<?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">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2015.615233</article-id><article-id pub-id-type="publisher-id">JMP-62518</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Theoretical Calculation of the Low-Lying Electronic States of the Molecule ScSe
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>awad</surname><given-names>Halabi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mahmoud</surname><given-names>Korek</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Faculty of Science, Beirut Arab University, Beirut, Lebanon</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>rawadhalabi555@hotmail.com(AH)</email>;<email>fkorek@yahoo.com(MK)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>12</month><year>2015</year></pub-date><volume>06</volume><issue>15</issue><fpage>2290</fpage><lpage>2296</lpage><history><date date-type="received"><day>11</day>	<month>October</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>28</month>	<year>December</year>	</date><date date-type="accepted"><day>31</day>	<month>December</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>
 
 
  Theoretical investigation of the lowest electronic states of ScSe molecule, in the representation 
  <sup>2s+1</sup>Λ
  <sup>(+/-)</sup>, has been performed via CASSCF and MRCI + Q (single and double excitations with Davidson correction) calculations. The calculated potential energy curves (PECs), permanent dipole moment curves (PDMCs), and spectroscopic constants are reported for the 14 lowest electronic states. The comparison of the present results with the rare available theoretical data in literature shows an overall good agreement. To the best of our knowledge, 13 electronic states of the ScSe molecule are not yet investigated either experimentally or theoretically; they are investigated in the present work for the first time.
 
</p></abstract><kwd-group><kwd>&lt;i&gt;ab initio&lt;/i&gt; Calculation</kwd><kwd> Electronic Structure</kwd><kwd> Spectroscopic Constants</kwd><kwd> Potential Energy Curves</kwd><kwd> Dipole Moments</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The electronic structures and nature of chemical bonds between a transition metal and a main group element are of great interest in many areas of science, e.g., in surface chemistry [<xref ref-type="bibr" rid="scirp.62518-ref1">1</xref>] , catalysis [<xref ref-type="bibr" rid="scirp.62518-ref2">2</xref>] , astrophysics [<xref ref-type="bibr" rid="scirp.62518-ref3">3</xref>] -[<xref ref-type="bibr" rid="scirp.62518-ref5">5</xref>] , organometallic chemistry [<xref ref-type="bibr" rid="scirp.62518-ref6">6</xref>] , and high-temperature chemistry [<xref ref-type="bibr" rid="scirp.62518-ref7">7</xref>] . They can also serve as simple models for understanding the properties of more complex transition metal compounds. Scandium is the first transition metal atom which has only one d-electron in the ground state. Diatomic molecules like ScSe are simple transition metal- containing systems in which d-electrons take part in bonding and provide ideal models for understanding the electronic structure and reactivity (chemiluminescent reactions). To the best of our knowledge, no experimental works for the ScSe molecule have been done. The only theoretical works for ScSe in literature are those of Wu et al. [<xref ref-type="bibr" rid="scirp.62518-ref8">8</xref>] for the ground X<sup>2</sup>Σ<sup>+</sup> state using the density functional method.</p><p>Because of the lack of studies, either theoretical or experimental, for the excited electronic states of the molecule ScSe and based on our previous studies on diatomic molecules particularly the scandium compounds ScO [<xref ref-type="bibr" rid="scirp.62518-ref9">9</xref>] , ScS [<xref ref-type="bibr" rid="scirp.62518-ref10">10</xref>] , ScF [<xref ref-type="bibr" rid="scirp.62518-ref11">11</xref>] , ScCl [<xref ref-type="bibr" rid="scirp.62518-ref12">12</xref>] , ScBr [<xref ref-type="bibr" rid="scirp.62518-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.62518-ref14">14</xref>] and ScI [<xref ref-type="bibr" rid="scirp.62518-ref15">15</xref>] , we present in this work an ab initio investigations of the lowest lying electronic states of the ScSe molecule. In the second part we show that, the calculation has been performed via CAS-SCF/MRCI (Complete Active Space Self Consistent Field, Multireference Configuration Interaction) method. Multireference CI calculations (single and double excitations with Davidson corrections) in which the entire CAS-SCF configuration space was used as the reference, were performed to account the correlation effects. In the third part, the potential energy curves (PECs), the permanent dipole moment curves (DMCs) together with the energy minimum for the ground state T<sub>e</sub>, the equilibrium internuclear distance R<sub>e</sub>, the harmonic frequency ω<sub>e</sub> and the rotational constant B<sub>e</sub> are presented for the 14 lowest-lying electronic states. Thirteen electronic states have been investigated in the present work for the first time.</p></sec><sec id="s2"><title>2. Method of Calculations</title><p>In the present work, ab initio investigations of the lowest-lying electronic states of the ScSe molecule have been performed via CASSCF method. Multireference MRCI + Q calculations (single and double excitations with Davidson corrections) were performed to determine the correlation effects. The entire CASSCF configuration space was used as a reference in the MRCI calculation which have been performed via the computational chemistry program MOLPRO. The scandium species is treated as a system with 10 inner electrons taken into account using the basis ECP10MDF [<xref ref-type="bibr" rid="scirp.62518-ref16">16</xref>] for s, p and d functions for ScSe. The selenium atom is treated as a system with 28 inner electrons taken into account using the basis ECP28MWB [<xref ref-type="bibr" rid="scirp.62518-ref17">17</xref>] including s and p functions. In the range of the internuclear distance R<sub>e</sub> around equilibrium distances of its ground state, the ScSe molecule is assumed to be mainly ionic as many transition-metals Sc<sup>+</sup>Se<sup>−</sup>. Among the 55 electrons explicitly considered for ScSe (21 electrons for Sc and 34 for Se) 38 inner electrons were frozen in subsequent calculations so that 17 electrons were explicitly treated. The active space contains 6σ (Sc: 4s; Se: 4p<sub>0</sub>, 5s, 4d<sub>0</sub>, 5p<sub>0</sub>, 6s), 3π (Se: 4p<sub>&#177;</sub><sub>1</sub>, 4d<sub>&#177;</sub><sub>1</sub>, 5p<sub>&#177;</sub><sub>1</sub>) and 1δ (Se: 4d<sub>&#177;</sub><sub>2</sub>), this corresponds to 10 active molecular orbitals in the C<sub>2v</sub> symmetry distributed into irreducible representation in the following way: 7a<sub>1</sub>, 3b<sub>1</sub>, 3b<sub>2</sub>, 1a<sub>2</sub>, noted [7, 3, 3, 1]. The doubly occupied orbitals 4σ (Sc: 3s, 3p<sub>0</sub>, 3d<sub>0</sub>; Se: 4s), and 2π (Sc: 3p<sub>&#177;</sub><sub>1</sub>, 3d<sub>&#177;</sub><sub>1</sub>) and 1δ (Sc: 3d<sub>&#177;</sub><sub>2</sub>) have been considered as inactive in the CASSCF calculations. Correlation effects for the seven valence electrons have been taken into account through multireference calculations MRCI + Q (single and double excitations with Davidson correction) where the entire CASSCF configuration space has been used as reference. Calculations have been performed via the computational program MOLPRO<sup>1</sup> taking advantage of the graphical user interface GABEDIT [<xref ref-type="bibr" rid="scirp.62518-ref18">18</xref>] .</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>The potential energy curves for the doublet and quartet electronic states of ScSe molecule in the representation of <sup>2s+1</sup>Λ<sup>(+/−)</sup> have been calculated in term of the internuclear distance in the ranges 2.00 &#197; ≤ R ≤ 3.77 &#197; (Figures 1-3). The electric dipole moment is a fundamental electrostatic property to study the strength of the long-range dipole-dipole forces, and to understand the macroscopic properties of imperfect gases, liquids and solids. It is demonstrated that the strength of vibrational excitations depends on the variation of the dipole moment as function of geometry such that the DMCs are considered important as they may help to obtain accurate predictions of transition intensities. Hence, the static electric dipole moment of the considered doublet and quartet states are calculated in terms of the internuclear distance R and they will be mainly used here to discuss the bond nature and the polarity and interaction of the states. As the bond nature of an electronic state is related to the