<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JCT</journal-id><journal-title-group><journal-title>Journal of Cancer Therapy</journal-title></journal-title-group><issn pub-type="epub">2151-1934</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jct.2014.514140</article-id><article-id pub-id-type="publisher-id">JCT-52141</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Medicine&amp;Healthcare</subject></subj-group></article-categories><title-group><article-title>
 
 
  Deterministic Parsing Model of the Compound Biological Effectiveness (&lt;i&gt;CBE&lt;/i&gt;) Factor for Intracellular &lt;sup&gt;10&lt;/sup&gt;Boron Distribution in Boron Neutron Capture Therapy
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hintaro</surname><given-names>Ishiyama</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Quantum Beam Science Directorate, Japan Atomic Energy Agency, Naka-gun, Japan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>ishiyama.shintaro@jaea.go.jp</email></corresp></author-notes><pub-date pub-type="epub"><day>03</day><month>12</month><year>2014</year></pub-date><volume>05</volume><issue>14</issue><fpage>1388</fpage><lpage>1398</lpage><history><date date-type="received"><day>20</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>18</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>14</day>	<month>November</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
   Purpose: In defining the biological effects of the <sup>10</sup>B(n, α)<sup>7</sup>Li neutron capture reaction, we have previously developed a deterministic parsing model to determine the Compound Biological Effectiveness (CBE) factor in Borono-Phenyl-Alanine (BPA)-mediated Boron Neutron Capture Therapy (BNCT). In present paper, we demonstrate that the CBE factor is directly and unambiguously derivable by the new formula for any case of intracellular <sup>10</sup>Boron (<sup>10</sup>B) distribution, which is founded on this model for tissues and tumor. Method: To determine the CBE factor, we derive the following new calculation formula founded on the deterministic parsing model with three constants, CBE<sub>0</sub>, F, n and the eigen value N<sub>th</sub>/N<sub>max</sub>. <img src="Edit_c40f1f63-0069-484b-bd92-8f2dbe4215a2.bmp" alt="" />  where, N<sub>th</sub> and N<sub>max</sub> are the threshold value of boron concentration of N and saturation boron density in tissues and tumor. In order to determine these constants and the eigen values, iterative calculation technique was employed for the CEB factor and N<sub>max</sub> data set previously reported. Results and Conclusion: From the iterative calculation results, it is clear that the calculated CBE factor values obtained are almost identical to the original CBE factors and there is a good correlation between the original CBE factors and N<sub>th</sub>/N<sub>max</sub>, when CBE<sub>0</sub>, F and n are given as 0.5, 8 and 3, respectively. These constants provide a better understanding of different types of intracellular<sup>10</sup>B distribution. 
 
</html></p></abstract><kwd-group><kwd>Boron Neutron Capture Therapy</kwd><kwd> Compound Biological Effectiveness</kwd><kwd> Borono-Phenyl-Alanine</kwd><kwd> Tumor</kwd><kwd> &lt;sup&gt;10&lt;/sup&gt;B(&lt;i&gt;n</kwd><kwd> α&lt;/i&gt;)&lt;sup&gt;7&lt;/sup&gt;Li</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Many types of pilot innovative accelerator-based neutron source for neutron capture therapy with lithium target were designed [<xref ref-type="bibr" rid="scirp.52141-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.52141-ref3">3</xref>] and many inventions for the progressive power run-up were reported [<xref ref-type="bibr" rid="scirp.52141-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.52141-ref5">5</xref>] . In Japan, implemented deployment of accelerator-driven neutron source for Boron Neutron Capture Therapy (BNCT) is scheduled in 2014 in National Cancer Center, of which system was designed with the production of neutrons via threshold <sup>7</sup>Li(p, n)<sup>7</sup>Be reaction at 25 kW proton beam with energy of 2.5 MeV, which was designed to dovetail the narrow peak band resonance of lithium target and started its installation at middle of 2013. This BNCT device is expected to offer the potential for achieving the objects of which any treatment capable of sterilizing the primary tumor locally will result in a high probability of cure.