A COMBINED SPECTRAL MEASUREMENT AND IMAGING SENSOR
20190289228 ยท 2019-09-19
Assignee
Inventors
- Tsachi Mazliach (Rinatya, IL)
- Barry Ben Ezra (Ramat Hasharon, IL)
- Alan Then (Addison, TX, US)
- Brian Gamm (McKinney, TX, US)
Cpc classification
H04N23/10
ELECTRICITY
H04N1/486
ELECTRICITY
H04N23/11
ELECTRICITY
G01J3/36
PHYSICS
International classification
Abstract
A combined imaging and spectral measurement line-scan imaging sensor includes a plurality of pixel lines. Each pixel line includes a plurality of pixels. At least one of the pixel lines is an imaging line designated for acquiring at least one image of an object and other of the pixel lines are spectral measurement lines designated for acquiring a spectral measurement of light received from the object. Each imaging line is associated with a single respective spectral response within a spectral range. Each pixel in each spectral measurement line is associated with a respective spectral band. Each of at least three pixels in each of the spectral measurement lines is respectively associated with different respective pixel spectral bands. The different respective pixel spectral bands are non-identical to any one of the single spectral responses associated with each of the imaging spectral lines.
Claims
1. A combined imaging and spectral measurement line-scan imaging sensor including: a plurality of pixel lines, each pixel line including a plurality of pixels, at least one of said pixel lines being imaging lines designated for acquiring at least one image of an object and one other of said pixel lines being spectral measurement lines designated for acquiring a spectral measurement of light received from said object, each imaging line being associated with a single respective spectral response within a spectral range, each pixel in each spectral measurement line being associated with a respective spectral band, each of at least three pixels in each of said spectral measurement lines being respectively associated with different respective pixel spectral bands, said different respective pixel spectral bands being non-identical to any one of said single spectral responses associated with each said imaging spectral lines.
2. The combined imaging and spectral measurement line-scan imaging sensor according to claim 1, wherein each said spectral measurement line is divided into a plurality of groups of adjacent pixels, and wherein each said group is associated with the same group spectral band range and each pixel in said group is associated with a respective pixel spectral band
3. The combined imaging and spectral measurement line-scan imaging sensor according to claim 1, wherein a filter associated with a respective spectral band is placed over a group of at least three adjacent pixels completely covering a middle at least one of said at least three adjacent pixels, and wherein only the pixels that are completely covered by the filter are read out.
4. The combined imaging and spectral measurement line-scan imaging sensor according to claim 1, wherein each pair of vertically adjacent pixels, between two groups of four pixels is covered with an opaque material.
5. The combined imaging and spectral measurement line-scan imaging sensor according to claim 1, wherein the spectral range of each of said imaging lines is at least one of: Red spectral band; Green spectral band; Blue spectral band; and Infrared spectral range.
6. The combined imaging and spectral measurement line-scan imaging sensor according to claim 1, wherein a pixel spectral band is achieved by placing a wideband filter and a multi-band filter one on top of the other, wherein the bandwidth of the wideband filter is smaller than the bandwidths of the multi-band filter but wider than the bandwidth of each single band of the multiband filter.
7. The combined imaging and spectral measurement line-scan imaging sensor according to claim 6, wherein the wideband filters employed exhibit overlapping spectral sensitivity curves.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0008] The disclosed technique will be understood and appreciated more fully from the following detailed description taken in conjunction with the drawings in which:
[0009]
[0010]
[0011]
[0012]
[0013]
[0014]
[0015]
[0016]
[0017]
[0018]
DETAILED DESCRIPTION OF THE EMBODIMENTS
[0019] The disclosed technique overcomes the disadvantages of the prior art by providing a combined imaging and spectral measurement line-scan sensor array, which includes a plurality of sensor elements lines, each line including a plurality of sensor elements. The combined imaging and spectral measurement line-scan sensor array is integrated on a single semiconductor substrate. Herein, sensor elements are also referred as pixels. According to one alternative, a portion of the pixel lines are designated for acquiring an image, referred to herein as imaging lines while the remaining portion of the pixel lines are associated with spectral measurements and referred to herein as spectral measurement lines. According to another alternative, all of the pixel lines are imaging lines. Each imaging line acquires an image over a respective spectral band. The spectral bands may be mutually exclusive, partially overlapping or completely overlapping. As such, an image acquired by the imaging lines by a color image in a selected color space (e.g., Red, Green and BlueRGB, Cyan Magenta YellowCYM, XYZ and the like) as well as an image in the Short Wave Infrared (SWIR) and the Long Wave Infrared (LWIR) spectral bands or any combination thereof.
