1. Field of the Invention
The present invention relates to measuring the sub-pixel current of an emissive display such as an OLED (Organic Light-Emitting Diode) display.
2. Description of the Related Arts
An OLED display is generally comprised of an array of organic light emitting diodes (OLEDs) that have carbon-based films disposed between two charged electrodes. Generally one electrode is comprised of a transparent conductor, for example, indium tin oxide (ITO). Generally, the organic material films are comprised of a hole-injection layer, a hole-transport layer, an emissive layer and an electron-transport layer. When voltage is applied to the OLED, the injected positive and negative charges recombine in the emissive layer and transduce electrical energy to light energy. Unlike liquid crystal displays (LCDs) that require backlighting, OLED displays are self-emissive devices—they emit light rather than modulate transmitted or reflected light. Accordingly, OLEDs are brighter, thinner, faster and lighter than LCDs, and use less power, offer higher contrast and are cheaper to manufacture.
An OLED display typically includes a plurality of OLEDs arranged in a matrix form including a plurality of rows and a plurality of columns, with the intersection of each row and each column forming a pixel of the OLED display. An OLED display is generally activated by way of a current driving method that relies on either a passive-matrix (PM) or an active-matrix (AM) scheme.
In a passive matrix OLED display, a matrix of electrically-conducting rows and columns forms a two-dimensional array of picture elements called pixels. Sandwiched between the orthogonal column and row lines are thin films of organic material of the OLEDs that are activated to emit light when current is applied to the designated row and column lines. The brightness of each pixel is proportional to the amount of current applied to the OLED of the pixel. While PM OLEDs are fairly simple structures to design and fabricate, they demand relatively expensive, current-sourced drive electronics to operate effectively and are limited to the number of lines because only one line can be on at a time and therefore the PM OLED must have overall brightness equal to the desired average brightness times the number of lines. Thus, PM OLED displays are typically limited to under 100 lines. In addition, their power consumption is significantly higher than that required by an active-matrix OLED. PM OLED displays are most practical in alpha-numeric displays rather than higher resolution graphic displays.
An active-matrix OLED (AM OLED) display is comprised of OLED pixels that have been deposited or integrated onto a thin film transistor (TFT) array to form a matrix of pixels that emit light upon electrical activation. In contrast to a PM OLED display, where electricity is distributed row by row, the active-matrix TFT backplane acts as an array of switches coupled with sample and hold circuitry that control and hold the amount of current flowing through each individual OLED pixel during the total frame time. The active matrix TFT array continuously controls the current that flows to the OLEDs in the each of pixels, signaling to each OLED how brightly to illuminate.
As shown in
The continuous current flow to the OLEDs is controlled by the two TFTs T1, T2 of each sub-pixel. TFT T1 is used to start and stop the charging of storage capacitor Cs, and TFT T2 provides a voltage source at the level needed to create a constant current to the OLED D1. As a result, the AM OLED operates at all times (i.e., for the entire frame scan), avoiding the need for very high currents required for passive matrix operation. The TFT T1 samples the data on the data line (Data), which is held as charge stored in the storage capacitor Cs. The voltage held on the storage capacitor Cs is applied to the gate of the second TFT T2. In response, TFT T2 drives current through the OLED D1 to a specific brightness depending on the value of the sampled and held data signal as stored in the storage capacitor Cs.
The OLED display requires regulated current in each sub-pixel to produce a desired brightness from the pixel. Ideally, the TFTs T2 in each sub-pixel 100 should be good current sources that deliver the same current for the same gate voltage over the lifetime of the OLED display. Also each current source TFT T2 in the active TFT matrix must deliver the same current for the same data voltage stored in the storage capacitor Cs in order that the display is uniform. However, uniform TFTs are very difficult to produce and thus the current supplied by TFTs T2 in conventional OLED displays is often non-uniform, resulting in non-uniform display brightness. In order to correct such non-uniformities in the drive current through the OLEDs in the OLED display, it is necessary to measure the actual current through each OLED of the sub-pixels in the OLED display.
