Liquid-crystal antenna device

Abstract

A liquid-crystal antenna device includes a signal source, a driving module, a correction module, and a plurality of radiation units. The signal source provides an input electromagnetic wave. The driving module outputs a plurality of initial voltage signals according to a radiation address. The correction module receives the initial voltage signals and outputs a plurality of corrected voltage signals according to a lookup table. The radiation units respectively receive the corrected voltage signals and are coupled to the input electromagnetic wave to generate an output electromagnetic wave.

Claims

1. A liquid-crystal antenna device, comprising: a signal source, providing an input electromagnetic wave; a driving module, outputting a plurality of initial voltage signals according to a radiation address; a correction module, receiving the plurality of initial voltage signals and outputting a plurality of corrected voltage signals according to a lookup table; and a plurality of radiation units, receiving the plurality of corrected voltage signals and coupling with the input electromagnetic wave to generate an output electromagnetic wave.

2. The liquid-crystal antenna device as claimed in claim 1, wherein the lookup table includes an initial voltage-capacitance curve, and a plurality of corrected voltage-capacitance curves respectively corresponding to the plurality of radiation units, and wherein the correction module determines a plurality of initial capacitance values that respectively correspond to the plurality of initial voltage signals according to the initial voltage-capacitance curve, and then determines the plurality of corrected voltage signals that respectively correspond to the plurality of initial capacitance values according to the plurality of corrected voltage-capacitance curves.

3. The liquid-crystal antenna device as claimed in claim 1, wherein each of the radiation units comprises a common electrode, a pixel electrode, and a liquid-crystal layer disposed between the common electrode and the pixel electrode.

4. The liquid-crystal antenna device as claimed in claim 3, wherein each of the radiation units further comprises a thin film transistor electrically connected to the pixel electrode.

5. The liquid-crystal antenna device as claimed in claim 3, wherein the common electrode comprises a slit.

6. The liquid-crystal antenna device as claimed in claim 5, wherein the pixel electrode overlaps the slit.

7. The liquid-crystal antenna device as claimed in claim 3, wherein the pixel electrode receives one of the plurality of corrected voltage signals.

8. The liquid-crystal antenna device as claimed in claim 1, further comprising a waveguide transmitting the input electromagnetic wave from the signal source to the plurality of radiation units.

9. The liquid-crystal antenna device as claimed in claim 1, wherein at least one of the plurality of initial voltage signals is different from at least one of the plurality of corrected voltage signals.

10. A liquid-crystal antenna device, comprising: a plurality of radiation units, emitting or receiving an electromagnetic wave, wherein the radiation units include a first radiation unit; a driving module, outputting a plurality of initial voltage signals according to a radiation address, wherein the plurality of initial voltage signals include a first voltage signal corresponding to the first radiation unit; and a correction module, receiving the plurality of initial voltage signals and outputting a plurality of corrected voltage signals to the plurality of radiation units, wherein the plurality of corrected voltage signals include a second voltage signal corresponding to the first radiation unit; wherein the first voltage signal is different from the second voltage signal, wherein the correction module determines an initial capacitance value that corresponds to the first voltage signal according to an initial voltage-capacitance curve, and then determines the second voltage signal that corresponds to the initial capacitance value according to a corrected voltage-capacitance curve.

11. The liquid-crystal antenna device as claimed in claim 10, wherein each of the radiation units comprises a common electrode, a pixel electrode, and a liquid-crystal layer disposed between the common electrode and the pixel electrode.

12. The liquid-crystal antenna device as claimed in claim 11, wherein each of the radiation units further comprises a thin film transistor electrically connected to the pixel electrode.

13. The liquid-crystal antenna device as claimed in claim 11, wherein the common electrode comprises a slit.

14. The liquid-crystal antenna device as claimed in claim 13, wherein the pixel electrode overlaps the slit.

15. The liquid-crystal antenna device as claimed in claim 11, wherein the pixel electrode receives one of the plurality of corrected voltage signals.

