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Image-Based Separation of Reflective and Fluorescent Components Using Illumination Variant

Image-Based Separation of Reflective and Fluorescent Components Using Illumination Variant
Image-Based Separation of Reflective and Fluorescent Components Using Illumination Variant

Image-Based Separation of Reflective and Fluorescent Components Using Illumination Variant and Invariant Color

Cherry Zhang and Imari Sato,Member,IEEE

Abstract—Traditionally,researchers tend to exclude fluorescence from color appearance algorithms in computer vision and image processing because of its complexity.In reality,fluorescence is a very common phenomenon observed in many objects,from gems and corals,to different kinds of writing paper,and to our clothes.In this paper,we provide detailed theories of fluorescence

phenomenon.In particular,we show that the color appearance of fluorescence is unaffected by illumination in which it differs from ordinary reflectance.Moreover,we show that the color appearance of objects with reflective and fluorescent components can be represented as a linear combination of the two components.A linear model allows us to separate the two components using images taken under unknown illuminants using independent component analysis(ICA).The effectiveness of the proposed method is

demonstrated using digital images of various fluorescent objects.

Index Terms—Reflectance components separation,fluorescence emission,diffuse reflection,illumination

?

1I NTRODUCTION

I N the field of computer vision,recognizing objects and patterns by their color has always been a difficult problem because the color appearance of objects varies dramatically with surrounding illumination.Researchers in computa-tional color constancy proposed many algorithms and models to discount the effect of illumination and recover the true color of objects[1],[8],[4].Researchers in image reproduction and realistic rendering strive to accurately predict the color of objects under arbitrary illuminants. While the algorithms and techniques compute color appearance differently,they share one common assump-tion:None of the objects in the scene exhibit fluorescence. Fluorescence is the emission of visible light by objects that are exposed to a source light covering the ultraviolet range, (e.g.,sunlight and UV light).In reality,fluorescence is a very common phenomenon observed in many objects,from gems and corals,to different kinds of writing paper,and to our clothes(Fig.1).Through intensive studies on color constancy algorithms,Barnard concluded that fluorescent surfaces are common and present in20percent of randomly constructed scenes[3].Therefore,to handle color accurately, computer vision and image synthesis algorithms ought to take fluorescence into account.

By experimentation,we discovered that a composite object with both ordinary reflective and fluorescent compo-nents has the color appearance that is the sum of the two components interacting with illumination differently.To handle the two components correctly,it is necessary to separate them.This motivated us to develop a method for separating fluorescence from reflectance.Assume,in an ordinary color camera,the color of a generic pixel p c on the captured image is a linear contribution

p c?a c p c;Otb c p c;F;e1Twhere c?f R;G;B g,p c;O and p c;F are the color of the ordinary reflective and fluorescent components.Here,we assume that each surface point corresponding,i.e.,each pixel,contains single fluorescent components.Let a c and b c be the coefficients to represent the amount of contribution from each component to the pixel color p c.a c and b c depend on the interactions between each component and the light source that illuminates the object.Since we do not know the illumination condition under which p c is taken,we need to solve for p c;O and p c;F when only the pixel colors,p c,are known.To make this hard problem solvable,we assume that the reflective and fluorescent components of an image are statistically independent.The assumption is reasonable because,in the absence of image interpretation,the spatial distribution of fluorescent component provides no predic-tion on the spatial distribution of the reflective component. Based on the linear contribution model,we show that given the complete set of pixels f p c g for two images taken under different illuminants,p c;O and p c;F can be effectively recovered using independent component analysis(ICA).

This paper describes an attempt at separating the reflective and fluorescent components of an image.It makes the following contributions in the area of realistic color imaging:

.Providing a theory of fluorescent phenomenon.

.Showing that the color of a fluorescent surface is not affected by the color of its illuminant,in which it

differs from an ordinary reflective surface.

. C.Zhang is with Goldman Sachs.

.I.Sato is with the National Institute of Informatics,2-1-2Hitotsubashi,

Tokyo101-8430,Japan.E-mail:imarik@nii.ac.jp.

Manuscript received2Mar.2012;revised1Aug.2012;accepted16Sept.

2012;published online28Nov.2012.

Recommended for acceptance by P.Felzenszwalb,D.Forsyth,P.Fua,and

T.E.Boult.

For information on obtaining reprints of this article,please send e-mail to:

tpami@https://www.wendangku.net/doc/fb9941873.html,,and reference IEEECS Log Number

TPAMSI-2012-03-0159.

Digital Object Identifier no.10.1109/TPAMI.2012.255.

0162-8828/13/$31.00?2013IEEE Published by the IEEE Computer Society

.Proposing a method for separating the reflective and fluorescent components of an image using ICA,and

an improved method for relighting images under an

arbitrary illuminant.

The remainder of the paper is structured as follows: Section2summarizes earlier research in color constancy, color appearance,and rendering algorithms for fluorescent surfaces,as well as research in image separation.Section3 presents the theories and experimental results explaining how fluorescent surfaces interact with illuminants.Our algorithm and the results for separating ordinary reflective and fluorescent components of an image are presented in Sections4and5.Section6demonstrates the effectiveness of separating ordinary reflective and fluorescent components of an image for relighting scenes.In the conclusion,we discuss issues and future directions of our research.

2R ELATED W ORK

The color appearance of nonfluorescent surfaces has always been the main focus of color-related computer vision algorithms.For example,in computational color constancy, researchers attempt to recover the“true color”of objects under a reference illuminant[1],[8].The true color is then modified to predict the appearance of objects under other illuminants.Barnard et al.studied and compared existing color constancy algorithms by evaluating their performance with a large set of test images[4].Some of the test images contain fluorescent objects,but all of the evaluated color constancy algorithms treat them as ordinary objects.