magnitude of the dipole moment at a given distance, an ionic nature is indicated from a relatively large magnitude. It is quite common for the molecular electronic states of the potential energy curves to make crossings or avoided crossings. In fact, the avoided crossing regions are likely to be a leakage channels along which the molecules flow from the higher down to the lower potential energy curves. Such crossings or avoided crossings can dramatically alter the stability of the molecules. If these crossings are overlooked, then low barrier transitions can</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Potential energy curves of the electronic states X<sup>2</sup>Σ<sup>+</sup>, (1)<sup>2</sup>Δ, (2)<sup>2</sup>Δ, (2)<sup>2</sup>Σ<sup>+</sup> and (3)<sup>2</sup>Σ<sup>−</sup> of the molecule ScSe</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-7502490x8.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Potential energy curves of the electronic states (1)<sup>4</sup>Π, (1)<sup>2</sup>Π, (2)<sup>2</sup>Π, (2)<sup>4</sup>Π, (1)<sup>4</sup>Φ, (1)<sup>2</sup>Φ and (3)<sup>4</sup>Π of the molecule ScSe</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-7502490x9.png"/></fig><p>be missed and an incorrect chemical picture will arise. In the range of R, several avoided crossings have been detected in the potential energy curves for the excited electronic states of the considered molecule ScSe.</p><p>For the ScSe molecule, the spectroscopic constants such as the vibration harmonic constant ω<sub>e</sub>, the internuclear distance at equilibrium R<sub>e</sub>, the rotational constant B<sub>e</sub> and the electronic transition energy with respect to the ground state T<sub>e</sub> have been calculated by fitting the energy values around the equilibrium position to a polynomial in terms of the internuclear distance R. These values are given in <xref ref-type="table" rid="table1">Table 1</xref> together with the available data in the literature. The only values available in literature for the molecule ScSe is that for the ground state X<sup>2</sup>Σ<sup>+</sup> calculated by using the DFT-B3LYP technique [<xref ref-type="bibr" rid="scirp.62518-ref8">8</xref>] . The comparison of our investigated values of R<sub>e</sub> for the ground states with those given by Wu et al. [<xref ref-type="bibr" rid="scirp.62518-ref8">8</xref>] for the considered molecule shows a good agreement with the relative differences δR<sub>e</sub>/R<sub>e</sub> = 4.7% for the ScSe molecule. A good agreement is obtained by comparing our calculated</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Potential energy curves of the electronic states (1)<sup>4</sup>Σ<sup>+</sup>, (2)<sup>4</sup>Σ<sup>+</sup>, (3)<sup>4</sup>Σ<sup>−</sup>, (4)<sup>4</sup>Σ<sup>−</sup>, (1)<sup>4</sup>Δ, (2)<sup>4</sup>Δ, (3)<sup>4</sup>Δ, (4)<sup>4</sup>Δ, (5)<sup>4</sup>Δ, and (1)<sup>4</sup>Γ of the molecule ScSe</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-7502490x10.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Calculated spectroscopic constants for the lowest 14 electronic states of ScSe</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >States</th><th align="center" valign="middle" >T<sub>e</sub> (cm<sup>−1</sup>)</th><th align="center" valign="middle" >R<sub>e</sub> (Ǻ)</th><th align="center" valign="middle" >ω<sub>e</sub> (cm<sup>−1</sup>)</th><th align="center" valign="middle" >B<sub>e </sub>&#215; 10<sup>2</sup> (cm<sup>−1</sup>)</th></tr></thead><tr><td align="center" valign="middle" >X<sup>2</sup>Σ<sup>+</sup></td><td align="center" valign="middle" >0.0<sup>a</sup> 0.0<sup>b</sup></td><td align="center" valign="middle" >2.3794<sup>a</sup> 2.272<sup>b</sup></td><td align="center" valign="middle" >348.7<sup>a </sup> 424<sup>b</sup></td><td align="center" valign="middle" >10.395</td></tr><tr><td align="center" valign="middle" >(1)<sup>2</sup>Δ</td><td align="center" valign="middle" >8322<sup> </sup></td><td align="center" valign="middle" >2.409</td><td align="center" valign="middle" >401.1</td><td align="center" valign="middle" >10.186</td></tr><tr><td align="center" valign="middle" >(1)<sup>4</sup>Σ<sup>+</sup></td><td align="center" valign="middle" >8486</td><td align="center" valign="middle" >2.695</td><td align="center" valign="middle" >252.8</td><td align="center" valign="middle" >8.104</td></tr><tr><td