JP3023369B2 - Light amount correction device for digital scanner - Google Patents

Description

Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a light source light amount correction device in a digital scanner using a fluorescent lamp.

2. Description of the Related Art The configuration of a conventional digital scanner will be described with reference to FIG. Document 1 for reading is contact glass 2
A reference white plate 4 is provided between the contact glass 2 and the scale 3 placed on the end of the contact glass 2. The fluorescent lamp 5 as a light source is located below the contact glass 2 and its longitudinal direction is the reading direction T.
It is arranged so as to be orthogonal to. A fluorescent lamp heater 6 is provided around the fluorescent lamp 5, and the light emitted by the fluorescent lamp 5 is reflected by the contact glass surface and goes downward, and the first mirror 7, the second mirror 8, and the third mirror The light flux is sequentially reflected by the light source 9 and changes its optical path, and a part of the light flux is condensed by the condensing lens 11 while passing through the shading correction plate 10, so that the light flux is condensed by the CCD 13 provided on the image reading plate 12. Light is received, and the image recorded on the document 1 is read.

Problems to be Solved by the Invention In the device as described above, when a fluorescent lamp 5 (in particular, an aperture type) is used as a light source for illumination,
It is generally known that the illuminance of the document 1 is affected by the document image. Such a phenomenon occurs because the secondary reflected light from the original 1 enters the fluorescent lamp 5 and is reflected again in the fluorescent lamp 5.

As a result, the illuminance distribution and the illuminance itself in the longitudinal direction of the fluorescent lamp 5 are affected and change during reading of one original 1. As a result, the original is read and copied despite the original density being constant. The density distribution of the obtained data is different from the density distribution of the original document 1. Therefore, it is necessary to correct the illuminance of the original of the fluorescent lamp 5 which changes due to the re-reflection from the original. However, there is no conventional illuminance correction of the amount of the light source. .

Means for Solving the Problems In order to solve such a problem, the present invention relates to a digital scanner using a fluorescent lamp as a light source, wherein at least two light sources arranged in the longitudinal direction of the fluorescent lamp are provided. At least one of the sensors is arranged at an end of the effective image area of the fluorescent lamp, and image data calculated and read by interpolation calculation obtained by the light amount sensor based on output data obtained by the light amount sensor. The light source light amount illuminance correction means for correcting the illuminance of the light source is provided.

Therefore, even if the original illuminance of the fluorescent lamp changes due to re-reflection from the original, the change in the light amount is received by the light amount sensor, and the image data calculated and read by the interpolation calculation obtained by the light amount sensor by the light source light amount illuminance correction means. , The original illuminance of the fluorescent lamp can be made uniform, whereby the density of the read image data can be reproduced in the same manner as the original.

Embodiment An embodiment of the present invention will be described with reference to FIGS. The same parts as those in the prior art (see FIG. 9) are denoted by the same reference numerals.

FIG. 1 shows a basic configuration of the present embodiment. In the longitudinal direction of the fluorescent lamp 5, three light quantity sensors 14 are arranged, and the light quantity between the light quantity sensors 14 is calculated by interpolation calculation to correct the illuminance of the read image data. Is provided. In this case, the light source light quantity illuminance correction means 15 includes five ROMs 16a, 16b, 16c, 16d, 16e.
And ADDOR17 to which data from these ROMs are sent,
ROM 18 to which data and image data from ADDOR 17 are sent
And a RAM 19 to which address data is sent, and a ROM 29 to which data from the RAM 19 and the ROM 18 are sent.

In such a configuration, FIGS. 2 and 3 show how the three light quantity sensors 14 and the light source light quantity illuminance correction means 15 described above are incorporated in an actual scanner (see FIG. 9). . Therefore, a method of calculating the light amount between the light amount sensors 14 by interpolation using the light amount sensors 14 arranged at such a fixed interval will be sequentially described below.

Now, in the case of a scanner configured as shown in FIG.
S (x) read from the document and the like, and the original reflectance T (x)
Is as shown in the following equation.

