<?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">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1111081</article-id><article-id pub-id-type="publisher-id">OALibJ-130525</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Mass Stopping Power and Range of Alpha Particles in Biological Human Body (Water and Eye Lens Tissue)
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Arwa</surname><given-names>Alshibel</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>Khalda</surname><given-names>T. Osman</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Physics, College of Sciences, Qassim University, Buraidah, Saudi Arabia</addr-line></aff><pub-date pub-type="epub"><day>03</day><month>01</month><year>2024</year></pub-date><volume>11</volume><issue>01</issue><fpage>1</fpage><lpage>18</lpage><history><date date-type="received"><day>6,</day>	<month>December</month>	<year>2023</year></date><date date-type="rev-recd"><day>14,</day>	<month>January</month>	<year>2024</year>	</date><date date-type="accepted"><day>17,</day>	<month>January</month>	<year>2024</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>
 
 
  We used the MATLAB Program to calculate the mass stopping power and range of alpha particles in biological human body tissues (such as water and the eye lens tissues) at energies between 0.2 and 200 MeV. The Bethe Block formula was used to calculate the mass stopping power, and the simple integration (continuous slowing down approximation) method was used to calculate the alpha particle ranges. Empirical formulae were developed to determine mass-stopping power and ranges of water and eye lens tissues. The results of graphing the mass-stopping power versus energy and range versus energy are presented, and compared the ASTAR (Alpha Stopping Power and Range) results with the present results for the mass-stopping powers and ranges of water. The results indicated remarkable agreement, particularly for energies that extend from 2 to 200 MeV, with a percentage deviation error of 4.81% - 6.39%. A graphical representation of the mass stopping power of water and eye lens tissue with their compositions is also provided. In addition, various radiation parameters essential in cancer treatment, such as absorbed dose, equivalent dose, effective dose, alpha particle depth, and linear energy transfer, are computed in this study.
 
</p></abstract><kwd-group><kwd>Human Body Tissues</kwd><kwd> Alpha Particles</kwd><kwd> MATLAB</kwd><kwd> Mass Stopping Power</kwd><kwd> Range</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>For the last century, scientists have been studying how charged particles interact with matter in order to understand their stopping power and energy dissipation. This research has a wide range of important applications, including ion implantation, fundamental particle physics, nuclear physics, radiation damage, and radiography [<xref ref-type="bibr" rid="scirp.130525-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref4">4</xref>] . As heavy charged particles move through matter, they primarily lose energy through ionization and atomic excitation. This process has been extensively researched and is crucial to various scientific and technological advancements.</p><p>When heavy charged particles travel through matter, they tend to lose energy primarily through ionization and atomic excitation [<xref ref-type="bibr" rid="scirp.130525-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref6">6</xref>] .</p><p>The stopping power is defined as the mean energy loss per unit path length ?dE/dx. It depends on the charge and velocity of the projectile and, of course, the target material [<xref ref-type="bibr" rid="scirp.130525-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref9">9</xref>] . Early investigations of the energy loss of charged particles traversing matter arrive at a general stopping power formula. If an ion beam penetrates through matter, it loses energy due to collisions with electrons (electronic stopping) and target nuclei (nuclear stopping) [<xref ref-type="bibr" rid="scirp.130525-ref1">1</xref>] . The total stopping power is then just the sum of the stopping powers due to electronic and nuclear interactions [<xref ref-type="bibr" rid="scirp.130525-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref6">6</xref>] . At low energies the total energy loss is usually described in terms of electronic stopping power [<xref ref-type="bibr" rid="scirp.130525-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.130525-ref6">6</xref>] . The nuclear component of the stopping power can also be ignored [<xref ref-type="bibr" rid="scirp.130525-ref1">1</xref>] .</p><p>In this work, we will examine the interactions between alpha particles and matter. The mass stopping power of alpha particles will be studied at a range of energies, from 0.2 to 200 MeV. We will also investigate how these interactions affect water and eye lens tissues. Additionally, we will calculate the alpha particle ranges in water and lens tissues at energies between 0.2 and 200 MeV.</p></sec><sec id="s2"><title>2. Stopping Power</title><p>The electronic mass stopping power for alpha particles on water and eye lens tissues is calculated by the Bethe-Bloch formula. The full expression for the Bethe-Bloch formula can be written as:</p><p>− d E d x = 5.08 &#215; 10 − 31 z 2 n β 2 [ F ( β ) − ln I ] (1)</p><p>where: β is v/c where v is the velocity and c is light speed, I is the mean excitation energy and F(β) is given by [<xref ref-type="bibr" rid="scirp.130525-ref10">10</xref>] :</p><p>F ( β ) = ln ln 1.02 &#215; 10 6 β 2 1 − β 2 − β 2 (2)</p><p>The electron density n is calculated by:</p><p>n = N a v 〈 z A 〉 = 6.02 &#215; 10 23 ρ 〈 z A 〉 (3)</p><sec id="s2_1"><title>2.1. Mass Stopping Power of Eye Lens</title><p>The mass stopping power of eye lens tissues is calculated after substituting the appropriate constant of electron density n and mean excitation energy I given in <xref ref-type="table" rid="table1">Table 1</xref> in Equation (1) by the following equation:</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Basic data for calculating mass stopping powers</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n = ρ z N a A (electrons/m<sup>3</sup>)</th><th align="center" valign="middle" >Density (ρ) (g/cm<sup>3</sup>)</th><th align="center" valign="middle" >I (eV)</th><th align="center" valign="middle" ></th><th align="center" valign="middle" >Material</th></tr></thead><tr><td align="center" valign="middle" >3.52987 &#215; 10<sup>29</sup></td><td align="center" valign="middle" >1.070E+00</td><td align="center" valign="middle" >74.3</td><td align="center" valign="middle" >0.54709</td><td align="center" valign="middle" >Eye Lens (ICRU-44)</td></tr><tr><td align="center" valign="middle" >3.34713 &#215; 10<sup>29</sup></td><td align="center" valign="middle" >1.000E+00</td><td align="center" valign="middle" >75.0</td><td align="center" valign="middle" >0.55508</td><td align="center" valign="middle" >Water</td></tr></tbody></table></table-wrap><p>− d E d x ρ = 0.717269584 β 2 &#215; 1.070 [ F ( β ) − 4.308110952 ] (4)</p></sec><sec id="s2_2"><title>2.2. Mass Stopping Power of Water</title><p>The mass stopping power of water is calculated after substituting the appropriate constant of electron density n and mean excitation energy I given in <xref ref-type="table" rid="table1">Table 1</xref> in Equation (1) by the following equation:</p><p>− d E d x ρ = 0.680136816 β 2 &#215; 1.00 [ F ( β ) − 4.317488114 ] (5)</p></sec></sec><sec id="s3"><title>3. Calculation of Alpha Particles Range</title><p>As it passes through the material, the alpha particle’s range ionizes, reducing its energy slowly until it is almost zero. Because of the infinite range of Coulomb, the particle interacts with multiple electrons simultaneously and loses energy gradually but steadily as it moves. Following a predetermined distance, it then runs out of energy. The alpha particle range is the name given to this distance. The alpha particle’s range is therefore defined as the average distance covered before it loses all of its initial kinetic energy [<xref ref-type="bibr" rid="scirp.130525-ref11">11</xref>] .</p><p>The range of charged particle is computed by numerical integration of the stopping power [<xref ref-type="bibr" rid="scirp.130525-ref12">12</xref>] . The range of the alpha particles for the tissues under considerations is calculated using the following relation:</p><p>R = ∫ E 0 E f d E M S ( E ) (6)</p><p>where, E 0 is the initial energy of incident charged particle in material, E f is the final energy of incident charged particle in material and M S ( E ) is the mass stopping power.</p><p>The higher alpha particles energy, the stronger their penetration through a given substance because the more Colombian interactions between the particles of alpha and absorption electrons will be required to dissipate energy before coming to rest [<xref ref-type="bibr" rid="scirp.130525-ref12">12</xref>] . All calculations were done using MATLAB program.</p></sec><sec id="s4"><title>4. Alpha Depths, Absorbed Dose, Equivalent Dose, and Effective Dose</title><p>The Depth</p><p>The depth of a charged particles in the tissue or substance is given by the following relation:</p><p>T = R ρ (7)</p><p>where R is the range and is ρ the density of the tissue or substance.