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A Novel Defect Inspection Method for the TFT-LCD Image Based on ...

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The light is diffused and c<strong>on</strong>centrated through <str<strong>on</strong>g>the</str<strong>on</strong>g>se sheets.<br />

But <str<strong>on</strong>g>the</str<strong>on</strong>g>re still exist some illuminati<strong>on</strong> variati<strong>on</strong>s measured<br />

by LU of more than 80%. Above 80% LU is c<strong>on</strong>sidered<br />

acceptable in industry. The luminance values <str<strong>on</strong>g>for</str<strong>on</strong>g> calculating<br />

<str<strong>on</strong>g>the</str<strong>on</strong>g> LU are acquired from <str<strong>on</strong>g>the</str<strong>on</strong>g> predetermined positi<strong>on</strong>s.<br />

Mura defects are darker or brighter than <str<strong>on</strong>g>the</str<strong>on</strong>g>ir neighboring<br />

normal regi<strong>on</strong>s in <str<strong>on</strong>g>TFT</str<strong>on</strong>g>-<str<strong>on</strong>g>LCD</str<strong>on</strong>g> images. They have various<br />

shapes and strengths according to <str<strong>on</strong>g>the</str<strong>on</strong>g> cause of generati<strong>on</strong>.<br />

Some of <str<strong>on</strong>g>the</str<strong>on</strong>g>m occur when unexpected <str<strong>on</strong>g>for</str<strong>on</strong>g>eign materials are<br />

inserted into <str<strong>on</strong>g>the</str<strong>on</strong>g> layers in a display panel and <str<strong>on</strong>g>the</str<strong>on</strong>g>y can be<br />

generated due to n<strong>on</strong>-uni<str<strong>on</strong>g>for</str<strong>on</strong>g>m liquid crystal distributi<strong>on</strong>, air<br />

inserti<strong>on</strong>, and partial press by external <str<strong>on</strong>g>for</str<strong>on</strong>g>ces, etc [8].<br />

Because of <str<strong>on</strong>g>the</str<strong>on</strong>g> n<strong>on</strong>-uni<str<strong>on</strong>g>for</str<strong>on</strong>g>m illuminati<strong>on</strong> characteristic of <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

background signal, dark Mura can be brighter than <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

normal background regi<strong>on</strong>. Two of our experimental <str<strong>on</strong>g>TFT</str<strong>on</strong>g>-<br />

<str<strong>on</strong>g>LCD</str<strong>on</strong>g> panel images are shown in Fig. 3(a), (b). Fig. 3(a)<br />

includes 4 White and Dark Mura defects and Fig. 3(b) has<br />

<str<strong>on</strong>g>the</str<strong>on</strong>g> signal generated Muras with various size and strength.<br />

The positi<strong>on</strong> of Muras are encircled or marked with arrows.<br />

The line profile of dotted circle and arrow is shown in Fig.3<br />

(c). From <str<strong>on</strong>g>the</str<strong>on</strong>g>se figures, <str<strong>on</strong>g>the</str<strong>on</strong>g> illuminati<strong>on</strong> of <str<strong>on</strong>g>TFT</str<strong>on</strong>g>-<str<strong>on</strong>g>LCD</str<strong>on</strong>g> image<br />

shows local and global variati<strong>on</strong>s at <str<strong>on</strong>g>the</str<strong>on</strong>g> same time.<br />

3 Proposed <str<strong>on</strong>g>Defect</str<strong>on</strong>g> Detecti<strong>on</strong> Algorithm<br />

No<br />

Not Mura<br />

Input <str<strong>on</strong>g>Image</str<strong>on</strong>g><br />

Discrete Cosine Trans<str<strong>on</strong>g>for</str<strong>on</strong>g>m<br />

Adapted CSF Filtering<br />

Inverse<br />

Discrete Cosine Trans<str<strong>on</strong>g>for</str<strong>on</strong>g>m<br />

Polynomial Regressi<strong>on</strong> Analysis<br />

Tri-modal Thresholding<br />

Labeling<br />

L<br />

if C<br />

L<br />

Result <str<strong>on</strong>g>Image</str<strong>on</strong>g><br />

Mura<br />

Fig.4. The proposed block diagram <str<strong>on</strong>g>for</str<strong>on</strong>g> <str<strong>on</strong>g>TFT</str<strong>on</strong>g>-<str<strong>on</strong>g>LCD</str<strong>on</strong>g> image defect detecti<strong>on</strong><br />