</p><p>BNCT is a targeted radio-therapeutic modality used for the treatment of brain tumors and melanoma and a bimodal approach to cancer therapy. Before BNCT, Boron-10(<sup>10</sup>B)-enriched compounds are used to deliver <sup>10</sup>B to tumors. Once tumor uptake of a given boron delivery agent relative to the surrounding normal tissues and blood has been maximized and then irradiation with low-energy neutron takes place. An alternative boron delivery agent, p-borononphenylalaine (BPA) instead of administration of the boron delivery agent borocaptate sodium (BSH), is being used together with mode deeply penetrating epithermal neutron beam [<xref ref-type="bibr" rid="scirp.52141-ref6">6</xref>] . BNCT was extensively reviewed in two recent articles [<xref ref-type="bibr" rid="scirp.52141-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.52141-ref8">8</xref>] and the targeting effectiveness of BNCT was dependent upon the preferential delivery of <sup>10</sup>B to the primary tumor and its metastatic spread.</p><p>In defining the biological effects of the <sup>10</sup>B(p, α)<sup>7</sup>Li neutron capture reaction relative to photons, the term compound biological effectiveness (CBE) factor was used as an alternative to RBE. Calculation of the CBE factor is similar to that of the RBE factor [<xref ref-type="bibr" rid="scirp.52141-ref9">9</xref>] . Equating the X-ray ED<sub>50</sub> dose with a BNC dose (beam + BSH) that gives the same end point of a 50% incident of ulceration produces the following equation:</p><p>The CBE factor = [(X-ray ED<sub>50</sub>) − (thermal beam component of ED<sub>50</sub> &#215; RBE]/<sup>10</sup>B(p, α)<sup>7</sup>Li component of ED<sub>50</sub>.</p><p>Recently, the CBE factors concerning to tumor, skin lung, liver [<xref ref-type="bibr" rid="scirp.52141-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.52141-ref11">11</xref>] , heart [<xref ref-type="bibr" rid="scirp.52141-ref12">12</xref>] and oral mucosal tissues [<xref ref-type="bibr" rid="scirp.52141-ref13">13</xref>] were reported and prospect of actually using BNCT for the patients has been developing under the right cir- cumstances. However, there is no theoretical unified explanation of the CBE factors for normal tissues and tumor, despite the fact that significance of high precision of the CBE factor evaluation is requested for the patients.</p><p>The purpose of the present investigation was to demonstrate the deterministic parsing model of the CBE factor for intracellular <sup>10</sup>B distribution and discover the unified methodology for the evaluation of the CBE factors for normal tissues and tumor in BNCT.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. <sup>10</sup>B Concentration and the CEB Factors of BPA</title><p>As for the CBE factor and boron concentration data set of BPA previously obtained in biological test for normal tumor, skin lung, liver [<xref ref-type="bibr" rid="scirp.52141-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.52141-ref11">11</xref>] , heart [<xref ref-type="bibr" rid="scirp.52141-ref12">12</xref>] and oral mucosal tissues [<xref ref-type="bibr" rid="scirp.52141-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.52141-ref14">14</xref>] , we can classify these data into two main groups, tumor and normal tissue and no relationship between N<sub>B-max</sub> and CBE factor was not found in normal tissue group (<xref ref-type="table" rid="table1">Table 1</xref>, <xref ref-type="fig" rid="fig1">Figure 1</xref>).</p></sec><sec id="s2_2"><title>2.2. Mathematical Analysis Model for the CBE Factor</title><sec id="s2_2_1"><title>2.2.1. Definition of the Duplicate Volume of the α Range and Proximity of Boron Atoms</title><p>Thermal neutrons or epithermal neutrons, which become thermalized at depth in tissue, are captured by <sup>10</sup>B atoms, with the resultant fission reaction producing α-particles and lithium-7 (<sup>7</sup>Li) ions in BNCT.</p><p>These particles have a limited range of &lt;9 μm in tissue. Thus, it is possible to selectively irradiate a tumor with high Linear Energy Transfer (LET) radiation, while sparing the adjacent normal tissues, theoretically. <sup>10</sup>BPA is designed to be selectively spatially-integrated into the tumor cells and boron atoms are distributed in a</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The data set of the CBE factor and N<sub>max</sub> for normal tissues and tumour obtained in the case of BPA administration</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >No.