</p><p>Absorbed Dose</p><p>Two different materials, if subjected to the same gamma-ray exposure, will in general absorb different amounts of energy. Because many important phenomena, including changes in physical properties or induced chemical reactions, would be expected to scale as the energy absorbed per unit mass of the material, a unit that measures this quantity is of fundamental interest. The mean energy absorbed from any type of radiation per unit mass of the absorber is defined as the absorbed dose. The historical unit of absorbed dose has been the rad, defined as 100 ergs/gram. As with other historical radiation units, the rad has been replaced by its SI equivalent, the gray (Gy) defined as 1 joule/kilogram. The two units are therefore simply related by: 1 Gy = 100 rad the absorbed dose is a reasonable measure of the chemical or physical effects created by a given radiation exposure in an absorbing material. The absorbed dose is calculated by the following relation:</p><p>A d = E 1   grm 1.6 &#215; 10 − 13   J 1   MeV 10 7   erg 1   J 1   rad 100   erg gram (8)</p><p>Equivalent Dose</p><p>The equivalent dose is calculated by the following relation:</p><p>H T = ∑ R W R &#215; D (9)</p><p>where W R = Weighting factor = 20 for Alpha particle and D is Absorbed dose.</p><p>Effective Dose</p><p>The tissues differ in their sensitivity to the late effects of radiation, which represent the biological responses to the tissue, which are delayed for a long period of time, often several years. The effective dose is used to estimate the incidence of delayed effects in the future. If a part of the body such as the lungs receives a radiation dose, it represents a risk factor of lung cancer. If the same dose is given to another organ, it causes a different risk factor and is called the dose measured by the effective dose, is designated E.</p><p>E = ∑ T W T H T (10)</p><p>where W T is the weighting factor of tissue.</p><p>And for water and eye lens W T = 0.12 .</p></sec><sec id="s5"><title>5. Percentage Deviation Error</title><p>The percentage deviation error for the present results of mass stopping power and that of ASTAR results of water are calculating by the following relation:</p><p>DeviationError = ( PresentResult − ASTARResult ASTARResult ) &#215; 100 % (11)</p><p>the Percentage deviation error was calculated in a <xref ref-type="table" rid="table1">Table 1</xref>3 for the tissues that were compared to the Aster.</p></sec><sec id="s6"><title>6. Results and Discussion</title><p>The Bethe Block theory and the MATLAB application were used in the current work to determine the mass stopping power using Equation (4) and Equation (5). The range of alpha particles in water and eye lens tissues is calculated using Equation (6). <xref ref-type="table" rid="table2">Table 2</xref> shows the elemental composition of water and eye lens. The results of mass stopping powers and range of alpha particles in water, and eye lens respectively are given in <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref>. In <xref ref-type="table" rid="table5">Table 5</xref> a comparison between the present results and that of ASTAR results of mass stopping powers of water are given while a comparison between the present results and that of ASTAR result of alpha particles range for water are given in <xref ref-type="table" rid="table6">Table 6</xref>. <xref ref-type="table" rid="table7">Table 7</xref> is Values of mass stopping power of Water and its compositions and <xref ref-type="table" rid="table8">Table 8</xref> for the Values of mass stopping power of Eye lens and its some of compositions.</p><p>To study the relation between the mass stopping power and the alpha particles energy the graphical method is used as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> for the tissues under consideration. The empirical formula for calculating mass stopping powers knowing alpha particles energy are obtained for all tissues under study as given in <xref ref-type="table" rid="table9">Table 9</xref>. <xref ref-type="fig" rid="fig3">Figure 3</xref> depicts a comparison of the mass stopping power of an alpha particle in water for the current results and those of ASTAR. In <xref ref-type="fig" rid="fig4">Figure 4</xref> and <xref ref-type="fig" rid="fig5">Figure 5</xref> the relationship between the range and alpha particles for the tissues under study are shown while the empirical formula for calculating alpha particles range of all studied tissues is given in <xref ref-type="table" rid="table1">Table 1</xref>0. In <xref ref-type="table" rid="table1">Table 1</xref>1 and <xref ref-type="table" rid="table1">Table 1</xref>2 the calculated depth of alpha particles, LET, absorbed dose, equivalent dose and effective dose of alpha particle for both water and eye lens are given. The percentage deviation errors of mass stopping power for water are given in <xref ref-type="table" rid="table1">Table 1</xref>3.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Elemental composition of water and eye lens</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Composition</th><th align="center" valign="middle" >Material</th></tr></thead><tr><td align="center" valign="middle" >1:0.096000 H 6:0.195000 C 7:0.057000 N 8:0.646000 O 11:0.001000 Na 15:0.001000 P 16:0.003000 S 17:0.001000 Cl</td><td align="center" valign="middle" >Eye Lens (ICRU-44)</td></tr><tr><td align="center" valign="middle" >1:0.111898 H 8:0.888102 O</td><td align="center" valign="middle" >Water</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Values of mass stopping power (MeV∙cm<sup>2</sup>/g) of water and eye lens</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >d E d x ρ ( MeV ⋅ cm 2 g ) Eye lens</th><th align="center" valign="middle" >d E d x ρ ( MeV ⋅ cm 2 g ) Water</th><th align="center" valign="middle" >Energy (MeV)</th></tr></thead><tr><td align="center" valign="middle" >2408.65305062471</td><td align="center" valign="middle" >2384.22475403096</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >3375.76682499890</td><td align="center" valign="middle" >3395.26985256277</td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >3097.31868738319</td><td align="center" valign="middle" >3122.68961199742</td><td align="center" valign="middle" >0.6</td></tr><tr><td align="center" valign="middle" >2773.60364305991</td><td align="center" valign="middle" >2799.21374595122</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >2498.50202763589</td><td align="center" valign="middle" >2523.07437079105</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >1683.53933217218</td><td align="center" valign="middle" >1702.16894269649</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >1291.72133621023</td><td align="center" valign="middle" >1306.61486200367</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >1058.91422947724</td><td align="center" valign="middle" >1071.40076011691</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" >903.055516828838</td><td align="center" valign="middle" >913.861598045919</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >790.624160042245</td><td align="center" valign="middle" >800.185413092180</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >705.273148707949</td><td align="center" valign="middle" >713.871579595160</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >638.030206437612</td><td align="center" valign="middle" >645.859346277533</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >583.537500926490</td><td align="center" valign="middle" >590.736276465791</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >538.386718633458</td><td align="center" valign="middle" >545.058465969393</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >312.624876337861</td><td align="center" valign="middle" >316.595133121707</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >225.355761871248</td><td align="center" valign="middle" >228.250022083824</td><td align="center" valign="middle" >30</td></tr><tr><td align="center" valign="middle" >178.032310775232</td><td align="center" valign="middle" >180.334690817695</td><td align="center" valign="middle" >40</td></tr><tr><td align="center" valign="middle" >148.021536980534</td><td align="center" valign="middle" >149.945174521898</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >127.162424591830</td><td align="center" valign="middle" >128.821123405981</td><td align="center" valign="middle" >60</td></tr><tr><td align="center" valign="middle" >111.759310349188</td><td align="center" valign="middle" >113.221409208821</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >99.8844855919807</td><td align="center" valign="middle" >101.194424044129</td><td align="center" valign="middle" >80</td></tr><tr><td align="center" valign="middle" >90.4296777128844</td><td align="center" valign="middle" >91.6180727928889</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >82.7105618050238</td><td align="center" valign="middle" >83.7994542394653</td><td align="center" valign="middle" >100</td></tr><tr><td align="center" valign="middle" >76.2807946937883</td><td align="center" valign="middle" >77.2866088775882</td><td align="center" valign="middle" >110</td></tr><tr><td align="center" valign="middle" >70.8363332270320</td><td align="center" valign="middle" >71.7716546686581</td><td align="center" valign="middle" >120</td></tr><tr><td align="center" valign="middle" >66.1626241157140</td><td align="center" valign="middle" >67.0373213031586</td><td align="center" valign="middle" >130</td></tr><tr><td align="center" valign="middle" >62.1037638892161</td><td align="center" valign="middle" >62.9257258579161</td><td align="center" valign="middle" >140</td></tr><tr><td align="center" valign="middle" >58.5436331508260</td><td align="center" valign="middle" >59.3192711893148</td><td align="center" valign="middle" >150</td></tr><tr><td align="center" valign="middle" >55.3938980512388</td><td align="center" valign="middle" >56.1284969629590</td><td align="center" valign="middle" >160</td></tr><tr><td align="center" valign="middle" >52.5861224863810</td><td align="center" valign="middle" >53.2840926935507</td><td align="center" valign="middle" >170</td></tr><tr><td align="center" valign="middle" >50.0664326671761</td><td align="center" valign="middle" >50.7314950861815</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >47.7918173890647</td><td