of low light utilization efficiency of the backlight module.

The liquid crystal panel module of the present invention comprises a liquid crystal panel and a diffraction grating layer. The liquid crystal panel has a plurality of pixels. The diffraction grating layer is disposed on the liquid crystal panel, and the maximum period of the grating of the diffraction grating layer is substantially less than one tenth of the size of the pixel.

In an embodiment of the liquid crystal panel module of the present invention, the grating of the diffraction grating layer is a phase grating, such as a sinusoidal phase grating. Further, the peak-to-valley phase delay of the phase grating is, for example, 2.9 or less. In addition, the peak-to-valley phase delay of the phase grating is, for example, greater than or equal to two. Alternatively, the peak-to-valley phase delay of the phase grating is, for example, greater than or equal to 0.9. In addition, phase The diffraction angle of the bit grating is, for example, between 20 and 65 degrees. In addition, the period of the phase grating is, for example, between 205 nm and 1900 nm. Furthermore, the peak-to-valley thickness difference of the phase grating is, for example, less than 1800 nm. Furthermore, the peak to valley thickness difference of the phase grating is, for example, between 108.9 nm and 223.5 nm. In an embodiment of the liquid crystal panel module of the present invention, the grating of the diffraction grating layer is a blazed grating. In addition, the peak-to-valley thickness difference of the blazed grating is, for example, less than 1950 nm. In addition, the peak-to-valley thickness difference of the blazed grating is, for example, between 70 nm and 713 nm. Furthermore, the diffraction angle of the blazed grating is, for example, between 20 and 65 degrees. In addition, the period of the blazed grating is, for example, between 209 nm and 1900 nm. In addition, the blazed grating is, for example, a binary approximation blazed grating.

In an embodiment of the liquid crystal panel module of the present invention, the liquid crystal panel module further includes a first polarizing plate and a second polarizing plate. The liquid crystal panel is disposed between the first polarizing plate and the second polarizing plate. The first polarizing plate includes a first protective film, a polarizing layer and a diffraction grating layer. The polarizing layer is disposed between the first protective film and the diffraction grating layer. In addition, the first polarizer may further include an anti-glare layer, and the diffraction grating layer is disposed between the polarizing layer and the anti-glare layer. In addition, the first polarizing plate may further include a second protective film disposed between the second protective layer and the diffraction grating layer. Furthermore, there is, for example, an air layer or a medium having a refractive index different from that of the diffraction grating layer between the second protective layer and the anti-glare treatment layer. In addition, the first polarizing plate may further include a second protective film, and the diffraction grating layer is disposed between the polarizing layer and the second protective layer. In addition, there is, for example, an air layer between the second protective film and the diffraction grating layer or a medium having a refractive index different from that of the diffraction grating layer. In addition, the first polarizer may further include a The anti-reflection layer is disposed between the diffraction grating layer and the polarization layer.

In an embodiment of the liquid crystal panel module of the present invention, the period of the grating of the diffraction grating layer is not constant.

In an embodiment of the liquid crystal panel module of the present invention, the grating of the diffraction grating layer has a plurality of arrangement directions.

In an embodiment of the liquid crystal panel module of the present invention, the distance between the diffraction grating layer and the liquid crystal panel is between 0.5 mm and 100 mm.

A liquid crystal display device of the present invention includes a backlight module and the aforementioned liquid crystal panel module. The liquid crystal panel module is disposed on the backlight module.

In an embodiment of the liquid crystal display device of the present invention, the liquid crystal panel is located between the diffraction grating layer and the backlight module.

In an embodiment of the liquid crystal display device of the present invention, the diffraction grating layer is located between the liquid crystal panel and the backlight module.

Another liquid crystal display device of the present invention includes the foregoing backlight module and a liquid crystal panel module. The liquid crystal panel module is disposed on the backlight module.

Based on the above, the liquid crystal panel module of the present invention utilizes multi-level diffracted light to compensate for the problem of large-view character bias, and the diffraction grating layer can also be used to positively convert the large-angle incident light provided by the backlight module. Further, the liquid crystal display device of the present invention can employ the aforementioned liquid crystal panel module.

The above described features and advantages of the invention will be apparent from the following description.