S (x) = A ₁ (x) · A ₂ (x) · B (x) · C (x) · L ₁ (x, t, T) · T (x) + L ₂ (x, t, T) .. (1) x: address of CCD, etc., t: time A ₁ (x): reflectance of mirror A ₂ (x): lens characteristic B (x): lens characteristic correction coefficient (shading correction plate characteristic) C (x ): CCD sensitivity L ₁ (x, t, T): Original image illuminance L ₂ (x, t, T): Light entering the CCD from outside the optical path (flare) At this time, L ₂ is reduced to zero by the scanner configuration It can be ignored because it is made to be.

In addition, since A ₁ , A ₂ , B, and C are time-invariant, in order to eliminate these coefficients, generally, Sref (x) when the reference white plate Tref (x) is read is used. Then, when the image data Sa (x) is obtained as the relative brightness with respect to the reference white plate 4, Becomes

t ₀ : time when the reference white plate 4 is read T ₀ : density of a portion where the reflected light enters the fluorescent lamp 5 (reference white plate, sheet metal, etc.) Here, since the reference white plate 4 has a constant reflectance, , Then Becomes

Therefore, By performing the following calculation, the relative value Ta
A value D (x) proportional to (x) can be obtained.

Here, if equation (4) is rewritten, Becomes

here, Then It can be expressed as.

Further, the document surface illuminance L ₁ (x, t, T) can be expressed as shown below based on FIG.

Here, rewriting the above formula, From dS = d ₀・ dψ ・ dza, Becomes

Here, since the variation of the luminance I in the ψ direction is sufficiently small, the calculation is performed assuming that I (ψ, za, t) = I (za, t). Becomes

Note that the illuminance at an arbitrary position Za ₀ because it is the illuminance at the equation (9) is the origin O is replaced with Za = Za-Za _0, It is expressed as

From this equation (10), to obtain the illuminance at a certain point,
It is understood that it is necessary to know the luminance over the entire length of the fluorescent lamp 5. However, in this case, since the sample points are finite, this equation is obtained by performing interpolation.

Now, assuming that the luminance at each sample point is I _{1 to} In−1, Ii
The luminance Ix between the Ii + 1 (however, I ₁ is an active pixel edge), with reference to Figure 6, h (Δx): Interpolation coefficient σ, Δx: obtained as an address of CCD or the like.

here, After all, Becomes

Here, Za = ρ (i + x) ρ: the reciprocal of the reduction ratio of the lens system Here, if d ₀ ² + ρ ² (xi−x + Δx) ² = Q (xi−x, Δx), Becomes

here, Then, when this equation (13) is transformed, Becomes However, equation (14) shows a case where n≫4.

Then, in the case of the present embodiment, assuming that the number of samples n = 3 (see FIG. 4) in equation (14), F (x) = I ₀ · Gσ + Δx, x ₁ (x) + I ₁ · ｛Gσ + Δx, x ₂ (x) + GΔx, x ₁ (x)｝ + I ₂ · ｛GΔx, x ₂ (x) + Gσ-Δx, x ₁ (x)｝ + I ₃ · ｛Gσ-Δx, x ₂ (x) + G2σ-Δx , x ₁ (x)｝ + I ₄ · G2σ−Δx, x ₂ (x) (15)

In the equation (15), I ₀ and I ₄ are eigenvalues, and values are set such that the calculated light amount at the end of the fluorescent lamp 5 is close to the actual value. In this case, of course, depending on the arrangement of the light amount sensor, I ₀
= I ₄ = 0.

Now, when the expression (10) is converted using the expression (15), L ₁ (x, t, T) = − d ₀ ³ [cosψ] ^{ψ 2} _{ψ 1} ▼ · F
(X) ... (16) and substituting equation (16) into equation (5) gives Becomes

Therefore, the value of D (x) proportional to the document reflectance T (x) can be obtained by performing the calculation of the expression (17).