align="center" valign="middle" >48.4271415891798</td><td align="center" valign="middle" >190</td></tr><tr><td align="center" valign="middle" >45.7275059064572</td><td align="center" valign="middle" >46.3358150948924</td><td align="center" valign="middle" >200</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Values of range (in g/cm<sup>2</sup>) of water and eye lens</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Range (g/cm<sup>2</sup>) Eye lens</th><th align="center" valign="middle" >Range (g/cm<sup>2</sup>) Water</th><th align="center" valign="middle" >Energy (MeV)</th></tr></thead><tr><td align="center" valign="middle" >1.71824E−05</td><td align="center" valign="middle" >1.71308E−05</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >5.59033E−05</td><td align="center" valign="middle" >5.5658E−05</td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >0.000111467</td><td align="center" valign="middle" >0.000110888</td><td align="center" valign="middle" >0.6</td></tr><tr><td align="center" valign="middle" >0.000181882</td><td align="center" valign="middle" >0.000180834</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >0.000265908</td><td align="center" valign="middle" >0.000264257</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >0.000865136</td><td align="center" valign="middle" >0.000858572</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >0.00172501</td><td align="center" valign="middle" >0.001710535</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >0.002814734</td><td align="center" valign="middle" >0.00278951</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" >0.00411508</td><td align="center" valign="middle" >0.004076382</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >0.00561235</td><td align="center" valign="middle" >0.005557546</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >0.007296056</td><td align="center" valign="middle" >0.007222584</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >0.009157786</td><td align="center" valign="middle" >0.009063144</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >0.011190566</td><td align="center" valign="middle" >0.011072309</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >0.013388481</td><td align="center" valign="middle" >0.013244206</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >0.043559648</td><td align="center" valign="middle" >0.043030551</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >0.086854372</td><td align="center" valign="middle" >0.085729848</td><td align="center" valign="middle" >30</td></tr><tr><td align="center" valign="middle" >0.141722047</td><td align="center" valign="middle" >0.139806674</td><td align="center" valign="middle" >40</td></tr><tr><td align="center" valign="middle" >0.207194516</td><td align="center" valign="middle" >0.204303086</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >0.282582158</td><td align="center" valign="middle" >0.278537097</td><td align="center" valign="middle" >60</td></tr><tr><td align="center" valign="middle" >0.367356877</td><td align="center" valign="middle" >0.361986677</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >0.461095058</td><td align="center" valign="middle" >0.454233224</td><td align="center" valign="middle" >80</td></tr><tr><td align="center" valign="middle" >0.56344569</td><td align="center" valign="middle" >0.554929976</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >0.674110839</td><td align="center" valign="middle" >0.663782684</td><td align="center" valign="middle" >100</td></tr><tr><td align="center" valign="middle" >0.792832893</td><td align="center" valign="middle" >0.780536979</td><td align="center" valign="middle" >110</td></tr><tr><td align="center" valign="middle" >0.919385798</td><td align="center" valign="middle" >0.904969697</td><td align="center" valign="middle" >120</td></tr><tr><td align="center" valign="middle" >1.053568786</td><td align="center" valign="middle" >1.036882674</td><td align="center" valign="middle" >130</td></tr><tr><td align="center" valign="middle" >1.195201767</td><td align="center" valign="middle" >1.176098184</td><td align="center" valign="middle" >140</td></tr><tr><td align="center" valign="middle" >1.344121825</td><td align="center" valign="middle" >1.322455475</td><td align="center" valign="middle" >150</td></tr><tr><td align="center" valign="middle" >1.500180515</td><td align="center" valign="middle" >1.475808098</td><td align="center" valign="middle" >160</td></tr><tr><td align="center" valign="middle" >1.663241735</td><td align="center" valign="middle" >1.636021795</td><td align="center" valign="middle" >170</td></tr><tr><td align="center" valign="middle" >1.833180013</td><td align="center" valign="middle" >1.80297281</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >2.009879121</td><td align="center" valign="middle" >1.976546519</td><td align="center" valign="middle" >190</td></tr><tr><td align="center" valign="middle" >2.193230933</td><td align="center" valign="middle" >2.156636302</td><td align="center" valign="middle" >200</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Comparison of mass stopping power (MeV∙cm<sup>2</sup>/g) of this work and that of ASTAR results for water</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >d E d x ρ ( MeV ⋅ cm 2 g )</th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >A star</td><td align="center" valign="middle"  colspan="2"  >This work (water)</td></tr><tr><td align="center" valign="middle" >1.582E+03</td><td align="center" valign="middle"  colspan="2"  >2384.22475403096</td></tr><tr><td align="center" valign="middle" >2.062E+03</td><td align="center" valign="middle"  colspan="2"  >3395.26985256277</td></tr><tr><td align="center" valign="middle" >2.240E+03</td><td align="center" valign="middle"  colspan="2"  >3122.68961199742</td></tr><tr><td align="center" valign="middle" >2.256E+03</td><td align="center" valign="middle"  colspan="2"  >2799.21374595122</td></tr><tr><td align="center" valign="middle" >2.190E+03</td><td align="center" valign="middle"  colspan="2"  >2523.07437079105</td></tr><tr><td align="center" valign="middle" >1.624E+03</td><td align="center" valign="middle"  colspan="2"  >1702.16894269649</td></tr><tr><td align="center" valign="middle" >1.255E+03</td><td align="center" valign="middle"  colspan="2"  >1306.61486200367</td></tr><tr><td align="center" valign="middle" >1.034E+03</td><td align="center" valign="middle"  colspan="2"  >1071.40076011691</td></tr><tr><td align="center" valign="middle" >8.848E+02</td><td align="center" valign="middle"  colspan="2"  >913.861598045919</td></tr><tr><td align="center" valign="middle" >7.771E+02</td><td align="center" valign="middle"  colspan="2"  >800.185413092180</td></tr><tr><td align="center" valign="middle" >6.949E+02</td><td align="center" valign="middle"  colspan="2"  >713.871579595160</td></tr><tr><td align="center" valign="middle" >6.301E+02</td><td align="center" valign="middle"  colspan="2"  >645.859346277533</td></tr><tr><td align="center" valign="middle" >5.776E+02</td><td align="center" valign="middle"  colspan="2"  >590.736276465791</td></tr><tr><td align="center" valign="middle" >5.340E+02</td><td align="center" valign="middle"  colspan="2"  >545.058465969393</td></tr><tr><td align="center" valign="middle" >3.144E+02</td><td align="center" valign="middle"  colspan="2"  >316.595133121707</td></tr><tr><td align="center" valign="middle" >2.284E+02</td><td align="center" valign="middle"  colspan="2"  >228.250022083824</td></tr><tr><td align="center" valign="middle" >1.815E+02</td><td align="center" valign="middle"  colspan="2"  >180.334690817695</td></tr><tr><td align="center" valign="middle" >1.516E+02</td><td align="center" valign="middle"  colspan="2"  >149.945174521898</td></tr><tr><td align="center" valign="middle" >1.308E+02</td><td align="center" valign="middle"  colspan="2"  >128.821123405981</td></tr><tr><td align="center" valign="middle" >1.155E+02</td><td align="center" valign="middle"  colspan="2"  >113.221409208821</td></tr><tr><td align="center" valign="middle" >1.036E+02</td><td align="center" valign="middle"  colspan="2"  >101.194424044129</td></tr><tr><td align="center" valign="middle" >9.416E+01</td><td align="center" valign="middle"  colspan="2"  >91.6180727928889</td></tr><tr><td align="center" valign="middle" >8.645E+01</td><td align="center" valign="middle"  colspan="2"  >83.7994542394653</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >77.2866088775882</td></tr><tr><td align="center" valign="middle" >7.215E+01</td><td align="center" valign="middle"  colspan="2"  >71.7716546686581</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >67.0373213031586</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >62.9257258579161</td></tr><tr><td align="center" valign="middle" >6.229E+01</td><td align="center" valign="middle"  colspan="2"  >59.3192711893148</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >56.1284969629590</td></tr><tr><td align="center" valign="middle" >5.505E+01</td><td align="center" valign="middle"  colspan="2"  >53.2840926935507</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >50.7314950861815</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >48.4271415891798</td></tr><tr><td align="center" valign="middle" >4.950E+01</td><td align="center" valign="middle"  colspan="2"  >46.3358150948924</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> Comparison of range (in g/cm<sup>2</sup>) of water of this work and ASTAR results</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >Range (cm<sup>2</sup>/g)</th></tr></thead><tr><td align="center" valign="middle" >ASTAR</td><td align="center" valign="middle" >This work (water)</td></tr><tr><td align="center" valign="middle" >2.151E−04</td><td align="center" valign="middle" >1.71308E−05</td></tr><tr><td