Patent Grant
7911418
This Application is a U.S. National Phase Application of PCT International Application PCT/JP2007/071683.
The present invention relates to a driving method of a plasma display panel used in a wall-hanging television (TV) or a large monitor, and a plasma display device.
A typical AC surface discharge type panel used as a plasma display panel (hereinafter referred to as “panel”) has many discharge cells between a front plate and a back plate that are faced to each other.
The front plate has the following elements:
The front plate and back plate are faced to each other so that the display electrode pairs and the data electrodes three-dimensionally intersect, and are sealed. Discharge gas containing xenon at a partial pressure of 5%, for example, is filled into a discharge space. Discharge cells are disposed in intersecting parts of the display electrode pairs and the data electrodes. In the panel having this structure, ultraviolet rays are emitted by gas discharge in each discharge cell. The ultraviolet rays excite respective phosphors of red, green, and blue to emit light, and thus provide color display.
A subfield method is generally used as a method of driving the panel. In this method, one field period is divided into a plurality of subfields, and the subfields at which light is emitted are combined, thereby performing gradation display.
Each subfield has an initializing period, an address period, and a sustain period. In the initializing period, initializing discharge is performed to form a wall charge required for a subsequent addressing operation on each electrode. The initializing operation includes an initializing operation (hereinafter referred to as “all-cell initializing operation”) of causing initializing discharge in all discharge cells, and an initializing operation (hereinafter referred to as “selective initializing operation”) of selectively causing initializing discharge in a discharge cell having performed sustain discharge in the sustain period of the last subfield.
In the address period, address discharge is selectively performed to form a wall charge in a discharge cell where display is to be performed. In the sustain period, sustain pulses are alternately applied to the display electrode pairs formed of the scan electrodes and the sustain electrodes, sustain discharge is caused in the discharge cell having performed address discharge, and a phosphor layer of the corresponding discharge cell is light-emitted, thereby displaying an image.
Of the subfield method, a panel driving method is proposed. In this driving method, the contrast can be kept sharp by reducing the background luminance, and the dynamic false contour can be reduced by suppressing the variation in brightness of picture. This method is disclosed in patent document 1, for example.
Of the subfield method, a new driving method is disclosed. In this driving method, the initializing discharge is performed using a gently varying ramp waveform voltage, and the initializing discharge is selectively applied to the discharge cell having performed sustain discharge. Thus, light emission that is not related to the gradation display is minimized, and the contrast ratio is improved.
Specifically, in the initializing period of one of a plurality of subfields, the all-cell initializing operation of causing discharge from all discharge cells is performed. In the initializing period of another subfield, the selective initializing operation of initializing only the discharge cell having performed sustain discharge in the sustain period of the last subfield is performed. As a result, light emission that is not related to the display is only the light emission accompanying the discharge of the all-cell initializing operation, and an image having high contrast can be displayed. This driving method is disclosed in patent document 2, for example.
In a panel where the partial pressure of xenon is increased to improve the light emitting efficiency, the initializing discharge becomes unstable, and a address failure can occur in the subsequent address period. A driving method of the panel where high-quality image is displayed by stabilizing the initializing discharge is proposed. The driving method is disclosed in patent document 3, for example.
Recently, while the improvement of image display quality has been demanded, factors destabilizing the discharge have been increased by enlargement of the panel, refining of the discharge cell, or increase in the xenon partial pressure. If the above-mentioned all-cell initializing operation becomes unstable dependently on the display image and a malfunction (hereinafter referred to as “false lighting”) for causing sustain discharge in the discharge cell that has not caused address discharge occurs, the image display quality can be reduced significantly.
[Patent document 1] Japanese Patent Unexamined Publication No. 2001-255847
[Patent document 2] Japanese Patent Unexamined Publication No. 2000-242224
[Patent document 3] Japanese Patent Unexamined Publication No. 2005-326612
The driving method of a plasma display panel of the present invention is a driving method of a plasma display panel having a plurality of discharge cells including a display electrode pair that is formed of a scan electrode and a sustain electrode. The driving method having the following steps:
A plasma display device of the present invention has the following elements:
A driving method of a panel and a plasma display device in accordance with an exemplary embodiment of the present invention will be described hereinafter with reference to the accompanying drawings.