Next, the flow of this calculation will be described with reference to FIG. First, the luminance of the fluorescent lamp 5 is read by the light quantity sensor 14. At this time, if there is a variation in the light quantity sensor itself, accurate calculation cannot be performed. I do. This sensor unit has a circuit configuration as shown in FIG.
Using the converted and output I _{1 to} I ₃ and the fixed values I ₀ and I ₄ and the address data x, first, F
Calculate the value of (x).

That is, in ROM16a～ROM16e, the calculation of light corresponding to I ₀ ~I _4.

Specifically, FI ₀ (x) = I ₀ · Gσ + Δx, x ₁ (x) FI ₁ (x) = I ₁ · {Gσ + Δx, x ₂ (x) + GΔx, x ₁ (x)} FI ₂ (x _{) = I 2 · {GΔx,} x 2 (x) + Gσ-Δx, x 1 (x)} FI 3 (x) = I 3 · {Gσ + Δx, x 2 (x) + G2σ-Δx, x 1 (x)} Each calculation of FI ₄ (x) = I ₄ · G2σ−Δx, x ₂ (x) is performed.

Then, in ADDOR17, it is possible to obtain the F (x) by adding the value of _{FI 0 (x) ~FI 4 (} x). That, F (x) becomes _{F (x) = FI 0 (} x) + FI 1 (x) + FI 2 (x) + FI 3 (x) + FI 4 (x) ... (18).

Next, in the ROM 18, the expression (17) Is calculated.

At this time, the data Sref (x) when the reference white plate 4 is read
Is calculated in the RAM 19.

And in the last ROM20, By performing the above calculation, it is possible to obtain corrected image data corresponding to a change in the so-called document illuminance in which the light amount between the light amount sensors 14 is calculated by the interpolation calculation.

In this embodiment, FIG. 8 (an enlarged view of FIG. 2)
As shown in the above, in order to monitor the brightness of the fluorescent lamp 5,
A double slit 21 is provided in front of the light amount sensor 14. The solid angle ω from the light amount sensor 14 is obtained by the double slit.
Is smaller, the position of the fluorescent lamp 5 and the light amount sensor 14 can be made independent of the light amount by the light cone principle. In addition, an opposing reflection plate 22 is provided in front of the slit 21.

Effect of the Invention As described above, the present invention relates to a digital scanner using a fluorescent lamp as a light source, wherein at least one of at least two light quantity sensors disposed in the longitudinal direction of the fluorescent lamp is an effective light source for the fluorescent lamp. It is arranged at the end of the image range, and based on the output data obtained by these light amount sensors, the light amount between the light amount sensors is calculated by interpolation, and the read image data is normalized by the light amount calculated by the interpolation calculation. Since the light source light amount illuminance correction means for performing the illuminance correction is provided, it is possible to make the original illuminance of the fluorescent lamp uniform.

[Brief description of the drawings]

FIG. 1 is a block diagram showing an embodiment of the present invention, FIGS. 2 and 3 are configuration diagrams showing the state of a light source light amount correcting device, and FIG. 4 shows the relationship of a reading position with respect to a fluorescent lamp. FIG. 5 is an explanatory diagram showing the relationship between the document surface illuminance and a coordinate axis, FIG. 6 is an explanatory diagram showing the positional relationship of luminance at each sample point, FIG. 7 is a circuit diagram showing an example of a sensor unit, FIG. 8 is an enlarged configuration diagram showing a state where a slit is positioned in front of the light amount sensor, and FIG. 9 is a configuration diagram showing a conventional example. 5 fluorescent light, 14 light intensity sensor, 16 light source light intensity illuminance correction means

Claims (1)

(57) [Claims] 1. A digital scanner using a fluorescent lamp as a light source, wherein at least two fluorescent lamps are arranged in a longitudinal direction of the fluorescent lamp.
At least one of the light quantity sensors is arranged at the end of the effective image range of the fluorescent lamp, and the light quantity between the light quantity sensors is calculated by interpolation based on the output data obtained by these light quantity sensors. A light source light amount correcting device for a digital scanner, further comprising a light source light amount illuminance correction unit for correcting illuminance by normalizing the read image data with the light amount calculated by the interpolation calculation.