<?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.2015.68083</article-id><article-id pub-id-type="publisher-id">JCT-58899</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>
 
 
  Determination of the Compound Biological Effectiveness (CBE) Factors Based on the &lt;i&gt;ISHIYAMA-IMAHORI&lt;/i&gt; Deterministic Parsing Model with the Dynamic PET Technique
 
</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"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yoshio</surname><given-names>Imahori</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jun</surname><given-names>Itami</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hanna</surname><given-names>Koivunoro</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Quantum Beam Science Center, Japan Atomic Energy Agency, Tokai-mura, Naka-gun, Ibaraki, Japan</addr-line></aff><aff id="aff3"><addr-line>Department of Radiation Oncology, National Cancer Center, Tsukiji, Chuo-ku, Tokyo, Japan</addr-line></aff><aff id="aff2"><addr-line>Cancer Intelligence Care Systems, Inc., Koto-ku, Ariake, Tokyo, Japan</addr-line></aff><aff id="aff4"><addr-line>Department of Oncology,Helsinki University Central Hospital, Helsinki, Finland</addr-line></aff><pub-date pub-type="epub"><day>28</day><month>07</month><year>2015</year></pub-date><volume>06</volume><issue>08</issue><fpage>759</fpage><lpage>766</lpage><history><date date-type="received"><day>18</day>	<month>July</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>16</month>	<year>August</year>	</date><date date-type="accepted"><day>19</day>	<month>August</month>	<year>2015</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 proposed a deterministic parsing model (ISHIYAMA-IMAHORI 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 a specific method of how the application of the case of application to actual patient data, which is founded on this model for tissues and tumor. Method: To determine the CBE factor, we derived 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_c5457c69-5d05-4340-9225-38322db5796c.bmp" alt="" /> (1), where, N<sub>th</sub> and N<sub>max</sub> are the threshold value of boron concentration of N and saturation boron density and CBE<sub>0</sub>, F and n are given as 0.5, 8 and 3, respectively. In order to determine N<sub>th</sub> and N<sub>max</sub> in the formula, sigmoid logistic function was employed for <sup>10</sup>B concentration data, D<sub>b</sub>(t) obtained by dynamic PET technique. <img src="Edit_12b6c9f7-1cc3-40ab-b404-1d6bea28e675.bmp" alt="" /> (2), where, A, a and t<sub>0</sub> are constants. Results and Conclusion: From the application of sigmoid function to dynamic PET data, it is concluded that the N<sub>th</sub> and N<sub>max</sub> for tissue and tumor are identified with the parameter constants in the sigmoid function in Equation (2) as: <img src="Edit_768bae3d-6756-42e0-ba09-d80321b4c094.bmp" alt="" /> (3). And the calculated CBE factor values obtained from Equation (1), with N<sub>th</sub>/N<sub>max</sub>. 