Yes<br />

The flow chart of <str<strong>on</strong>g>the</str<strong>on</strong>g> proposed algorithm is seen in Fig.<br />

4. First, <str<strong>on</strong>g>the</str<strong>on</strong>g> input image is DCT trans<str<strong>on</strong>g>for</str<strong>on</strong>g>med and <str<strong>on</strong>g>the</str<strong>on</strong>g>n<br />

proposed ACSF filter is applied to enlarge <str<strong>on</strong>g>the</str<strong>on</strong>g> Mura signal.<br />

After <str<strong>on</strong>g>the</str<strong>on</strong>g> signal is inverse Discrete Cosine Trans<str<strong>on</strong>g>for</str<strong>on</strong>g>med,<br />

polynomial regressi<strong>on</strong> (PR) process is employed <str<strong>on</strong>g>for</str<strong>on</strong>g><br />

flattening. Then <str<strong>on</strong>g>the</str<strong>on</strong>g> enhanced image is segmented by trimodal<br />

thresholding to find White and Dark Mura at <strong>on</strong>ce.<br />

To leave out reliable defects, false defects are eliminated if<br />

<str<strong>on</strong>g>the</str<strong>on</strong>g> mean gray level of a defect does not have much<br />

difference from <str<strong>on</strong>g>the</str<strong>on</strong>g>ir background.<br />

3.1 Adapted CSF in DCT Domain<br />

The human visual system(HVS) has different<br />

frequency sensitivity and that is ma<str<strong>on</strong>g>the</str<strong>on</strong>g>matically represented<br />

as CSF given by <str<strong>on</strong>g>the</str<strong>on</strong>g> experiment[8][9][10]. The HVS can<br />

detect more easily <str<strong>on</strong>g>the</str<strong>on</strong>g> difference varying in low frequency<br />

than high frequency. The CSF can be expressed by a<br />

functi<strong>on</strong> and CSF graph is shown in Fig. 5.<br />

Where,<br />

1.<br />

1<br />

H( f ) 2.<br />

6(<br />

0.<br />

192 0.<br />

114 f ) exp( (<br />

0.<br />

114 f ) ) (2)<br />

f f f is <str<strong>on</strong>g>the</str<strong>on</strong>g> frequency having unit of<br />

2<br />

x<br />

2<br />

y<br />

cycle/degree. HVS have best sensitivity around<br />

8[cycles/degree] and above 40[cycles/degree] its value<br />

become smaller and smaller.<br />

CSF Value<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

CSF Graph<br />

0 4 8 12 16 20 24 28 32 36 40 44 48 52 56 60<br />

Frequency[Cycle/Degree]<br />

Fig.5. The c<strong>on</strong>trast sensitivity functi<strong>on</strong> graph.<br />

There have been many ef<str<strong>on</strong>g>for</str<strong>on</strong>g>ts to use CSF to <str<strong>on</strong>g>the</str<strong>on</strong>g>ir<br />

applicati<strong>on</strong>s, especially in compressi<strong>on</strong>. In order to use <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

CSF in real applicati<strong>on</strong> relative sensitivity value is<br />

important[10]. Without loss of generality, <str<strong>on</strong>g>the</str<strong>on</strong>g> maximum<br />

CSF frequency can be normalized as 2 in DCT domain.<br />

The DCT has good energy compacti<strong>on</strong> property and it has<br />

also fast algorithm. The DCT has no phase in<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong>, it<br />

<strong>on</strong>ly c<strong>on</strong>sider <str<strong>on</strong>g>the</str<strong>on</strong>g> magnitude of trans<str<strong>on</strong>g>for</str<strong>on</strong>g>med data. The CSF<br />

has <strong>on</strong>ly magnitude, so it will be enough to c<strong>on</strong>sider <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

proposed ACSF in DCT domain. The proposed adapted CSF<br />

in DCT is ma<str<strong>on</strong>g>the</str<strong>on</strong>g>matically expressed by <str<strong>on</strong>g>the</str<strong>on</strong>g> followings.

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