[0020] Each imaging line is associated with a respective spectral band referred to herein as the line spectral band. Each pixel in each spectral measurement line is associated with a respective spectral band referred to herein as the pixel spectral band. Each of multiple (e.g., of at least three, at least four, at least five etc.) pixels in each of spectral measurement lines is respectively associated with different respective pixel spectral bands. The different respective pixel spectral bands are non-identical to any one of the line spectral bands associated with each of the imaging spectral lines. In general, the line spectral bands are substantially larger (i.e., exhibit a larger bandwidth) than the pixel spectral band. Also, each spectral measurement line may be divided into a plurality of groups of adjacent pixels. Each group is associated with the same group spectral range and each pixel in the group is associated with a respective pixel spectral band.
[0021] Reference is now made to
[0022] Line 102.sub.3 is a spectral measurement line, for example, for measuring the spectrum of light received (e.g., reflected) from an object. Each one of pixels 104.sub.1-104.sub.N in line 102.sub.3 is associated with a respective one of pixel spectral bands B.sub.1-B.sub.N. Accordingly, a filter (e.g., a Fabry-Perot filter) exhibiting a response over the desired spectral band is placed over each one of pixels 104.sub.1-104.sub.N in lines 102.sub.3. It is noted that the term placed herein above and below relates to the physical association between a filter and respective pixel of group of pixels. In practice, for example, the filter or filters to be placed over pixels in an imaging sensor may be produced on a glass plate, covering the sensor area. The glass plate is then positioned over the sensor in alignment with the pixels. Also, the filter or filters may be directly deposited on the sensor itself. It is further noted that in
[0023] In general, within spectral measurement line 102.sub.3, each of multiple pixels 104.sub.1-104.sub.N is respectively associated with different respective spectral band (i.e., multiples of spectral bands B.sub.1-B.sub.N are different from each other). The different respective pixel spectral bands are non-identical to any one of the single spectral responses associated with each of the imaging spectral lines. Furthermore, these spectral bands need not be adjacent to each other (i.e., may not result in a single continuous band).
[0024] Optionally, as depicted in
[0025] It is noted that a combined imaging and spectral measurements line-scan sensor may include more than two imaging lines and more than one spectral measurement lines. For example, when acquiring a Cyan, Magenta, Yellow and Black (CMYK) image simultaneously with a spectral measurement of the light reflected of object being imaged, an imaging sensor according to the disclosed technique shall include at least five lines, four imaging lines and one spectral measurement line. Three imaging lines exhibit a spectral response corresponding to cyan, magenta and yellow (i.e., in the visible part of the spectrum) and the fourth imaging line exhibit a spectral response in the IR part of the spectrum from which the value of black is derived. The fifth line is a spectral measurement line similar to the spectral measurement line described above. Also, each spectral measurement line may be divided into a plurality of groups of adjacent pixels. Each group is associated with the same group spectral range and each pixel in the group is associated with a respective pixel spectral band.
[0026] Reference is now made to
[0027] Each of one imaging lines 152.sub.1, 152.sub.3 and 152.sub.5 is associated with a single respective line spectral response. To that end, a filter exhibiting a response in the desired spectral band is placed over the pixels in each line. In sensor 150, the spectral response associated with line 152.sub.1 is in the long visible band also referred to herein as red spectral band (e.g., between 380 nm and 490 nm). The spectral response associated with line 152.sub.3 is in the medium visible bands (e.g., between 490 nm and 610 nm) also referred to herein as green spectral bands. The spectral response associated with line 152.sub.3 is in the short visible band (e.g., between 490 nm and 720 nm) also referred to herein as blue spectral band.