align="center" valign="middle" >(1)<sup>4</sup>Δ</td><td align="center" valign="middle" >9339</td><td align="center" valign="middle" >2.713</td><td align="center" valign="middle" >246.5</td><td align="center" valign="middle" >7.994</td></tr><tr><td align="center" valign="middle" >(3)<sup>2</sup>Σ<sup>−</sup></td><td align="center" valign="middle" >10,269</td><td align="center" valign="middle" >2.732</td><td align="center" valign="middle" >236.6</td><td align="center" valign="middle" >7.884</td></tr><tr><td align="center" valign="middle" >(2)<sup>2</sup>Σ<sup>+</sup></td><td align="center" valign="middle" >10,437</td><td align="center" valign="middle" >2.399</td><td align="center" valign="middle" >380.5</td><td align="center" valign="middle" >10.213</td></tr><tr><td align="center" valign="middle" >(4)<sup>2</sup>Σ<sup>−</sup></td><td align="center" valign="middle" >12,540</td><td align="center" valign="middle" >2.735</td><td align="center" valign="middle" >240.5</td><td align="center" valign="middle" >7.869</td></tr><tr><td align="center" valign="middle" >(1)<sup>4</sup>Π</td><td align="center" valign="middle" >12,979</td><td align="center" valign="middle" >2.734</td><td align="center" valign="middle" >252.6</td><td align="center" valign="middle" >7.878</td></tr><tr><td align="center" valign="middle" >(2)<sup>4</sup>Π</td><td align="center" valign="middle" >15,513</td><td align="center" valign="middle" >2.507</td><td align="center" valign="middle" >568.5</td><td align="center" valign="middle" >9.361</td></tr><tr><td align="center" valign="middle" >(2)<sup>4</sup>Δ</td><td align="center" valign="middle" >20,244</td><td align="center" valign="middle" >2.715</td><td align="center" valign="middle" >234.7</td><td align="center" valign="middle" >7.985</td></tr><tr><td align="center" valign="middle" >(2)<sup>4</sup>Σ<sup>+</sup></td><td align="center" valign="middle" >20,364</td><td align="center" valign="middle" >2.717</td><td align="center" valign="middle" >237.4</td><td align="center" valign="middle" >7.974</td></tr><tr><td align="center" valign="middle" >(1)<sup>4</sup>Γ</td><td align="center" valign="middle" >20,795</td><td align="center" valign="middle" >2.721</td><td align="center" valign="middle" >234.5</td><td align="center" valign="middle" >7.951</td></tr><tr><td align="center" valign="middle" >(3)<sup>4</sup>Δ</td><td align="center" valign="middle" >20,933</td><td align="center" valign="middle" >2.725</td><td align="center" valign="middle" >234.3</td><td align="center" valign="middle" >7.924</td></tr><tr><td align="center" valign="middle" >(1)<sup>4</sup>Ф</td><td align="center" valign="middle" >24,076</td><td align="center" valign="middle" >2.377</td><td align="center" valign="middle" >351.3</td><td align="center" valign="middle" >10.417</td></tr></tbody></table></table-wrap><p><sup>a</sup>Present Theoretical study; <sup>b</sup>Ref [<xref ref-type="bibr" rid="scirp.62518-ref8">8</xref>] .</p><p>value of ω<sub>e</sub> for ScSe molecule with that given in Ref. [<xref ref-type="bibr" rid="scirp.62518-ref8">8</xref>] with the relative difference δω<sub>e</sub>/ω<sub>e</sub> = 17.6%. No comparisons for the other investigated data for the excited electronic states with other values, since they are given here for the first time.</p><p>The dipole moment function of these states exhibits an abrupt change reflecting the avoided crossing between the two states as also observed at the potential energy curves. The positions of these crossings and avoid crossing are given in <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>In Figures 4-6 we show the agreement between the positions of the avoided crossings of the PECs and the</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Positions of the avoided crossings between the different electronic states (ScSe)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >State 1</th><th align="center" valign="middle" >State 2</th><th align="center" valign="middle" >Avoided crossing between (n<sub>1</sub>) state1/(n<sub>2</sub>) state2</th><th align="center" valign="middle" >R<sub>AC</sub> (Ǻ)</th><th align="center" valign="middle" >ΔE<sub>AC</sub> (cm<sup>−1</sup>)</th></tr></thead><tr><td align="center" valign="middle" ><sup>2</sup>Δ</td><td align="center" valign="middle" ><sup>2</sup>Δ</td><td align="center" valign="middle" >1/2</td><td align="center" valign="middle" >2.69</td><td