Front substrate 21 and back substrate 31 are faced to each other so that display electrode pairs 24 cross data electrodes 32 with a fine discharge space sandwiched between them, and the outer peripheries of them are sealed by a sealing material such as glass frit. The discharge space is filled with discharge gas containing xenon at a partial pressure ratio of 10%. The discharge space is partitioned into a plurality of sections by barrier ribs 34. Discharge cells are formed in the intersecting parts of display electrode pairs 24 and data electrodes 32. The discharge cells discharge and emit light to display an image.
The structure of panel 10 is not limited to the above-mentioned one, but may be a structure having striped barrier ribs, for example.
Next, a driving voltage waveform and its operation for driving panel 10 are described. Panel 10 performs gradation display by a subfield method. In this method, one field period is divided into a plurality of subfields, and emission and non-emission of light of each display cell are controlled every subfield. Each subfield has an initializing period, an address period, and a sustain period. In the present embodiment, an abnormal charge erasing period is disposed as necessary between the initializing period and the address period
In the initializing period, initializing discharge is performed to form a wall charge required for a subsequent address discharge on each electrode. The initializing operation at this time includes an all-cell initializing operation and a selective initializing operation. In the abnormal charge erasing period, if the initializing operation in the previous all-cell initializing period becomes unstable and abnormal charge is accumulated in any discharge cell, the abnormal charge in the discharge cell is erased. In the address period, address discharge is selectively caused in a discharge cell to emit light, thereby forming a wall charge. In the sustain period, as many sustain pulses as the number proportional to luminance weight are alternately applied to display electrode pairs 24, sustain discharge is caused in the discharge cell having caused address discharge, thereby lighting up or emitting light. The subfield having the initializing period when the all-cell initializing operation is performed is called an all-cell initializing subfield, and the subfield having the initializing period when the selective initializing operation is performed is called a selective initializing subfield.
The detail of the subfield structure will be described later, and the detail and operation of the driving voltage waveform of a subfield are described.
The driving voltage waveform of the subfield that is an all-cell initializing subfield and has no abnormal charge erasing period is described with reference to
In the first half of the all-cell initializing period, 0 (V) is applied to data electrodes D1 through Dm and sustain electrodes SU1 through SUn, and a ramp waveform voltage is applied to scan electrodes SC1 through SCn. Here, the ramp waveform voltage gradually increases from voltage Vi1 that is not higher than a breakdown voltage to sustain electrodes SU1 through SUn to voltage Vi2 that is higher than the breakdown voltage.
While the ramp waveform voltage increases, feeble initializing discharge occurs between scan electrodes SC1 through SCn and sustain electrodes SU1 through SUn, and feeble initializing discharge occurs between scan electrodes SC1 through SCn and data electrodes D1 through Dm. Negative wall voltage is accumulated on scan electrodes SC1 through SCn, and positive wall voltage is accumulated on data electrodes D1 through Dm and sustain electrodes SU1 through SUn. Here, the wall voltage on the electrodes means the voltage generated by the wall charges accumulated on the dielectric layer covering the electrodes, the protective layer, and the phosphor layer.
In the last half of the initializing period, positive voltage Ve1 is applied to sustain electrodes SU1 through SUn. A ramp waveform voltage is applied to scan electrodes SC1 through SCn. Here, the ramp waveform voltage gradually decreases from voltage Vi3 that is not higher than the breakdown voltage to sustain electrodes SU1 through SUn to voltage Vi4 that is higher than the breakdown voltage. While the ramp waveform voltage decreases, feeble initializing discharge occurs between scan electrodes SC1 through SCn and sustain electrodes SU1 through SUn, and feeble initializing discharge occurs between scan electrodes SC1 through SCn and data electrodes D1 through Dm. The negative wall voltage on scan electrodes SC1 through SCn and the positive wall voltage on sustain electrodes SU1 through SUn are reduced, positive wall voltage on data electrodes D1 through Dm is adjusted to a value suitable for the addressing operation. Thus, the all-cell initializing operation of applying initializing discharge to all discharge cells is completed.
The case where the all-cell initializing operation is normally performed has been described. When the discharge is destabilized by increase or the like of discharge delay, though the gradually varying ramp waveform voltage is applied, strong discharge can occur between scan electrodes SC1 through SCn and data electrodes D1 through Dm or between scan electrodes SC1 through SCn and sustain electrodes SU1 through SUn. This strong discharge is hereinafter referred to as “abnormal initialing discharge”.