[0028] Also in sensor 150, each one of spectral measurement lines 152.sub.2, 152.sub.4 and 152.sub.6 is divided into a plurality of groups of adjacent pixels. Spectral measurement line 152.sub.2 is divided into groups 154.sub.1-154.sub.M. Spectral measurement line 152.sub.4 is divided into groups 158.sub.1-158.sub.M and spectral measurement line 152.sub.6 is divided into groups 160.sub.1-160.sub.M. Each group in each spectral measurement line is associated with the same group spectral range. Thus, the spectral band associated with groups 154.sub.1-154.sub.M is between 600 nm and 710 nm. The spectral band associated with groups 158.sub.1-158.sub.M is between 500 nm and 610 nm and the spectral band associated with groups 160.sub.1-160.sub.M is between 400 nm and 510 nm.
[0029] Furthermore, the corresponding pixels in each group of pixels are associated with the same respective pixel spectral band. To that end, a filter (e.g., a Fabry-Perot filter) exhibiting a response in the desired spectral band is placed over each pixel. For example, pixels 154.sub.11, 154.sub.21, . . . , 154.sub.M1 are associated with the same spectral band (i.e., 600-620), pixels 158.sub.11, 158.sub.21, . . . , 158.sub.M1 are associated with the same spectral band (i.e., 500-520) and pixels 160.sub.11, 160.sub.21, . . . , 160.sub.M1 are associated with the same spectral band (i.e., 400-420). Similarly, pixels 154.sub.12, 154.sub.22, . . . , 154.sub.M2 are associated with the same spectral band (i.e., 610-630), pixels 158.sub.12, 158.sub.22, . . . , 158.sub.M1 are associated with the same spectral band (i.e., 510-530) and pixels 160.sub.12, 160.sub.22, . . . , 160.sub.M2 are associated with the same spectral band (i.e., 410-430) etc. In general, similar to as mentioned above, within at least one of spectral measurement lines 152.sub.2, 152.sub.4 and 152.sub.6 each of multiple pixels is respectively associated with different respective pixel spectral bands. The different respective pixel spectral bands are non-identical to any one of the single spectral responses associated with each of the imaging spectral lines.
[0030] Optionally, as depicted in
[0031] It is noted that spacing is required between the lines due to the uncertainty in the size of each pixel and filter regardless of the spectral response of the filters. For example, two adjacent pixels may exhibit width of 10 micrometers. However the filters placed over these pixels may exhibit widths different from 10 micrometers (e.g., due to manufacturing tolerances). As such, there is a probability that the coverage of a filter associate with one pixel overlaps adjacent pixels. Therefore, employing spacing such as described above alleviates such an uncertainty and result in a one to one correspondence between a filter and corresponding pixel or pixels. Nevertheless, when the process employed during manufacturing of an imaging sensor of the disclosed technique results in a sufficiently low probability that the coverage of a filter associated with one pixel would overlap adjacent pixels, then the use of metal strips or spacing may not be necessary. For example, the process employed may result in a probability of 1 percent that a filter shall overlap with a neighboring pixel by at most 100 nanometers. The designer may decide that with such probability and overlap, the performance of the sensor (e.g., Signal to Noise RatioSNR) would not be affected such that the sensor is rendered un-usable. As such, the designer may decide that opaque strips or spacing are not necessary.