</th><th align="center" valign="middle"  rowspan="2"  >Tissue</th><th align="center" valign="middle" >N<sub>B-max</sub></th><th align="center" valign="middle" >CBE</th></tr></thead><tr><td align="center" valign="middle" >(μg/g)</td><td align="center" valign="middle" >Factor</td></tr><tr><td align="center" valign="middle" >1<sup>1)</sup></td><td align="center" valign="middle" >Tumor</td><td align="center" valign="middle" >72</td><td align="center" valign="middle" >3.8</td></tr><tr><td align="center" valign="middle" >2<sup>2)</sup></td><td align="center" valign="middle" >Normal skin tissue</td><td align="center" valign="middle" >28.8</td><td align="center" valign="middle" >2.5</td></tr><tr><td align="center" valign="middle" >3<sup>3)</sup></td><td align="center" valign="middle" >Normal brain tissue</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >1.34</td></tr><tr><td align="center" valign="middle" >4<sup>4)</sup></td><td align="center" valign="middle" >Normal oral mucosal tissue</td><td align="center" valign="middle" >21.5</td><td align="center" valign="middle" >4.87</td></tr><tr><td align="center" valign="middle" >5<sup>5)</sup></td><td align="center" valign="middle" >Normal liver tissue</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >4.25</td></tr><tr><td align="center" valign="middle" >6<sup>6)</sup></td><td align="center" valign="middle" >Normal lung tissue</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >2.3</td></tr><tr><td align="center" valign="middle" >7<sup>7)</sup></td><td align="center" valign="middle" >Normal heart tissue</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >1.35</td></tr></tbody></table></table-wrap><p><sup>1)</sup>Fukuda et al., 1994, <sup>2)</sup>Kiger et al., 2008, <sup>3)</sup>Suzuki et al., 2000, <sup>4)-7)</sup>Morris et al., 1997 with BPA experiments of mice.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The relationship between the CBE factor and N<sub>max</sub> in the case of <sup>10</sup>BPA administration</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x7.png"/></fig><p>cell and to damage these area due to <sup>10</sup>B(n, α)<sup>7</sup>Li reaction (<xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>Distance r<sub>0</sub> and 2r were defined as α range and distance between boron atoms in the figure. There are two conditions of boron atom exists beyond the α range (r<sub>0</sub> ≤ r) (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)) and boron atoms within α range (r<sub>0</sub> &gt; r) mainly investigated in present study (<xref ref-type="fig" rid="fig2">Figure 2</xref>(c)).</p><p>In the case study of (c), there is the duplicate volume V<sub>d</sub>, where is exposed under duplicated irradiation by α particles from the both side of boron atoms.</p><p>Here, we postulate the correlation between the CBE factor and V<sub>d</sub> in the case of (c) as;</p><disp-formula id="scirp.52141-formula249"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x8.png"  xlink:type="simple"/></disp-formula><p>where proximity F is the number of boron atoms surrounding to in the centered born atom and the geometric duplicated volume of V<sub>d</sub> is given by the formula of the volume of spherical cap with r<sub>0</sub> and r;</p><disp-formula id="scirp.52141-formula250"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x9.png"  xlink:type="simple"/></disp-formula><p>Here, V<sub>d</sub> is normalized by the volume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8902044x10.png" xlink:type="simple"/></inline-formula> given as the α range volume, and the normalized duplicate volume V<sub>dnor</sub> can be expressed as the ratio of V<sub>d</sub> and V<sub>0</sub> (<xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><disp-formula id="scirp.52141-formula251"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x11.png"  xlink:type="simple"/></disp-formula><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Images of irradiation damage and its effective area caused by (a) γ ray, α particle irradiation due to <sup>10</sup>B(n, α)<sup>7</sup>Li reaction in the (b) access distance (r<sub>0</sub> &lt; r) and (c) distance of closet approach (r<sub>0</sub> &gt; r) between boron atoms.</title></caption><fig id ="fig2_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x12.png"/></fig></fig-group><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Definition of (a) the duplicate volume of spherical cap of two α range volumes and (b) the change in the duplication volune as a function of the distance between boron atoms.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x13.png"/></fig></fig-group></sec><sec id="s2_2_2"><title>2.2.2. Space Factor n</title><p>After BPA administration, bio-distribution of <sup>10</sup>B atoms is provided into a cell (<xref ref-type="fig" rid="fig4">Figure 4</xref>) and boron atoms become closer with each other, but exist beyond α range in the case of <xref ref-type="fig" rid="fig4">Figure 4</xref>(a).</p><p>In contrast to this case, boron atoms are spatially-integrated selectively in a cell as BPA administration pro- ceeds, very high dose of boron concentration is achieved as shown in the <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(c).