16. The liquid-crystal antenna device as claimed in claim 10, further comprising a signal source providing the electromagnetic wave.

17. The liquid-crystal antenna device as claimed in claim 16, further comprising a waveguide transmitting the electromagnetic wave from the signal source to the plurality of radiation units.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) FIG. 1 is a diagrammatic view of a liquid-crystal antenna device of an embodiment of the present disclosure.

(2) FIG. 2 is a schematic perspective view of the liquid-crystal antenna device of FIG. 1.

(3) FIG. 3 is a top view of the radiation unit in FIG. 2.

(4) FIG. 4 is a cross-sectional view along line B-B in FIG. 3.

(5) FIG. 5A is a graph illustrating a relationship between voltage and capacitance of the radiation unit in FIG. 1 in the ideal state.

(6) FIG. 5B is a graph illustrating a relationship between voltage and capacitance of the radiation unit in FIG. 1 in the practical state.

(7) FIG. 6A is an equivalent circuit diagram of an integrator for measuring a capacitance of a radiation unit of an embodiment of the present disclosure.

(8) FIG. 6B is an equivalent circuit diagram of FIG. 6A after connecting to a test capacitance.

(9) FIGS. 7A-7C are equivalent circuit diagrams of the radiation unit of FIG. 1 at different voltages.

DETAILED DESCRIPTION

(10) The following disclosure provides many different embodiments, or examples, for implementing different features of the subject matter provided. Specific examples of components and arrangements are described below to simplify the present disclosure. These are merely examples and are not intended to be limiting. For example, the formation of a first feature over or on a second feature in the description that follows may include embodiments in which the first and second features are formed in direct contact, and may also include embodiments in which additional features may be formed between the first and second features, such that the first and second features may not be in direct contact.

(11) In addition, the present disclosure may repeat reference numerals and/or letters in the various examples. This repetition is for the purpose of simplicity and clarity and does not in itself dictate a relationship between the various embodiments and/or configurations discussed.

(12) The terms such as the first and the second in the present disclosure are merely for clarity and are not intended to correspond to or limit the scope of the patent. In addition, the terms such as the first feature and the second feature are not limited to the same or different features.

(13) Spatially relative terms, such as below or above, and the like, are merely used herein for ease of description to describe one element or feature's relationship to another element(s) or feature(s) as illustrated in the figures. The spatially relative terms are intended to encompass different orientations of the device in use or operation in addition to the orientation depicted in the figures. For clarity, the description of the first feature disposed on the second feature or the lower means that the first feature is on or under the second feature in the stacking direction of the figures in the present disclosure.

(14) The shape, size, and thickness in the drawings may not be drawn to scale or simplified for clarity of discussion; rather, these drawings are merely intended for illustration.

(15) FIG. 1 is a diagrammatic view of a liquid-crystal antenna device 1 of an embodiment of the present disclosure. A liquid-crystal antenna device 1 can be used to emit an electromagnetic wave signal, which includes a memory unit 10, a signal source 20, and a plurality of radiation units RU1, RU2 . . . RUn. The memory unit 10 includes a driving module 11 and a correction module 12, wherein the driving module 11 according to a radiation address outputs a plurality of initial voltage signals S1, S2 . . . Sn, the correction module 12 receives the initial voltage signals S1, S2 . . . Sn and then outputs a plurality of corrected voltage signals S1, S2 Sn, and the radiation units RU1, RU2 . . . RUn receive the corrected voltage signals S1, S2 . . . Sn and are coupled to an input electromagnetic wave provided by the signal source 20 to generate an output electromagnetic wave W, and emit the output electromagnetic wave W to the radiation address. In the embodiment, the correction module 12 outputs the corrected voltage signals S1, S2 . . . Sn according to a lookup table 121, but are not limited thereto. In the embodiment, the radiation address is defined by the zenith angle and the azimuth angle of a Spherical coordinate system. And, at least one of the plurality of initial voltage signals is different from at least one of the plurality of corrected voltage signals.