Later on,researchers realized that assuming all objects are nonfluorescent greatly limits the accuracy of color algorithms because many objects around us exhibit fluores-cence.What makes fluorescence different from ordinary reflection is the transfer of energy from one wavelength to another:fluorescent materials absorb light at a certain wavelength and then re-emit it at other wavelengths, whereas ordinary reflective components reflect light at the same wavelength as incident.Glassner first incorporated the wavelength-shifting property of fluorescence into Kajiya’s rendering equation[10].In Johnson and Fairchild’s research,they provided brief explanations of fluorescence,and extended spectral rendering algorithms to take fluorescence into account[14].Later,Wilkie et al.proposed to render fluorescent emissions as diffuse reflections with a wave-length-shifting property,i.e.,a diffuse surface that reflects light at a wavelength different from the incident one[24].

Hullin et al.proposed new ways to model and render fluorescent objects by acquiring their bispectral bidirec-tional reflectance and reradiation distribution functions and the results showed significant improvement in fluorescent object modeling[12].Furthermore,Barnard proposed ways to improve color constancy algorithms to include spectral data of several fluorescent materials[3].Although Barnard solved some problems by including fluorescent objects in color constancy algorithms,his work was mainly based on experimental measurements.His paper did not provide comprehensive models for fluorescent surfaces.In our paper,we extend Barnard’s research by providing more detailed theories and accurate models for fluorescence.

To accurately predict the appearance of composite objects with both reflective and fluorescent components,it is important to separate the two components.Research in natural science[20]shows necessary procedures for measuring color of fluorescent materials in the spectral domain using optical devices.For example,Haneishi and Kamimura used spectral data taken under multiple light sources under known spectral distributions for characteriz-ing fluorescent samples[15].Alterman et al.separated the appearance of each fluorescent dye from a mixture by unmixing multiplexed images[2].

Nakajima and Tominaga used statistics of fluorescent materials to estimate fluorescent components of real material using multispectral images seen under sunlight [17].Recently,Tominaga et al.proposed a method for estimating the spectral radiance factor of fluorescent objects by using an imaging system consisting of a multiband camera and ordinary light sources[22].In the early stage of our research,we successfully separated the components of fluorescent sheets using spectral data captured by a spectrometer.The successful results motivated us to develop a more practical system for doing the separation using images taken by an ordinary digital camera.

The computer vision community has several methods for separating components of an image[18],[23].Some algo-rithms separate specular reflections from diffuse reflections. Some algorithms separate noncorrelated components of images.For example,Farid and Adelson proposed a method for separating a painting from the reflection of an observer on the glass in front of the painting,using two images[7].

Through the research of fluorescence microscopy,several separation techniques were developed for separating the spectra and concentration of fluorescent materials simulta-neously from given a hyperspectral image[11].Neher et al. proposed an algorithm based on nonnegative matrix factorization(NMF)for estimating the concentration of multiple fluorescence dyes of an image[19].Neher et al. concluded that NMF was very effective when there is little overlap between spectra of fluorescence materials and their concentration varies in the image.In our case,some overlap between reflective and fluorescent components in an image

Fig.1.Examples of fluorescent objects:gems bouncy balls,banana peel,and fluorescent sheets.

is expected,and thus NMF might not be effective.We found that Farid and Adelson’s problem closely resembles the fluorescence-separation problem we are interested in.More specifically,we assume that the reflective and fluorescent components of an image are statistically independent.The assumption is reasonable because,in the absence of image interpretation,the spatial distribution of fluorescent com-ponent provides no prediction on the spatial distribution of the reflective component.From this,an approach based on ICA is used in our case for separating reflective and fluorescent components.Gobinet et al.also suggested the use of ICA for estimation the concentrations of fluorescent materials[11].

3P ROPERTIES OF F LUORESCENT S URFACES

We start by looking at what fluorescence is.Most typical fluorescent material absorbs light in the near ultraviolet(UV) range from200nm to380nm,and re-emit visible light in 380nm to720nm.Some material absorbs short-wavelength visible light and re-emit longer wavelength visible light.The first type of special UV lights are not required to observe fluorescence because many natural lightings,such as day-light and cool fluorescent light,have strong UV components (Fig.2).After decades of studies,researchers can explain fluorescence phenomenon and two unique properties of fluorescent materials with concepts in quantum theory[6], [20]:Fluorescent material always emits light at longer wavelengths than the absorbed light,and the emission spectra of each fluorescent material always have the same frequency distribution(e.g.,shape)regardless of the spectra of incident light.

Due to their unique properties,the appearance of fluorescent surfaces must be computed differently than the reflective surfaces.The color of a reflective surface depends only on the illuminant and its reflectance.For example,the observed spectrumèe Tof a nonfluorescent object under illuminant I is

èe T?Ie TRe T;e2Twhere Ie Tis the spectrum of the illuminant and Re Tis the reflectance of the object at wavelength .

Fluorescent objects interact with illuminants differently than nonfluorescent objects.1Based on the molecular physics of fluorescent objects,researchers in computer graphics developed algorithms for rendering fluorescent objects[21],[14].For a pure fluorescent surface,the observed spectrum depends on the illuminant,the material’s excitation spectrum,and the emission spectrum. The excitation spectrum of a fluorescent object shows how much energy from the illuminant is absorbed at each wavelength;it is a function of the wavelength of the illuminant.For each wavelength in an excitation spectrum, there is a corresponding emission spectrum that shows the frequency distribution and intensity of the emitted light. Usually the emission spectrum is a function of wavelength in the visible range.The frequency distribution of all emission spectra is constant,but the intensity varies.

The properties of fluorescent objects are well shown with experimental results.Fig.3a shows the measured emission spectra of a red-orange fluorescent sheet.Each colored spectrum corresponds to the illuminant at different wavelengths,and they have the same frequency distribu-tion as one another.2Figs.3b and3c show the normalized3 excitation(dotted line)and emission(solid line)spectra of the red-orange and green-yellow fluorescent sheets,respec-tively.From the emission spectrum we can see that the red-orange sheet appears reddish orange when it is illuminated by light in the range of380nm to650nm(Fig.3b).We can also see that the green-yellow exhibits strong fluorescence only for illuminants with much energy between450nm and525nm(Fig.3c).