align="center" valign="middle" >1779.46</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" >1/2</td><td align="center" valign="middle" >2.60</td><td align="center" valign="middle" >978.78</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" >1/2</td><td align="center" valign="middle" >2.66</td><td align="center" valign="middle" >640.4</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" >2/3</td><td align="center" valign="middle" >2.54</td><td align="center" valign="middle" >1112.04</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>−</sup></td><td align="center" valign="middle" ><sup>4</sup>Σ<sup>−</sup></td><td align="center" valign="middle" >3/4</td><td align="center" valign="middle" >2.54</td><td align="center" valign="middle" >1632.84</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Δ<sup> </sup></td><td align="center" valign="middle" ><sup>4</sup>Δ<sup> </sup></td><td align="center" valign="middle" >2/3</td><td align="center" valign="middle" >2.28</td><td align="center" valign="middle" >224.51</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Δ<sup> </sup></td><td align="center" valign="middle" ><sup>4</sup>Δ</td><td align="center" valign="middle" >2/3</td><td align="center" valign="middle" >3.03</td><td align="center" valign="middle" >534.92</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Positions of the crossings between the different electronic states (ScSe)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >State 1</th><th align="center" valign="middle" >State 2</th><th align="center" valign="middle" >Crossing between (n<sub>1</sub>) state1/(n<sub>2</sub>) state2</th><th align="center" valign="middle" >R<sub>c</sub> (Ǻ)</th></tr></thead><tr><td align="center" valign="middle" ><sup>2</sup>Σ</td><td align="center" valign="middle" ><sup>2</sup>Δ</td><td align="center" valign="middle" >2/2</td><td align="center" valign="middle" >2.57</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>2</sup>Φ</td><td align="center" valign="middle" >1/1</td><td align="center" valign="middle" >2.60</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>2</sup>Φ</td><td align="center" valign="middle" >2/1</td><td align="center" valign="middle" >2.54</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" ><sup>2</sup>Φ</td><td align="center" valign="middle" >1/1</td><td align="center" valign="middle" >2.81</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" >1/1</td><td align="center" valign="middle" >2.84</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" >2/1</td><td align="center" valign="middle" >3.02</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>4</sup>Φ</td><td align="center" valign="middle" >2/1</td><td align="center" valign="middle" >2.09</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" ><sup>4</sup>Φ</td><td align="center" valign="middle" >3/1</td><td align="center" valign="middle" >2.54</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Π</td><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" >2/2</td><td align="center" valign="middle" >2.15</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Π</td><td align="center" valign="middle" ><sup>2</sup>Φ</td><td align="center" valign="middle" >2/1</td><td align="center" valign="middle" >2.30</td></tr><tr><td align="center" valign="middle" ><sup>2</sup>Φ</td><td align="center" valign="middle" ><sup>4</sup>Φ</td><td align="center" valign="middle" >1/1</td><td align="center" valign="middle" >2.30</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>+ </sup></td><td align="center" valign="middle" ><sup>4</sup>Δ</td><td align="center" valign="middle" >1/4</td><td align="center" valign="middle" >2.93</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>+ </sup></td><td align="center" valign="middle" ><sup>4</sup>Σ<sup>−</sup></td><td align="center" valign="middle" >1/3</td><td align="center" valign="middle" >2.33</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>+ </sup></td><td align="center" valign="middle" ><sup>4</sup>Σ<sup>−</sup></td><td align="center" valign="middle" >1/4</td><td align="center" valign="middle" >2.33</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>− </sup></td><td align="center" valign="middle" ><sup>4</sup>Δ</td><td align="center" valign="middle" >3/1</td><td align="center" valign="middle" >2.36</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>− </sup></td><td