(16) The liquid-crystal antenna device 1 mentioned above outputs a plurality of the corrected voltage signals S1, S2 . . . Sn to the radiation units RU1, RU2 . . . RUn through the correction module 12 in order to adjust the liquid-crystal capacitance value of the radiation units RU1, RU2 . . . RUn to control the resonance frequency of the liquid-crystal antenna device 1. When the resonance frequency of the liquid-crystal antenna device 1 matches the frequency of the input electromagnetic wave provided by the signal source 20, the liquid-crystal antenna device 1 will emit the electromagnetic wave W to the radiation address.

(17) FIG. 2 is a schematic perspective view of the liquid-crystal antenna device 1 of FIG. 1. The liquid-crystal antenna device 1 includes a plurality of arrayed radiation units RU (including the aforementioned radiation units RU1, RU2, . . . , RUn) and a waveguide WG, wherein the arrangement of a plurality of arrayed radiation units RU may vary by design, and are not intended to be limited. After correction by the aforementioned correction mechanism, the phase difference and the amplitude of the electromagnetic wave emitting into space may be controlled by each radiation unit RU so as to stack and form the electromagnetic wave W. The waveguide WG transmits the electromagnetic wave from the signal source 20 to the radiation units RU.

(18) Referring to FIG. 3 and FIG. 4, FIG. 3 is a top view showing one of the radiation units in FIG. 2, and FIG. 4 is a cross-sectional view along line B-B in FIG. 3. The radiation unit RU includes a common electrode 31, a pixel electrode 32, and a thing film transistor TFT. The common electrode 31 and the pixel electrode 32 are disposed respectively on a first substrate SUB1 and a second substrate SUB2, and the thin film transistor TFT electrically connects to the common electrode 31 and the pixel electrode 32 respectively, wherein the thin film transistor TFT may be used to transmit the aforementioned corrected voltage signals to the pixel electrode 32. In another embodiment, the thin film transistor TFT electrically connects to the pixel electrode 32, and a common voltage source electrically connects to the common electrode 31. The common electrode 31 and the pixel electrode 32 may be a metal thin layer, which may be made of or include copper, silver, gold, aluminum, any suitable materials or a combination alloy thereof. The common electrode 31 and the pixel electrode 32 may also be a transparent conductive thin layer, which may be made of or include indium tin oxide (ITO), indium zinc oxide (IZO), indium gallium zinc aluminum oxide (IGZAO), any suitable transparent conductor or a combination thereof. The common electrode 31 and the pixel electrode 32 may be any suitable conductor and are not limited thereto, wherein the common electrode 31 is formed with a slit 311, so that the electromagnetic wave transmitting in the waveguide (not shown) under the common electrode 31 may be radiated to the liquid-crystal layer LC between the common electrode 31 and the pixel electrode 32. In some embodiments, the pixel electrode 32 overlaps the slit 311.

(19) The first substrate SUB1 and the second substrate SUB2 may be made of or include quartz, glass, wafer, metal foil, polymethylmethacrylate (PMMA), polyimide (PI), polyethylene terephthalate (PET), polyethylene naphthalate (PEN), and polybutylene naphthalate (PBN), but are not limited thereto, and any material applicable for the first substrate SUB1 and the second substrate SUB2 may be used. Liquid-crystal layer LC may include a plurality of liquid-crystal molecules.

(20) Still referring to FIG. 3 and FIG. 4, assuming that every radiation unit RU has the same size, the liquid-crystal capacitance of every radiation unit RU can be regarded as an ideal capacitance. The Equation 1 below can be simplified as a function of voltage when the size of the ideal capacitance is fixed, which means that all of the radiation units RU can have a consistent liquid-crystal capacitance C.sub.LC via an initial voltage-capacitance curve C.sub.initial (as shown in FIG. 5) when inputting a specific voltage value:

(21) $\begin{array}{cc}{C}_{\mathrm{LC}}={\mathrm{.Math.}}_{\mathrm{LC}}\left(V\right)\frac{A}{d}& \left(\mathrm{Equation}1\right)\end{array}$

(22) Here, .sub.LC(V) is a relation of the liquid-crystal dielectric coefficient to the applied voltage difference, A is the sum of overlapping areas of the common electrode 31 and the pixel electrode 32 in FIG. 3, d is the distance between the common electrode 31 and the pixel electrode 32 in FIG. 4.