To obtain the observed spectrum of a pure fluorescent surface,we must consider the overall contribution from its illuminant,excitation,and emission.Suppose the illuminant is I and its intensity at wavelength i is Ie iT.Let K and J represent the normalized excitation and emission spectrum, respectively.Then the observed spectrum,èe ; iT,result-ing from the illuminant at i is

èe ; iT?Ie iTK0e iTJe T;e3Twhere

K0e iT

Ke iT

R

Ke iTd i

is the relative intensity of the excitation caused by the illuminant at wavelength i.Since Ie iTK0e iTis a scalar,all èe ; iTs have the same shape as Je T.Considering the illuminant at all wavelengths,the overall observed spec-trum is computed by summing upèe ; iTs for all wavelength i,i.e.,

èe T?

Z

Ie iTK0e iTd i

Je T:e4T

Note that the range of i depends on the illuminant,and the range of is the range of the observed light we wish to measure.

3.1Mechanism of Fluorescence

The fluorescence phenomenon is explained by theories in molecular physics[16](Fig.4).Initially,the molecules of a fluorescent object are structured as a lattice in equilibrium in the ground energy state A.When the lattice is irradiated

Fig.2.Natural daylight and a fluorescent lamp both have strong UV and short-wavelength components.

1.Section 3.1describes the fluorescence phenomena by theories in molecular physics.

2.Here,the differences in the long wavelength are caused due to the measurement noise that does not reappear in other measurements.

3.Spectral power distribution is normalized so that the minimum intensity is0and the maximum intensity is1.0.

with incident light,the electrons are excited from the ground state A to a higher energy state B .After the transition,a rearrangement of the ions in the lattice takes place and the system assumes an equilibrium state C .Some energy is dissipated within the lattice during the transition from B to C .From the equilibrium state C ,light is emitted when electrons drop back to the ground state D .From D ,the structure of the lattice is rearranged again to reach the stable equilibrium ground state A .The lifetime of the excitation from state A to state B is 105times longer than the period of lattice rearrangement (B to C ).Thus,no matter how the electrons reach the excited state B ,the system comes to an equilibrium state (C )before emission.This implies that the intensity of the emitted spectra of a fluorescent object depends on the incident light,but the frequency distribution does not.

A nonfluorescent object absorbs photons and the elec-trons in the molecules are excited to a higher energy level but immediately drop back to the original energy state,releasing energy in the form of emitting a photon of equal wavelength.

3.2

Spectrum of Composite Object with Both Ordinary Reflective and Fluorescent Components

Many objects we see every day are neither pure reflective nor pure fluorescent,they are composites of ordinary reflective and fluorescent components.We measured the spectrum of a composite object under the illuminant at different wavelengths.Fig.5shows a typical setup of the experiment.The equipment needed is spectrometer,light source (lamp),and monochromator.The spectrometer is used to measure object’s spectrum.The light source covers both UV and visible light range (e.g.,Xe lamp).The monochromator is used to filter the light source to obtain illumination at a single wavelength.

Fig.6a shows the overall change in the observed spectrum of such object.Each colored line represents the observed spectrum corresponding to the illuminant at a particular wavelength.When the wavelength of the illuminant falls in the UV range or the high-energy range of the object’s excitation spectrum,the fluorescent component dominates;thus we observe fluorescence only (Fig.6b).When the wavelength of the illuminant falls in the visible light range,we observe a mixture of fluorescence and reflectance (Fig.6c).When the illuminant is in the low-energy range of visible light

Fig.

4.Energy-level diagram illustrating

fluorescence.

Fig.3.Measured excitation and emission spectra of fluorescent sheets.

Fig.5.Setup of the experiment.

and falls outside of the excitation spectrum,fluorescence diminishes and we only observe reflectance(Fig.6d).

Clearly,an object’s reflective and fluorescent compo-nents behave significantly differently.In the next section, we will show a unique property of the fluorescent component,and present our findings on how it interacts with illuminants differently from the reflective component.3.3Constant Chromaticity

The most intriguing property of fluorescence we discovered is that the emission spectrum of a fluorescent surface is,up to a constant,independent of its illuminant.Thus,fluor-escent surfaces have constant chromaticity when the illumination condition varies.The proof of this property can be shown mathematically.We can compute the tristimulus values of a fluorescent surface from(4)as

X?

Z

Ie iTK0e iTd i

Z

"xe TJe Td ;e5TY?

Z

Ie iTK0e iTd i

Z

"ye TJe Td ;e6TZ?

Z

Ie iTK0e iTd i

Z

"ze TJe Td ;e7T

where"xe T;"ye T;"ze Tare the CIE color matching functions that specify the“unit amount”of tristimulus values at each wavelength, i is integrated over the range of the illuminant wavelength, is integrated over the range of visible light wavelength(380nm to720nm),and K0e iTis defined in(3).Let

X0?

Z

"xe TJe Td ;e8T

Y0?

Z

"ye TJe Td ;e9T

Z0?

Z

"ze TJe Td e10T

be the reference tristimulus values of the normalized emission spectrum J.Substituting(8)-(10)into(5)-(7),we have X?kX0,Y?kY0,and Z?kZ0with k?

R

Ie iTK0e iTd i. Note that k is a scalar and its value depends on the spectral power distribution of the illuminant and the excitation spectrum.

Now,define reference chromaticities as

x0?

X0

X0tY0tZ0

;

y0?

Y0

X0tY0tZ0

:

Then the x-chromaticity of the object under an arbitrary illuminant becomes

x?

X

XtYtZ

?

kX0

kX0tkY0tkZ0

?

X0

X0tY0tZ0

?x0:

e11T

Similarly,y?y0.Thus,the chromaticity of the fluorescent material is independent of both the illuminant and excita-tion spectrum;it only depends on the emission spectrum.