[0032] Reference is now made to
[0033] Line 202 is an imaging line associated with the red spectral band. Accordingly, each of the pixels in line 202 includes a respective filter (e.g., a red dichroic filter). Line 204 is an imaging line associated with the green spectral band. Accordingly, each of the pixels in line 204 includes a respective filter (e.g., a green dichroic filter). Lines 206.sub.1 and 206.sub.2 are imaging lines associated with the blue spectral band. As such, similar to lines 202 and 204, each of the pixels in lines 206.sub.1 and 206.sub.2 includes a respective filter (e.g., a blue dichroic filter). When employed for line scanning (similarly to as explained below in conjunction with
[0034] Optionally, an opaque strip such as metal strip 210 is positioned between line 202 and 204. This metal strip prevents light from the filters located over the pixels in line 202 to be received by the pixels in line 204. Also optionally, line 204 and line 206.sub.1 are separated with a combination of a metal strip 211 and two gaps W1 between line 204 and metal strip 211 and a gap W2 between metal strip 211 and line 206.sub.1. W2, separate line 206.sub.2 and line 208.sub.1. Similar to as described above, a gap and a metal strip or a combination thereof have the same functionality of preventing light from the filters located over the pixels in one line to be received by the pixels in an adjacent line. It is noted that no spacing exists between lines 206.sub.1 and 206.sub.2 and between lines 208.sub.1 and 208.sub.2 since the pixels in these lines are designated to receive the same spectral band.
[0035] Spectral measurement lines 208.sub.1 and 208.sub.2 are divided into a plurality of groups 212.sub.1-212.sub.M of adjacent pixels. In the example depicted in
[0036] Similar to as described above, in general, within spectral measurement lines 208.sub.1 and 208.sub.2 each of multiples of vertically adjacent pixels 214.sub.1, 214.sub.2, 214.sub.3, . . . , 214.sub.N are respectively associated with different respective spectral bands. The different respective spectral bands are non-identical to any one of the single spectral responses associated with each of the imaging spectral lines. In other words, at least two pairs of vertically adjacent pixels 214.sub.1, 214.sub.2, 214.sub.3, . . . , 214.sub.N is each associated with a different respect spectral band. It is noted that pairs of vertically adjacent pixels are brought herein as an example only, according to the disclosed technique, triplets, quadruplets etc. may be similarly employed.
[0037]
[0038] Reference is now made to
[0039] Line-scan sensor 230 is similar to line-scan sensor 200 however with differences described below. In sensor 230, Lines 232, 234, 236.sub.1, 236.sub.2 are imaging lines and lines 238.sub.1 and 238.sub.2 are spectral measurement lines. In
[0040] Line 232 is an imaging line associated with the red spectral band. Accordingly, each of the pixels in line 232 includes a respective filter (e.g., a red dichroic filter). Line 234 is an imaging line associated with the green spectral band. Accordingly, each of the pixels in line 234 includes a respective filter (e.g., a green dichroic filter). Lines 236.sub.1 and 236.sub.2 are imaging lines associated with the blue spectral band. As such, similar to lines 232 and 234, each of the pixels in lines 236.sub.1 and 236.sub.2 includes a respective filter (e.g., a blue dichroic filter). When employed for line scanning (similarly to as explained below in conjunction with
[0041] Optionally, an opaque strip such as metal strip 240 is positioned between line 232 and 234. This metal strip prevents light from the filters located over the pixels in line 232 to be received by the pixels in line 234. Also optionally, a gap, W1, separates line 234 and line 236.sub.1 and a gap, W2, separates line 236.sub.2 and line 238.sub.1. Similar to as described above, a gap and a metal strip or a combination thereof have the same functionality of preventing light from the filters located over the pixels in one line to be received by the pixels in an adjacent line. It is noted that no spacing exists between lines 236.sub.1 and 236.sub.2 and between lines 238.sub.1 and 238.sub.2 since the pixels in these lines are designated to receive the same spectral band.
[0042] Spectral measurement lines 238.sub.1 and 238.sub.2 are divided into a plurality of groups 242.sub.1-242.sub.M of adjacent pixels. In the example depicted in
[0043] Similar to as described above, in general, within spectral measurement lines 238.sub.1 and 238.sub.2 at least a group of four pixels 244.sub.1, 244.sub.2, 244.sub.3, . . . , 244.sub.N and a second group of four pixels 244.sub.1, 244.sub.2, 244.sub.3, . . . , 244.sub.N are respectively associated with a first spectral band and a second spectral band. The first spectral band is different from the second spectral band. In other words, at least two groups of four pixels 244.sub.1, 244.sub.2, 244.sub.3, . . . , 244.sub.N is each associated with a different respect spectral band.