</p><p>Therefore, it can be assumed that there is a relationship between boron concentration N and distance of boron atoms r within the limited volume and space of cells (20 - 200 μm);</p><disp-formula id="scirp.52141-formula252"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x14.png"  xlink:type="simple"/></disp-formula><p>Thus, we expressed the relationship between normalized boron concentration N/N<sub>th</sub> and normalized r/r<sub>0</sub> here as;</p><disp-formula id="scirp.52141-formula253"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x15.png"  xlink:type="simple"/></disp-formula><p>where n is the space factor (=1, 2, 3) and N<sub>th</sub> is the threshold of N.</p><p>From Equation (3) and (5), V<sub>dnol</sub> in Equation (3) is replaced as;</p><disp-formula id="scirp.52141-formula254"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x16.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2_3"><title>2.2.3. Definition of the Deterministic Parsing CBE Factor Model</title><p>From Equations (1) and (6), we defined the deterministic parsing CBE factor model as;</p><disp-formula id="scirp.52141-formula255"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x17.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52141-formula256"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x18.png"  xlink:type="simple"/></disp-formula><p>where N<sub>max</sub> is the saturated boron concentration mentioned-below and CBE<sub>0</sub>, F and n are constants.</p></sec></sec><sec id="s2_3"><title>2.3. Theoretical Calculation Method and Its Procedure</title><p>Iterative calculation technique was applied to obtain constants CBE<sub>0</sub>, F, n and the eigen values of N<sub>th</sub> in Equation (7) for each cases (<xref ref-type="fig" rid="fig5">Figure 5</xref>).</p><p>We started iteration calculation with data set of (N<sub>max</sub>, CBE) in <xref ref-type="table" rid="table1">Table 1</xref> and arbitrary values of CBE<sub>0</sub>, F and n in Equation (7) to obtain N<sub>th</sub> value, where n was give as a number of 1 - 3 (process (a)). With the calculation results of N<sub>th</sub> value obtained in each cases, first data set was rewritten as (N<sub>th</sub>/N<sub>max</sub>, CBE) and calculated again to optimize constants CBE<sub>0</sub> and F in the equation by least square method with these new data set (process (b)). Then, these calculation processes were terminated when the identical calculated CBE values to the original CBE values were obtained.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Concentration process of boron atoms into cell after BPA administration</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x19.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Iterative calculation process to obtain constants CBE<sub>0</sub>, F, n and eigen value N<sub>th</sub> in Equation (7)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x20.png"/></fig></sec></sec><sec id="s3"><title>3. Results and Discussions</title><sec id="s3_1"><title>3.1. The CBE Factor Model for Normal Tissues and Tumor</title><p>The calculated CBE values obtained by the above-mentioned theoretical calculation procedure are listed with the original CBE values in the table (<xref ref-type="table" rid="table2">Table 2</xref>).</p><p>According to <xref ref-type="table" rid="table2">Table 2</xref>, it was found that the calculated CBE values obtained are almost identical to the original CBE factors, when CBE<sub>0</sub>, F and n are selected as 0.5, 8 and 3, respectively. Threshold values, N<sub>th</sub> given by this calculation method are also listed for all cases in this table.</p><p>With these results, the original CBE factors are plotted as a function of the ratio, N<sub>th</sub>/N<sub>max</sub> and the solid line in this figure was provided by Equation (7) (<xref ref-type="fig" rid="fig6">Figure 6</xref>).</p><p>It is clear that there is a good correlation between the original CBE factors and N<sub>th</sub>/N<sub>max</sub> for all cases including tumor and it is concluded that the original CBE factors can be well expressed by Equation (7) with a parameter N<sub>th</sub>/N<sub>max</sub>.</p><p>Here we emphasise that the a threshold N<sub>th</sub> exists to surmount the potential barrier of BPA concentration, for which less than N<sub>th</sub>, remarkable damages by α particles cannot occur in BNCT [<xref ref-type="bibr" rid="scirp.52141-ref15">15</xref>] .</p></sec><sec id="s3_2"><title>3.2. Definition of Three Constants in the CBE Factor Model</title><sec id="s3_2_1"><title>3.2.1. Determination of the CBE Factor Depend on Boron Dose Level</title><p>The CBE<sub>0</sub> was defined as a intercept constant in Equation (7) and the CBE factor is given by CBE<sub>0</sub> value, which is determined as 0.5 for each intracellular distribution patterns (<xref ref-type="fig" rid="fig7">Figure 7</xref>).