The claim of constant chromaticity was verified with experiments.The chromaticities of eight fluorescent and

Fig.6.Observed spectra of fluorescent sheet containing both reflective and fluorescent components.

nonfluorescent surfaces (Fig.7)were measured under 16different illuminants using a spectrometer.The illumi-nants include four CIE standard daylights,five indoor lights,and six colored illuminants whose chrominances were randomly chosen (Fig.8).Table 1shows the correlated color temperatures (CCT)of the CIE standard daylights and indoor lights.

Figs.9and 10show the chromaticities versus illuminants plots of the experiments.The color of each line corresponds to the color of a test surface under white light.The plots show that as illuminants change,the chromaticities of fluorescent surfaces do not change as dramatically as reflective surfaces.Table 2provides a more quantitative comparison.Under standard daylights,both the x -and y -chromaticities of nonfluorescent surfaces on average vary twice as much as fluorescent surfaces.Table 3shows that under random

colored illuminants,the variation in x -chromaticities of nonfluorescent surfaces is twice as much as fluorescent surfaces,and the y -chromaticities varies more than five times.The average euclidean distances of the fluorescent red-orange and yellow-orange surfaces are so small that a human cannot detect those color changes (for reference,see MacAdam ellipses).

The fluorescent green-yellow surface has a greater variance than red-orange and yellow-orange surfaces because its reflective component is more prominent than other fluorescent surfaces and its excitation spectrum also covers a narrower wavelength range;it exhibits strong fluorescence only for illuminants with energy between 450nm and 525nm (Fig.3c).Some colored illuminants in the experiments have weaker intensity in the 450nm to 520nm range.Therefore,a fluorescent green-yellow surface

Fig.7.Fluorescent and nonfluorescent

test surfaces.Left

to

right:red-orange,green-yellow,yellow-orange,cyan,yellow,red,green,purple.

Fig.8.Illuminants used in verifying constant chromaticity.

Descriptions and CCT’s of CIE Standard

Illuminants

Fig.9.x -chromaticities (top)and y -chromaticities (bottom)plots for test surfaces under various illuminants.

has a greater variance in color change due to its reflective component than red-orange and yellow-orange surfaces.Another interesting observation is that fluorescent surfaces tend to show higher saturation and lightness values than nonfluorescent surfaces.This observation is consistent with the psychophysical study by Fujine et al.that suggests that high-saturation and high-lightness surfaces are perceived as fluorescent [9].

The property of having constant chromaticity gives us a great way to distinguish fluorescence from reflectance.In the next section,a method for separating fluorescence from reflectance is presented.

4

S EPARATING R EFLECTIVE AND F LUORESCENT C OMPONENTS OF AN I MAGE

A regular charged-couple device (CCD)camera has three color channels:Red (R),Green (G),and Blue (B).When we take an image of composite objects with both ordinary reflective and fluorescent components using a CCD camera,the color of the pixel p c for each channel c ?f R;G;

B g is the sum of the color for reflective component p c;O and fluorescent component p c;F .That is,

p c ?p c;O tp c;F :

e12T

As mentioned before,the proposed approach assumes single fluorescent component for each surface point:(12)is not valid for a surface point made of multiple fluorescent components.

The color of a reflective component is computed as

p c;O ?Z

"c e TI e TR e Td ;e13Twhere "c

e Tis the response curve of channel c for the CCD camera. is integrated over the range of visible light.

The color of the fluorescent component can be computed from (4)as

p c;F ?Z I e i TK 0

e i Td i Z

"c e TJ e Td :e14TSubstituting (13)and (14)to (12),we have

p c ?Z

"c

e TI e TR e Td t

Z

I e i TK 0e i Td i

Z

"c e TJ e Td :e15T

We assume that the responses of a CCD camera have

fairly narrow bandwidth,that is,light goes through the camera at a particular wavelength to reach the sensor [5].The narrowband assumption is often used in color con-stancy algorithms,so we can simplify (15)as

TABLE 2

Variations in the Chromaticities under CIE Standard Daylights and Indoor

Lights

Variations in the Chromaticities under

Random Colored

Illuminants

Fig.10.xy -chromaticity plots for test surfaces under various illuminants.

p c ?"c e c TI e c TR e c TtZ I e i TK 0e i Td i

"c

e c TJ e c T;e16T

where c for c ?f R;G;B g is set to be the wavelength of

each R,G,B channel of the camera.This narrowband assumption is nearly valid if hyperspectral cameras are used instead of an RGB camera.

Now,for each channel,p is represented as a linear combination of the reflective component R and fluorescent component J .Both R and J are unknown to us.The spectral distribution of the illuminant under which p is taken is also unknown.To tackle the problem of blindly separating R and J from the only known variable p ,we make the assumption that the two components are independent.This assumption is reasonable since in our case,the spatial distribution of fluorescent component provides no predic-tion of the spacial distribution of the ordinary reflective components;we expect no correlation between images of the two components.Based on this assumption and (16),we solve the blind separation problem by applying ICA [13]to images of the objects taken under different illuminants.Since ICA requires the number of measurements to be greater than or equal to the number of independent components,we take images P 1and P 2of a fluorescent object under two distinct illuminants I 1and I 2.4Formulate the problem based on (16)for each c ?f R;G;B g channel as

P j 1e c T

P j 2e c T !?r 1e c Tf 1e c Tr 2e c Tf 2e c T !R j e c TJ j e c T

!;e17Twhere P j i is the j th pixel value for i th illumination,R j and

J j are the ordinary reflectance and fluorescence at the j th pixel,r i e c T?"c e c TI i e c T,and

f i e c T?"c e c TZ

I i e i TK 0e i Td i :Here,j represent all pixels in the image.