The abnormal initialing discharge is apt to occur in a discharge cell that hardly generates the sustain discharge, namely a discharge cell for displaying “black”. When the abnormal initialing discharge occurs in the last half of the all-cell initializing period, positive wall voltage is accumulated on scan electrodes SC1 through SCn, negative wall voltage is accumulated on sustain-electrodes SU1 through SUn, and some wall voltage is also accumulated on data electrodes D1 through Dm. When the abnormal initialing discharge occurs in the first half of the all-cell initializing period, the abnormal initialing discharge occurs again in the last half of the all-cell initializing period, and hence the wall voltages are accumulated. These wall voltages disturb the normal operation, so that the wall charge that generates the wall voltages is hereinafter referred to as “abnormal charge”.
In the subsequent address period, voltage Ve2 is applied to sustain electrodes SU1 through SUn, and voltage Vc is applied to scan electrodes SC1 through SCn.
Next, negative scan pulse voltage Va is applied to scan electrode SC1 in the first column, positive writing pulse voltage Vd is applied to data electrode Dk (k is 1 through m), of data electrodes D1 through Dm, in the discharge cell to be made to light up in the first column. The voltage difference in the intersecting part of data electrode Dk and scan electrode SC1 is derived by adding the difference between the wall voltage on data electrode Dk and that on scan electrode SC1 to the difference (Vd−Va) of the external applied voltage, and exceeds the breakdown voltage. Address discharge occurs between data electrode Dk and scan electrode SC1 and between sustain electrode SU1 and scan electrode SC1. Positive wall voltage is accumulated on scan electrode SC1, negative wall voltage is accumulated on sustain electrode SU1, and negative wall voltage is also accumulated on data electrode Dk.
Thus, an addressing operation is performed that causes address discharge in the discharge cell to be made to light up in the first column and accumulates wall voltage on each electrode. The voltage in the intersecting parts of scan electrode SC1 and data electrodes D1 through Dm to which writing pulse voltage Vd is not applied does not exceed the breakdown voltage, so that address discharge does not occur. This addressing operation is repeated up to the discharge cell in the n-th column, and the address period is completed.
The discharge cell having abnormal charge does not have wall voltage required for address discharge, so that normal address discharge does not occur.
In the subsequent sustain period, positive sustain pulse voltage Vs is firstly applied to scan electrodes SC1 through SCn, and 0 (V) is applied to sustain electrodes SU1 through SUn. In the discharge cell having caused the address discharge, the voltage difference between scan electrode SC1 and sustain electrode SU1 is obtained by adding the difference between the wall voltage on scan electrode SC1 and that on sustain electrode SU1 to sustain pulse voltage Vs, and exceeds the breakdown voltage.
Sustain discharge occurs between scan electrode SC1 and sustain electrode SU1, and ultraviolet rays generated at this time causes phosphor layer 35 to emit light. Negative wall voltage is accumulated on scan electrode SC1, and positive wall voltage is accumulated on sustain electrode SU1. Positive wall voltage is also accumulated on data electrode Dk. In the discharge cell where address discharge has not occurred in the address period, sustain discharge does not occur, and the wall voltage at the completion of the initializing period is kept.
Subsequently, 0 (V) is applied to scan electrodes SC1 through SCn, and sustain pulse voltage Vs is applied to sustain electrodes SU1 through SUn. In the discharge cell having caused the sustain discharge, the voltage difference between sustain electrode SU1 and scan electrode SC1 exceeds the breakdown voltage. Therefore, sustain discharge occurs between sustain electrode SU1 and scan electrode SC1 again, negative wall voltage is accumulated on sustain electrode SU1, and positive wall voltage is accumulated on scan electrode SC1. Hereinafter, similarly, as many sustain pulses as the number derived by multiplying the luminance weight by luminance magnification are alternately applied to scan electrodes SC1 through SCn and sustain electrodes SU1 through SUn, and potential difference is caused between the electrodes of the display electrode pairs 24. Thus, sustain discharge in the discharge cell that has caused the address discharge in the address period occurs continuously, and the discharge cell to be made to light up comes on.
At the end of the sustain period, so called narrow pulse-like voltage difference is applied between scan electrodes SC1 through SCn and sustain electrodes SU1 through SUn, and the wall voltage on scan electrode SC1 and sustain electrode SU1 is erased in the state where positive wall voltage is kept on data electrode Dk.