100, 102, 52‧‧‧ LCD panel module

110‧‧‧LCD panel

112‧‧‧ pixels

120A, 120B, 120C, 120D‧‧‧ first polarizer

122‧‧‧Diffraction grating layer

124‧‧‧Protective film

126‧‧‧Polarization layer

128‧‧‧Anti-glare treatment layer

130‧‧‧Second polarizer

A10‧‧‧Medium with different refractive index and refractive index of the diffraction grating layer

L10‧‧‧Anti-reflective layer

P10‧‧‧ pixel size

Λ‧‧ Cycle

N1, n2‧‧‧ refractive index

D‧‧•Crest to trough thickness difference

200, 54, 300, 400‧‧‧ backlight module

210, 310, 410‧‧‧ light guide plates

212, 412‧‧‧ shine surface

214, 314, 414‧‧‧ into the glossy surface

220, 420‧‧‧Lighting elements

230, 330‧‧‧Diffraction Grating Film

416‧‧‧ bottom

430‧‧‧Reflective Diffraction Grating Film

432‧‧‧reflective material layer

50‧‧‧Liquid crystal display device

56‧‧‧ front box

Θ‧‧‧ glare angle of the glare grating

322‧‧‧Circuit board

324‧‧‧Lighting diode

N10‧‧‧ main optical axis

R10, R20‧‧‧ area

FIG. 1 is a schematic diagram of a liquid crystal panel module according to an embodiment of the invention.

2A is a partial enlarged view of a diffraction grating layer of the liquid crystal panel module of FIG. 1.

2B to 2D are three other variations of the first polarizing plate of Fig. 1.

3 is a graph showing the relationship between the q-th order diffraction efficiency of the phase grating and the peak-to-valley phase delay m.

4 is a graph showing the relationship between the first-order and zero-order diffraction energy ratios of the phase grating and the peak-to-valley phase delay m.

Figure 5 is a graph showing the relationship between the period of the phase grating and the diffraction angle of the first order.

Figure 6 is a plot of peak-to-valley thickness difference versus peak-to-valley phase delay for a phase grating.

7 and FIG. 8 are respectively a relationship between luminance and gray scale values before and after the application of the diffraction grating layer in the liquid crystal panel module.

FIG. 9 is a partially enlarged view of a diffraction grating layer of a liquid crystal panel module according to another embodiment of the present invention.

Figure 10 is a graph showing the relationship between the q-th order diffraction efficiency and the peak-to-valley thickness difference of a blazed grating.

Figure 11 is a graph showing the relationship between the period of the blazed grating and the first-order diffraction angle.

Figure 12 is a partial enlarged view of a diffraction grating layer according to still another embodiment of the present invention.

FIG. 13 is a schematic diagram of a liquid crystal panel module according to still another embodiment of the present invention.

FIG. 14 is a schematic diagram of a backlight module according to an embodiment of the invention.

FIG. 15 is a schematic diagram of a backlight module according to another embodiment of the present invention.

FIG. 16 is a schematic diagram of a backlight module according to still another embodiment of the present invention.

Figure 17 is an exploded view of a liquid crystal display device in accordance with an embodiment of the present invention.

1 is a schematic view of a liquid crystal panel module according to an embodiment of the present invention, and FIG. 2A is a partially enlarged view of a diffraction grating layer of the liquid crystal panel module of FIG. 1. Referring to FIG. 1 and FIG. 2A , the liquid crystal panel module 100 of the present embodiment includes a liquid crystal panel 110 and a diffraction grating layer 122 . The liquid crystal panel 110 has a plurality of pixels 112. The diffraction grating layer 122 is disposed on the liquid crystal panel 110, and the maximum period 光栅 of the grating of the diffraction grating layer 122 is less than one tenth of the size P10 of the pixel 112.

According to the optical principle, by utilizing the undulation of light, a diffraction of light can be generated in a minute structure, that is, the forward incident light passes through the diffraction grating layer 122 to deflect a portion of the light to the upper and lower directions. In other words, the forward light emitted from the liquid crystal panel 110 is turned to the upper and lower viewing angles as it passes through the diffraction grating layer 122, so that the problems of color shift, gray scale inversion, and low brightness of the upper and lower viewing angles can be improved. Furthermore, by designing the maximum period 光栅 of the grating of the diffraction grating layer 122 to be smaller than the size P10 of the pixel 112, the moiré caused by the diffraction grating layer 122 and the pixel 112 can be further avoided. The grating of the diffraction grating layer 122 of this embodiment can be designed in a single cycle or in a plurality of cycles.

