1. Field of the Invention
The present invention relates to the pixel circuits and drive method of an active matrix display comprising light-emitting devices that emits light by conducting a driving current through a light emitting material such as an organic semiconductor thin film. Such pixel circuits comprise active elements, such as thin film transistors, for controlling the light emitting operation of the respective light emitting devices. More specifically, the present invention provides pixel circuits comprising an active conducting channel between a data input electrode and a scan electrode, and a method to operate such pixel circuits. Furthermore, pixel circuits in the present invention are structured with alternating conducting channels, controlled by a multi-functional control electrode. Pixel circuits capable of performing current-controlled drive scheme, with reduced complexity than existing solutions, are provided as preferred application of the present invention.
2. Description of the Prior Art
Organic light emitting diode displays (OLED) have attracted significant interests in commercial application in recent years. Its excellent form factor, fast response time, lighter weight, low operating voltage, and prints-like image quality make it the ideal display devices for a wide range of application from cell phone screen to large screen TV. Passive OLED displays, with relatively low resolution, have already been integrated into commercial cell phone products. Next generation devices with higher resolution and higher performance using active matrix OLEDs are being developed. Initial introduction of active matrix OLED displays have been seen in such products as digital camera and small portable video devices. Demonstration of OLED displays in large size screens further propels the development of a commercially viable active matrix OLED technology. The major challenges in achieving such a commercialization include (1) improving the material and device operating life, and (2) reducing device variation across the display area. Several methods have been suggested to address the second issue by including more active switching devices in individual pixels, by switching of power supply lines externally, or by reading back the pixel parameters combined with an external memory and tuning circuit. As more elaborated control circuits being incorporated into individual pixels as proposed in these solutions, concerns over complexity and practical manufacturing issues arise.
The operation of an OLED display differs from a liquid crystal display (LCD) in that each and every pixel in an OLED display comprises a light emitting element. The light output of such light emitting elements is more conveniently controlled by the current directed to the pixel. In contrast, an LCD is readily operable by voltage signals as its optical response being more favorably expressed in a simple form of applied voltage. While typical storage devices hold information in the form of voltage, operating an active matrix OLED display via a typical storage element requires a conversion mechanism within a pixel to convert a stored voltage data into specific current output. In practice, a conversion method needs to be reliable and fairly independent of such factors as pixel-to-pixel variation in the characteristics that affect said conversion, to make an OLED display operable with fair uniformity.
Basic examples of using organic material to form an LED are found in U.S. Pat. No. 5,482,896, U.S. Pat. No. 5,408,109 and U.S. Pat. No. 5,663,573, and examples of using organic light emitting diode to form active matrix display devices are found in U.S. Pat. No. 5,684,365 and U.S. Pat. No. 6,157,356, all of which are hereby incorporated by reference.
An active matrix OLED display (
As illustrated in the above example, the electrical current for producing light output is directed to the light emitting element via a current path that comprises at least a control element that regulates the current. In a conventional light emitting device display, these control elements are fabricated on a thin film of amorphous silicon on glass. Power consumed in such control elements are converted to heat rather than yielding any light. To reduce such power consumption, polycrystalline silicon is preferred over amorphous silicon for its better mobility. More elaborated methods employing self-regulated multiple-stage conversions suitable for pixel circuit using polysilicon base material may be found in U.S. Pat. No. 6,501,466 and U.S. Pat. No. 6,580,408. These methods provide a current drive scheme while largely eliminated the impact from material and transistor non-uniformity typically associated with thin film polysilicon on glass base plate. In these methods, typically a minimum of four transistors are required to achieve such self-regulated, multi-stage conversion to achieve a pixel-independent current drive for the light emitting device display. An example of such methods is illustrated in
The circuit in
These examples of prior art provide a brief overview of the existing solutions considered in the art to resolve the uniformity issue. Comparing to the basic pixel circuit in
The present invention provides a multi-functional scan electrode for pixel access that carries the conventional pixel select function and providing a conversion function for converting a data current to a data voltage. The present invention further provides multiple conducting channels in a pixel, for setting the data voltage and delivering drive current. The pixel structure so constructed comprises a direct current path from a data electrode to a scan electrode, and may further comprise a direct current path from a scan-power electrode to the light emitting element. The turning-on and off of such channels are fully controlled by the voltage applied on a scan-power electrode.