align="center" valign="middle" >3.230E−04</td><td align="center" valign="middle" >5.5658E−05</td></tr><tr><td align="center" valign="middle" >4.150E−04</td><td align="center" valign="middle" >0.000110888</td></tr><tr><td align="center" valign="middle" >5.034E−04</td><td align="center" valign="middle" >0.000180834</td></tr><tr><td align="center" valign="middle" >5.931E−04</td><td align="center" valign="middle" >0.000264257</td></tr><tr><td align="center" valign="middle" >1.123E−03</td><td align="center" valign="middle" >0.000858572</td></tr><tr><td align="center" valign="middle" >1.829E−03</td><td align="center" valign="middle" >0.001710535</td></tr><tr><td align="center" valign="middle" >2.711E−03</td><td align="center" valign="middle" >0.00278951</td></tr><tr><td align="center" valign="middle" >3.759E−03</td><td align="center" valign="middle" >0.004076382</td></tr><tr><td align="center" valign="middle" >4.967E−03</td><td align="center" valign="middle" >0.005557546</td></tr><tr><td align="center" valign="middle" >6.330E−03</td><td align="center" valign="middle" >0.007222584</td></tr><tr><td align="center" valign="middle" >7.842E−03</td><td align="center" valign="middle" >0.009063144</td></tr><tr><td align="center" valign="middle" >9.500E−03</td><td align="center" valign="middle" >0.011072309</td></tr><tr><td align="center" valign="middle" >1.130E−02</td><td align="center" valign="middle" >0.013244206</td></tr><tr><td align="center" valign="middle" >3.668E−02</td><td align="center" valign="middle" >0.043030551</td></tr><tr><td align="center" valign="middle" >7.452E−02</td><td align="center" valign="middle" >0.085729848</td></tr><tr><td align="center" valign="middle" >1.240E−01</td><td align="center" valign="middle" >0.139806674</td></tr><tr><td align="center" valign="middle" >1.845E−01</td><td align="center" valign="middle" >0.204303086</td></tr><tr><td align="center" valign="middle" >2.557E−01</td><td align="center" valign="middle" >0.278537097</td></tr><tr><td align="center" valign="middle" >3.372E−01</td><td align="center" valign="middle" >0.361986677</td></tr><tr><td align="center" valign="middle" >4.287E−01</td><td align="center" valign="middle" >0.454233224</td></tr><tr><td align="center" valign="middle" >5.300E−01</td><td align="center" valign="middle" >0.554929976</td></tr><tr><td align="center" valign="middle" >6.409E−01</td><td align="center" valign="middle" >0.663782684</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.780536979</td></tr><tr><td align="center" valign="middle" >9.588E−01</td><td align="center" valign="middle" >0.904969697</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.036882674</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.176098184</td></tr><tr><td align="center" valign="middle" >1.333E+00</td><td align="center" valign="middle" >1.322455475</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.475808098</td></tr><tr><td align="center" valign="middle" >1.760E+00</td><td align="center" valign="middle" >1.636021795</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.80297281</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.976546519</td></tr><tr><td align="center" valign="middle" >2.240E+00</td><td align="center" valign="middle" >2.156636302</td></tr></tbody></table></table-wrap><table-wrap id="table7" ><label><xref ref-type="table" rid="table7">Table 7</xref></label><caption><title> Values of mass stopping power (in MeV∙cm<sup>2</sup>/g) of water and its compositions</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Energy (MeV)</th><th align="center" valign="middle"  colspan="3"  >Mass stopping power (MeV∙cm<sup>2</sup>/g)</th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >Water</td><td align="center" valign="middle" >H</td><td align="center" valign="middle"  colspan="2"  >O</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >2384.22475403096</td><td align="center" valign="middle" >6.019E+03</td><td align="center" valign="middle"  colspan="2"  >1.272E+03</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >3395.26985256277</td><td align="center" valign="middle" >7.915E+03</td><td align="center" valign="middle"  colspan="2"  >1.639E+03</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >3122.68961199742</td><td align="center" valign="middle" >8.222E+03</td><td align="center" valign="middle"  colspan="2"  >1.792E+03</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >2799.21374595122</td><td align="center" valign="middle" >7.808E+03</td><td align="center" valign="middle"  colspan="2"  >1.820E+03</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2523.07437079105</td><td align="center" valign="middle" >7.157E+03</td><td align="center" valign="middle"  colspan="2"  >1.777E+03</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1702.16894269649</td><td align="center" valign="middle" >4.588E+03</td><td align="center" valign="middle"  colspan="2"  >1.329E+03</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1306.61486200367</td><td align="center" valign="middle" >3.351E+03</td><td align="center" valign="middle"  colspan="2"  >1.038E+03</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1071.40076011691</td><td align="center" valign="middle" >2.675E+03</td><td align="center" valign="middle"  colspan="2"  >8.602E+02</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >913.861598045919</td><td align="center" valign="middle" >2.242E+03</td><td align="center" valign="middle"  colspan="2"  >7.395E+02</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >800.185413092180</td><td align="center" valign="middle" >1.939E+03</td><td align="center" valign="middle"  colspan="2"  >6.519E+02</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >713.871579595160</td><td align="center" valign="middle" >1.713E+03</td><td align="center" valign="middle"  colspan="2"  >5.845E+02</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >645.859346277533</td><td align="center" valign="middle" >1.538E+03</td><td align="center" valign="middle"  colspan="2"  >5.313E+02</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >590.736276465791</td><td align="center" valign="middle" >1.398E+03</td><td align="center" valign="middle"  colspan="2"  >4.880E+02</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >545.058465969393</td><td align="center" valign="middle" >1.283E+03</td><td align="center" valign="middle"  colspan="2"  >4.520E+02</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >316.595133121707</td><td align="center" valign="middle" >7.238E+02</td><td align="center" valign="middle"  colspan="2"  >2.688E+02</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >228.250022083824</td><td align="center" valign="middle" >5.156E+02</td><td align="center" valign="middle"  colspan="2"  >1.963E+02</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >180.334690817695</td><td align="center" valign="middle" >4.047E+02</td><td align="center" valign="middle"  colspan="2"  >1.564E+02</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >149.945174521898</td><td align="center" valign="middle" >3.353E+02</td><td align="center" valign="middle"  colspan="2"  >1.309E+02</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >128.821123405981</td><td align="center" valign="middle" >2.875E+02</td><td align="center" valign="middle"  colspan="2"  >1.131E+02</td></tr><tr><td align="center" valign="middle" >70</td><td align="center" valign="middle" >113.221409208821</td><td align="center" valign="middle" >2.524E+02</td><td align="center" valign="middle"  colspan="2"  >9.997E+01</td></tr><tr><td align="center" valign="middle" >80</td><td align="center" valign="middle" >101.194424044129</td><td align="center" valign="middle" >2.256E+02</td><td align="center" valign="middle"  colspan="2"  >8.979E+01</td></tr><tr><td align="center" valign="middle" >90</td><td align="center" valign="middle" >91.6180727928889</td><td align="center" valign="middle" >2.043E+02</td><td align="center" valign="middle"  colspan="2"  >8.166E+01</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >83.7994542394653</td><td align="center" valign="middle" >1.870E+02</td><td align="center" valign="middle"  colspan="2"  >7.502E+01</td></tr><tr><td align="center" valign="middle" >110</td><td align="center" valign="middle" >77.2866088775882</td><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >-</td></tr><tr><td align="center" valign="middle" >120</td><td align="center" valign="middle" >71.7716546686581</td><td align="center" valign="middle" >1.552E+02</td><td align="center" valign="middle"  colspan="2"  >6.270E+01</td></tr><tr><td align="center" valign="middle" >130</td><td align="center" valign="middle" >67.0373213031586</td><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >-</td></tr><tr><td align="center" valign="middle" >140</td><td align="center" valign="middle" >62.9257258579161</td><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >-</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >59.3192711893148</td><td align="center" valign="middle" >1.334E+02</td><td align="center" valign="middle"  colspan="2"  >5.418E+01</td></tr><tr><td align="center" valign="middle" >160</td><td align="center" valign="middle" >56.1284969629590</td><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >-</td></tr><tr><td align="center" valign="middle" >170</td><td align="center" valign="middle" >53.2840926935507</td><td align="center" valign="middle" >1.174E+02</td><td align="center" valign="middle"  colspan="2"  >4.792E+01</td></tr><tr><td align="center" valign="middle" >180</td><td align="center" valign="middle" >50.7314950861815</td><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >-</td></tr><tr><td align="center" valign="middle" >190</td><td align="center" valign="middle" >48.4271415891798</td><td align="center" valign="middle" >-</td><td align="center" valign="middle"  colspan="2"  >-</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >46.3358150948924</td><td align="center" valign="middle" >1.053E+02</td><td align="center" valign="middle"  colspan="2"  >4.311E+01</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table8" ><label><xref ref-type="table" rid="table8">Table 8</xref></label><caption><title> Values of mass stopping power (in MeV∙cm<sup>2</sup>/g) of Eye lens and its some of compositions</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Energy (MeV)</th><th align="center" valign="middle"  colspan="5"  >Mass stopping power (MeV∙cm<sup>2</sup>/g)</th></tr></thead><tr><td align="center" valign="middle" >Eye lens</td><td align="center" valign="middle" >H</td><td align="center" valign="middle" >C</td><td align="center" valign="middle" >O</td><td align="center" valign="middle" >N</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >2408.65305062471</td><td align="center" valign="middle" >6.019E+03</td><td align="center" valign="middle" >1.595E+03</td><td align="center" valign="middle" >1.272E+03</td><td align="center" valign="middle" >1.486E+03</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >3375.76682499890</td><td align="center" valign="middle" >7.915E+03</td><td align="center" valign="middle" >1.862E+03</td><td align="center" valign="middle" >1.639E+03</td><td align="center" valign="middle" >1.940E+03</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >3097.31868738319</td><td align="center" valign="middle" >8.222E+03</td><td align="center" valign="middle" >1.906E+03</td><td align="center" valign="middle" >1.792E+03</td><td align="center" valign="middle" >2.086E+03</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >2773.60364305991</td><td align="center" valign="middle" >7.808E+03</td><td align="center" valign="middle" >1.866E+03</td><td align="center" valign="middle" >1.820E+03</td><td align="center" valign="middle" >2.069E+03</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2498.50202763589</td><td align="center" valign="middle" >7.157E+03</td><td align="center" valign="middle" >1.795E+03</td><td align="center" valign="middle" >1.777E+03</td><td align="center" valign="middle" >1.978E+03</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1683.53933217218</td><td align="center" valign="middle" >4.588E+03</td><td align="center" valign="middle" >1.372E+03</td><td align="center" valign="middle" >1.329E+03</td><td align="center" valign="middle" >1.406E+03</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1291.72133621023</td><td align="center" valign="middle" >3.351E+03</td><td align="center" valign="middle" >1.085E+03</td><td align="center" valign="middle" >1.038E+03</td><td align="center" valign="middle" >1.088E+03</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1058.91422947724</td><td align="center" valign="middle" >2.675E+03</td><td align="center" valign="middle" >8.982E+02</td><td align="center" valign="middle" >8.602E+02</td><td align="center" valign="middle" >8.985E+02</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >903.055516828838</td><td align="center" valign="middle" >2.242E+03</td><td align="center" valign="middle" >7.720E+02</td><td align="center" valign="middle" >7.395E+02</td><td align="center" valign="middle" >7.711E+02</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >790.624160042245</td><td align="center" valign="middle" >1.939E+03</td><td align="center" valign="middle" >6.804E+02</td><td align="center" valign="middle" >6.519E+02</td><td align="center" valign="middle" >6.785E+02</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >705.273148707949</td><td align="center" valign="middle" >1.713E+03</td><td align="center" valign="middle" >6.102E+02</td><td align="center" valign="middle" >5.845E+02</td><td align="center" valign="middle" >6.080E+02</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >638.030206437612</td><td align="center" valign="middle" >1.538E+03</td><td align="center" valign="middle" >5.544E+02</td><td align="center" valign="middle" >5.313E+02</td><td align="center" valign="middle" >5.523E+02</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >583.537500926490</td><td align="center" valign="middle" >1.398E+03</td><td align="center" valign="middle" >5.090E+02</td><td align="center" valign="middle" >4.880E+02</td><td align="center" valign="middle" >5.069E+02</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >538.386718633458</td><td align="center" valign="middle" >1.283E+03</td><td align="center" valign="middle" >4.712E+02</td><td align="center" valign="middle" >4.520E+02</td><td align="center" valign="middle" >4.691E+02</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >312.624876337861</td><td align="center" valign="middle" >7.238E+02</td><td align="center" valign="middle" >2.788E+02</td><td align="center" valign="middle" >2.688E+02</td><td align="center" valign="middle" >2.777E+02</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >225.355761871248</td><td align="center" valign="middle" >5.156E+02</td><td align="center" valign="middle" >2.028E+02</td><td align="center" valign="middle" >1.963E+02</td><td align="center" valign="middle" >2.021E+02</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >178.032310775232</td><td align="center" valign="middle" >4.047E+02</td><td align="center" valign="middle" >1.612E+02</td><td align="center" valign="middle" >1.564E+02</td><td align="center" valign="middle" >1.608E+02</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >148.021536980534</td><td align="center" valign="middle" >3.353E+02</td><td align="center" valign="middle" >1.348E+02</td><td align="center" valign="middle" >1.309E+02</td><td align="center" valign="middle" >1.344E+02</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >127.162424591830</td><td align="center" valign="middle" >2.875E+02</td><td align="center" valign="middle" >1.163E+02</td><td align="center" valign="middle" >1.131E+02</td><td align="center" valign="middle" >1.161E+02</td></tr><tr><td align="center" valign="middle" >70</td><td align="center" valign="middle" >111.759310349188</td><td align="center" valign="middle" >2.524E+02</td><td align="center" valign="middle" >1.027E+02</td><td align="center" valign="middle" >9.997E+01</td><td align="center" valign="middle" >1.025E+02</td></tr><tr><td align="center" valign="middle" >80</td><td align="center" valign="middle" >99.8844855919807</td><td align="center" valign="middle" >2.256E+02</td><td align="center" valign="middle" >9.214E+01</td><td align="center" valign="middle" >8.979E+01</td><td align="center" valign="middle" >9.197E+01</td></tr><tr><td align="center" valign="middle" >90</td><td align="center" valign="middle" >90.4296777128844</td><td align="center" valign="middle" >2.043E+02</td><td align="center" valign="middle" >8.375E+01</td><td align="center" valign="middle" >8.166E+01</td><td align="center" valign="middle" >8.360E+01</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >82.7105618050238</td><td align="center" valign="middle" >1.870E+02</td><td align="center" valign="middle" >7.690E+01</td><td align="center" valign="middle" >7.502E+01</td><td align="center" valign="middle" >7.677E+01</td></tr><tr><td align="center" valign="middle" >110</td><td align="center" valign="middle" >76.2807946937883</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >120</td><td align="center" valign="middle" >70.8363332270320</td><td align="center" valign="middle" >1.552E+02</td><td align="center" valign="middle" >6.420E+01</td><td align="center" valign="middle" >6.270E+01</td><td align="center" valign="middle" >6.410E+01</td></tr><tr><td align="center" valign="middle" >130</td><td align="center" valign="middle" >66.1626241157140</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >140</td><td align="center" valign="middle" >62.1037638892161</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >58.5436331508260</td><td align="center" valign="middle" >1.334E+02</td><td align="center" valign="middle" >5.543E+01</td><td align="center" valign="middle" >5.418E+01</td><td align="center" valign="middle" >5.536E+01</td></tr><tr><td align="center" valign="middle" >160</td><td align="center" valign="middle" >55.3938980512388</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >170</td><td align="center" valign="middle" >52.5861224863810</td><td align="center" valign="middle" >1.174E+02</td><td align="center" valign="middle" >4.899E+01</td><td align="center" valign="middle" >4.792E+01</td><td align="center" valign="middle" >4.894E+01</td></tr><tr><td align="center" valign="middle" >180</td><td align="center" valign="middle" >50.0664326671761</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >190</td><td align="center" valign="middle" >47.7918173890647</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >45.7275059064572</td><td align="center" valign="middle" >1.053E+02</td><td align="center" valign="middle" >4.406E+01</td><td align="center" valign="middle" >4.311E+01</td><td align="center" valign="middle" >4.401E+01</td></tr></tbody></table></table-wrap><table-wrap id="table9" ><label><xref ref-type="table" rid="table9">Table 9</xref></label><caption><title> The empirical formulae for calculating mass stopping powers</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >y = y 0 + A 1 ∗ ( 1 − exp ( − x / t 1 ) ) + A 2 ∗ ( 1 − exp ( − x / t 2 ) )</th><th align="center" valign="middle" >Equation</th></tr></thead><tr><td align="center" valign="middle" >A<sub>1</sub> = −525.17835 &#177; 281.24707 t<sub>1</sub> = 30.29513 &#177; 27.2601 A<sub>2</sub> = −2749.90762 &#177; 270.11886 t<sub>2</sub> = 2.72637 &#177; 0.627 y<sub>0</sub> = 3330.68748 &#177; 146.50026 R<sup>2</sup> = 0.96955</td><td align="center" valign="middle" >Water</td></tr><tr><td align="center" valign="middle" >A<sub>1</sub> = −531.86671 &#177; 269.70529 t<sub>1</sub> = 29.57687 &#177; 25.25264 A<sub>2</sub> = −2739.78871 &#177; 