In addition, the liquid crystal panel module 100 further includes a first polarizing plate 120A and a second polarizing plate 130. The liquid crystal panel 110 is disposed on the first polarizing plate 120A and the second Between the polarizing plates 130. The first polarizing plate 120A includes at least one protective film 124, a polarizing layer 126, and a diffraction grating layer 122. The polarizing layer 126 and the diffraction grating layer 122 are disposed between the polarizing layer 126 and the protective film 124. When the thickness or intensity of the diffraction grating layer 122 is sufficient, the diffraction grating layer 122 itself can be used to protect the polarization layer 126. Optionally, the diffraction grating layer 122 may further have a protective layer 124, an anti-reflection layer or an anti-glare layer. The material of the protective film 124 is, for example, Triacetyl Cellulose (TAC). In addition, the surface of the first polarizing plate 120A away from the liquid crystal panel 110 can be subjected to anti-glare treatment to prevent the diffraction pattern generated by the ambient light from being incident on the diffraction grating layer 122 from affecting the display effect. In addition, the period of the grating of the diffraction grating layer 122 can also be designed to be non-determined, that is, the grating has various periods, and the degree to which the diffraction pattern affects the display effect can be slowed down. Alternatively, the peaks of the gratings of the diffraction grating layer 122 may not all be arranged in the same direction, so that the peaks of the gratings of different blocks may be arranged in different directions, and the degree of influence of the diffraction pattern on the display effect may also be slowed down.

2B to 2D are three other variations of the first polarizing plate of Fig. 1. Referring to FIG. 2B, the first polarizer 120B of the present embodiment is similar to the first polarizer 120A of FIG. 1, but the first polarizer 120B further includes an anti-glare layer 128 and another protective film 124. To protect the polarizing layer 126. The diffraction grating layer 122 is disposed between the polarizing layer 126 and the anti-glare processing layer 128, and the anti-glare processing layer 128 is disposed between the upper protective layer 124 and the diffraction grating layer 122. In addition, between the upper protective layer 124 and the anti-glare treatment layer 128, for example, an air layer or other medium A10 having a refractive index different from that of the diffraction grating layer 122 is interposed. The anti-glare treatment layer 128 is, for example, formed directly on the surface of the diffraction grating layer 122, while the upper protective layer 124 is Placed on the anti-glare layer 128. Referring to FIG. 2C, the first polarizer 120C of the present embodiment is similar to the first polarizer 120B of FIG. 2B, but the first polarizer 120C does not have the anti-glare layer 128 of FIG. 2B. That is, the upper protective layer 124 is directly placed on the diffraction grating layer 122 with an air layer or other medium A10 having a refractive index different from that of the diffraction grating layer 122. Referring to FIG. 2D, the first polarizer 120D of the present embodiment is similar to the first polarizer 120A of FIG. 1, but the first polarizer 120B further includes an anti-reflective layer L10 disposed on the diffraction grating layer 122 and the polarizing layer 126. between. The anti-reflection layer L10 can reduce the probability that the light passing through the polarizing layer 126 is reflected by the diffraction grating layer 122 to increase the overall light transmittance of the first polarizing plate 120D.

In this embodiment, the grating of the diffraction grating layer 122 is a phase grating, for example, a sinusoidal phase grating, that is, the cross section of the diffraction grating layer 122 is substantially sinusoidal, and the cross section of the diffraction grating layer 122 may also be sawtooth. shape. The qth order diffraction efficiency of the phase grating can be expressed as ,As shown in Figure 3.

Where m is the peak to peak phase delay of the phase grating, m = 2π(n2-n1)d/λ, and J is a Bessel function such as sine, cosine, and the like. In order to maintain the brightness of the positive viewing angle and moderately generate the splitting of the large viewing angle, at least the efficiency of the 0th order diffraction is greater than or equal to the efficiency of the 1st order diffraction. As can be seen from Fig. 3, m/2 ≦ 1.45, that is, the peak-to-valley phase delay of the phase grating is in the range of 2.9 or less, and the efficiency of the 0-order diffraction is ensured to be greater than or equal to the efficiency of the first-order diffraction. In addition, the peak-to-valley phase retardation of the phase grating is, for example, 2 or more, to appropriately generate the splitting of a large viewing angle.