Let Q c ?M c S c be the short form of the matrix equation above.We call Q c the input matrix ,M c the mixing matrix ,and S c the signal matrix .If we input Q c to ICA,5ICA will first

estimate M c ,and S c is computed as M à1

c Q c .To obtain the image with only the reflective component,we combine R j e c Tin S c for c ?f R;G;B g .Similarly,to obtain the image with only the fluorescent component,we combine J j e c Tin S c .

4.1Ambiguities of ICA

Even though ICA works well for solving our problem,it imposes two ambiguities.First,we cannot determine the “order”of the independent components R and J .In other words,we do not know which resulting component is for fluorescence and which is for reflectance.The reason is that both the mixing matrix and the signal matrix are unknown;for the same set of data Q c ,ICA could recover the pair M c and S c as either

M c ?r

1

f 1r 2

f 2

!;S c ?R

j J j !or

M c ?f

1

r 1f 2

r 2

!;S c ?J

j R j

!:The second ambiguity is “scaling.”ICA recovers the mixing matrix within a scale factor of the true mixing matrix.In other words,we cannot compute the absolute intensity of the pixels for each component.Again,the reason is that both M c and S c are unknown;any multipliers in M c can be canceled out by dividing the same scalars in S c .That is,

r 1f 1r 2f 2 !R j

J j !?r 1= f 1= r 2= f 2= ! R j J j

!:

4.1.1Solving the “Ordering”Ambiguity

We solve the ordering ambiguity by using the unique

property of the fluorescent component.Let x j i and y j

i represent the x -,y -chromaticity of the j th pixel in the i th https://www.wendangku.net/doc/fb9941873.html,pute the chromaticity difference at the j th pixel between two input images as

d j

?????????????????????????????????????????????????àx j 1àx j 2á2tày j 1ày j 2á2q :e18TIn Section 3,we showed that d j is very small if j shows the brightness of fluorescent component.Let s j 1and s j

2be the recovered intensities at the j th pixel in the two images computed by ICA.

If each image pixel contains either a fluorescent or a nonfluorescent reflective component,the ordering ambi-guity can be solved by simply counting the number of pixels with high chromaticity difference in these two images.However,in this work,we consider a composite object with both ordinary reflective and fluorescent compo-nents and this makes each image pixel contain some contributions from both components.

To handle this,we first normalize s j 1and s j

2as

s 0j 1?às j 1á2P i às i 1á2;s 0j

2?às j 2á2P i às i 2á2:e19TThen multiply the relative intensities by the chromaticity

difference d j ,and sum over all pixels

t 1?

X j

s 0j 1d j ;t 2?X j

s 0j

2d j :e20TIf t 1is smaller than t 2,then the image represented by s 1is the fluorescent component.Otherwise,the image repre-sented by s 1is the fluorescent component.Intuitively,if the j th pixel contains the fluorescent component,s 0j will be big but d j is small.Therefore,the overall t value for image with fluorescent component is always smaller.This technique assumes that the objects have much stronger fluorescent component than ordinary reflective component.

4.1.2Solving the “Scaling”Problem In the mixing matrix,the integral part of scalar f 1e c T?"c

e c TR I i e i TK 0e i Td i depends only on the spectral dis-tribution of the illuminant and excitation of the fluorescent

4.The formula considers single fluorescent material.The number of measurements should be increased depending on the number of fluorescent components to treat each material as an independent component.

5.We used the FastICA package in MATLAB in our experiments.

component and thus must be the same among all RGB channels.This fact can be used for solving the scaling ambiguity of the fluorescent component if"ce cTare known. For each c?f R;G;B g,we scale the computed s c by f1="ce cT.That is,

J0je cT?s c"ce cT=f1:e21TJ0je cTs estimate the relative intensities in RGB channels and provide the necessary color balance in the final image for fluorescent component.

To achieve correct color balance for the reflective components,we look for or include a reference patch with white reflectance in the input images.The recovered images for RGB channels are combined in a way such that the white patch remains white in the reflectance-only image.If we have a material of known fluorescence such as white paper with bluish fluorescence,we can utilize the known fluores-cence for achieving correct color balance of fluorescent component as well.

4.2Independence of Reflective and Fluorescent

Components

ICA allows two source signals to be separated from two mixed signals based on the assumption that the sources are statistically independent.The use of ICA leads to some limitations on the types of scenes applicable to the proposed approach.First,ICA needs to examine input signals where source signals are mixed differently.From this,the spectra of illumination should vary largely but cover some portions of the spectral reflectance of reflective components as well as the excitation spectra of fluorescent components so that the contribution of both components are noticeable.In addition,cast shadows are not desirable and are thus avoided.

Second,the reflective and fluorescent components should be distributed differently among scene points. Wilkie showed that there is a similarity between the fluorescence emission and the ideal diffuse reflection in terms of their shadings[24].A reasonable separation cannot be achieved by the proposed approach if a scene contains an object that contains uniform diffuse reflective and fluor-escent components.In general,natural objects such as gems and corals contain reflective and fluorescent components with different concentrations from place to place.This should contribute to making their reflective and fluorescent components statistically independent.

The mutual information is one measure of the depen-dence between two source signals.To examine the dependence of the reflective and fluorescent components observed in an image,we provide a test scene and separately observe the reflective and fluorescent compo-nents of the scene using two light sources whose spectral distributions are carefully chosen based on the knowledge of the excitation and emission spectra of the fluorescent component(Fig.3c).

The test scene consists of green-yellow fluorescent sheets (flower)on top of a nonfluorescent background image (Fig.11left).We use a blue light whose spectrum is within the range of the excitation spectrum for observing the fluorescent component and a red light whose spectrum is outside of the excitation spectra for observing the reflective component.Fig.11shows the reflective(middle)and fluorescent(right)components observed under each light in the red channel of a CCD camera.

Then the mutual information between two images P1 and P2is defined as

TeP1;P2T?