(23) However, the actual size of each radiation unit RU may have slight difference due to the process capability of precision is limited. Therefore, every radiation unit RU will each have their own corrected voltage-capacitance curve C1, C2 . . . Cn (as shown in FIG. 5B). The corrected voltage-capacitance curves C1, C2 . . . Cn of the radiation unit RU in the practical situation can be obtained by substituting A (the sum of overlapping areas of the common electrode 31 and the pixel electrode 32) and d (the distance between the common electrode 31 and the pixel electrode 32) into the aforementioned equation.

(24) The corrected voltage-capacitance curves C1, C2 . . . Cn may not only be obtained by the aforementioned equation but also be acquired by directly measuring and calculating the liquid-crystal capacitance C.sub.LC of the radiation unit RU in the practical situation. Referring to FIG. 6A, which is an equivalent circuit diagram of an integrator for measuring a capacitance of a radiation unit in an embodiment of the present disclosure. First, the accumulated standard electric quantity Q.sub.standard of the standard capacitance C.sub.standard with known capacitance value under the standard applied voltage V.sub.standard can be calculated through the integrator according to the following equation 2.
Q.sub.standardC.sub.standardV.sub.standard(Equation 2)

(25) Next, referring to FIG. 6B, a fully charged test capacitance (capacitance to be tested) C.sub.test (for example, a capacitance formed by the radiation unit RU) may connect with the integrator of FIG. 6A, wherein the reduction of the discharge electric quantity Q.sub.discharge results from the discharge of the standard capacitance C.sub.standard as shown in the following equation 3:
Q.sub.discharge=C.sub.standardV.sub.out(Equation 3)

(26) Here, output voltage V.sub.out is a function of time t as shown in the following equation 4:

(27) $\begin{array}{cc}{V}_{\mathrm{out}}\left(t\right)=-\frac{1}{{\mathrm{RC}}_{\mathrm{standard}}}{}_{t_{\mathrm{start}}}^{t_{\mathrm{end}}}{V}_{\mathrm{in}}\left(t\right)\mathrm{dt}+V_{\mathrm{standard}}& \left(\mathrm{Equation}4\right)\end{array}$

(28) In Equation 4, R is the resistance value of the resistor R connected with the aforementioned integrator, V.sub.in(t) is a function of the input voltage V.sub.in to the time t, t.sub.start and t.sub.end are the start time and the end time of the input voltage.

(29) Subsequently, as shown in Equation 5, the electric quantity Q.sub.test of the test capacitance C.sub.test is obtained by subtracting discharge electric quantity Q.sub.discharge from the standard electric quantity Q.sub.standard:
Q.sub.test=Q.sub.standardQ.sub.standard(Equation 5)

(30) Since the voltage difference V.sub.test of the fully charged test capacitance C.sub.test is known, test capacitance C.sub.test is obtained by the following equation 6:

(31) $\begin{array}{cc}{C}_{\mathrm{test}}=\frac{Q_{\mathrm{test}}}{V_{\mathrm{test}}}& \left(\mathrm{Equation}6\right)\end{array}$

(32) However, as the capacitance formed by the radiation unit RU includes the liquid-crystal capacitance C.sub.LC and the storage capacitance C.sub.st (which includes parasitic capacitance as well) of the radiation unit RU, a special circuit design is needed to determine the liquid-crystal capacitance C.sub.LC of the radiation unit RU. FIGS. 7A-7C, which represent equivalent circuit diagrams of the radiation unit of FIG. 1 at different voltages. As shown in FIG. 7A, the equivalent circuit of the radiation unit RU includes the source terminal which receives the source voltage V.sub.S, wherein the liquid-crystal capacitance C.sub.LC and the storage capacitance C.sub.st connect to a common voltage terminal V.sub.com_CLC and V.sub.com_CLC respectively.