align="center" valign="middle" ><sup>4</sup>Δ</td><td align="center" valign="middle" >4/1</td><td align="center" valign="middle" >2.36</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>− </sup></td><td align="center" valign="middle" ><sup>4</sup>Δ</td><td align="center" valign="middle" >4/5</td><td align="center" valign="middle" >2.54</td></tr><tr><td align="center" valign="middle" ><sup>4</sup>Σ<sup>− </sup></td><td align="center" valign="middle" ><sup>4</sup>Δ</td><td align="center" valign="middle" >4/2</td><td align="center" valign="middle" >3.41</td></tr></tbody></table></table-wrap><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Dipole moment curves of the electronic states X<sup>2</sup>Σ<sup>+</sup>, (1)<sup>2</sup>Δ, (2)<sup>2</sup>Δ, (2)<sup>2</sup>Σ<sup>+</sup> and (3)<sup>2</sup>Σ<sup>−</sup> of the molecule ScSe</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-7502490x11.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Dipole moment curves of the electronic states (1)<sup>4</sup>Π, (1)<sup>2</sup>Π, (2)<sup>2</sup>Π, (2)<sup>4</sup>Π, (1)<sup>4</sup>Φ, (1)<sup>2</sup>Φ and (3)<sup>4</sup>Π of the molecule ScSe</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-7502490x12.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Dipole moment curves of the electronic states (1)<sup>4</sup>Σ<sup>+</sup>, (2)<sup>4</sup>Σ<sup>+</sup>, (3)<sup>4</sup>Σ<sup>−</sup>, (4)<sup>4</sup>Σ<sup>−</sup>, (1)<sup>4</sup>Δ, (2)<sup>4</sup>Δ, (3)<sup>4</sup>Δ, (4)<sup>4</sup>Δ, (5)<sup>4</sup>Δ, and (1)<sup>4</sup>Γ states of the molecule ScSe</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/15-7502490x13.png"/></fig><p>positions of the crossing of the corresponding DMCs. This agreement can be considered as confirmation of the accuracy of the present results on the ScSe molecule. In the present calculation of the DMCs, we considered the Sc atom at the origin. One can notice that, most of the DMCs for the considered molecule are in the negative regions, where the electronegativity of the Sc atom is higher than those of Se atom in these regions and it is independent either on the internuclear distance or the different electronic states. But only for the (2)<sup>4</sup>Δ of the ScSe molecule an inversion in the sign is occurred at R &gt; 3 &#197;. At large internuclear distances the decreased value of the dipole moment can be explained by the polarization of the orbital in the direction of the negatively charged ligand whereas this orbital polarization tends toward the covalent nature for the electronic state (2)<sup>4</sup>Δ of this molecule.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In the present work, the ab initio investigation for 14 low-lying electronic states of the ScSe molecule has been performed via CASSCF and MRCI + Q (single and double excitations with Davidson correction) calculations. The calculated potential energy curves, the permanent dipole moment curves, and spectroscopic constants T<sub>e</sub>, R<sub>e</sub>, ω<sub>e</sub> and the rotational constant B<sub>e</sub> are reported for the 14 lowest electronic states of the molecule ScSe. The overall agreement between our calculated values of the spectroscopic constants for the ground states and those of Wu et al. [<xref ref-type="bibr" rid="scirp.62518-ref8">8</xref>] and the agreement between the positions of avoided crossing of the PECs and the crossing of the DMCs for the 13 new excited states confirm the validity and the accuracy of the present results. These investigated data may help for more experimental or theoretical studies in the future for higher electronic states. It is hoped that our computational results will stimulate further experimental studies on such diatomic molecule.</p></sec><sec id="s5"><title>Cite this paper</title><p>RawadHalabi,MahmoudKorek, (2015) Theoretical Calculation of the Low-Lying Electronic States of the Molecule ScSe. Journal of Modern Physics,06,2290-2296. doi: 10.4236/jmp.2015.615233</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.62518-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Prutton, M. (1994) Introduction to Surface Physics. 4th Edition, Oxford University Press, New York, 128.</mixed-citation></ref><ref id="scirp.62518-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Silberberg, M. 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