In a conventional pixel driving circuit, a scanning electrode carries a scanning function of turning on and off control switches in a pixel to enable or disengage data input from data electrodes. Such scanning electrodes do not participate in setting actual value of data information to a storage element in the pixel, and do not communicate with data electrode directly. The present invention provides a pixel circuit for an active matrix light emitting device display comprising a multi-functional scan electrode. The present invention further provides a method for driving an active matrix light emitting device display wherein a scanning electrode directly communicate with data electrodes during a scanning operation, and provides reference voltage to set actual data value in the pixel.
The present invention provides pixel circuits and a drive method to operate said pixel circuits, where a pixel comprises a conducting channel between a data electrode and a scanning electrode; the enabling and inhibiting of such conducting channel are fully operated by the control signal voltages applied to the scan electrode. Furthermore, a pixel circuit comprising two alternating conducting channels, one between a data electrode and a scan electrode, and the other between a scan electrode and said reference voltage source via said light emitting element, are provided as an extension in the present invention.
As a preferred embodiment of the present invention, the conducting channel between a data electrode and a scan electrode is structured to convert a data current directed thereto to a data voltage to be stored at a storage element. Such stored data voltage controls a drive current to the light emitting element in a pixel. The conducting channel between a scan electrode and a reference voltage source provides a means to supply drive current via a scan electrode (in this case, named herein as a scan-power electrode) to the light emitting element, making a pixel circuit more compact and allowing additional control functions to be incorporated in a single control electrode.
Preferred embodiments of the present invention are provided for the operation of a display in current drive scheme to eliminate dependency on threshold voltage variation and OLED characteristics. The present invention also utilizes a drive method that merges conventional power delivering electrode and scanning electrode into a single access electrode (scan-power electrode). Preferred embodiments in three-transistor implementation are provided to illustrate the application to the solutions for current drive scheme within the present invention. Additional embodiments are provided as illustration of a broader implementation principle.
Additional features and advantages of the present invention will be set forth in the description which follows, 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 drawings.
The present invention and claimed subjects disclosed herein are directed to the operation of active matrix light emitting device display.
The present invention provides active matrix pixel circuits and a method to drive such. The circuit comprises a conducting channel between a data electrode and a scan electrode, controlled by the signal applied to scan electrode. Furthermore, the present invention provides two conducting channels in a pixel, enabled alternately by the signals applied to the same scan control electrode, where the second conducting channel provides current to drive a light emitting element in a pixel. A conventional scan electrode thus operates to perform both a scanning function and a power delivery function, and referred to as scan-power electrode in such embodiments. Preferred embodiments of the present invention are provided for the current drive scheme to eliminate dependency on threshold voltage variation and OLED characteristics. Preferred embodiments in three transistor implementation are provided to illustrate the solutions for current drive scheme within the present invention. Additional embodiments are provided as illustration of a broader implementation principle.
Preferred embodiments of the present invention are herein described using organic light emitting diodes as illustration. Examples of using organic material to form an LED are found in U.S. Pat. No. 5,482,896 and U.S. Pat. No. 5,408,109, and examples of using organic light emitting diode to form active matrix display devices are found in U.S. Pat. No. 5,684,365 and U.S. Pat. No. 6,157,356, all of which are hereby incorporated by reference.
As evidenced in the prior art, the conventional method of constructing and operating a light emitting device display involves a scanning electrode (or referred to as SELECT electrode, GATE electrode, or other names carrying similar meaning) and a power supply electrode (VDD). The scanning electrode interacts with a pixel through high impedance gates of switching elements in the pixel and does not participate in delivering drive current to the light emitting device.
The present invention provides pixel circuits and operating method that a current is directed to a conducting channel between a data electrode and a scan electrode. Such conducting channel is controlled according to a signal voltage applied to the scan electrode and may be arranged to provide a conversion function to convert a input current into a voltage, and set an internal storage element to said voltage.
The present invention further combines with a scan-power electrode that operates to deliver drive power via a scan electrode. The same electrode that selects a pixel for data writing delivers a full amount of drive current in a subsequent operating period. A pixel so constructed utilizes a scan-power electrode that delivers drive current while inhibiting data transfer between said data electrode and said pixel in one period, and enables data writing from data electrode into said pixel according a scanning signal in another period.
A pixel so constructed comprises a conducting channel between a data electrode and a scan electrode (now referred to as DS). A combined circuit further comprises a second conducting channel (now referred to as SP) between a scan-power electrode and the voltage source that supplies the drive power to the light emitting device in a the pixel. The enabling and inhibiting of conducting channel SP are fully controlled by voltage signals applied to the scan-power electrode.
The channel DS is also referred to as the first conducting channel, and channel SP is referred to as the second conducting channel.