Since positive wall voltage is accumulated on the scan electrode of the discharge cell having abnormal charge, and negative wall voltage is accumulated on the sustain electrode of the discharge cell, sustain discharge can occur to cause false lighting in the sustain period. However, the abnormal charge is too small to certainly generate sustain discharge, so that false lighting accidentally occurs. When false lighting does not occur in the sustain period of the first subfield, false lighting can occur in the sustain period of the next subfield. Thus, the discharge cell having abnormal charge can discharge whenever sustain voltage Vs is applied to one electrode of display electrode pair 24. Once false lighting occurs in the sustain period, however, initializing operation is performed normally in the subsequent initializing period. Therefore, normal operation is performed in the subsequent subfield.
Next, the driving voltage waveform of the subfield that is an all-cell initializing subfield and has an abnormal charge erasing period is described with reference to
The driving voltage waveform in the first half and last half of the all-cell initializing period is the same as that in
In the abnormal charge erasing period, while data electrodes D1 through Dm are kept at 0 (V), voltage Vs is applied to scan electrodes SC1 through SCn and 0 (V) is applied to the sustain electrodes. Voltage applied to each electrode at this time is the same as that when sustain pulse voltage Vs is firstly applied to scan electrodes SC1 through SCn in the sustain period.
The abnormal charge erasing period is provided just after the initialing period and before the address period, so that discharge does not occur in a normal discharge cell in the abnormal charge erasing period. Since sustain voltage Vs is applied to scan electrodes SC1 through SCn in the discharge cell having abnormal charge, however, discharge can occur. The time period when sustain voltage Vs is applied to scan electrodes SC1 through SCn is set longer than the duration of the sustain pulse in the sustain period. Therefore, the probability that the discharge cells having abnormal charge discharge in the abnormal charge erasing period is extremely higher than that of discharge by the sustain pulse, and most of the discharge cells having abnormal charge can be made to discharge in the abnormal charge erasing period.
Next, while data electrodes D1 through Dm and sustain electrodes SU1 through SUn are kept at 0 (V), negative voltage Va is applied to scan electrodes SC1 through SCn. The discharge cell having abnormal charge discharges again, and the abnormal charge is erased. Therefore, sustain discharge does not occur in the subsequent sustain period.
The driving voltage waveform in the subsequent address period and sustain period is the same as that in
Next, the driving voltage waveform of the subfield that is a selective initializing subfield and has no abnormal charge erasing period is described with reference to
In the selective initializing period, voltage Ve1 is applied to sustain electrodes SU1 through SUn and 0 (V) is applied to data electrodes D1 through Dm, a ramp waveform voltage gradually decreasing from voltage Vi3′ to voltage Vi4 is applied to scan electrodes SC1 through SCn.
In the discharge cell that has caused the sustain discharge in the sustain period of the last subfield, feeble initializing discharge occurs, and the wall voltage on scan electrode SC1 and sustain electrode SU1 is reduced. Regarding data electrode Dk, sufficient positive wall voltage is accumulated on data electrode Dk by the last sustain discharge, so that the wall voltage is discharged by the excessive amount to be adjusted to be appropriate for the addressing operation.
While, in the discharge cell that has not caused the sustain discharge in the last subfield, discharge is not performed and the wall charge at the completion of the initializing period of the last subfield is kept. In the selective initializing operation, initializing discharge is selectively performed in the discharge cell where a sustain operation is performed in the sustain period of the last subfield.
The operation of the subsequent address period is similar to the operation of the address period of the all-cell initializing subfield, and hence it is not described. The operation of the subsequent sustain period is similar except for the number of sustain pulses.
Next, the driving voltage waveform of the subfield that is a selective initializing subfield and has an abnormal charge erasing period is described with reference to
The selective initializing operation in the initializing period, the addressing operation in the address period, and the sustain operation in the sustain period are the same as respective operations in the selective initializing subfield having no abnormal charge erasing period, and hence they are not described.
The abnormal charge erasing period is the same as that described using
Then, while data electrodes D1 through Dm and sustain electrodes SU1 through SUn are kept at 0 (V), negative voltage Va is applied to scan electrodes SC1 through SCn. At this time, the discharge cell having abnormal charge discharges again, and the abnormal charge is erased. Therefore, false lighting does not occur in the subsequent sustain period. Since the wall charge required for the addressing operation is erased also when the abnormal charge is erased, and the addressing operation cannot be performed. This state of the wall charge continues until the next all-cell initializing operation is performed.