X

j2P1

X

i2P2

Bej;iTlog

Bej;iT

;e22T

where Bej;iTis the joint probability distribution function of P1and P2and BejTand BeiTare the marginal probability distribution functions of P1and P2,respectively.In this example,neither BejTnor BeiTfollows the normal distribu-tion,and the mutual information between the reflective component image and the fluorescent component image is 0.26bit.For reference,the entropy of the image(8bit grayscale)of the scene seen under white light in the red channel of the camera is6.7bit.In this example,the mutual information between two images is very low and it is reasonable to assume that the reflective and fluorescent components are statistically independent.

This example above shows the statistical independence of one particular scene.Further investigation of how statistical independence is valid for natural scenes by analyzing more sample scenes is important.We will further investigate this issue as one of our future research directions.

5R ESULTS AND A NALYSIS

We tested our method with images taken with an ordinary CCD camera.The spectral sensitivities of this camera is shown in Fig.12.The first scene is an image made with color sheets.The sheets contain different amounts of fluorescence and reflectance(Fig.13a).The top two flowers are made of fluorescent sheets that appear bright yellow and bright red-orange under white light.The flower in the middle and the leaves are made of dark red and dark green

Fig.11.Image seen under white light(left),reflective component image (middle),and fluorescent component image

(right).

Fig.12.Spectral sensitivities of the camera.

nonfluorescent sheets.The background is made of a nonreflective light purple sheet.

We first recovered fluorescent and reflective components using images taken under a green illuminant and a pink illuminant (Fig.14a).The recovered fluorescent component (Fig.14b)shows that the color of the fluorescent component of the yellow fluorescent sheet is,in fact,green.In Section 3,we showed the measured emission spectrum of the sheet (Fig.3c),which suggests that the color of the fluorescent component is green.Furthermore,we took images of the fluorescent flowers under UV light,which provided “ground truth”for the color of the fluorescent components (Fig.13b).Our recovered appearance agrees with experi-mental results,as well as the “ground truth.”The dark red and dark green sheets used in making the scene have ordinary reflectance only since the color of the middle flower and the leaves in the recovered reflective component (Fig.14c)is the same as the color seen under white light.It is also worth noting that the yellow fluorescent flower appears to be orange in the recovered image for the reflective https://www.wendangku.net/doc/fb9941873.html,bining the orange color with the green color in the fluorescent component gives the flower its final yellow appearance.Moreover,the red-orange fluorescent sheet has much stronger fluorescence compare to the yellow fluorescent sheet.Therefore,its color

appearance is almost all contributed by the fluorescent component.

The second scene consists of two fluorescent sheets on top of a nonfluorescent background image with complex color patterns.Our method succeeded in identifying the green and red-orange color of the fluorescent sheets.The recovered image for fluorescent component (Fig.15b (left))does not show the background image at all,which clearly demon-strates the correctness and effectiveness of our method.Our method is effective on scenes with nonplanar surfaces as well.Fig.16shows the recovered results for a scene consists of nonplanar objects.The fluorescent sticks and nonfluorescent jar are separated into two images.The color of the sticks (Fig.16d)matches with the ground truth (Fig.16b),and the shadings of the objects are included in the recovered reflective and fluorescent components.

6A PPLICATION IN R ELIGHTING I MAGES

The ability to separate ordinary reflective and fluorescent components of an image allows an alternative yet better way to relight images.Traditional relight algorithms relight an image uniformly by multiplying the ratio between the source illumination and target illumination to the image seen under the source illumination.

For instance,Fig.17a is an image seen under white light.The image consists of two fluorescent sheets (the flowers)on top of a nonfluorescent background image with ordinary reflective surfaces.If we apply a straightforward relight algorithm based on the illumination ratio,we obtain an image in which the color of fluorescent objects in particular is not reproduced accurately (Fig.17c).In contrast,Fig.17d shows the result produced by separately processing ordinary reflective and fluorescent components of the image.Here we relight only the reflective component using the traditional approach and preserve the fluorescent https://www.wendangku.net/doc/fb9941873.html,pared to the result produced by traditional relighting algorithms (Fig.17c),it is evident that the new approach produces output image with more accurate color.It should be noted that the intensity of the fluorescent components should change depending on illumination spectra.This phenomenon cannot be handled by the current

Fig.14.

Recovered fluorescent

and reflective

components

using images taken under green and pink illuminants.

Fig.15.Fluorescent objects

on top of a reflective image with complex color patterns.

Fig.13.Colored sheets under white light and fluorescent sheets under UV light.

approach.One of the future directions of this research includes estimating the excitation spectra of fluorescent components to simulate this phenomenon.

Extracting the fluorescent components of real objects has great potential for many applications such as quality inspection of plants,food hygiene,hygiene maintenance of a factory,and medical diagnosis.

7D ISCUSSIONS ,L IMITATION,AND C ONCLUSIONS

We provided theories of fluorescence phenomenon and explained the difference in appearance between fluores-cence and reflectance.We also proposed a method for separating the fluorescent and reflective components of objects using images captured under two illuminants.The results showed that our method is robust and effective under a variety of situations.Traditionally,researchers in computer vision have been excluding fluorescent objects from their consideration due to the complexity and lack of theoretical basis on fluorescence phenomenon.Our separa-tion method provides additional information about objects in a scene,which has great importance to improving existing computer vision algorithms that consider object appearance.Our result showed that the intensity of fluorescence varies proportionally to the illuminant;we may be able to use this property to infer information about the illuminants.

There are a few limitations to our research that are worth attention and further investigation.First,we assume that for an image,there is no correlation between the spatial distributions of reflective and fluorescent components.We will further explore statistical evidence to support the

assumption.Second,the experiments were conducted in a setting that allows us to have full control of the illumination conditions,environments,inputs,and noise levels.The results we obtained in a well-controlled setting allow us to derive a theoretical model more easily.In the future,we would conduct experiments with settings that resemble the reality more,such as outdoors with natural light,and use the results to fine-tune our model.Third,the proposed separation method assumes that a CCD camera has narrowband responses since such an assumption allows us to derive an initial model.Even though this assumption is made by many color constancy algorithms,it remains controversial.Therefore,it is worth fine-tuning the model more to take non-narrowband responses into consideration.