A scan-power electrode represents an access electrode that is structured to perform both a scanning operation where a scanning signal is delivered to enable data input in selected pixels in one period of the operation, and a drive operation where a drive current is delivered to a light emitting device in another period of operation. A scan electrode represents an access electrode that performs a scanning (or select) operation. A scanning (or data writing) cycle is a period that a pixel is selected to allow data to be transferred from a data electrode to the selected pixel. The transferred data information is stored in a storage element in the pixel thereafter until the next scanning period.
In the description of this invention, a direct current path is a current path not interrupted by or ended on a capacitor; it may comprise such elements as resistor, drain-to-source and emitter-to-collector channel of a transistor, anode-to-cathode of a diode, and conductive lines that allow a current to continue. A direct current path in this description implies that it is enabled and conducts intended current in at least one of the operation periods for operating a display device. A charging current ended on or via a capacitor does not constitute a direct current path. Transient currents arising from charging of input gate or parasitic capacitors are not considered as providing valid current path. The reverse leakage of a diode, the leakage current in a transistor in its off-state, and current via the high impedance input terminals (such as a base or a gate) are also not considered as valid current paths. Accordingly, a direct current path in this description is a current path that allows the conduction of an intended current for the purpose of operating a display pixel, and allows such current to continue for as long as the set conditions persist.
An active element comprises a high-impedance control terminal and a channel between a second terminal and a third terminal. In operation, said high-impedance control terminal receives a control signal and regulates the current directed along said channel according to the control signal. A preferred embodiment of an active element is an MOS transistor having a gate as the control terminal, and a channel between the other two terminals arranged as source and drain. Similarly, bipolar transistors and JFETs are alternatives as preferred embodiments. The results for all these active elements are similar, and may be exemplified by the operation of MOS devices.
An organic light emitting diode (OLED) is used in most preferred embodiments wherever appropriate; the presence of such a device in such embodiments should not be construed as setting forth a limitation on the present invention directed for light emitting devices in general. MOS devices are used in preferred embodiments for switching elements. Similar bipolar transistors will perform similar functions as MOS devices. Those skilled in the art can quickly derive variations by a substitution of an arbitrary light emitting device for the organic light emitting diode, or by different types and polarities of switching devices. Preferred operating condition and preferred input data format do not necessitate limitations on the operation of the present invention.
Preferred embodiments of the present invention will hereinafter be described in detail with reference to the drawings.
A preferred embodiment of a circuit element is provided in
In a preferred implementation, 602 may be assigned an n-channel transistor, and 603 a p-channel transistor. Terminal A operates as the source and B as the drain of n-channel transistor 602 when VSC is positive with respect to D; terminal A operates as the drain and B as the sourced when VSC is negative relative to D. By setting VSC substantially more negative (typically a few volts) than D, p-channel transistor 603 is turned on. A positive voltage on B-terminal makes B-terminal a source and A-terminal a drain of transistor 602. Furthermore, VGS=VDS as provided by the circuit connection, transistor 602 is turned on and set in its saturation region. Furthermore, the value of VDS is uniquely determined by the current directed from VSC to D since transistor 602 operates in its saturation point (VGS=VDS) as a two terminal device.
When VSC is set higher (more positive) than D, p-channel 603 is turned off. Transistor 603 is also set to its off state since A-terminal is settled at a divided voltage between 602 and 603, and is negative compared to B terminal. Such a configuration provides a gate-to-source short in 602. A proper operating condition for circuit 600 requires a scanning voltage VSC being switched between a VHI and a VLO, where the voltage difference between high and low exceeds a combined dynamic range covering both the dynamic voltage range of data signal and the voltage range of VREF. The reference voltage VREF for capacitor may be a dynamically varying voltage level in pixel operation.
The embodiment described in
A conducting channel between a data electrode and a scan electrode;
Said conducting channel being controlled by setting a voltage high or a voltage low on the scan electrode VSC;
A conversion from current input to a voltage output according to a saturation condition of a transistor;
A specific prescription in this transfer characteristics is that the output voltage is determined by an input current unambiguously according to the above mentioned conditions.