However, accurately measuring the actual current through each OLED of the subpixels of the OLED panel is not simple, due to the large number of pixels in an OLED display panel. A conventional way of measuring the current in one sub-pixel is to measure the current flowing in either the VDD line or the VSS line of the sub-pixel. The current in the VDD or VSS line is first measured with all pixels turned off to establish a background (leakage) current (also called the dark current). Then one sub-pixel is turned on, which would result in an increase in the current in the VDD and VSS line by the turned-on sub-pixel (OLED). Typically the current increase resulting from the turned-on sub-pixel is between a few nanoamperes and one microampere.
The background current, however, is comprised of the leakage current through all the TFTs T2 and Cs capacitors in the OLED display, because all the sub-pixels are tied to the supply voltages VDD and VSS through the column power lines in a conventional OLED display. For example, a VGA resolution (NTSC-monochromatic) display has 640×480 pixels (m=640, n=480). In the case of a full color display, each pixel is made up of three sub-pixels, red (R), green (G), and blue (B). Therefore, the total number of columns in a VGA full color display is 640×3=1920 columns (m=1920). Thus, the total number of sub-pixels in a full color VGA display is 1920×480=921,600 sub-pixels, or almost a million sub-pixels. Typically, the leakage in a single TFT T2 can be 10 picoamperes. Therefore, the total background (leakage) current of a VGA full color OLED display can be approximately 10 microamperes (1 million sub-pixels×10 pA). Since the background current (10 microamperes) is very large compared to the current increase resulting from a single turned-on sub-pixel (between a few nanoamperes and one microampere), it is extremely difficult to measure the sub-pixel current accurately.
Embodiments of the present invention include an active matrix drive system for driving an emissive display device and configured to measure sub-pixel current in the emissive display device, where one or more power column power lines of the emissive display device are disconnected from the supply voltage while sub-pixel current is measured. As a result, the sub-pixel current is relatively large compared to the background current of the emissive display device, which facilitates accurate measurement of the sub-pixel current.
In one embodiment, the active matrix drive system comprises an active matrix drive circuit configured to drive current through a plurality of emissive display elements arranged in a matrix of a plurality of rows and a plurality of columns where each of the emissive display elements corresponds to a subpixel of the emissive display device and is configured to have its current flow through a corresponding one of a plurality of column power lines, a plurality of first switches each coupled to a corresponding one or more of the column power lines where the corresponding one or more of the column power lines receives supply voltage and the current flows through the corresponding one or more of the column power lines if the corresponding first switch is turned on, but the corresponding one or more of the column power lines does not receive supply voltage and the current does not flow through the corresponding one or more of the column power lines if the corresponding first switch is turned off, and a current measurement device coupled to a common cathode of the emissive display elements where the current measurement device is configured to measure combined current from emissive display elements.
The features and advantages described in the specification are not all inclusive and, in particular, many additional features and advantages will be apparent to one of ordinary skill in the art in view of the drawings, specification, and claims. Moreover, it should be noted that the language used in the specification has been principally selected for readability and instructional purposes, and may not have been selected to delineate or circumscribe the inventive subject matter.
The teachings of the embodiments of the present invention can be readily understood by considering the following detailed description in conjunction with the accompanying drawings.
The Figures (FIG.) and the following description relate to preferred embodiments of the present invention by way of illustration only. It should be noted that from the following discussion, alternative embodiments of the structures and methods disclosed herein will be readily recognized as viable alternatives that may be employed without departing from the principles of the claimed invention.
Reference will now be made in detail to several embodiments of the present invention(s), examples of which are illustrated in the accompanying figures. It is noted that wherever practicable similar or like reference numbers may be used in the figures and may indicate similar or like functionality. The figures depict embodiments of the present invention for purposes of illustration only. One skilled in the art will readily recognize from the following description that alternative embodiments of the structures and methods illustrated herein may be employed without departing from the principles of the invention described herein.
Referring to
The common cathode 204 is connected to two switches Ua, Ub. Switch Ua connects the common cathode 204 to the current measurement circuit 202. Switch Ub is connected between the common cathode 204 and the negative supply voltage Vss.
As shown in
The continuous current flow to the OLEDs D1 is controlled by the two TFTs T1, T2 of each sub-pixel. TFT T1 is used to start and hold the charging of storage capacitor Cs, and TFT T2 provides a voltage source at the level needed to create a constant current to the OLED D1. More specifically, the TFT T1 samples the data on the data line (Data), which is held as charge stored in storage capacitor Cs. The voltage held on storage capacitor Cs is applied to the gate of the TFT T2. In response, TFT T2 drives current through the OLED D1 to a specific brightness depending on the value of the current, which is controlled by the sampled and held data signal as stored in storage capacitor Cs.
