D E TERMINATION MODEL OF CARCINOMA AND BENIGN TYPES USING PHYSICAL QUANTITIES OF THE CA MAMMAE MAMMOGRAPHY.

Vol 22, No. 7;Jul 2015

DETERMINATION MODEL OF CARCINOMA AND
BENIGN TYPES USING PHYSICAL QUANTITIES
OF THE CA MAMMAE MAMMOGRAPHY

Anak Agung Ngurah Gunawan, I Nyoman Widana
School of Physic, Faculty Mathematics and Natural Sciences, Udayana University, Denpasar, Bali.
Tel. 62-0361-484238
E-mail : agung1962sp@yahoo.co.id
The research is financed by: Dirjen Dikti Indonesia
Abstract
The article had been built the model to determine the carcinoma and benign types. Potentially, the
physical quantities could be differ of each them. The biopsy methods had developed in classifying the
both carcinoma and benign types. In this research, the probability of gray-level pairs on certain
distance are derived from the mathematical model of the mammography physical quantities are used.
In the previous research, determination of infiltrating ductal carcinoma and infiltrating lobuler
carcinomahistopathology types, breast cancer stadium, health level of contra lateral,andreadability
increasing x-ray mammography images on histopathology types determination on breast cancer using
special patern cropping are succeeded. In this research, the mathematical model of the mammography
physical quantities is succeeded to determine the carcinoma and benign histopathology types. The

model had been proposed for testing 120 the new patients mammogram at Dokter Soetomo Hospital,
Surabaya, Indonesia. The research results showed the physical quantities could be predict the
carcinoma and benign histopathology types in 86,67 %sensitivity for 2 x 2 cm sample sized and α = 5
%.
Keywords : mammography, ca mammae, carcinoma, benign.

1. Introduction
The following methods of the breast cancer early detection had been patented are employing histogram
peak detection [1], histogram alteration [2], pixel mapping [3], neural network [4], contour [5], wavelet
filter dan artificial neural networks [6], minimally invasive diagnosis and treatment [7], morphological
closing [8], histological analysis [9], blood vessel walls [10], but all the above methods detect the

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presence of microcalcification only, but determination of the type of carcinoma and benign breast
cancer are not supported.The classifying types of Infiltrating Duktal Carcinoma and Infiltrating

Lobuler Carcinoma breast cancer histopathology using physical parameter in86,36 % sensitivityin
previous research are succeeded [11]. The determination of the level of the contra lateral breast health
using physical parameters in 93.75% sensitivity [12], the breast cancer stadium state in 86.67%
sensitivity of [13]. Also, the readibility x-rays results of mammography on breast cancer
histopathological type determination using a special pattern croping through physical parameters in
97.5% sensitivity are succeeded too [14].
This paper organized as follows, section 2 discussing the radiation intensity on ca mammae, section 3
about physical quantities of the result of X-ray mammography images, the probability function in
section 4, section 5 about the multinomial linear regression function as an outcome types of carcinoma
and benign, results and discussion in section 6 and the last section are conclusions.

2. The Radiation Intensity on Ca Mammae
Increase of the radiation absorption intensity depends on breast cancer density increasing due to pixel
intensity values of carcinoma and benign types are different. So that the physical parameters between
the types of carcinoma and benign are different. The transmittance of the X-ray radiation intensity are
written in equation (2.1) bellow [11][12][13][14].
I1 = I0 e –μd

(2.1)


where I1, I0, μ, d are transmitted beam intensity, the intensity of light at first, absorption coefficient,
breast cancer density, respectively.

3. Physical Quantities of X-Ray Mammography Results
The following physical parameters are nonuniformity, contrast, uniformity, local homogeneity,
correlation, feature represents the nature, feature represents the density, nonuniformity of hdiff,
uniformity of hdiff and the feature represents the nature of hdiff derived from the x-ray mammography
results. All the physical parameters are written as follows equations [11][12][13][14][15].
(3.1)
(3.2)

(3.3)

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(3.4)

for
(3.5)
where,
(3.6)
(3.7)
(3.8)

(3.9)
(3.10)
(3.11)
(3.12)
(3.13)
With H(yq, yr, d) is distribution of probability of occurrence of a pair of gray-level value separated by
a given displacemen vector d.

4.

Probability Function

Consider probability functions bellows,

independent each others,
carcinoma,

) and
are fulfilled. For

dependent in

, for

liniearly

is output categories i.e for

,

, benign, and others. The logistic functions are written as follows:

(3.13)
further


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for example,
,
The qualitative mapping the entropy to carcinoma and benign ca mammae are in abnormal Gaussian
satisfied. So that,
, or

,
,
,
,


and

as statistics model of logistics multinomial regression, for

in all the cathegories are

, will be

, furthermore:

For all the histopathology categories are fullfiled with,

5.