In addition, since the color shift problem of the near-forward viewing angle is not large, and the probability that the user views the liquid crystal panel module 100 from a too large viewing angle is also low, the diffraction angle of the phase grating can be set to be between 20 degrees and 65 degrees. degree. The 1st order diffraction angle of the phase grating can be expressed as The relationship between the diffraction angle of the first order and the period of the phase grating is as shown in FIG.

Where λ is the wavelength of the incident light, n2 is the refractive index of the diffraction grating layer 122, and Λ is the period of the phase grating. It can be seen from Fig. 5 that when the first-order diffraction angle is between 20 and 65 degrees, the period Λ of the phase grating is approximately 205 nm to 1900 nm, or the period 相位 of the phase grating is approximately 555.5 nm to 1900. Nano.

According to the foregoing constraints, the peak-to-valley phase delay of the phase grating is less than or equal to 2.9, and the peak-to-valley thickness difference of the phase grating can be expressed as ,As shown in Figure 6.

Where λ is the wavelength of the incident light, n1 is the refractive index of the environment of the diffraction grating layer 122 (for example, the refractive index of air is 1), n2 is the refractive index of the diffraction grating layer 122, and Λ is the period of the phase grating. As can be seen from Fig. 6, the peak-to-valley thickness difference d of the phase grating is, for example, less than 1800 nm. In practical applications, the backlight is not only forward light, but also includes oblique light of 5 to 10 degrees. Since the light of the incident phase grating is not only positive light, other oblique light with a smaller incident angle can also be deflected to With a large viewing angle, it is therefore possible to design an efficiency ratio of the 0th order diffraction to the 1st order diffraction ratio of about 1:0.05. Referring to FIG. 4, it can be found that when m is 0.9, the efficiency of the 0th order diffraction and the 1st order winding are substantially satisfied. The efficiency ratio of the shot is about 1:0.05, that is, the peak-to-valley phase delay of the phase grating can be greater than or equal to 0.9. For example, if the angle of the grayscale inversion phenomenon is expected to be 20 degrees, it means that the 1st order diffraction of the phase grating should be set to 20 degrees, the peak of the grating is arranged in the horizontal direction, and the efficiency of the 0th order diffraction is 1 The efficiency ratio of the order diffraction is about 1:0.05, the period Λ of the phase grating should be between 555.5 nm and 1900 nm, and the peak-to-valley phase delay m of the phase grating is 0.9. If the refractive index n2 of the diffraction grating layer 122 is 1.5, the peak-to-valley thickness difference d of the phase grating should be between 108.9 nm and 223.5 nm.

7 and FIG. 8 are respectively a relationship between luminance and gray scale values before and after the application of the diffraction grating layer in the liquid crystal panel module. Referring to FIG. 7, when the diffraction grating layer is not disposed in the liquid crystal panel module, the gray angle inversion phenomenon occurs at a lower viewing angle of about 40 degrees. However, it can be seen from FIG. 8 that if the liquid crystal panel module is provided with a diffraction grating layer, there is almost no gray scale inversion phenomenon. The grating of the diffraction grating layer of FIGS. 7 and 8 has a period of about 1000 nm, and the thickness of the diffraction grating layer at the peak of the grating and the thickness of the diffraction grating layer at the valley of the grating are about 200 to 1000. Nano.

FIG. 9 is a partially enlarged view of a diffraction grating layer of a liquid crystal panel module according to another embodiment of the present invention. Referring to FIG. 9 , since the gray scale inversion problem of the conventional liquid crystal panel module is mainly serious in the lower viewing angle, the grating of the diffraction grating layer of the embodiment is a blazed grating, and the light is mainly deflected in a specific direction after passing through the blazed grating. Fold, rather than symmetrical toward both sides as a phase grating. Therefore, the blazed grating can be used to deflect the light mainly downward toward the lower viewing angle, so that the forward energy does not lose too much and the problem of the grayscale inversion of the lower viewing angle can be solved. The qth order diffraction efficiency of the blazed grating can be expressed as , as shown in Figure 10.