 
</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(n</kwd><kwd> α)&lt;sup&gt;7&lt;/sup&gt;Li</kwd><kwd> Sigmoid Function</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.58899-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.58899-ref3">3</xref>] and many inventions for the progressive power run-up were reported [<xref ref-type="bibr" rid="scirp.58899-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.58899-ref5">5</xref>] . In Japan, implemented deployment of accelerator-driven neutron source for Boron Neutron Capture Therapy (BNCT) was accomplished 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.58899-ref6">6</xref>] . BNCT is extensively reviewed in two recent articles [<xref ref-type="bibr" rid="scirp.58899-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.58899-ref8">8</xref>] and the targeting effectiveness of BNCT is 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.58899-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><disp-formula id="scirp.58899-formula397"><graphic  xlink:href="http://html.scirp.org/file/15-8902185x8.png"  xlink:type="simple"/></disp-formula><p>The CBE factors concerning to tumor, skin lung, liver [<xref ref-type="bibr" rid="scirp.58899-ref10">10</xref>] - [<xref ref-type="bibr" rid="scirp.58899-ref12">12</xref>] and oral mucosal tissues [<xref ref-type="bibr" rid="scirp.58899-ref13">13</xref>] are reported and prospect of actually using BNCT for the patients has been developing under the right circumstances. 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>Recently, the authors proposed deterministic parsing model of CBE factors (ISHIYAMA-IMAHORI model) and applied to human tumor brain cases and derived good results dovetailed with empirical facts [<xref ref-type="bibr" rid="scirp.58899-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.58899-ref15">15</xref>] .</p><p>The purpose of the present investigation was to demonstrate 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 Measurement of BPA by Dynamic PET Technique</title><p>33 brain tumor patients (grade AII (8 patients), AIII (11) and GBM (14)) were given low dose (approximately ~ 100 μg/g) of intravenous radioactively-labeled <sup>18</sup>F-BPA before BNCT and diagnosed cancer by Positron-Emis- sion-Tomography (PET) [<xref ref-type="bibr" rid="scirp.58899-ref16">16</xref>] . To obtain <sup>10</sup>B concentration in a body, <sup>18</sup>F-BPA was administrated to the patient by intravenous drip injection and PET inspection was performed in every 20 minutes to measure a change in <sup>10</sup>B concentrations in tumor, normal and blood of the patient, respectively.</p></sec><sec id="s2_2"><title>2.2. Mathematical Analysis Model for the <sup>10</sup>B Concentration Data</title><p>After <sup>10</sup>BPA administration, boron atoms are ingested into the cell model consisted of endoplasm and cell nucleus and Imahori [<xref ref-type="bibr" rid="scirp.58899-ref17">17</xref>] reported the kinetic analysis for brain tumor patients by using three-compartment rate constant (K<sub>1</sub>, k<sub>2</sub> and k<sub>3</sub>) (<xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>This model implied that the body injected <sup>10</sup>BPA begins to rapidly up-taken into cancer cell group at the injection initial and eventually suppressed increase with increasing <sup>10</sup>BPA-containing population.</p><p>As a function that can better represent this phenomenon, the sigmoid function are frequently applied as natural population increasing model. Accordingly, logistic function based on the sigmoid function was employed to analyze dynamic PET data. The logistic function in present study was defined as:</p><disp-formula id="scirp.58899-formula398"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-8902185x9.png"  xlink:type="simple"/></disp-formula><p>where D<sub>b</sub><sub>normal</sub> and D<sub>b</sub><sub>tumor</sub> are <sup>10</sup>B concentrations in tumor, normal tissues and time-dependent function. A, a and t<sub>0</sub> in Equation (1) are constants, respectively. Iteration calculation technique was employed to obtain constants A, a and t<sub>0</sub> in Equation (1) for normal tissue and tumor cases, respectively [<xref ref-type="bibr" rid="scirp.58899-ref15">15</xref>] .