The multinomial linear regression function as the outcome of carcinoma and benign types

Consider linear regression function bellows,

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where Zk is outcome for
with

, entirely. Zk0 as outcome initial values for
.

is pertubation parameters for a

are in linear form. For last term,

number

,

as outcome correction factors for all


. For example:

Illustratively, the above expression are depicted in figure 1 as bellows.

Figure 1. Logistic and Linear Regression Model

6. Results and Discussion
Figures 2, 3, are types of carcinoma and benign mammogram images, respectively.

(2)
Figure 2. Carcinoma Type

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(3)
Figure 3. Benign Type

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Mammography images had been taken from radiology installations at Dr. Soetomo Hospital,Surabaya,
RSUP Sanglah and RSU. Primamedika, Denpasar, supported by Sony Brand ICR type 3600M
apparatus. All the images in bmp format are stored which sample sized in 2 cm x 2 cm matrices.

Table 1. Physical Quantity Intervals
No
1
2
3
4
5
6
7

Physical Quantity
Anguler Secound Moment
Inverse Difference Moment
Mean
Deviation

Entropy of the Difference Second Order
Histogram
The Second Anguler Moment of the
Difference Second Order Histogram
Mean of the Difference Second Order
Histogram

Benign
0,00015 - 0.01013
0.01527 - 0.08977
71.55468 - 195.80523
18.84672 - 56.86512

Carcinoma
0.00013 - 0.08280
0.01106 - 0.39200
71.16284 - 220.92240
11.06751 - 93.33126

1.32977 - 2.05756

1.29424 - 2.14790

0.01051 - 0.05878

0.00806 - 0.11134

7.65163 - 43.77752

7.27355 - 55.92737

All the physical quantities above formulated bellows:
Z:= -17056.786 + 13939360.273*MA[9]
123275.512*MD[6]

-14975532.439*MA[10] + 79507.135*MD[5]

-52858.798 * MD[7]

-29317.721*MD[8]

+

-46033.962*MD[9] -

84405.247*MD[10] -2616.686*MN[1] + 5924.284*MN[2] -3119.844*MN[3] -453.778*MN[4] 1114.523*MN[5] + 3720.727*MN[6] -3618.971*MN[7] + 11.610*MN[8] + 2152.569*MN[9] 885.095MN[10] -1327.391*D[1] + 2202.098*D[2] -3.143*D[3] -3364.818*D[4] + 7916.137*D[5] 10676.240*D[6]

+ 6323.275*D[7] + 415.555*D[8]

-1671.692*D[9] + 197.645*D[10]

+

23576.501*EH[1] + 7048.037*EH[2] -98617.823*EH[3] + 59177.808*EH[4] -53465.845*EH[5] +
81134.008*EH[6] + 743.337*EH[7] -81311.924*EH[8] + 74475.699*EH[9] -4742.767*EH[10] +
169258.070*MAH[1] + 31944.202*MAH[2]

-1083908.718*MAH[3] + 826751.786*MAH[4]

+

888282.531*MAH[5] -918006.126*MAH[6]

-487749.444*MAH[7] -1455971.004*MAH[8]

+

1382311.075*MAH[9]

+

844659.147*MAH[10]

-124.008*MHD[1]

+

74.265*MHD[2]

-

744.240*MHD[3] + 1741.103*MHD[4] + 430.726*MHD[5] -116.272*MHD[6] -1461.422*MHD[7]
-1022.368*MHD[8] + 894.912*MHD[9] + 346.808*MHD[10];
Probability for carcinoma and benign types each are formulated,

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The uniformity, local homogeneity, feature represents the nature, feature represents the density,
nonuniformity of hdiff, uniformity of hdiff, feature represents the nature of hdiff parameters are
optimium to differ carcinoma and benign types in this research.

7. Conclusion
Determination of carcinoma and benign types on breast cancer using physical quantities on the 120
samples in 86.67% sensitivity are resulted with 16 samples are errors. That is the diagnostics
performance of the carcinoma and benign types are increased. The optimum physical parameters :
Angular Second Moment distance between pixels 9, 10, Inverse Difference Moment on the distance
between pixels 5,6,7,8,9,10, Mean, Deviation, Entropy of the Difference Second Order Histogram,
Angular Second Moment of the Difference Second Order Histogram, Mean of the Difference Second
Order Histogram on the distance between pixels 1,2,3,4,5,6,7,8,9,10 are obtained.

Acknowledgments
We would like to thank the Indonesian government has provided funding of research through the
National Competitive Fundamental Grant, Rector of Udayana University and chairman of LPPM Unud
which has provided research funding. Dean of the Faculty Udayana University and Chairman of the
Department of Physics Faculty Udayana University who has given permission to study, also we would
like to thank the director of hospital are Dr. Soetomo Hospital, Surabaya, RSUP Sanglah Hospital and
Primamedika Hospital, Denpasar, Indonesia for the research supporting.

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