258.80006 t<sub>2</sub> = 2.66924 &#177; 0.59292 y<sub>0</sub> = 3327.15093 &#177; 142.5736 R<sup>2</sup> = 0.97145</td><td align="center" valign="middle" >Eye lens</td></tr></tbody></table></table-wrap><table-wrap id="table10" ><label><xref ref-type="table" rid="table1">Table 1</xref>0</label><caption><title> The empirical formulae for calculating range</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >y = a &#215; x<sup>b</sup></th><th align="center" valign="middle" >Equation</th></tr></thead><tr><td align="center" valign="middle" >a = 2.64257E−4 &#177; 1.99087E−18 b = 1.7 &#177; 1.47723E−15 R<sup>2</sup> = 1</td><td align="center" valign="middle" >Water</td></tr><tr><td align="center" valign="middle" >a = 2.65908E−4 &#177; 1.49334E−18 b = 1.702 &#177; 1.10114E−15 R<sup>2</sup> = 1</td><td align="center" valign="middle" >Eye lens</td></tr></tbody></table></table-wrap><table-wrap id="table11" ><label><xref ref-type="table" rid="table1">Table 1</xref>1</label><caption><title> Alpha depth in the tissue, LET, absorbed dose, equivalent dose and effective dose of Alpha particle in water</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Effective dose (rem)</th><th align="center" valign="middle" >Equivalent dose (rem)</th><th align="center" valign="middle" >Absorbed dose (rad)</th><th align="center" valign="middle" >LET (MeV/cm)</th><th align="center" valign="middle" >Alpha depth in the Water(cm)</th><th align="center" valign="middle" >Energy (MeV)</th></tr></thead><tr><td align="center" valign="middle" >7.68E−09</td><td align="center" valign="middle" >0.000000064</td><td align="center" valign="middle" >3.2E−09</td><td align="center" valign="middle" >2384.22475403096</td><td align="center" valign="middle" >1.71308E−05</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >1.54E−08</td><td align="center" valign="middle" >0.000000128</td><td align="center" valign="middle" >6.4E−09</td><td align="center" valign="middle" >3395.26985256277</td><td align="center" valign="middle" >5.5658E−05</td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >2.3E−08</td><td align="center" valign="middle" >0.000000192</td><td align="center" valign="middle" >9.6E−09</td><td align="center" valign="middle" >3122.68961199742</td><td align="center" valign="middle" >0.000110888</td><td align="center" valign="middle" >0.6</td></tr><tr><td align="center" valign="middle" >3.07E−08</td><td align="center" valign="middle" >0.000000256</td><td align="center" valign="middle" >1.28E−08</td><td align="center" valign="middle" >2799.21374595122</td><td align="center" valign="middle" >0.000180834</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >3.84E−08</td><td align="center" valign="middle" >0.00000032</td><td align="center" valign="middle" >1.6E−08</td><td align="center" valign="middle" >2523.07437079105</td><td align="center" valign="middle" >0.000264257</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >7.68E−08</td><td align="center" valign="middle" >0.00000064</td><td align="center" valign="middle" >3.2E−08</td><td align="center" valign="middle" >1702.16894269649</td><td align="center" valign="middle" >0.000858572</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >1.15E−07</td><td align="center" valign="middle" >0.00000096</td><td align="center" valign="middle" >4.8E−08</td><td align="center" valign="middle" >1306.61486200367</td><td align="center" valign="middle" >0.001710535</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >1.54E−07</td><td align="center" valign="middle" >0.00000128</td><td align="center" valign="middle" >6.4E−08</td><td align="center" valign="middle" >1071.40076011691</td><td align="center" valign="middle" >0.00278951</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" >1.92E−07</td><td align="center" valign="middle" >0.0000016</td><td align="center" valign="middle" >8E−08</td><td align="center" valign="middle" >913.861598045919</td><td align="center" valign="middle" >0.004076382</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >2.3E−07</td><td align="center" valign="middle" >0.00000192</td><td align="center" valign="middle" >9.6E−08</td><td align="center" valign="middle" >800.185413092180</td><td align="center" valign="middle" >0.005557546</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >2.69E−07</td><td align="center" valign="middle" >0.00000224</td><td align="center" valign="middle" >1.12E−07</td><td align="center" valign="middle" >713.871579595160</td><td align="center" valign="middle" >0.007222584</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >3.07E−07</td><td align="center" valign="middle" >0.00000256</td><td align="center" valign="middle" >1.28E−07</td><td align="center" valign="middle" >645.859346277533</td><td align="center" valign="middle" >0.009063144</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >3.46E−07</td><td align="center" valign="middle" >0.00000288</td><td align="center" valign="middle" >1.44E−07</td><td align="center" valign="middle" >590.736276465791</td><td align="center" valign="middle" >0.011072309</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >3.84E−07</td><td align="center" valign="middle" >0.0000032</td><td align="center" valign="middle" >1.6E−07</td><td align="center" valign="middle" >545.058465969393</td><td align="center" valign="middle" >0.013244206</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >7.68E−07</td><td align="center" valign="middle" >0.0000064</td><td align="center" valign="middle" >3.2E−07</td><td align="center" valign="middle" >316.595133121707</td><td align="center" valign="middle" >0.043030551</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >1.15E−06</td><td align="center" valign="middle" >0.0000096</td><td align="center" valign="middle" >4.8E−07</td><td align="center" valign="middle" >228.250022083824</td><td align="center" valign="middle" >0.085729848</td><td align="center" valign="middle" >30</td></tr><tr><td align="center" valign="middle" >1.54E−06</td><td align="center" valign="middle" >0.0000128</td><td align="center" valign="middle" >6.4E−07</td><td align="center" valign="middle" >180.334690817695</td><td align="center" valign="middle" >0.139806674</td><td align="center" valign="middle" >40</td></tr><tr><td align="center" valign="middle" >1.92E−06</td><td align="center" valign="middle" >0.000016</td><td align="center" valign="middle" >8E−07</td><td align="center" valign="middle" >149.945174521898</td><td align="center" valign="middle" >0.204303086</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >2.3E−06</td><td align="center" valign="middle" >0.0000192</td><td align="center" valign="middle" >9.6E−07</td><td align="center" valign="middle" >128.821123405981</td><td align="center" valign="middle" >0.278537097</td><td align="center" valign="middle" >60</td></tr><tr><td align="center" valign="middle" >2.69E−06</td><td align="center" valign="middle" >0.0000224</td><td align="center" valign="middle" >1.12E−06</td><td align="center" valign="middle" >113.221409208821</td><td align="center" valign="middle" >0.361986677</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >3.07E−06</td><td align="center" valign="middle" >0.0000256</td><td align="center" valign="middle" >1.28E−06</td><td align="center" valign="middle" >101.194424044129</td><td align="center" valign="middle" >0.454233224</td><td align="center" valign="middle" >80</td></tr><tr><td align="center" valign="middle" >3.46E−06</td><td align="center" valign="middle" >0.0000288</td><td align="center" valign="middle" >1.44E−06</td><td align="center" valign="middle" >91.6180727928889</td><td align="center" valign="middle" >0.554929976</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >3.84E−06</td><td align="center" valign="middle" >0.000032</td><td align="center" valign="middle" >1.6E−06</td><td align="center" valign="middle" >83.7994542394653</td><td align="center" valign="middle" >0.663782684</td><td align="center" valign="middle" >100</td></tr><tr><td align="center" valign="middle" >4.22E−06</td><td align="center" valign="middle" >0.0000352</td><td align="center" valign="middle" >1.76E−06</td><td align="center" valign="middle" >77.2866088775882</td><td align="center" valign="middle" >0.780536979</td><td align="center" valign="middle" >110</td></tr><tr><td align="center" valign="middle" >4.61E−06</td><td align="center" valign="middle" >0.0000384</td><td align="center" valign="middle" >1.92E−06</td><td align="center" valign="middle" >71.7716546686581</td><td align="center" valign="middle" >0.904969697</td><td align="center" valign="middle" >120</td></tr><tr><td align="center" valign="middle" >4.99E−06</td><td align="center" valign="middle" >0.0000416</td><td align="center" valign="middle" >2.08E−06</td><td align="center" valign="middle" >67.0373213031586</td><td align="center" valign="middle" >1.036882674</td><td align="center" valign="middle" >130</td></tr><tr><td align="center" valign="middle" >5.38E−06</td><td align="center" valign="middle" >0.0000448</td><td align="center" valign="middle" >2.24E−06</td><td align="center" valign="middle" >62.9257258579161</td><td align="center" valign="middle" >1.176098184</td><td align="center" valign="middle" >140</td></tr><tr><td align="center" valign="middle" >5.76E−06</td><td align="center" valign="middle" >0.000048</td><td align="center" valign="middle" >2.4E−06</td><td align="center" valign="middle" >59.3192711893148</td><td align="center" valign="middle" >1.322455475</td><td align="center" valign="middle" >150</td></tr><tr><td align="center" valign="middle" >6.14E−06</td><td align="center" valign="middle" >0.0000512</td><td align="center" valign="middle" >2.56E−06</td><td align="center" valign="middle" >56.1284969629590</td><td align="center" valign="middle" >1.475808098</td><td align="center" valign="middle" >160</td></tr><tr><td align="center" valign="middle" >6.53E−06</td><td align="center" valign="middle" >0.0000544</td><td