As explained above, a switch (U1, U2, . . . , or Um) is inserted at the head of each column connecting or disconnecting the column power line (221, 222, . . . , or 22m) to or from the supply voltage VDD. Control signal 232 controls the turning on and off of the switches (U1, U2, . . . , or Um). For example, the control signal 232 may be an m-bit signal with each bit corresponding to one of the column power lines (221, 222, . . . , 22m) and controlling the turning on and off of the corresponding one of the switches (U1, U2, . . . , or Um). When a switch (U1, U2, . . . , or Um) is turned on, the corresponding column power line (221, 222, . . . , or 22m) is connected to the supply voltage VDD. When a switch (U1, U2, . . . , or Um) is turned off, the corresponding column power line (221, 222, . . . , or 22m) becomes disconnected from the supply voltage VDD.
A current measurement device 202 is connected between the common cathode CC 204 and the negative supply voltage Vss through switch Ua. In addition, switch Ub is connected between the common cathode 204 and the negative supply voltage Vss directly, bypassing the current measurement device 202. Control signal 234 controls the turning on and off of switches Ua and Ub. Switches Ua and Ub are turned on and off in an alternating manner by the control signal 234. Specifically, when switch Ua is turned on, switch Ub is turned off and the common cathode 204 becomes connected to the current measurement device 202. As a result, the combined current from OLEDs D1 of all the sub-pixels can be measured by the current measurement device 202. On the other hand, when switch Ua is turned off, switch Ub is turned on, and the common cathode (CC) 204 is connected to the negative power supply Vss directly, bypassing the current measurement device 202. As a result, the OLED display operates in normal operation mode with no current measurement function involved.
Switches U1, U2, . . . , Um, Ua, and Ub may be formed as poly-silicon MOSFETs (Metal Oxide Semiconductor Field Effect Transistors), alpha-silicon MOSFETs, TFTs, single crystalline silicon MOSFETs, or any other semiconductor MOSFETs. Because the switches U1, U2, . . . , Um, Ua, and Ub handle a large amount of current combined from all the sub-pixels connected to one column or multiple columns, the size of the switches U1, U2, . . . , Um, Ua, and Ub is much larger than the size of the TFTs T1, T2 in each sub-pixel. In one embodiment, switches U1, U2, . . . , Um, Ua, and Ub may be formed together with the other TFTs T1, T2 of the active matrix in an integrated circuit. In another embodiment, switches U1, U2, . . . , Um, Ua, and Ub may be formed as discrete components separate from the TFTs T1, T2 of the active matrix for the OLED display.
As a result, current through the OLEDs D1 in one or more of the sub-pixels 200 of column C1 may be measured by the current measurement device 202. For example, if row R1 is turned on as well, current through the OLED D1 in the sub-pixel 200 corresponding to row R1, column C1 can be measured by the current measurement device 202. If more than one row is turned on, then the combined current through the OLEDs D1 in one or more of the turned-on sub-pixels of column C1 may be measured by the current measurement device 202. Theoretically, according to the embodiment shown in
However, some small leakage current in the open switches U2 through Um may be expected. For example, switches U1 through Um could be polysilicon thin film transistors deposited at the same time as the rest of the active matrix is deposited. Polysilicon TFTs are leaky and each polysilicon TFT could leak as much as 10 picoamperes. Therefore, the background current could be as much as 1920×10 picoamperes=19.2 nanoamperes. Such background current is a substantial improvement to the background current in a conventional VGA OLED display such as that shown in
Specifically, the current measurement device 202 in the embodiment of
Similar to the embodiment shown in
As the process is started 400, all sub-pixels of the OLED display are turned off 402. Then, one column is turned on 404, for example, column C1 is turned on by turning on switch U1 and turning off other switches U2 through Um with the control signal 232. In this manner, only column power line 221 is connected to the supply voltage VDD and the remaining column power lines 222 through 22m are disconnected from the supply voltage VDD. Then, the background current I1 is measured 406 using the current measurement device 202, with the remaining column power lines 222 through 22m disconnected from the supply voltage VDD. As explained above, switch Ua is turned on and switch Ub is turned off to active the current measurement device 202 in order to measure the background current of the OLED display. As explained above, the background current is very small compared to that of conventional OLED displays, because the other columns C2 through Cm (column power lines 222 through 22m0 are turned off.