</p></sec></sec><sec id="s3"><title>3. Results</title><sec id="s3_1"><title>3.1. Dynamic PET Measurement for Normal Tissues and Tumor</title><p>Typical changes in <sup>10</sup>B concentration in normal tissue, tumor and blood of a BGM patient are illustrated in the figure by <sup>10</sup>BPA administration by intravenous and drip injection methods (<xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>Sudden increase and peak in <sup>10</sup>B concentration in blood, normal tissue and tissue were found just before intravenous injection of BPA administration. Whereas, the changes in <sup>10</sup>BPA concentration after drip injection show modest slow changes in <sup>10</sup>B concentration in normal tissues, tumor and blood, respectively (<xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>These typical changes after <sup>10</sup>BPA administration indicate compatibility to define saturation boron concentra- tion, N<sub>max</sub> and threshold of boron density, N<sub>th</sub> for the determination of CBE factors by ISHIYAMA IMAHORI model [<xref ref-type="bibr" rid="scirp.58899-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.58899-ref15">15</xref>] as below:</p><disp-formula id="scirp.58899-formula399"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-8902185x10.png"  xlink:type="simple"/></disp-formula><p>and this is because that we chose drip injection in present study.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Gjeddle-Patlak model using three-compartment rate constants (K<sub>1</sub>, k<sub>2</sub> and k<sub>3</sub>)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-8902185x11.png"/></fig><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Typical change in <sup>10</sup>B concentration in tumor, normal tissues and blood measured by dynamic PET technique with <sup>10</sup>BPA administration by (a) intraveous injection and (b) drip injection methods.</title></caption><fig id ="fig2_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-8902185x12.png"/></fig></fig-group><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Change in <sup>10</sup>B concentration in blood, tumor and normal tissue measured by dynamic PET technique</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-8902185x13.png"/></fig><p>As for a typical change in <sup>10</sup>B concentration in blood, tumor and normal tissue of a brain tumor patient (Grade IV), logistic function in Equation (1) was applied to these data. Compatibility of the function to normal tissue and tumor are provided in <xref ref-type="fig" rid="fig4">Figure 4</xref> and <xref ref-type="fig" rid="fig5">Figure 5</xref>.</p><p>From these results, it is clear that very good data fitting curves of the logistic function to dynamic PET data were observed and each constant in Equation (1) are obtained in the tumor and normal tissue. These results are listed in <xref ref-type="table" rid="table1">Table 1</xref>.</p></sec><sec id="s3_2"><title>3.2. Determination of the CBE Factor Depend on Boron Dose Level</title><p>To obtained threshold and saturation density of boron, N<sub>th</sub> and N<sub>max</sub> in tumor and normal tissue from Equation (1), we defined N<sub>th</sub> and N<sub>max</sub> as follows:</p><disp-formula id="scirp.58899-formula400"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-8902185x14.png"  xlink:type="simple"/></disp-formula><p>These values of N<sub>th</sub>, N<sub>max</sub> and N<sub>th</sub>/N<sub>max</sub> for normal tissue and tumor are listed in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>From these results, The CBE factors for normal tissue and tumor in a brain tumor patient were calculated by Equation (2) and these results are given in <xref ref-type="table" rid="table3">Table 3</xref>.</p></sec></sec><sec id="s4"><title>4. Discussions</title><sec id="s4_1"><title>4.1. The CBE Factors Estimations by the Severity of the Brain Tumor</title><p>The difference between the previous report [<xref ref-type="bibr" rid="scirp.58899-ref15">15</xref>] and this paper mainly lies in the definition of the N<sub>th</sub> from the dynamic PET curves. From dynamic PET curves of 33 brain tumor patients contained of AII (8 patients), AII (11) and GBM (14) [<xref ref-type="bibr" rid="scirp.58899-ref16">16</xref>] , the CBE factors were calculated by the ISHIYAMA-IMAHORI model (Equation (2)) with definition of N<sub>th</sub>/N<sub>max</sub> by Equations (1) and (3), and plotted in <xref ref-type="fig" rid="fig6">Figure 6</xref>. From these data, it is clearly</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> A change in <sup>10</sup>B concentration in normal tissue measured by dynamic PET technique and logistic function</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-8902185x15.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> A change in <sup>10</sup>B concentration in tuomor measured by dynamic PET technique and logistic function</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-8902185x16.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> CBE factors calculated by ISHIYAMA-IMAHORI model with for three grade of brain tumor 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/15-8902185x17.