In the above description, in the abnormal charge erasing period, voltage Vs is applied as rectangular waveform voltage to scan electrodes SC1 through SCn. However, the present invention is not limited to this, and the following voltage is simply required to be applied to scan electrodes SC1 through SCn. At this voltage, there is possibility that the discharge cell having abnormal charge discharges, and there is no possibility that the discharge cell having no abnormal charge discharges. The voltage at which there is no possibility of discharge in the discharge cell having no abnormal charge is rectangular waveform voltage, for example. The voltage at which there is no possibility of discharge in the discharge cell having no abnormal charge is not limited to the rectangular waveform voltage, but the rectangular waveform voltage is taken as an example in the subsequent descriptions and drawings.
Next, the subfield structure of the present embodiment is described. One field is divided into 10 subfields. Each subfield has a greater luminance weight than the previous one. The 10 subfields are called a first SF, second SF, . . . , and 10th SF. The luminance weights of the first SF, second SF, . . . , and 10th SF are set to be 1, 2, 3, 6, 11, 18, 30, 44, 60 and 80, for example.
In the field corresponding to the black display signal, as shown in
On the other hand, in the field corresponding to the image signal other than the black display signal, as shown in
The reason why the subfield having the abnormal charge erasing period is varied in response to the image signal is described below.
As discussed above, a discharge cell having abnormal charge can accidentally and falsely light up in the sustain period of each subfield. Once the false lighting occurs, sustain discharge due to the false lighting continues until the completion of the sustain period. The light emitted by the false lighting is brighter in a subfield having larger luminance weight, namely in a subfield disposed more backward in the present embodiment. When the discharge cell that is not to light up emits bright light, the image display quality is significantly damaged. Therefore, the light emission luminance due to the abnormal charge must be minimized. For the minimization, preferably, an abnormal charge erasing period is disposed in a subfield disposed as forward as possible after the first all-cell initializing operation of the field, and the abnormal charge is erased.
When the abnormal charge erasing period is disposed after the subfield where the first all-cell initializing operation is performed in the field, however, it becomes clear that the following possibility is raised. When the panel is used in an extremely severe environment such as high temperature or low temperature, a discharge cell discharges in the abnormal charge erasing period though the all-cell initializing operation is performed normally. As discussed above, the discharge cell that has discharged in the abnormal charge erasing period cannot perform addressing operation in the address period of the subsequent subfield. Therefore, when a discharge cell to light up discharges in the abnormal charge erasing period, the discharge cell cannot emit light.
In the present embodiment, in the field corresponding to the image signal other than the black display signal, namely the image signal having the discharge cell that is to light up, an abnormal charge erasing period is not disposed after the initializing period of the first SF as the first all-cell initializing subfield, but an abnormal charge erasing period is disposed after the initializing periods of the subsequent second SF and fourth SF.
While, in the field corresponding to the black display signal, each discharge cell displays “black” and is apt to cause abnormal initializing discharge. Therefore, it is preferable that the abnormal charge is erased by disposing an abnormal charge erasing period in a subfield disposed as forward as possible after the all-cell initializing operation. In the present embodiment, an abnormal charge erasing period is disposed after the all-cell initializing period of the first SF.
Next, the circuitry of the plasma display device of the present embodiment of the present invention is described.
Plasma display device 100 has the following elements:
Here, data electrode driving circuit 52, scan electrode driving circuit 53, sustain electrode driving circuit 54, timing generating circuit 55, and black display detecting circuit 61 are collectively called a driving circuit.
Image signal processing circuit 51 converts an input image signal into image data that indicates emission or non-emission of light every subfield. Data electrode driving circuit 52 converts the image data every subfield into a signal corresponding to each of data electrodes D1 through Dm, and drives each of data electrodes D1 through Dm.
Black display detecting circuit 61 calculates lighting ratio of the discharge cell of each subfield, namely ratio of discharge cells for performing sustain discharge in the subfield to all discharge cells, based on image data. An image signal where the lighting ratio of all subfields is “0” is detected as an image signal for displaying black on the whole screen, namely a black display signal.