A CKNOWLEDGMENTS

This research was supported in part by the Ministry of Education,Science,Sports,and Culture Grant-in-Aid for Scientific Research on Innovative Areas.The authors are grateful to Dr.Shin’ya Nishida for helpful suggestions.

R EFERENCES

[1]V.Agarwal and B.R.Abidi,“An Overview of Color Constancy Algorithms,”J.Pattern Recognition Research,vol.1,pp.42-54,2006.[2]M.Alterman,Y.Schechner,and A.Weiss,“Multiplexed Fluores-cence Unmixing,”Proc.IEEE Int’l https://www.wendangku.net/doc/fb9941873.html,putational Photography,pp.1-8,2010.

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H.Farid and E.Adelson,“Separating Reflections and Lighting Using Independent Components Analysis,”Proc.IEEE https://www.wendangku.net/doc/fb9941873.html,puter Vision and Pattern Recognition,vol.1,pp.267-275,1999.

Fig.17.Ground truth versus relighted image produced by traditional and new relighting

algorithms.

Fig.16.Fluorescent and reflective components of an image with real objects.

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H.P.A.Lensch,“Acquisition and Analysis of Bispectral Bidirec-

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Algorithms and Applications,”The Official J.Int’l Neural Network Soc.,vol.13,nos.4/5,pp.411-430,2000.

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of Fluorescent Objects Using Visible Lights and an Imaging Device,”Proc.IS&T/SID’s19th Color Imaging Conf.,2011.

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for Diffuse Fluorescent Surfaces,”Proc.Fourth Int’l https://www.wendangku.net/doc/fb9941873.html,puter Graphics and Interactive Techniques in Australasia and Southeast Asia, pp.321-328,2006.

Cherry Zhang received the bachelor of mathe-

matics degree(honors in computer science,with

distinction)and the master’s degree in mathe-

matics,both from the University of Waterloo,

Canada,in2008and2011,respectively.During

her undergraduate studies,she worked at four

different companies as an intern.She gained

significant work experience in IT and network

administration,software development,and video

processing algorithm development.During her graduate studies,she focused on doing research in computer graphics under the supervision of Professor Bill Cowan.She also did a summer internship at the National Institute of Informatics in Japan,at which time, she published a paper in CVPR11and received a best student paper honorable mention award.She is currently working as a technology analyst at Goldman Sachs,an investment bank in New York.

Imari Sato received the BS degree in policy

management from Keio University,Japan,in

1994.After studying at the Robotics Institute of

Carnegie Mellon University as a visiting scholar,

she received the MS and PhD degrees in

interdisciplinary information studies from the

University of Tokyo in2002and2005,respec-

tively.In2005,she joined the National Institute

of Informatics,where she is currently an

associate professor.Her primary research inter-ests include the fields of computer vision(physics-based vision,image-based modeling)and computer graphics(image-based rendering, augmented reality).She has received various research awards, including the IPSJ Nagao Special Researcher Award(2010),The Young Scientists’Prize from The Commendation for Science and Technology by the Minister of Education,Culture,Sports,Science and Technology(2009),and the Microsoft Research Japan New Faculty award(2011).She is a member of the IEEE.

.For more information on this or any other computing topic, please visit our Digital Library at https://www.wendangku.net/doc/fb9941873.html,/publications/dlib.

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如何写先进个人事迹 篇一:如何写先进事迹材料 如何写先进事迹材料 一般有两种情况:一是先进个人,如先进工作者、优秀党员、劳动模范等;一是先进集体或先进单位,如先进党支部、先进车间或科室,抗洪抢险先进集体等。无论是先进个人还是先进集体,他们的先进事迹,内容各不相同,因此要整理材料,不可能固定一个模式。一般来说,可大体从以下方面进行整理。 (1)要拟定恰当的标题。先进事迹材料的标题,有两部分内容必不可少,一是要写明先进个人姓名和先进集体的名称,使人一眼便看出是哪个人或哪个集体、哪个单位的先进事迹。二是要概括标明先进事迹的主要内容或材料的用途。例如《王鬃同志端正党风的先进事迹》、《关于评选张鬃同志为全国新长征突击手的材料》、《关于评选鬃处党支部为省直机关先进党支部的材料》等。 (2)正文。正文的开头,要写明先进个人的简要情况,包括:姓名、性别、年龄、工作单位、职务、是否党团员等。此外,还要写明有关单位准备授予他(她)什么荣誉称号,或给予哪种形式的奖励。对先进集体、先进单位,要根据其先进事迹的主要内容,寥寥数语即应写明,不须用更多的文字。 然后,要写先进人物或先进集体的主要事迹。这部分内容是全篇材料

的主体,要下功夫写好,关键是要写得既具体,又不繁琐;既概括,又不抽象;既生动形象,又很实在。总之,就是要写得很有说服力,让人一看便可得出够得上先进的结论。比如,写一位端正党风先进人物的事迹材料,就应当着重写这位同志在发扬党的优良传统和作风方面都有哪些突出的先进事迹,在同不正之风作斗争中有哪些突出的表现。又如,写一位搞改革的先进人物的事迹材料,就应当着力写这位同志是从哪些方面进行改革的,已经取得了哪些突出的成果,特别是改革前后的.经济效益或社会效益都有了哪些明显的变化。在写这些先进事迹时,无论是先进个人还是先进集体的,都应选取那些具有代表性的具体事实来说明。必要时还可运用一些数字,以增强先进事迹材料的说服力。 为了使先进事迹的内容眉目清晰、更加条理化,在文字表述上还可分成若干自然段来写,特别是对那些涉及较多方面的先进事迹材料,采取这种写法尤为必要。如果将各方面内容材料都混在一起,是不易写明的。在分段写时,最好在每段之前根据内容标出小标题,或以明确的观点加以概括,使标题或观点与内容浑然一体。 最后,是先进事迹材料的署名。一般说,整理先进个人和先进集体的材料,都是以本级组织或上级组织的名义;是代表组织意见的。因此,材料整理完后,应经有关领导同志审定,以相应一级组织正式署名上报。这类材料不宜以个人名义署名。 写作典型经验材料-般包括以下几部分: (1)标题。有多种写法,通常是把典型经验高度集中地概括出来,一