Where λ is the wavelength of the incident light, n1 is the refractive index of the environment of the blazed grating (for example, the refractive index of air is 1), n2 is the refractive index of the blazed grating, and d is the peak-to-valley thickness difference of the blazed grating. It can be seen from Fig. 10 that the incident light has a wavelength of 380 nm to 780 nm, and the radiance grating has a refractive index of 1.2, and the peak-to-valley thickness difference d of the blazed grating is, for example, less than 1950 nm; The peak-to-valley thickness difference d of the blazed grating is, for example, less than 390 nm. If the efficiency ratio of the 0th order diffraction of the blazed grating to the first order diffraction is about 1:0.05, and the refractive index of the blazed grating is 1.2 to 2, the peak-to-valley thickness difference of the blazed grating is 70 nm. To 713 nm.

In addition, the diffraction angle of the blazed grating is set to be between 20 and 65 degrees. When the light is a forward incident blazed grating, the period of the blazed grating can be expressed as , as shown in Figure 11.

Where λ is the wavelength of the incident light, n2 is the refractive index of the blazed grating, q is the diffraction order (ie 1), and θq is the first-order diffraction angle of the blazed grating. As can be seen from FIG. 11, when the first-order diffraction angle is between 20 degrees and 65 degrees, the period 炫 of the blazed grating is approximately between 209 nm and 1900 nm. The slanting angle of the blazed grating of Fig. 9 is θ = tan ^-1 (d / Λ). Of course, the invention can also design a second order or higher or a high order diffraction angle of 20 to 65 degrees.

In addition, to further reduce the cost of the process, the blazed grating can use a binary approximation to blaze the grating, as shown in Figure 12.

FIG. 13 is a schematic diagram of a liquid crystal panel module according to still another embodiment of the present invention. Referring to FIG. 13 , the liquid crystal panel module 102 of the present embodiment is similar to the liquid crystal panel module 100 of FIG. 1 , but a distance D is maintained between the diffraction grating layer 102 and the liquid crystal panel 110 . When the distance D between the diffraction grating layer 102 and the liquid crystal panel 110 is maintained, the obliquely outgoing image and the forward-derived image that has been deflected by the grating may interfere with each other due to misalignment. Therefore, a positive user can see a clear image, but a beveled bystander can see an interference image in which a plurality of images are misaligned, thereby achieving a function of preventing others from peeking. Here, the 0th order and the 1st order diffraction of the diffraction grating layer 102 are simply considered, and the divergence angle of the image is assumed to be φ, and the 1st order diffraction angle of the diffraction grating layer 102 is θ1. It can be seen from FIG. 13 that when viewed at the viewing angle φ, another image will be seen at the extension of the light due to the relationship between the positive viewing angle and the side viewing angle light passing through the first order diffraction of the diffraction grating layer 102. The distance between images is x, and the relationship between D and angle of view φ can be expressed as Assuming that the distance x between the real image and the virtual image is between 0.1 mm and 100 mm, the distance D between the diffraction grating layer 102 and the liquid crystal panel 110 is between 0.5 mm and 100 mm.

If the first-order diffraction angle θ1 is 30 degrees, and it is desirable that the distance x between the virtual image and the real image is 3 mm when the viewing angle φ is 20 degrees, D is about 25 mm.

On the other hand, if the light first passes through the diffraction grating layer 122 and then enters the liquid crystal panel 110, the diffractive grating layer 122 can be designed to deflect the obliquely incident light. The liquid crystal panel 110 is incident in the forward direction to improve light utilization efficiency.