[0044] Reference is now made to
[0045] Optionally, as depicted in
[0046] The arrangement of lines 252.sub.1-252.sub.6, with respect to the line spectral bands thereof is brought herein as an example only. As another example the line spectral band associated with line 252.sub.1 is between 400 nm and 540 nm. The line spectral band associated with line 252.sub.2 is between 560 nm and 700 nm. The line spectral band associated with line 252.sub.3 is between 600 nm and 740 nm. The line spectral band associated with line 252.sub.4 is between 450 nm and 590 nm. The line spectral band associated with line 252.sub.5 is between 500 nm and 640 nm. The line spectral band associated with line 252.sub.6 is between 360 nm and 500 nm
[0047] In general, the complexity, and consequently the cost of a combined imaging and spectral measurement line-scan sensor, increases with the number of different filters employed (i.e., with respect to spectral response to the filter). In other words, the complexity increases as the number different filters exhibiting a different spectral response increases. As such, it would be advantageous to decrease the number of filters employed in a given system. Reference is now made to
[0048]
[0049]
[0050]
[0051] For the purpose of explanation, and as mentioned above, filters exhibiting a spectral response such as spectral response 306, 308 and 310 shall be referred to herein as multi-narrowband filters. Also, the bandwidths, .sub.R41, .sub.R42, .sub.R43 and .sub.R44, of each spectral band 306.sub.1, 306.sub.2, 306.sub.3 and 306.sub.4, are smaller than the bandwidth .sub.R4 of the spectral response 306 of the filter. Similarly, each of the bandwidths, .sub.R51, .sub.R52, .sub.R63 and .sub.R54, of each spectral band 308.sub.1, 308.sub.2, 308.sub.3 and 308.sub.4, are smaller than the bandwidth .sub.R5 of the spectral response 310 of the filter, and the bandwidths, .sub.R61, .sub.R62, .sub.R63 and .sub.R64, of each spectral band 310.sub.1, 310.sub.2, 310.sub.3 and 310.sub.4, is smaller than the bandwidth .sub.R6 of the spectral response 310 of the filter.
[0052] According to the embodiments of the disclosed technique described herein above in conjunction with
[0053] As mentioned above, according to one example, the filter exhibiting response 300, 302 and 304 are RGB filters, where the filter exhibiting response 300 is associated with the color blue (e.g., a blue dichroic filter), the filter exhibiting response 302 is associated with the color green (e.g., a green dichroic filter), the filter exhibiting response 304 is associated with the color red (e.g., a red dichroic filter). In general, such filters are commonly employed in color imaging sensors. As such, employing such filters, along with additional filters which exhibit responses similar to responses 306, 308 and 310 (
[0054] The spectral responses depicted in
[0055] Reference is now made to
[0056] Filters 352, 354, 356, 358, 360, 364, 364, 366 and 368 are positioned over respective pixels (not shown) on sensor 350. A filter 370 is placed over green filter 352, red filter 358, blue filter 364 and over pixel 376 (i.e., the space between pixel 376 and filter 370 is clear). Filter 370 exhibits, for example a spectral response similar to spectral response 306 (
[0057] A metal strip 382 is placed between the pixels corresponding to filters 364, 366 and 368 and pixels 376, 378 and 380. An opaque section 384 is placed between filter 370 and filter 372 and an opaque section 386 is placed between filter 372 and filter 374. A gap W.sub.v1 exists between green filter 352 and red filter 358, between green filter 354 and red filter 360, between green filter 356 and red filter 362. A gap W.sub.v2 exists between red filter 358 and blue filter 364, between red filter 360 and red blue 366 and between red filter 362 and blue filter 368. Similar to as mentioned above gaps W.sub.v1 and W.sub.v2 prevents light received by one pixel to be received by an adjacent pixel. Also similar to as mentioned above, either one of gaps W.sub.v1 and W.sub.v2 may be replaced with a metal strip or an opaque material suitable to be fabricated on a substrate of a sensor such as sensor 350. In the example brought forth above in