Timing generating circuit 55 generates various timing signals for controlling operation of each circuit block based on a horizontal synchronizing signal, a vertical synchronizing signal, and a detection output of black display detecting circuit 61, and supplies them to respective circuit blocks. Timing generating circuit 55 generates a timing signal so that two following fields have different subfield structures as shown in
Next, a method of generating a voltage waveform for erasing abnormal charge in the abnormal charge erasing period is described.
Scan electrode driving circuit 53 has the following elements:
Sustain pulse generating circuit 81 has the following elements:
Initializing waveform generating circuit 84 has the following elements:
Scan pulse generating circuit 88 has the following elements:
Next, operation of scan electrode driving circuit 53 is described.
First, 0 (V) is applied to scan electrodes SC1 through SCn. Switching element SW2 of sustain pulse generating circuit 81 and switching elements SWL1 through SWLn of switching units OUT1 through OUTn are set at ON, and the other switching elements are set at OFF.
At time t1, switching element SW2 of sustain pulse generating circuit 81 comes into the OFF state, and switching element SW1 comes into the ON state. At this time, voltage Vs is applied to scan electrodes SC1 through SCn via switching element SW1 and switching elements SWL1 through SWLn.
At time t2, switching element SW1 of sustain pulse generating circuit 81 comes into the OFF state, switching element SW2 comes into the ON state, and scan electrodes SC1 through SCn are temporarily returned to 0 (V). Then, switching element SW2 of sustain pulse generating circuit 81 comes into the OFF state, switching element SW3 of scan pulse generating circuit 88 comes into the ON state. Voltage Va is applied to scan electrodes SC1 through SCn via switching element SW2 and switching elements SWL1 through SWLn.
At time t3, switching elements SWL1 through SWLn of switching units OUT1 through OUTn come into the OFF state, switching elements SWH1 through SWHn come into the ON state, and voltage Vc is applied to scan electrodes SC1 through SCn. The period after t3 is the address period.
In the present embodiment, the period from time t1 to time t2 is set at 6 μsec. However, preferably, this period is set between 3 μsec and 30 μsec. In the present embodiment, the period from time t2 to time t3 is set at 2.5 μsec. However, preferably, this period is set between 1 μsec and 10 μsec.
In the present embodiment, in the field corresponding to an image signal other than the image signal for displaying black on the whole screen, an abnormal charge erasing period is disposed in the second SF and fourth SF. However, the present invention is not limited to this. An abnormal charge erasing period may be disposed in any subfield after the subfield where the all-cell initializing operation is firstly performed,
In the present embodiment, the number of subfields and the luminance weight of each subfield are not limited to the above-mentioned values, but other subfield structure may be employed.
Each specific numerical value used in the present embodiment is an example. Preferably, an optimum value is employed appropriately in response to the characteristic of the panel or the specification or the like of the plasma display device.
As a result, the present invention can provide a panel driving method and a plasma display device that do not cause false lighting even if the all-cell initializing operation becomes unstable, and do not significantly reduce the image display quality.
The present invention can provide a panel driving method that does not cause false lighting and does not significantly reduce the image display quality. Therefore, present invention is useful as a panel driving method and plasma display device.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2006-307433 | Nov 2006 | JP | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/JP2007/071683 | 11/8/2007 | WO | 00 | 10/2/2008 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2008/059745 | 5/22/2008 | WO | A |
| Number | Name | Date | Kind |
|---|---|---|---|
| 6404411 | Masuda et al. | Jun 2002 | B1 |
| 20040113871 | Kashio et al. | Jun 2004 | A1 |
| 20080048937 | Ogawa et al. | Feb 2008 | A1 |
| Number | Date | Country |
|---|---|---|
| 2000-242224(A) | Sep 2000 | JP |
| 2001-255847(A) | Sep 2001 | JP |
| 2002-082648(A) | Mar 2002 | JP |
| 2004-109838(A) | Apr 2004 | JP |
| 2004-191530(A) | Jul 2004 | JP |
| 2004-326068(A) | Nov 2004 | JP |
| 2005-301259(A) | Oct 2005 | JP |
| 2005-326612(A) | Nov 2005 | JP |
| 2006-308626(A) | Nov 2006 | JP |
| 2007099891(A1) | Sep 2007 | JP |
| WO 2005111974 | Nov 2005 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 20090096719 A1 | Apr 2009 | US |