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Constants in Equation (1) logistic function obtained for tumor and normal tissue</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >A</th><th align="center" valign="middle" >a</th><th align="center" valign="middle" >t<sub>0</sub></th></tr></thead><tr><td align="center" valign="middle" >Tumor</td><td align="center" valign="middle" >52</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >100</td></tr><tr><td align="center" valign="middle" >Normal</td><td align="center" valign="middle" >33</td><td align="center" valign="middle" >0.025</td><td align="center" valign="middle" >120</td></tr></tbody></table></table-wrap><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-8902185x18.png" xlink:type="simple"/></inline-formula>.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The values of N<sub>th</sub> and N<sub>max</sub> defined by Equation (3) for tumor and normal tissue</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >N<sub>th</sub></th><th align="center" valign="middle" >N<sub>max</sub></th></tr></thead><tr><td align="center" valign="middle" >Tumor</td><td align="center" valign="middle" >0.935</td><td align="center" valign="middle" >52</td></tr><tr><td align="center" valign="middle" >Normal</td><td align="center" valign="middle" >1.565</td><td align="center" valign="middle" >33</td></tr></tbody></table></table-wrap><p>N<sub>th</sub> = D at t = 0; N<sub>max</sub> = A.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> The values of N<sub>th</sub>/N<sub>max</sub> and CBE factor defined by Equation (2) for tumor and normal tissue</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >N<sub>th</sub>/N<sub>max</sub></th><th align="center" valign="middle" >CBE</th></tr></thead><tr><td align="center" valign="middle" >Tumor</td><td align="center" valign="middle" >0.018</td><td align="center" valign="middle" >6.97</td></tr><tr><td align="center" valign="middle" >Normal</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" >6.20</td></tr></tbody></table></table-wrap><p>categorized into three groups corresponding to the severity of the three grades and it can be given as individual numerical values for the individual patient in the same group.</p></sec><sec id="s4_2"><title>4.2. Application of ISHIYAMA-IMAHORI Model to Other Cancer Affected Area Position</title><p>The ISHIYAMA-IMAHORI model can provide CBE factors about not only brain tumors, also cancer affected part of a different site by 18F-BPA dynamic PET measuring technique. Typical lung cancer that can be observed by PET with 18F-BPA was shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. There is a ling cancer (adenocarcinoma) in lower right lung field and the diaphragm just above, but no metastasis to the brain in this case.</p><p>From dynamic PET curve obtained in this case, N<sub>th</sub> and N<sub>max</sub> values can be determined from temporal change in the color intensity of the target diseased part from the Equations (1) and (3), and the CBE factor in this case was evaluated as 6.35 from the ISHIYAMA-IMAHORI model.</p></sec><sec id="s4_3"><title>4.3. Application of the Calculation Method and Its Clinical Significance</title><p>The charm of the BNCT treatment is that again and again for the same patients and their affected area is capable of irradiation treatment. Therefore, the cure of intractable cancer in a short time by BNCT treatment is not a dream. However, BNCT treatment at this stage is time-consuming due to the following reasons. 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>So practical value of present research is that the diagnosis and treatment cycle can be achieved at the same time shorten with high accuracy.</p><p>Present research results, i.e. by 18F-BPA drip injection administration and dynamic PET measurement method, ISHIYAMA-IMAHORI model immediately provides a high-precision CBE factor and BNCT treatment for a kind of cancer and its severity in patients individual.</p></sec></sec><sec id="s5"><title>5. Conclusions</title><p>ISHIYAMA-IMAHORI model below immediately provides a high-precision CBE factor and BNCT treatment for a kind of cancer and its severity in patients’ individual by 18F-BPA drip injection administration and dynamic PET measurement method</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Typical lung cancer case that can be observed by PET with 18F-BPA</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-8902185x19.png"/></fig><disp-formula id="scirp.58899-formula401"><graphic  xlink:href="http://html.scirp.org/file/15-8902185x20.png"  xlink:type="simple"/></disp-formula><p>And N<sub>th</sub>/N<sub>max</sub> is obtained by the flowing logistic function</p><disp-formula id="scirp.58899-formula402"><graphic  xlink:href="http://html.scirp.org/file/15-8902185x21.png"  xlink:type="simple"/></disp-formula><p>where B<sub>b</sub> is <sup>10</sup>B concentration in tumor and normal tissue, and A, a and t<sub>0</sub> are constants.</p></sec><sec id="s6"><title>Cite this paper</title><p>ShintaroIshiyama,YoshioImahori,JunItami,HannaKoivunoro, (2015) Determination of the Compound Biological Effectiveness (CBE) Factors Based on the ISHIYAMA-IMAHORI Deterministic Parsing Model with the Dynamic PET Technique. 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