</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The results of iterative calculation of the CBE factor model presented in Equation (7)</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >No.</th><th align="center" valign="middle"  rowspan="2"  >Tissue</th><th align="center" valign="middle" >N<sub>max</sub></th><th align="center" valign="middle" >N<sub>th</sub></th><th align="center" valign="middle" >CBE</th><th align="center" valign="middle" >CBE</th><th align="center" valign="middle"  rowspan="2"  >N<sub>th</sub>/N<sub>max</sub></th></tr></thead><tr><td align="center" valign="middle" >(μg/g)</td><td align="center" valign="middle" >(μg/g)</td><td align="center" valign="middle" >Factor</td><td align="center" valign="middle" >(Calc.)</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Tumor</td><td align="center" valign="middle" >72</td><td align="center" valign="middle" >8.71</td><td align="center" valign="middle" >3.8</td><td align="center" valign="middle" >3.81</td><td align="center" valign="middle" >0.121</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >Normal skin tissue</td><td align="center" valign="middle" >28.8</td><td align="center" valign="middle" >7.2</td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >0.25</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >Normal brain tissue</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >9.3</td><td align="center" valign="middle" >1.34</td><td align="center" valign="middle" >1.35</td><td align="center" valign="middle" >0.465</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >Normal oral mucosal tissue</td><td align="center" valign="middle" >21.5</td><td align="center" valign="middle" >1.27</td><td align="center" valign="middle" >4.87</td><td align="center" valign="middle" >4.87</td><td align="center" valign="middle" >0.059</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >Normal liver tissue</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >2.21</td><td align="center" valign="middle" >4.25</td><td align="center" valign="middle" >4.25</td><td align="center" valign="middle" >0.092</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >Normal lung tissue</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >6.67</td><td align="center" valign="middle" >2.3</td><td align="center" valign="middle" >2.31</td><td align="center" valign="middle" >0.278</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >Normal heart tissue</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >11.14</td><td align="center" valign="middle" >1.35</td><td align="center" valign="middle" >1.35</td><td align="center" valign="middle" >0.464</td></tr></tbody></table></table-wrap><disp-formula id="scirp.52141-formula257"><graphic  xlink:href="http://html.scirp.org/file/11-8902044x21.png"  xlink:type="simple"/></disp-formula><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Deterministic parsing Model for the CBE factor with N<sub>th</sub>/N<sub>max</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x22.png"/></fig><fig-group id="fig7"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> The CBE factor defined by CBE<sub>0</sub> constant in the cases of intracellular distribution of boron. (a) r &lt; r<sub>0</sub>; (b) r = r<sub>0</sub>; (c) r &gt; r<sub>0</sub>.</title></caption><fig id ="fig7_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x23.png"/></fig></fig-group><p>In the figure, pattern a) is correspondent to lower boron concentration and boron atoms are distributed in a cell in heterogeneous condition. This condition can be defined in the case of r &gt; r<sub>0</sub> in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) and each boron atom induces irradiation damages individually and significant damage is not expected because of lack of boron concentration in the affected area. As BPA administration proceeding, born concentration increases to the level of conditions b) and c) in the figure. The condition b) is homogeneous and critical case of r = r<sub>0</sub>, in which boron dose N reaches to the threshold value N<sub>th</sub> (N = N<sub>th</sub>). In both cases of a) and b), the CBE factors are expected to be small value and given as constant level of CBE<sub>0</sub>.</p><p>In contrast with these conditions, the condition c) is homogeneous over-packed case and correspond to r &lt; r<sub>0 </sub>(N &gt; N<sub>th</sub>) in <xref ref-type="fig" rid="fig2">Figure 2</xref>(c). In this case, the CBE factor can be expressed by boron concentration N in Equation (7).