align="center" valign="middle" >2.72E−06</td><td align="center" valign="middle" >53.2840926935507</td><td align="center" valign="middle" >1.636021795</td><td align="center" valign="middle" >170</td></tr><tr><td align="center" valign="middle" >6.91E−06</td><td align="center" valign="middle" >0.0000576</td><td align="center" valign="middle" >2.88E−06</td><td align="center" valign="middle" >50.7314950861815</td><td align="center" valign="middle" >1.80297281</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >7.3E−06</td><td align="center" valign="middle" >0.0000608</td><td align="center" valign="middle" >3.04E−06</td><td align="center" valign="middle" >48.4271415891798</td><td align="center" valign="middle" >1.976546519</td><td align="center" valign="middle" >190</td></tr><tr><td align="center" valign="middle" >7.68E−06</td><td align="center" valign="middle" >0.000064</td><td align="center" valign="middle" >3.2E−06</td><td align="center" valign="middle" >46.3358150948924</td><td align="center" valign="middle" >2.156636302</td><td align="center" valign="middle" >200</td></tr></tbody></table></table-wrap><table-wrap id="table12" ><label><xref ref-type="table" rid="table1">Table 1</xref>2</label><caption><title> Alpha depth in the tissue, LET, absorbed dose, equivalent dose and effective dose of Alpha particle in eye lens</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Effective dose (rem)</th><th align="center" valign="middle" >Equivalent dose (rem)</th><th align="center" valign="middle" >Absorbed dose (rad)</th><th align="center" valign="middle" >LET (MeV/cm)</th><th align="center" valign="middle" >Alpha depth in the Eye lens(cm)</th><th align="center" valign="middle" >Energy (MeV)</th></tr></thead><tr><td align="center" valign="middle" >7.68E−09</td><td align="center" valign="middle" >0.000000064</td><td align="center" valign="middle" >3.2E−09</td><td align="center" valign="middle" >2577.25876416844</td><td align="center" valign="middle" >1.61E−05</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >1.54E−08</td><td align="center" valign="middle" >0.000000128</td><td align="center" valign="middle" >6.4E−09</td><td align="center" valign="middle" >3612.07050274882</td><td align="center" valign="middle" >5.22E−05</td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >2.3E−08</td><td align="center" valign="middle" >0.000000192</td><td align="center" valign="middle" >9.6E−09</td><td align="center" valign="middle" >3314.13099550001</td><td align="center" valign="middle" >1.04E−04</td><td align="center" valign="middle" >0.6</td></tr><tr><td align="center" valign="middle" >3.07E−08</td><td align="center" valign="middle" >0.000000256</td><td align="center" valign="middle" >1.28E−08</td><td align="center" valign="middle" >2967.75589807411</td><td align="center" valign="middle" >1.70E−04</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >3.84E−08</td><td align="center" valign="middle" >0.00000032</td><td align="center" valign="middle" >1.6E−08</td><td align="center" valign="middle" >2673.39716957040</td><td align="center" valign="middle" >2.49E−04</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >7.68E−08</td><td align="center" valign="middle" >0.00000064</td><td align="center" valign="middle" >3.2E−08</td><td align="center" valign="middle" >1801.38708542424</td><td align="center" valign="middle" >8.09E−04</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >1.15E−07</td><td align="center" valign="middle" >0.00000096</td><td align="center" valign="middle" >4.8E−08</td><td align="center" valign="middle" >1382.14182974495</td><td align="center" valign="middle" >1.61E−03</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >1.54E−07</td><td align="center" valign="middle" >0.00000128</td><td align="center" valign="middle" >6.4E−08</td><td align="center" valign="middle" >1133.03822554065</td><td align="center" valign="middle" >2.63E−03</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" >1.92E−07</td><td align="center" valign="middle" >0.0000016</td><td align="center" valign="middle" >8E−08</td><td align="center" valign="middle" >966.269403006857</td><td align="center" valign="middle" >3.85E−03</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >2.3E−07</td><td align="center" valign="middle" >0.00000192</td><td align="center" valign="middle" >9.6E−08</td><td align="center" valign="middle" >845.967851245202</td><td align="center" valign="middle" >5.25E−03</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >2.69E−07</td><td align="center" valign="middle" >0.00000224</td><td align="center" valign="middle" >1.12E−07</td><td align="center" valign="middle" >754.642269117505</td><td align="center" valign="middle" >6.82E−03</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >3.07E−07</td><td align="center" valign="middle" >0.00000256</td><td align="center" valign="middle" >1.28E−07</td><td align="center" valign="middle" >682.692320888245</td><td align="center" valign="middle" >8.56E−03</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >3.46E−07</td><td align="center" valign="middle" >0.00000288</td><td align="center" valign="middle" >1.44E−07</td><td align="center" valign="middle" >624.385125991344</td><td align="center" valign="middle" >1.05E−02</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >3.84E−07</td><td align="center" valign="middle" >0.0000032</td><td align="center" valign="middle" >1.6E−07</td><td align="center" valign="middle" >576.073788937800</td><td align="center" valign="middle" >1.25E−02</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >7.68E−07</td><td align="center" valign="middle" >0.0000064</td><td align="center" valign="middle" >3.2E−07</td><td align="center" valign="middle" >334.508617681511</td><td align="center" valign="middle" >4.07E−02</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >1.15E−06</td><td align="center" valign="middle" >0.0000096</td><td align="center" valign="middle" >4.8E−07</td><td align="center" valign="middle" >241.130665202236</td><td align="center" valign="middle" >8.12E−02</td><td align="center" valign="middle" >30</td></tr><tr><td align="center" valign="middle" >1.54E−06</td><td align="center" valign="middle" >0.0000128</td><td align="center" valign="middle" >6.4E−07</td><td align="center" valign="middle" >190.494572529498</td><td align="center" valign="middle" >1.32E−01</td><td align="center" valign="middle" >40</td></tr><tr><td align="center" valign="middle" >1.92E−06</td><td align="center" valign="middle" >0.000016</td><td align="center" valign="middle" >8E−07</td><td align="center" valign="middle" >158.383044569171</td><td align="center" valign="middle" >1.94E−01</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >2.3E−06</td><td align="center" valign="middle" >0.0000192</td><td align="center" valign="middle" >9.6E−07</td><td align="center" valign="middle" >136.063794313258</td><td align="center" valign="middle" >2.64E−01</td><td align="center" valign="middle" >60</td></tr><tr><td align="center" valign="middle" >2.69E−06</td><td align="center" valign="middle" >0.0000224</td><td align="center" valign="middle" >1.12E−06</td><td align="center" valign="middle" >119.582462073631</td><td align="center" valign="middle" >3.43E−01</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >3.07E−06</td><td align="center" valign="middle" >0.0000256</td><td align="center" valign="middle" >1.28E−06</td><td align="center" valign="middle" >106.876399583419</td><td align="center" valign="middle" >4.31E−01</td><td align="center" valign="middle" >80</td></tr><tr><td align="center" valign="middle" >3.46E−06</td><td align="center" valign="middle" >0.0000288</td><td align="center" valign="middle" >1.44E−06</td><td align="center" valign="middle" >96.7597551527863</td><td align="center" valign="middle" >5.27E−01</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >3.84E−06</td><td align="center" valign="middle" >0.000032</td><td align="center" valign="middle" >1.6E−06</td><td align="center" valign="middle" >88.5003011313755</td><td align="center" valign="middle" >6.30E−01</td><td align="center" valign="middle" >100</td></tr><tr><td align="center" valign="middle" >4.22E−06</td><td align="center" valign="middle" >0.0000352</td><td align="center" valign="middle" >1.76E−06</td><td align="center" valign="middle" >81.6204503223535</td><td align="center" valign="middle" >7.41E−01</td><td align="center" valign="middle" >110</td></tr><tr><td align="center" valign="middle" >4.61E−06</td><td align="center" valign="middle" >0.0000384</td><td align="center" valign="middle" >1.92E−06</td><td align="center" valign="middle" >75.7948765529242</td><td align="center" valign="middle" >8.59E−01</td><td align="center" valign="middle" >120</td></tr><tr><td align="center" valign="middle" >4.99E−06</td><td align="center" valign="middle" >0.0000416</td><td align="center" valign="middle" >2.08E−06</td><td align="center" valign="middle" >70.7940078038140</td><td align="center" valign="middle" >9.85E−01</td><td align="center" valign="middle" >130</td></tr><tr><td align="center" valign="middle" >5.38E−06</td><td align="center" valign="middle" >0.0000448</td><td align="center" valign="middle" >2.24E−06</td><td align="center" valign="middle" >66.4510273614613</td><td align="center" valign="middle" >1.12E+00</td><td align="center" valign="middle" >140</td></tr><tr><td align="center" valign="middle" >5.76E−06</td><td align="center" valign="middle" >0.000048</td><td align="center" valign="middle" >2.4E−06</td><td align="center" valign="middle" >62.6416874713838</td><td align="center" valign="middle" >1.26E+00</td><td align="center" valign="middle" >150</td></tr><tr><td align="center" valign="middle" >6.14E−06</td><td align="center" valign="middle" >0.0000512</td><td align="center" valign="middle" >2.56E−06</td><td align="center" valign="middle" >59.2714709148255</td><td