[0058] Sensor 350 may be employed, for example, for acquiring spectral measurements in the visible spectral band as well as in the IR band. With reference to
[0059] Similarly, pixel 378 receives energy over spectral ranges .sub.R51, .sub.R52, .sub.R53 and .sub.R54. Spectral ranges .sub.R51, .sub.R52, .sub.R53 are in the visible spectral band and spectral range .sub.R54 is in the IR band. The pixel corresponding to filter 354 receives energy in the spectral range .sub.R51 (i.e., filter 354 filters out spectral ranges .sub.R52, .sub.R53 and .sub.R54). The pixel corresponding to filter 360 receives energy in spectral range .sub.R52 (i.e., filter 360 filters out spectral ranges .sub.R51, .sub.R53 and .sub.R54). The pixel corresponding to filter 366 receives energy in spectral range .sub.R53 (i.e., filter 366 filters out spectral ranges .sub.R51, .sub.R52 and .sub.R54). The energy received over spectral range .sub.R54 is a function of the energy received by each of the pixels corresponding to filters 354, 360 and 366 and the energy received by pixel 378.
[0060] Further similarly, pixel 380 receives energy over spectral ranges .sub.R61, .sub.R62, .sub.R63 and .sub.R64. Spectral ranges .sub.R61, .sub.R62, .sub.R63 are in the visible spectral band and spectral range .sub.R64 is in the IR band. The pixel corresponding to filter 356 receives energy in spectral range .sub.R61 (i.e., filter 356 filters out spectral ranges .sub.R62, .sub.R63 and .sub.R64). The pixel corresponding to filter 362 receives energy in over spectral range .sub.R62 (i.e., filter 362 filters out spectral ranges .sub.R61, .sub.R63 and .sub.R64). The pixel corresponding to filter 368 receives energy in spectral range .sub.R63 (i.e., filter 368 filters out spectral ranges .sub.R61, .sub.R62 and .sub.R64). The energy received over spectral range .sub.R64 is determined as a function of the energy received by each of the pixels corresponding to filters 356, 362 and 368 and the energy the received by pixel 380. Thus sensor 350 acquires an image over all of spectral ranges .sub.1, .sub.2, .sub.3, .sub.4, .sub.5, .sub.6, .sub.7, .sub.8, .sub.9, .sub.10, .sub.11 and .sub.12.
[0061] As mentioned above, the spectral responses of the filters should be designed according to design specifications and requirements. Such specification and requirements include, for example, overlapping of the transmittance spectral response between spectrally adjacent filters, the spectrum of the light illuminating the object, the inherent quantum efficiency (i.e., relative signal generated by light at each wavelength) of each pixel and the quantization resolution. Reference is now made to
[0062] With reference to
[0063] Spectral sensitivity curve 412.sub.3 is between wavelength 6.5 and 7.5, spectral sensitivity curve 410.sub.2 is between wavelength 4 and 5 and spectral sensitivity curve 412.sub.1 is between wavelength 1.5 and 2.5 (i.e., mutually exclusive with reflectance curve 406). However, since the value of reflectance curve 406 between wavelengths 4 and 5 is 0.5, the value of the reflectance curve 406, as would be determined by a filter exhibiting spectral sensitivity curve 412.sub.2 would have been 0.5. Therefore, the values generated by pixels covered with filters exhibiting sensitivity curves such as sensitivity curves 412.sub.1, 412.sub.2 and 412.sub.3 and receiving light exhibiting reflectance curve 406 are also [0.00, 0.50, 1.00]. Employing a 4-bit quantization analog to digital conversion both system results in quantized values of [0, 8, 15] representing reflectance curve 404 as well as reflectance curve 406. Thus, it would have been impossible to discern between reflectance curve 404 and reflectance curve 406 when employing filters which exhibit non-overlapping spectral sensitivity curves.