</p><p>Therefore, the CBE factor can be defined by CBE<sub>0</sub> as following;</p><disp-formula id="scirp.52141-formula258"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-8902044x24.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_2_2"><title>3.2.2. Sterically-Oriented Intracellular Distribution of Boron Atom</title><p>There are many types of sterically congested mode of <sup>10</sup>B atom distribution (<xref ref-type="fig" rid="fig8">Figure 8</xref>). Here, confront factor F in Equation (7) is defined as a sterically-oriented number of boron atoms surrounding center boron atom and is given as 8 in previous caption (2.1).</p><p>F = 8 (10)</p><p>This result indicates that the data case in present study is corresponding to octahedron type and 8 boron atoms confronted to the center boron atom (<xref ref-type="fig" rid="fig8">Figure 8</xref>(d)).</p><p>Higher mode pattern also suggests a higher level of boron concentration under surgically observation and it is interest that proximity F informs sterically-oriented intracellular distribution of boron atom concentrated in the affected area.</p></sec><sec id="s3_2_3"><title>3.2.3. Intracellular Cubic Array of Boron Atom</title><p>To define the relationship between the distance between boron atoms in a limited cell space, space factor n was adopted in Equation (5). There are allowable three patterns of space factor under the Equation (5) (<xref ref-type="fig" rid="fig9">Figure 9</xref>).</p><p>The space factor n = 1, 2 and 3 addresses liner, planar and stereo type cubic array, respectively. The space factor n is calculated as 3 in caption (2.1), this fact indicates that high level of boron concentration are achieved by stereo type cubic array formed after BPA administration in normal tissues and tumor cases.</p><p>n = 3 (11)</p><p>The space factor n suggests cubic array structural extension of intracellular boron concentration, whereas F implied sterically-oriented intracellular proximity above-mentioned.</p><p>Two of these constant F and n are very important parameters to well-understanding boron concentration in normal tissues and tumor and to determine the effectiveness of BNCT.</p></sec></sec><sec id="s3_3"><title>3.3. Application of the CBE Factor Model for Human Brain Tumor</title><p>It is evident that the CBE factors for BPA, calculated using Equation (7) are the almost same values with those obtained in previous animal experiments [<xref ref-type="bibr" rid="scirp.52141-ref10">10</xref>] - [<xref ref-type="bibr" rid="scirp.52141-ref13">13</xref>] and well expressed without distinction of tissues and tumor. Considered overall, the CBE factor is given as a function of boron concentration ratio, N<sub>th</sub>/N<sub>max</sub>.</p><p>In this section, we applied this calculation method to estimate the CBE factors for many types of human brain tumor.</p><p>Imahori reported dynamic PET analysis of 33 brain tumor patients contained of AII (8 patients), AIII (11) and GBM (14 Glio Blastoma Multiforme) [<xref ref-type="bibr" rid="scirp.52141-ref16">16</xref>] and presented typical change in <sup>10</sup>B concentration of blood, brain tumor and normal brain measured by dynamical PET technique during L-BPA-18F administration (<xref ref-type="fig" rid="fig1">Figure 1</xref>0).</p><p>To determine the CBE factor, the values of N<sub>th</sub> and N<sub>max</sub> can be derived from the points on these typical dynamic PET curves. The N<sub>th</sub> values were determined at the intersection points of two of fitting lines on <sup>10</sup>B concentration curves in low dose level and N<sub>max</sub> values were defined at the peak value of the curves, respectively.</p><p>With these N<sub>th</sub> and N<sub>max</sub> data, the CBE factors were calculated by Equation (7) for all grade of brain tumor (<xref ref-type="fig" rid="fig1">Figure 1</xref>1).</p><fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Typical intracellular distribution pattern of proximity F. (a) Dihedral; (b) Tetrahedron; (c) Hexahedron; (d) Octahedron.</title></caption><fig id ="fig8_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x25.png"/></fig></fig-group><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Intracellular cubic array of boron atom as a function of r/r<sub>0</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x26.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Typical change in <sup>10</sup>B concentration of brain tumour, blood and normal brain measured by dynamic PET technique</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x27.png"/></fig><p>From these results, it is found that all of these CBE factors on the lime of the CBE factor model in Equation (7), increases with tumor grade and categorized into three groups. These data were re-plotted to show more precise relationship between the CBE factor and tumor grade (<xref ref-type="fig" rid="fig1">Figure 1</xref>2).