align="center" valign="middle" >1.40E+00</td><td align="center" valign="middle" >160</td></tr><tr><td align="center" valign="middle" >6.53E−06</td><td align="center" valign="middle" >0.0000544</td><td align="center" valign="middle" >2.72E−06</td><td align="center" valign="middle" >56.2671510604277</td><td align="center" valign="middle" >1.55E+00</td><td align="center" valign="middle" >170</td></tr><tr><td align="center" valign="middle" >6.91E−06</td><td align="center" valign="middle" >0.0000576</td><td align="center" valign="middle" >2.88E−06</td><td align="center" valign="middle" >53.5710829538784</td><td align="center" valign="middle" >1.71E+00</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >7.3E−06</td><td align="center" valign="middle" >0.0000608</td><td align="center" valign="middle" >3.04E−06</td><td align="center" valign="middle" >51.1372446062992</td><td align="center" valign="middle" >1.88E+00</td><td align="center" valign="middle" >190</td></tr><tr><td align="center" valign="middle" >7.68E−06</td><td align="center" valign="middle" >0.000064</td><td align="center" valign="middle" >3.2E−06</td><td align="center" valign="middle" >48.9284313199092</td><td align="center" valign="middle" >2.05E+00</td><td align="center" valign="middle" >200</td></tr></tbody></table></table-wrap><table-wrap id="table13" ><label><xref ref-type="table" rid="table1">Table 1</xref>3</label><caption><title> Percentage of deviation error of stopping power for water</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Deviation (water)</th><th align="center" valign="middle" >Energy (MeV)</th></tr></thead><tr><td align="center" valign="middle" >5.07E+01</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >6.47E+01</td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >3.94E+01</td><td align="center" valign="middle" >0.6</td></tr><tr><td align="center" valign="middle" >2.41E+01</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >1.52E+01</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >4.81E+00</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >4.11E+00</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >3.62E+00</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" >3.28E+00</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >2.97E+00</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >2.73E+00</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >2.50E+00</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >2.27E+00</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >2.07E+00</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >6.98E−01</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >−6.57E−02</td><td align="center" valign="middle" >30</td></tr><tr><td align="center" valign="middle" >−6.42E−01</td><td align="center" valign="middle" >40</td></tr><tr><td align="center" valign="middle" >−1.09E+00</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >−1.51E+00</td><td align="center" valign="middle" >60</td></tr><tr><td align="center" valign="middle" >−1.97E+00</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >−2.32E+00</td><td align="center" valign="middle" >80</td></tr><tr><td align="center" valign="middle" >−2.70E+00</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >−3.07E+00</td><td align="center" valign="middle" >100</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" >110</td></tr><tr><td align="center" valign="middle" >−5.24E−01</td><td align="center" valign="middle" >120</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" >130</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" >140</td></tr><tr><td align="center" valign="middle" >−4.77E+00</td><td align="center" valign="middle" >150</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" >160</td></tr><tr><td align="center" valign="middle" >−3.21E+00</td><td align="center" valign="middle" >170</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" >190</td></tr><tr><td align="center" valign="middle" >−6.39E+00</td><td align="center" valign="middle" >200</td></tr></tbody></table></table-wrap></sec><sec id="s7"><title>7. Conclusions</title><p>Our research aims to evaluate how much energy alpha particles deposit in water and eye lens tissues. We used energy levels between 0.2 and 200 MeV and calculated the mass stopping power for each beam with the Bethe-Bloch formula. Based on our findings, we can draw the following conclusions:</p><p>1) The mass stopping power is proportional to Z (the charge of the incident particles), Z/A (the ratio of atomic and mass’ number of the tissue) and I (the ionization energy of the tissues).</p><p>2) The mass stopping power increases rapidly at low energies reaches a maximum and decreases gradually with increasing energy.</p><p>3) The mass stopping power allows us to calculate the range of the heavy particles in the absorber material.</p><p>4) The current fitting curves for mass stopping power and alpha particle range in water are excellent and accord with ASTAR data in the alpha energy rage of 2 to 200 MeV, with a deviation error of 4.81% - 6.39%.</p><p>5) Semi-empirical formulas for mass stopping power and range of alpha particles in water and eye lens tissues were developed for alpha particle energies ranging from 0.2 to 200 MeV.</p><p>6) The mass stopping power of alpha particles in water and eye lens tissues is equal to their average composition values.</p></sec><sec id="s8"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest.</p></sec><sec id="s9"><title>Cite this paper</title><p>Alshibel, A. and Osman, K.T. (2024) Mass Stopping Power and Range of Alpha Particles in Biological Human Body (Water and Eye Lens Tissue). Open Access Library Journal, 11: e1081. https://doi.org/10.4236/oalib.1111081</p></sec></body><back><ref-list><title>References</title><ref id="scirp.130525-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Berger, M.J. (1993) ESTAR, PSTAR, ASTAR. A PC Package for Calculating Stopping Powers and Ranges of Electrons, Protons and Helium Ions. Version 2 (No. IAEA-NDS-144), International Atomic Energy Agency, Vienna. https://2u.pw/wiKocY4</mixed-citation></ref><ref id="scirp.130525-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">National Research Council (1990) Health Effects of Exposure to Low Levels of Ionizing Radiation: BEIR V. https://2u.pw/jKZskul</mixed-citation></ref><ref id="scirp.130525-ref3"><label>3</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>El-Ghossain</surname><given-names> M.O. </given-names></name>,<etal>et al</etal>. (<year>2017</year>)<article-title>Calculations of Stopping Power, and Range of Ions Radiation (Alpha Particles) Interaction with Different Materials and Human Body Parts</article-title><source> International Journal of Physics</source><volume> 5</volume>,<fpage> 92</fpage>-<lpage>98</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.130525-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Porter, L.E. (2003) Further Observations of Projectile-z Dependence in Target Parameters of Modified Bethe-Bloch Theory. International Journal of Quantum Chemistry, 95, 504-511. https://2u.pw/mRH1duC 
&lt;br /&gt;https://doi.org/10.1002/qua.10589</mixed-citation></ref><ref id="scirp.130525-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Almutairi, A.S. and Osman, K.T. (2021) Mass Stopping Power and Range of Protons in Biological Human Body Tissues (Ovary, Lung and Breast). International Journal of Medical Physics, Clinical Engineering and Radiation Oncology, 11, 48-59.  
https://2u.pw/pZbO9Xe 
&lt;br /&gt;https://doi.org/10.4236/ijmpcero.2022.111005</mixed-citation></ref><ref id="scirp.130525-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Osman, K.T. (2020) Stopping Powers of Protons in Biological Human Body Substances (Water, Tissue, Muscles and Bones). International Journal of Novel Research in Physics Chemistry &amp; Mathematics, 7, 8-12. https://2u.pw/NGDFF5H</mixed-citation></ref><ref id="scirp.130525-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Almutairi, A.S. and Osman, K.T. (2022) Calculation of Mass Stopping Power and Range of Protons as Well as Important Radiation Quantities in Some Biological Human Bodyparts (Water, Muscle, Skeletal and Bone, Cortical). International Journal of Medical Physics, Clinical Engineering and Radiation Oncology, 11, 99-112.  
https://2u.pw/ouff9QE 
&lt;br /&gt;https://doi.org/10.4236/ijmpcero.2022.112009</mixed-citation></ref><ref id="scirp.130525-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Alshibel, A. and Osman, K.T. (2023) Mass Stopping Power and Range of Alpha Particles in Biological Human Body Tissues (Blood, Brain, Adipose and Bone). Open Access Library Journal, 10, 1-17. https://2u.pw/1JX1Jb9 
&lt;br /&gt;https://doi.org/10.4236/oalib.1110775</mixed-citation></ref><ref id="scirp.130525-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Osman, K.T. (2020) Stopping Powers of Alpha particles in Biological Human Body Substances (Water, Tissue, Muscules and Bones). International Journal of Novel Research and Development, 5, 362-398. https://2u.pw/5QSO9aJ</mixed-citation></ref><ref id="scirp.130525-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Osman, K.T. (2020) Mass Stopping Powers of Alpha Particles in Eye Lens and Its COMPOSITIONS (H, C, N, O, Na, P, S, Cl). International Journal of Novel Research in Physics Chemistry &amp; Mathematics, 7, 5-8.  
https://2u.pw/oOWBVXx</mixed-citation></ref><ref id="scirp.130525-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Krane, K.S. (1991) Introductory Nuclear Physics. John Wiley &amp; Sons, New York.  
https://2u.pw/lBJQfAk</mixed-citation></ref><ref id="scirp.130525-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">L’Annunziata, M.F. (2016) Radioactivity: Introduction and History, from the Quantum to Quarks. Elsevier, New York. https://2u.pw/yQWvDkS</mixed-citation></ref></ref-list></back></article>