Additional preferred embodiments of a conducting channel between a data electrode and a scan electrode are provided in
A preferred implementation of
With reference to the circuit of
1. Data signal and desired output. When a current is direct to an OLED, its light output may be closely represented as linear to the drive current. In order to maintain a uniform control of light output that is not disturbed by variation from pixel to pixel, it is convenient to devise a pixel circuit that provides a transfer function converting input signal from a data electrode linearly into output current on OLED. Such a transfer function needs to be independent of variation of major parameters in a pixel circuit such as threshold voltage of control transistors and forward operating voltage of OLED. A drive method by formatting the data information into respective current value externally and delivering such current to the respective pixels has shown more promise than driving in voltage form. Here the description of operation will be developed along a current drive principle, using a current source IW delivered on a data electrode to produce a current output ID on an OLED. A preferred circuit and its operation are expected to produce an output current in a drive cycle that is linear to input current in the scanning cycle.
2. Scan and data writing cycle. A voltage low VLO (scanning voltage) for selecting pixels for data input is applied to a scan-power electrode 810, turning on p-channel transistor 803 and allowing data current IW to enter the pixel, where VLO is equal to VREF, and is set to be the lowest potential in a display system. As input data current Iw is directed toward the gate of n-channel 802 and capacitor 804, a non-zero current causes a continued accumulation of positive charge (and voltage) on capacitor 804 and on the gate of transistor 802, thereby turning on 802 to allow a current diversion through 802 for the circuit to approach a steady state. Since B-terminal of 802 is set to VLO that is the lowest voltage level of the system, A and B terminals operate as drain and source of 802, respectively, as discussed above regarding
VGS2=VDS2 (1)
where VGS2 is the gate-to-source voltage of transistor 802, and VDS2 is the drain-to-source voltage on 802.
According to the characteristics of MOS transistors, the condition given in Eq. (1) ensures that 802 is at the onset of saturation, and the current (ID) through 802 is control by the gate voltage according to a formula:
ID2C2(VGS2−VTH2)2 (2)
where VTH2 is the threshold voltage of 802, and C1 is a constant determined by the width, length, and intrinsic parameters such as the mobility of silicon, the thickness and dielectric constant of the gate oxide of transistor 802. Approaching the end of a scan cycle, the current branched into the capacitor 804 diminishes to zero, and the entire data current IW is channeled through transistor 802, thereby giving
ID2=IW (3)
It should be noted that the voltage VC on capacitor 804 is the same as VGS2 (i.e. VGS2=VC) since the line voltage on 810 is at the same level as VREF in a scanning cycle.
3. Drive cycle. After data is written into a pixel and the capacitor 804 charged to a voltage VC=VGS2 that sets transistor 802 in saturation region, electrode 810 is raised to a voltage high (VHI) (drive voltage) sufficient to provide a full forward bias on LED 805, and to keep transistor 801 in its saturation region. A preferred voltage high (VHI) is typically equal to, or higher than the sum of the maximum LED forward operating voltage and the maximum voltage on a data electrode output. For a small-molecule OLED operating in 7.5 volt range, a typical NMOS TFT for drive transistor, and a dynamic data range of 3 volts, a preferred voltage high is in the range of 11-13 volts above VREF. Such a condition for VHI ensures that the voltage drop VDS1 from drain to source of transistor 801, in a drive cycle, is higher than the stored voltage VC in the capacitor 804 written in a scan cycle, thereby pinning transistor 801 into its saturation region. As electrode 810 being set high, p-channel transistor 803 is turned off. Transistor 802 has its drain and source reversed from the scanning cycle as described above in the discussion related to
ID1=C1 (VGS1−VTH1)2 (4)
where ID1 is the current through 801, C1 is a constant determined by the width, length, and intrinsic parameters such as the mobility of silicon, the thickness and dielectric constant of the gate oxide of transistor 801, and VGS1 is the gate-to-source voltage of transistor 801 in a drive cycle, noting that VGS1=VC=VGS2.
Given the close proximity between 801 and 802, all the intrinsic parameters and the thickness of oxide are expected to be fairly the same for both. That gives VTH1=VTH2, and the C's only be different through dimensional parameters of length (L) and width (W) by design. It is straightforward for those skilled in the art to conclude that the current ID1 so delivered in a drive cycle is proportional to the input current IW:
ID1/IW=C1/C2=W1L2/W2L1 (5)
or
ID1∞IW
where W1 and W2 are the width and L1 and L2 are the length of transistor 801 and 802, respectively.