Target speaker separation

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Index Terms:Multisource noise,speech enhancement,speech qual-ity,non-stationary noise. 1.INTRODUCTION Target speaker separation describes the problem of estimating an unknown clean speech signal recorded by one or several micro-phones in a noisy environment with possible presence of competing speaker(s).The problem?nds applications in many different areas of speech communications,including mobile telephony,robust au-tomatic speech recognition and hearing aids.The research in this area has been carried on for decades-with reporting some success-ful high quality speech enhancement systems.As a noise reduc-tion device is expected to work in noisy environment without a prior knowledge of the noise type,recent research effort has been directed toward studying the robustness of these algorithms in nonstationary noise,including low signal-to-noise ratios(SNRs)[1]. As one step toward studying the problem of enhancing a tar-get speech signal in a multisource environment with nonstationary background noise,recently,the PASCAL challenge,termed as com-putational hearing in multisource environments(CHiME)was orga-nized[2].The challenge addresses several critical aspects on the The work of Pejman mowlaee was partially funded by the European project DIRHA(FP7-ICT-2011-7-288121),by ASD(Acoustic Sensing& Design)and Speech Processing Solutions GmbH Vienna.The work of Rahim Saeidi was funded by the European Community’s Seventh Framework Pro-gramme(FP72007-2013)under grant agreement no.238803.original problem of enhancing and recognizing of a target speech from its noisy version observed in a real-life listening environment mainly characterized by rather low SNR ratios whereas the noise sources are unpredictable,abrupt and highly non-stationary. 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Throughout our study we report how much improvement is achiev-able by incorporating speaker-dependent?lters inside the speech en-hancement algorithm to successfully handle the nonstationary noise. 2.PREVIOUS METHODS Previous noise reduction techniques are classi?ed as single and multi-channel.In a multichannel scenario,a beamformer algorithm leads to a promising cancellation of directional noise sources.Still, the usefulness of the beamforming techniques for enhancement pur-pose gets quite limited,especially when used individually under highly non-stationary or diffused noise scenarios[13].For single-channel speech enhancement methods,a minimum mean square er-ror(MMSE)estimator in the amplitude(MMSE-STSA)[10]and in the log-amplitude(MMSE-LSA)[9]domain are well-known for dealing well with the stationary additive noise scenario while other algorithms were suggested to handle non-stationary noise types [3,14].These techniques mainly rely on noise estimates typically provided by a noise estimation scheme(noise power spectral density (PSD)trackers[4,14])in a decision-directed manner,and further assume that the noise signal shows less changes in its second order statistics compared to that of the target speech signal.Such an as-sumption is not valid for real-life scenarios where the noise signal is highly time-varying and unpredictable or when the noise signal has a statistical characteristic close to the speech.Therefore,the achiev-able performance obtained by the methods in this group,gets limited when used in such adverse noise conditions[15]. To take advantage of both groups,several methods on com-bining a beamforming stage with a speech enhancement stage as a post-processor have been suggested[5,16].The post-processor at-

关于时间管理的英语作文 manage time

How to manage time Time treats everyone fairly that we all have 24 hours per day. Some of us are capable to make good use of time while some find it hard to do so. Knowing how to manage them is essential in our life. Take myself as an example. When I was still a senior high student, I was fully occupied with my studies. Therefore, I hardly had spare time to have fun or develop my hobbies. But things were changed after I entered university. I got more free time than ever before. But ironically, I found it difficult to adjust this kind of brand-new school life and there was no such thing called time management on my mind. It was not until the second year that I realized I had wasted my whole year doing nothing. I could have taken up a Spanish course. I could have read ten books about the stories of successful people. I could have applied for a part-time job to earn some working experiences. B ut I didn’t spend my time on any of them. I felt guilty whenever I looked back to the moments that I just sat around doing nothing. It’s said that better late than never. At least I had the consciousness that I should stop wasting my time. Making up my mind is the first step for me to learn to manage my time. Next, I wrote a timetable, setting some targets that I had to finish each day. For instance, on Monday, I must read two pieces of news and review all the lessons that I have learnt on that day. By the way, the daily plan that I made was flexible. If there’s something unexpected that I had to finish first, I would reduce the time for resting or delay my target to the next day. Also, I would try to achieve those targets ahead of time that I planed so that I could reserve some more time to relax or do something out of my plan. At the beginning, it’s kind of difficult to s tick to the plan. But as time went by, having a plan for time in advance became a part of my life. At the same time, I gradually became a well-organized person. Now I’ve grasped the time management skill and I’m able to use my time efficiently.

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英语演讲稿:未来的工作 这篇《英语演讲稿范文:未来的工作》,是特地,希望对大家有所帮助! 热门演讲推荐:竞聘演讲稿 | 国旗下演讲稿 | 英语演讲稿 | 师德师风演讲稿 | 年会主持词 | 领导致辞 everybody good afternoon:. first of all thank the teacher gave me a story in my own future ideal job. everyone has a dream job. my dream is to bee a boss, own a pany. in order to achieve my dreams, i need to find a good job, to accumulate some experience and wealth, it is the necessary things of course, in the school good achievement and rich knowledge is also very important. good achievement and rich experience can let me work to make the right choice, have more opportunities and achievements. at the same time, munication is very important, because it determines whether my pany has a good future development. so i need to exercise their municative ability. i need to use all of the free time to learn

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