</p><p>It is found that the CBE factors for AII and AIII vary widely whereas values for GBM display small variation and the same level of the CBE factor range of AIII.</p><p>After BPA administration, boron atoms are ingested into the cell model consisted of endoplasm and cell nucleus and Imahori reported [<xref ref-type="bibr" rid="scirp.52141-ref16">16</xref>] the kinetic analysis for these brain tumor patients by the Gjeddl-Patlak model [<xref ref-type="bibr" rid="scirp.52141-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.52141-ref18">18</xref>] using three-compartment rate constants (K<sub>1</sub>, k<sub>2</sub> and k<sub>3</sub>) (<xref ref-type="fig" rid="fig1">Figure 1</xref>3).</p><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> CBE factors calculated by CBE factor model in Equation (7) for three grade of brain tumour patients as a function of N<sub>th</sub>/N<sub>max</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x28.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Distribution of the CBE factor range of brain tu- mour grade</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x29.png"/></fig><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> The rate constants of three compartment model for 33 brain tumor patients</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8902044x30.png"/></fig><p>From the results, it is found that rate constant K<sub>1</sub> into cell increases drastically as tumor grade proceeding, whereas k<sub>3</sub> into cell nucleus decreases. This result means that the damage on toughness of these membranes deteriorates blocking capability and retention of BPA in cells due to attack of tumor to membrane of cell and nucleus, especially in GBM [<xref ref-type="bibr" rid="scirp.52141-ref16">16</xref>] .</p><p>This fact indicated that the effectiveness of BNCT treatment achieves improvement in the brain tumor patients of grade AII and AIII, however its effectiveness is saturated for the grade of GBM.</p></sec><sec id="s3_4"><title>3.4. Application of the Calculation Method and Its Clinical Significance</title><p>Normally, cancer patients are given low doses of intravenous radioactively-labelled 18F-BPA before BNCT and diagnosed cancer by Positron-Emission-Tomography (PET). Physicians developed a treatment plan by BNCT based on PET diagnosis and then after administrates high dose of BPA to the patients.</p><p>In present paper, we emphasized existence of N<sub>th</sub> and showed a calculation method of the CBE factor with N<sub>th</sub>/N<sub>max</sub> in caption (2.1). Here, the most important thing for this calculation run is how to determined N<sub>th</sub> and N<sub>max</sub> values, and we presented N<sub>th</sub> and N<sub>max</sub> determination method in the case of brain tumor measured by dynamic PET technique in caption (2.3).</p><p>In practical use of this calculation method, 18F-BPA and BPA two-in-one medical mixture should be administrated into body and a small increment change of BPA concentration in tumor and normal tissue should be measured by dynamic PET technique simultaneously, as shown in the <xref ref-type="fig" rid="fig1">Figure 1</xref>0. Then, N<sub>th</sub> and N<sub>max</sub> for tumor and normal tissue can be determined respectively, and the CBE factors for tumor and normal tissue can be defined by the calculation formula in Equation (7).</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>In present study, deterministic parsing model of the CBE factor for intracellular <sup>10</sup>B distribution was proposed in the following equation and at pretty much the same values as original CBE factor were obtained by the calculation to the original CBE factors for normal tissues and tumor by iteration calculation technique.</p><disp-formula id="scirp.52141-formula259"><graphic  xlink:href="http://html.scirp.org/file/11-8902044x31.png"  xlink:type="simple"/></disp-formula><p>In this equation, constants values of CBE<sub>0</sub>, F and n are key factors for well-understanding of <sup>10</sup>B structural distribution in the cells analytically derived as 0.5,8 and 3 respectively in present study.</p><p>This CBE factor model was applied to human tumor brain cases and derived good results dovetailed with empirical facts.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.52141-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Bayanov, B., Belov, V., Kindyuk, V., Oparin, E. and Taskaev, S. 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