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34     CHAPTER 2  Diagnostic imaging in cancer




                            The guided equation for photo-thermoacoustic computed tomography (CT) is
                         explained as follow:

                                                    1  ∂  2      β ∂
                                           ∇ pr t(, ) −  2  2  pr t)  =−  Hr t ,)        (2.4)
                                                                      (
                                                         (,
                                             2
 2
 2
 ∇ p(r→,t)−1vS2∂ ∂t p(r→,t)=−βCp∂∂                  v S  ∂t     C  p  ∂x
 2
 xH(r→,t)
 H(r→,t)                 where Hr t(, ) heating function, v  is the speed of sound in the medium, C  specific
                                                   S
                                                                                     p
                         heat capacity, and β is thermal expansion coefficient. To assure that heat diffusion
                         is negligible during pulse laser irradiation, the pulse laser frequency is chosen much

 P(r→,t)                 shorter than the thermal relaxation time. Pr t(, ) in the above equation is obtained as
                         follow:

                                                 β     dr ′ ∂Hr  )
                                                             ( ′′ t,
                                          (,
                                         pr t) =    ∫                r  − ′ r /  v s     (2.5)
 p(r→,t)=β4πCp∫dr′→r→−r′→∂Hr′                   4 πC p  r  − ′ r  ∂ ′ t  t ′=− t
 →,t′∂t′t′=t−r→−r′→/vs
                         when laser pulse frequency is much shorter than laser relaxation time, the stress is
                         confined and as a result, the above equation is rewritten as follow:

                                                                        r
                                                 1  ∂  1            r − ′  
                                                                ′
                                           (,
                                          pr t) =  2    ∫  dr ′pr () δ t  −           (2.6)
                                                                  
                                                             0
                                                      
 p(r→,t)=14πvS2∂∂t1vst∫dr′→p (r′→               4 πv S  ∂  t vt      v S    
                                                        s
 0
 )δt−r→−r′→vS
                         where p  is the initial photoacoustic pressure.
                               0
                         2.4.1.2  Electrical impedance tomography
                         EIT is a kind of noninvasive medical imaging determines the electrical permittivity,
                         conductivity and impedance of the interior part of the body from surface electrode.
                         Conducting surface electrodes are attached to the skin and small alternating currents
                         at a single or multiple frequency are applied to the electrodes, then the electrical
                         potentials are measured and used to build a tomographic image of the target. EIT
                         imaging technic is based on the measuring the tissue impedance consisting of mem-
                         branes, cells, and fluids. Cells and membranes act as small imperfect capacitors with
                         high resistivity, while fluids are the resistive component that contribute a frequency
                         dependence for liquids in the outside of the cells. At high frequencies (in the range of
                         MHz), the only resistive component is related to the conduction through extracellular
                         and intracellular fluid, while at low frequencies (in the range of Hz to kHz), mem-
                         branes impede the current and can be used to obtain valuable information regarding
                         the size, morphology, and electrical properties of cells [32]. There are two types of
                         EIG systems including absolute EIT and difference EIT. Difference EIT focuses on
                         the study of the changes in conductivity during a period of time. Absolute EID is
                         more difficult since channel noise and electrode impedance need to be calculated.
                         One of the most clinical applications of EID for cancer diagnosis is related to the
                         detection of malignant breast tumors from benign lesions [33].
                         2.4.1.3  Near-infrared optical tomography
                         NIR optical tomography is a noninvasive imaging technic with high contrast features
                         for blood cells. This is mainly due to the fact that hemoglobin absorbs NIR light
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