A High Performance Dithering Method for Gray and ... - IEEE Xplore

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LanZhou University, LanZhou, China. Abstract—Dithering has been established as an important technique for producing visually appealing images on many.
A HIGH PERFORMANCE DITHERING METHOD FOR GRAY AND COLOR IMAGE QUANTIZATION Yi Wan, member IEEE,

Zhijun Yao,

Information science and engineering department,

Information science and engineering department, LanZhou

LanZhou University, LanZhou, China.

University, LanZhou, China. Abstract—Dithering has been established as an important technique for producing visually appealing images on many printing and display devices. Although various error diffusion filters have been developed for dithering, there has been in general a lack of results guided by both visual quality and objective measure on the image quality. In this paper we present a dithering method by designing the error diffusion filter coefficients

through

solving

a

constrained

least

Figure 1. Gray error diffusion, (a)Error diffusion to a single pixel. (b)The Floyd-Steinberg error diffusion coefficients.

square

optimization problem. The result minimizes the total square error between the final image and the original image in the error

A well-known choice of the {hs} are developed in [2]. Fig. 1 shows the grayscale error diffusion diagram and the

diffusion framework. Simulation results show that this method

Floyd-Steinberg error diffusion coefficients.

produces better visual quality than other commonly used methods. Keywords-error diffusion; dithering; halftone; quantization

The rest of the paper is organized as follows. Section II introduces the method of optimal design of the error diffusion filters following a least square optimization problem

INTRODUCTION

formulation. We introduce our method for dithering gray and

In digital image processing, whenever a quantization

color images separately. Simulation results are presented in

I.

process is carried out on an image, some information will be

section 3. Finally, we draw conclusions in section 4.

lost and the so-called blocky artifact often occurs. A typical

II.

example happens when displaying information on a printer,

For grayscale images, the error n(t) is the quantization

where the color pallet has far less number of color tones than

error at a single pixel t and (1) is a function of scalar

that of the original image. Digital halftoning is a technique for

coefficients {hs}. For color images, we can treat each color

exchanging the image spatial resolution for tonal resolution

band separately and do three independent scalar error

[1], [3]-[10]. On the other hand, dithering is a technique that

diffusion problems. But this approach ignores the correlation

doesn’t sacrifice the spatial resolution while producing

among the color bands. A better way is to allow the error to

visually appealing result. It diffuses the quantization error in a

diffuse across different color bands. In the following

local area of an image to its neighboring area. Mathematically

subsections we first develop the scalar error diffusion

it can be formulated as the following:

optimization procedure, then extend it to the case of color

~

x(t ) = x(t ) + ∑ hs n(t − s)

(1)

SCALAR AND VECTOR ERROR DIFFUSION

images. A. Scalar Error Diffusion

s

where x(t) is the original pixel value, the non-negative coefficients {hs } has the total sum of 1. n(t-s) is the quantization error o f i t s neighboring pixels.

Assume a grayscale image x of size N1 × N2. After the dithering process another image y is obtained through the relation

978-1-4244-3709-2/10/$25.00 ©2010 IEEE

~

(2)

y (t ) = Q( x(t ))

˜(t) is defined in (1). where x To minimize visual distortion, we expect the difference

Notice that in (8) the set {hs(k ) } is computed based on the set {hs( k −1) } . After the updating step, {hs(k ) } may no longer

between x and y to be minimized. The most commonly used

satisfy the constraint (5). We thus do a projection onto the

such difference measure is the squared Euclidean distance

hyperplane determined by (5), i.e.,

between them, i.e., ~

E =|| x − y ||2 = ∑ [ x(t ) − y (t )]2 = ∑[ x(t ) − Q( x(t ))]2 t

(3)

t

which will be the measure we use in this paper. Note that by using (3) can be equivalently expressed through n as

⎧⎡h1( k ) ⎤ ⎡1⎤ ⎫⎡1⎤ ⎡h1( k ) ⎤ ⎡h1( k ) ⎤ ⎪⎢ ( k ) ⎥ ⎢ ⎥ ⎪⎢ ⎥ ⎢ ( k ) ⎥ ⎢ (k ) ⎥ (9) ⎢h2 ⎥ − 1 ⎪⎨⎢h2 ⎥ • ⎢1⎥ ⎪⎬⎢1⎥ → ⎢h2 ⎥ ⎢h3( k ) ⎥ 4 ⎪⎢h3( k ) ⎥ ⎢1⎥ ⎪⎢1⎥ ⎢h3( k ) ⎥ ⎢ (k ) ⎥ ⎪⎢⎣⎢h4( k ) ⎥⎦⎥ ⎢⎣1⎥⎦ ⎪⎢⎣1⎥⎦ ⎢⎣⎢h4( k ) ⎥⎦⎥ ⎣⎢h4 ⎦⎥ ⎩ ⎭ The iteration procedure continues until a local minimum

as sufficiently closely reached. In this paper we use the condition

(4)

E = ∑ [n(t ) − ∑ hs n(t − s )]

2

t

E ( k −1) − E ( k )