FIG. 14 is a schematic diagram of a backlight module according to an embodiment of the invention. Referring to FIG. 14, the backlight module 200 of the present embodiment includes a light guide plate 210, a light emitting element 220, and a diffraction grating film 230. The grating of the diffraction grating film 230 may be a blazed grating or a phase grating or the like. The light guide plate 210 has an adjacent light emitting surface 212 and at least one light incident surface 214. The light-emitting element 220 is disposed beside the light-incident surface 214, and the light-emitting element 220 may be a cold cathode fluorescent tube, a light-emitting diode, or other light-emitting element. The diffraction grating film 230 is disposed on the light exit surface 212. Since the light provided by the light-emitting element 220 enters the light guide plate 210 from the light-incident surface 214 located on the same side of the light guide plate 210, most of the light emitted from the light-emitting surface 212 is not forwardly emitted, but is as shown in FIG. The light exits in a direction away from the light emitting element 220. However, the light that has passed through the diffraction grating film 230 is deflected toward the light-emitting element 220, that is, as far as possible in a direction that is positive with respect to the light-emitting surface 212. Alternatively, the diffraction grating film 230 may be disposed on the other surface of the light guide plate 210 with respect to the light-emitting surface 212. After the light is emitted from the light-emitting element 220, the light is incident on the reflective diffraction grating film 230, and is reflected and then incident on the liquid crystal in a collimated direction. Panel 110. Thereby, the brightness of the forward light provided by the backlight module 200 can be improved, and the use amount of the expensive light-increasing sheet can be reduced to reduce the cost of the backlight module 200. At the same time, the diffraction grating film 230 has the advantage of a smaller optical package than the conventional enamel-type addition film, that is, the brightness distribution is more uniform. In order to reduce process cost, the grating of the diffraction grating film 230 may employ a binary approximation blazed grating.

The period 光栅 of the grating of the diffraction grating film 230 of the present embodiment is between 380 nm and 2281 nm, and the peak-to-valley thickness difference of the grating of the diffraction grating film 230 is d. For example, between 280 nm and 4910 nm.

FIG. 15 is a schematic diagram of a backlight module according to another embodiment of the present invention. Referring to FIG. 15 , the backlight module 300 of the present embodiment includes a light guide plate 310 , a light emitting element 320 , and a diffraction grating film 330 . The grating of the diffraction grating film 330 may be a blazed grating, a binary approximate blazed grating, or Phase grating and so on. The light guide plate 310 has at least one light incident surface 314. The light-emitting element 320 is disposed beside the light-incident surface 314, and the diffraction grating film 230 is disposed between the light-emitting element 320 and the light-incident surface 314. By the action of the diffraction grating film 230, the light provided by the light-emitting element 320 can be incident on the light guide plate 310 at a large divergence angle to improve the problem that the divergence angle is too small, which may cause uneven brightness of the light source near the light-incident surface 314.

The light-emitting element 320 of the present embodiment includes a circuit board 322 and a plurality of light-emitting diodes 324 arranged on the circuit board 322. The light provided by each of the light-emitting diodes 324 is deflected in a direction away from each of the light-emitting diodes after passing through the diffraction grating film 330. Specifically, with the main optical axis N10 of each of the light-emitting diodes 324 as the center, the grating of the region R10 of the diffraction grating film 330 on the right side of the main optical axis N10 is such that the light provided by the light-emitting diode 324 is shifted to the right. The grating of the region R20 of the diffraction grating film 330 on the left side of the main optical axis N10 is such that the light provided by the light-emitting diode 324 is deflected to the left. In other words, the gratings of the regions R10 and R20 of the diffraction grating film 330 on both sides of the main optical axis N10 are symmetrical with each other with the main optical axis N10 as the center of symmetry. In addition, the diffraction grating film 330 may not need to be provided with a grating in a region where the light provided by the LED 324 does not pass, thereby further saving cost.

FIG. 16 is a schematic diagram of a backlight module according to still another embodiment of the present invention. Please refer to The backlight module 400 of the present embodiment is similar to the backlight module 300 of FIG. 15 . The difference is that the backlight module 400 of the embodiment adopts a reflective diffraction grating film 430, and the light-emitting element 420 is a cold cathode. The fluorescent tube is exemplified but not limited thereto. The light guide plate 410 has at least one light incident surface 412, a light exit surface 414 and a bottom surface 416, wherein the light exit surface 414 is opposite to the bottom surface 416. The light emitting element 420 is disposed beside the light incident surface 412. The reflective diffraction grating film 430 is disposed beside the bottom surface 416. The reflective diffraction grating film 430 can abut or be at a distance from the bottom surface 416. At least part of the light provided by the light-emitting element 420 passes through the light-incident surface 412 and the bottom surface 416 in sequence, and is reflected by the reflective diffraction grating film 430 and then emitted through the bottom surface 416 to be emitted from the light-emitting surface 414. The reflective diffraction grating film 430 can replace the reflective sheet in the conventional backlight module, and can also replace the dots or other microstructures for diffusing light at the bottom of the conventional light guide plate. Therefore, the use of the reflective diffraction grating film 430 helps to reduce the overall cost of the backlight module 400. In addition, a reflective material layer 432 may be disposed on the surface of the reflective diffraction grating film 430 behind the light guide plate 410 to further increase the reflectivity.