(33) First, as shown in FIG. 7B, a voltage V.sub.com_CLC+Cst may be applied to the common voltage terminals Vcom.sub._CLC and V.sub.com_Cst of the liquid-crystal capacitance C.sub.LC and the storage capacitance C.sub.st, and the voltage Vcom.sub._CLC+Cst is not equal to the source voltage V.sub.S, so as to measure and calculate the parallel equivalent capacitance value of the liquid-crystal capacitance C.sub.LC and the storage capacitance C.sub.st.

(34) Referring to FIG. 7C, a voltage equal to the source voltage V.sub.S may be applied to the common voltage terminal V.sub.com_CLC of the liquid-crystal capacitance C.sub.LC, and the other voltage V.sub.com may be applied to the common voltage terminal V.sub.com_Cst of the storage capacitance C.sub.st, wherein the voltage V.sub.com is not equal to the source voltage V.sub.S, so as to measure and calculate the capacitance value of the storage capacitance C.sub.st. Next, the liquid-crystal capacitance C.sub.LC of the radiation unit RU can be obtained by subtracting the single capacitance value of the storage capacitance Cst from the parallel equivalent capacitance value of the liquid-crystal capacitance C.sub.LC and the storage capacitance C.sub.st.

(35) As a result, the corrected voltage-capacitance curve C1, C2 . . . Cn of each radiation unit RU can be obtained by the two aforementioned methods, and the initial voltage-capacitance curve C.sub.initial (FIG. 5A) and the corrected voltage-capacitance C1, C2 . . . Cn (FIG. 5B) will be stored in the correction module 12 in order to correct the initial voltage signal S1, S2 . . . Sn. Taking the first radiation unit RU1 as an example, after the correction module 12 receives the initial voltage signal S1 corresponding to the first radiation unit RU1, the correction module 12 can determine an initial capacitance value C.sub.0 corresponding to the initial voltage signal S1 (V.sub.0 in FIG. 5A) according to an initial voltage-capacitance curve, subsequently determine a corrected voltage signal S1 (V.sub.1 in FIG. 5A) corresponding to the initial capacitance value C.sub.0 according to the corrected voltage-capacitance curve C1 of the first radiation unit RU1, and then output the corrected voltage signal S1 to the aforementioned first radiation unit RU1. The initial voltage signal S1 corresponding to the first radiation unit RU1 is different from the corrected voltage signal S1 due to the correction. In some embodiments, initial voltage-capacitance curve C.sub.initial and the corrected voltage-capacitance curves C1, C2 . . . Cn may be stored in the lookup table 121 of the correction module 12, but are not limited thereto.

(36) The present disclosure provides two methods for obtaining the corrected voltage-capacitance curves C1, C2 . . . Cn, but those are merely examples and are not intended to be limited.

(37) In summary, the present disclosure utilizes the correction module 12 to correct the voltage signal outputting to the radiation unit RU, which can improve the output electromagnetic wave distortion caused by the non-uniformity of the liquid-crystal layer or the difference of the electrode areas due to the limitation of the process capability of precision, so as to achieve the desired output electromagnetic radiation patterns.

(38) The disclosed features may be combined, modified, or replaced in any suitable manner in one or more disclosed embodiments, but are not limited to any particular embodiments.

(39) While the disclosure has been described by way of example and in terms of preferred embodiment, it is to be understood that the disclosure is not limited thereto. On the contrary, it is intended to cover various modifications and similar arrangements (as would be apparent to those skilled in the art). Therefore, the scope of the appended claims should be accorded the broadest interpretation so as to encompass all such modifications and similar arrangements.