Next, one of the sub-pixels is turned on 408. For example, the sub-pixel at row R1, column C1 is turned on by turning on switch U1 and asserting appropriate data to the Data lines connected to TFTs T1, T2. Specifically, in order to turn on a sub-pixel (for example, subpixel at R1, C1), the corresponding column power line 221 is turned on by closing the corresponding switch U1, data is loaded on the data line (Data), and the row line (also referred to as gate line 250) which is connected to all the gates of TFTs T1s in a row is turned on. In normal operation, the data for a row is loaded to a line buffer (not shown), and when the row line 250 is activated all the TFTs T1 in the row are turned on to allow the data voltage in the line buffer transfer to all the storage capacitors Cs in the row through the data line (Data). Using the current measurement device 202, the current I2 through that turned-on sub-pixel is measured 410. Again, switch Ua is turned on and switch Ub is turned off to activate the current measurement device 202 in order to measure the sub-pixel current. The remaining column power lines 222 through 22m are disconnected from the positive supply voltage VDD by the turned-off switches U2 through Um while the sub-pixel current is measured. Then, the difference (I2−I1) between the measured sub-pixel current I2 and the background current I1 is determined 412. Such difference (I=I2−I1) is the measure of the actual sub-pixel current without the background current and can be stored in a storage device (not shown).
Then, it is determined 414 whether the measured sub-pixel is the last sub-pixel in the turned-on column. If the measured sub-pixel is not the last sub-pixel in the turned-on column, the process moves 416 to the next sub-pixel (for example, R2/C1, R3/C1, and so on) to repeat steps 408, 410, 412, 414. Alternatively, the process may go back from step 416 to step 406 to re-measure 406 the background current and repeat steps 406, 408, 410, 412, 414 for the next sub-pixel. If the measured sub-pixel is the last sub-pixel in the turned-on column, then it is determined 418 whether the turned-on column is the last column in the OLED display. If the turned-on column is not the last column in step 418, then all the sub-pixels in the OLED display are again turned off 420 and the process moves 422 to the next column (for example, C2, C3, . . . , and so on) to repeat steps 404, 406, 408, 410, 412, 414, 416, 418. If the turned-on column is the last column in step 418, then the current in all sub-pixels have been measured and the process ends 424. Note that the order in which the sub-pixels are measured as illustrated herein is merely exemplary and that the sub-pixel current may be measured in other sequences.
In one embodiment, the present invention may be used to measure sub-pixel current from the TFTs T2 while they are biased to operate in saturation mode. Such sub-pixel current measurements with TFTs T2 in saturation can be used to compensate for the difference in sub-pixel current from sub-pixel to sub-pixel through compensation techniques (not explained herein) and to force uniformity of the sub-pixel current for the active matrix in OLED displays where the active matrix itself is not able to provide uniform sub-pixel current in a stand-alone manufacturing process.
In another embodiment, the present invention can be used to measure the sub-pixel current when the TFTs T2 are biased to operate in their linear region. Such sub-pixel current measurements with TFTs T2 operating in their linear region can be used to correct non-uniform pixel brightness that occurs as the pixels of the OLED display age. Therefore, stuck images (ghosting, burned in images, etc.) and color drift due to uneven aging of the three colors (RGB) in the OLED display may be corrected.
Upon reading this disclosure, those of skill in the art will appreciate still additional alternative structural and functional designs for measuring sub-pixel current in emissive displays such as OLED displays. Thus, while particular embodiments and applications of the present invention have been illustrated and described, it is to be understood that the invention is not limited to the precise construction and components disclosed herein and that various modifications, changes and variations which will be apparent to those skilled in the art may be made in the arrangement, operation and details of the method and apparatus of the present invention disclosed herein without departing from the spirit and scope of the invention as defined in the appended claims.
This application claims priority under 35 U.S.C. § 119(e) from co-pending U.S. Provisional Patent Application No. 60/925,990 entitled “Sub-pixel Current Measurement” filed on Apr. 24, 2007, which is incorporated by reference herein in its entirety.
Number | Date | Country | |
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60925990 | Apr 2007 | US |