[0064] With reference to
[0065] The values generated by pixels covered with filters exhibiting sensitivity curves such as sensitivity curves 414.sub.1, 414.sub.2 and 414.sub.3 and receiving light exhibiting reflectance curve 404 are [0.00, 0.50, 1.00]. As above, employing 4-bit quantization analog to digital conversion will result in quantized values of [0, 8, 15] representing reflectance curve 404. However, the values generated by pixels covered with filters exhibiting sensitivity curves such as sensitivity curves 416.sub.1, 416.sub.2 and 416.sub.3 and receiving light exhibiting reflectance curve 406 are [0.1, 0.40, 0.9] representing reflectance curve 406. Employing 4-bit quantization analog to digital conversion will result in quantized values of [2, 6, 15]. The differences between the quantized pixel values of reflectance curve 404 and reflectance curve 406 is enough to sufficiently discern therebetween even is with an increase in the system noise.
[0066] With reference to
[0067] The values generated by pixels covered with filters exhibiting sensitivity curves such as sensitivity curves 418.sub.1, 418.sub.2 and 418.sub.3 and receiving light exhibiting reflectance curve 404 are [0.00, 0.50, 1.00]. As above, employing 4-bit quantization analog to digital conversion will result in quantized values of [0, 8, 15] representing reflectance curve 404. However, the values generated by pixels covered with filters exhibiting sensitivity curves such as sensitivity curves 420.sub.1, 420.sub.2 and 420.sub.3 and receiving light exhibiting reflectance curve 406 are [0.01, 0.45, 1.0] representing reflectance curve 406. Employing 4-bit quantization analog to digital conversion will result in quantized values of [0, 7, 16]. Although the differences between the quantized pixel values of reflectance curve 404 and reflectance curve 406 is enough to sufficiently discern therebetween any increase in noise may render these two curves indiscernible. Increasing the quantization resolution (e.g., 8-bit, 12-bit etc.) shall result in a larger difference between the quantized values of reflectance curves 404 and reflectance curve 406.
[0068] The description hereinabove in conjunction with
[0069] As mentioned above, a combined spectral measurement and imaging line-scan sensor according to the disclosed technique may be employed in a line scan camera. Such combined imaging and spectral measurement line-scan cameras may be employed in a printing press for either image acquisition, color measurement & control or inspection functionality. Reference is now made to
[0070] Typically, the size of color targets 510.sub.1-510.sub.6 are on the order of several millimeters square (e.g., 4 millimeters by 4 millimeters). Typically, the size of a magnified pixel (i.e., the size of a pixel in the field of view on the web) is on the order of tens to hundreds of micrometers. Thus, with reference to the example brought forth in
[0071] During the print run, image 506 and color targets 510.sub.1-510.sub.6 pass in front of camera 500 and camera 500 acquires a plurality of combined line images and spectral measurement. Camera 500 provides these combined line images and spectral measurement to processor 502. Processor 502 renders a two dimensional image (e.g., an RGB image) of the entire substrate width from images acquired by the imaging lines of sensor 501. Processor 502 may employ this two dimensional image to locate color targets 510.sub.1-510.sub.6 in the image. Processor 502 then employs the location of color targets 510.sub.1-510.sub.6 in the two dimensional image to determine the spectral measurement information associated with each of color targets 510.sub.1-510.sub.6 from the corresponding pixels or groups of pixels in the spectral measurement lines of sensor 501. In essence, the spectral measurement information provides the spectral response of each of color targets 510.sub.1-510.sub.6. Accordingly, processor 502 may determine the color associated with each of color targets 510.sub.1-510.sub.6 in a selected color space (e.g., CIEL*a*b*, CIEL*u*v* and the like). The processor 502 may employ the two dimensional image to determine further press parameters such as pressure.
[0072] It will be appreciated by persons skilled in the art that the disclosed technique is not limited to what has been particularly shown and described hereinabove. Rather the scope of the disclosed technique is defined only by the claims, which follow.