The drive method and pixel circuit provided herein thus provide a three-transistor solution to current control drive for light emitting device displays, therein eliminated the impact by the variation in characteristics of its circuit elements. The ratios of dimensional parameters in Eq. (5) are constant by design, and remain constant to the first order of process variation, thereby providing a transfer function that is not impacted by spatial fluctuation in processing. It should be noted that the linearity between the input and output is a preferred transfer characteristics, but not a necessary condition for this invention to operate. It should also be noted that the ratio C1/C2 is not necessarily the same for all current levels. A slightly higher C1/C2 at lower current IW than at higher IW is typical. This is due to the boundary condition of a constant total voltage across the light emitting element 805 and transistor 801, resulting in an increase in drain-to-source voltage VDS1 on drive transistor 801 from VDS2 on 802 when setting VC. Such a deviation is more at lower IW than at higher IW, and thus pushing 801 deeper into saturation from the onset point at lower current IW. For transistors exhibit incomplete saturation, this causes an increase in C1, and a deviation of the ratio C1/C2. To the first order of operation, this deviation may be neglected; for more accurate image reproduction, this deviation may be compensated in input IW, or with additional offset elements.
As described hereinabove, the preferred embodiment in
It should be noted that various electrical elements may be further inserted or divided in such a current path to further modify the operation. These further modifications shall be construed as not violating the provision of a current path between a scan-power electrode and a data electrode to incorporate a drive function into the same scan-power electrode, as described in the present invention.
The preferred embodiment of
The preferred embodiment of
During the period when a drive voltage (VHI) is applied to the scan-power electrode, all paths leading to the storage element 804 are inhibited, isolating the capacitor (and the gate of transistor 801) from any other influence.
An active matrix display may be constructed from the pixel unit provided in this embodiment by forming such pixels at intersects between a plurality of data electrodes and a plurality of scan-power electrodes. As an example for a complete display unit, a current driver unit with matching number of output terminals is attached to the edge of such matrix display where each data electrode is connected to an output terminal of the data driver unit to provide data current signal. A scan-power driver is attached to another edge of such display matrix where each scan-power electrode is connected to an output terminal of the scan-power driver unit to receive scanning pulses and driver current.
In a preferred implementation of the embodiment of
In a non-select period when the data writing is directed to pixels controlled by other scanning electrodes, a logic high equal to VDD is applied to this scan-power electrode 910, turning off transistor 902 and 903. As discussed above, a preferred condition is to set VDD 11-13 volts, and set VLO equal to or a fractional volt below VREF, where VLO is set to be the lowest voltage in the system. A numerical example of such operating voltages and data range are similarly to that provided in the above example of
In a scanning period, the n-channel transistor 902 is thus biased in a configuration with A node being the drain and B node being the source, and operates in its saturation region since the VGS=VDS. In a non-select period, the data electrode is isolated from the pixel as transistor 903 is in its off-state. The scanning electrode is also isolated from this pixel as B node is more positive than A node, setting transistor in a configuration where gate of 902 is short to its source, or VGS=0. Following the same operation analysis as above for
The preferred embodiment of
Said conducting channel in this embodiment comprises circuit elements so arranged that an input data current ID, directed from said data electrode to said scan electrode, is converted into a data voltage by said conducting channel. Furthermore, such converted voltage is generated at the gate of a transistor 902, and sets the voltage of the storage element 904.
Furthermore, the A node of transistor 902 operates as a drain when the voltage of scan electrode 910 is set to VLO, lower than the voltage on the data electrode.
During the period when a de-select voltage (VHI) is applied to the scan-power electrode, all paths leading to the storage element 804 are inhibited, isolating the capacitor (and the gate of transistor 801) from any external influence.
The operation of pixel circuits in
A further extension of the present invention provides a configuration using a different voltage reference for storage capacitor.
The present invention is described herein with specific combinations of transistors and polarity of OLED in each embodiment. Examples of the preferred embodiments illustrate a drive scheme and principles to implement pixel circuit using a basic circuit element of
Furthermore, inserting resistors or capacitors at various nodes in the circuit provided hereinbefore to pre-condition a signal, modify its transient property, or provide fine adjustment of voltage drop, as commonly practiced in the art, while leaving the basic circuit operation the same as discussed in this disclosure falls well within the scope of the present invention.
Although various embodiments utilizing the principles of the present invention have been shown and described in detail herein, those skilled in the art can readily devise many other variances, modifications, and extensions that still incorporate the principles disclosed in the present invention. The scope of the present invention embraces all such variances, and shall not be construed as limited by the number of active elements, wiring options of such, or the polarity of a light emitting device therein.
The present application claims the benefit of U.S. Provisional Patent Application No. 60/522,239, filed on Sep. 3, 2004, which is hereby incorporated by reference.
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Number | Date | Country | |
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20060050040 A1 | Mar 2006 | US |
Number | Date | Country | |
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60522239 | Sep 2004 | US |