Figure 17 is an exploded view of a liquid crystal display device in accordance with an embodiment of the present invention. Referring to FIG. 17, the liquid crystal display device 50 of the present embodiment includes a liquid crystal panel module 52 and a backlight module 54. The liquid crystal panel module 52 is disposed on the backlight module 54. When the liquid crystal panel module 52 adopts the liquid crystal panel module of the embodiment of FIG. 1 or FIG. 9 and the diffraction grating layer is located on the side of the liquid crystal panel module 52 away from the backlight module 54, the liquid crystal display device 50 has a large viewing angle. The problem of color shift, grayscale inversion, and low brightness can be improved. When the liquid crystal panel module 52 adopts the liquid crystal panel module of the embodiment of FIG. 1 or FIG. 9 , and the diffraction grating layer is located near the backlight module 54 of the liquid crystal panel module 52 . On one side, the display image of the liquid crystal display device 50 will have a large brightness and contrast. When the liquid crystal panel module 52 adopts the liquid crystal panel module of the embodiment of FIG. 13 and the diffraction grating layer is located on the side of the liquid crystal panel module 52 away from the backlight module 54, the liquid crystal display device 50 has the function of preventing others from peeking. . When the backlight module 54 adopts the backlight module of the embodiment of FIG. 14, the display image of the liquid crystal display device 50 has a large brightness and contrast. Of course, when the liquid crystal panel module of the foregoing embodiments is used in the liquid crystal panel module 52, the backlight module 54 can also use the backlight module of the foregoing embodiment. In addition, the liquid crystal display device 50 can further have a front frame 56 for allowing the liquid crystal panel module 52 to be more stably disposed on the backlight module 54.

In summary, the liquid crystal panel module of the present invention utilizes a diffraction grating layer to generate multi-order diffracted light to solve the problem of large-view character bias and gray-scale inversion, and can also provide a backlight module by using a diffraction grating layer. The large angle incident light is being turned to improve light utilization. In addition, the backlight module of the present invention also uses a diffraction grating film to straighten the obliquely outgoing light to improve light utilization efficiency. The liquid crystal display device of the present invention can simultaneously or separately adopt the liquid crystal panel module and the backlight module, which not only has the aforementioned advantages, but also has the advantages of low cost and more environmental protection.

Although the present invention has been disclosed in the above embodiments, it is not intended to limit the invention, and any one of ordinary skill in the art can make some modifications and refinements without departing from the spirit and scope of the invention. The scope of the invention is defined by the scope of the appended claims.

100‧‧‧LCD panel module

110‧‧‧LCD panel

112‧‧‧ pixels

120A‧‧‧first polarizer

122‧‧‧Diffraction grating layer

124‧‧‧Protective film

126‧‧‧Polarization layer

130‧‧‧Second polarizer

P10‧‧‧ pixel size

Claims (7)

A liquid crystal panel module comprising: a liquid crystal panel having a plurality of pixels; and a diffraction grating layer disposed on the liquid crystal panel, the maximum period of the grating of the diffraction grating layer being substantially smaller than the pixels One tenth of the size, wherein the grating of the diffraction grating layer is a phase grating having a peak-to-valley phase delay of 2.9 or less, and the phase-to-valley phase delay of the phase grating is greater than or equal to 0.9. The liquid crystal panel module of claim 1, wherein the phase grating has a diffraction angle of between 20 degrees and 65 degrees. The liquid crystal panel module of claim 2, wherein the phase grating has a period of from 205 nm to 1900 nm. The liquid crystal panel module of claim 1, wherein the phase grating has a peak-to-valley thickness difference of less than 1800 nm. The liquid crystal panel module of claim 1, wherein the grating of the diffraction grating layer is a blazed grating. The liquid crystal panel module of claim 1, further comprising a first polarizing plate and a second polarizing plate, wherein the liquid crystal panel is disposed between the first polarizing plate and the second polarizing plate, the first A polarizing plate includes a first protective film, a polarizing layer and the diffraction grating layer, and the polarizing layer is disposed between the first protective film and the diffraction grating layer. The liquid crystal panel module of claim 1, wherein the period of the grating of the diffraction grating layer is not constant.