<?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">OJM</journal-id><journal-title-group><journal-title>Open Journal of Microphysics</journal-title></journal-title-group><issn pub-type="epub">2162-2450</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojm.2013.32007</article-id><article-id pub-id-type="publisher-id">OJM-31731</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>
 
 
  Search for High Energy Electrons from New Neutral Massive Gauge Boson Decay in the CMS Detector at the LHC Using Monte Carlo Simulation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>M. M. Mansour</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>Nady</surname><given-names>Bakhet</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>Department of Physics, Faculty of Science, Cairo University, Giza, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mansourhesham@yahoo.com(.MMM)</email>;<email>nady.bakhet@cern.ch(NB)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>22</day><month>05</month><year>2013</year></pub-date><volume>03</volume><issue>02</issue><fpage>34</fpage><lpage>42</lpage><history><date date-type="received"><day>March</day>	<month>4,</month>	<year>2013</year></date><date date-type="rev-recd"><day>April</day>	<month>6,</month>	<year>2013</year>	</date><date date-type="accepted"><day>April</day>	<month>15,</month>	<year>2013</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>
 
 
  The existence of new heavy neutral massive boson Z′ is a feature of many extensions of Standard Model models as the two-Higgs-doublet model (2HDM), the Hidden Abelian Higgs Model (HAHM), Left-Right Symmetric Model (LRSM), Sequential Standard Model (SSM) and Baryon number minus Lepton number Model (B-L). In the present work we search for two high energy electrons produced from decaying<inline-formula><inline-graphic xlink:href="dit_f16b1d16-b2c9-4b2c-bc9d-200768f726d4.png" xlink:type="simple"/></inline-formula>heavy neutral massive boson in the events produced in proton-proton collisions at LHC and can be detected by CMS detector. We used the data which is produced from proton-proton collisions by Monte Carlo events generator for different energies at LHC
  ,
   then we use the angular distribution, invariant mass, combined transverse momentum and combined rapidity distributions for the two high en
  ergy electrons produced from <inline-formula><inline-graphic xlink:href="dit_4eb16bf8-0051-449a-abfb-6600adbc1cbe.png" xlink:type="simple"/></inline-formula>decay channel to detect the<inline-formula><inline-graphic xlink:href="dit_a91ed167-9d06-4aaa-b5ed-ac516f4b61c2.png" xlink:type="simple"/></inline-formula>signal. B-L extension of the SM model predicts the existence of a<inline-formula><inline-graphic xlink:href="dit_78b915f2-2f2c-4274-bd9e-953b212215b3.png" xlink:type="simple"/></inline-formula>heavy neutral massive boson at high energies. From our results which we had simulated using MC programs for<inline-formula><inline-graphic xlink:href="dit_b8f74eee-5021-4ad2-a982-0e7d52879279.png" xlink:type="simple"/></inline-formula>in the B-L extension of standard model, we predict a possible existence of new gauge<inline-formula><inline-graphic xlink:href="dit_4412929d-6310-4cbb-bc58-b252a6e21eed.png" xlink:type="simple"/></inline-formula>at LHC in the mass range 1 TeV to 1.5 TeV via electrons identification of the two high energy electrons by CMS detector.
 
</p></abstract><kwd-group><kwd>LHC; CMS; Monte Carlo Simulation; New Boson; SM; B-L; Gauge Boson</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Ionic liquids are low-melting-point molten salts, defined as that form liquids at room temperature or even at temperatures lower than the boiling point of water. The property is owing to that the liquid state is thermodynamically favorable due to the large size and conformational flexibility of the ions, in which these behaviors lead to small lattice enthalpies and large entropy changes that favor the liquid state [1,2]. In the past more than a decade, ionic liquids have attracted much attention due to their specific characteristics such as excellent thermal stabilities, a negligible vapor pressure, and controllable physical and chemical properties [<xref ref-type="bibr" rid="scirp.31731-ref3">3</xref>]. Beyond these traditional properties of ionic liquids, recently, interests and applications on ionic liquids have been extended to the researches related to biological macromolecules such as naturally occurring polysaccharides, because of specific good affinities of ionic liquids for them [<xref ref-type="bibr" rid="scirp.31731-ref4">4</xref>].</p><p>Polysaccharides are widely distributed in nature and have been regarded as structural materials and as suppliers of water and energy [<xref ref-type="bibr" rid="scirp.31731-ref5">5</xref>]. Of the many kinds of polysaccharides, cellulose and chitin are the most important biomass resources because they are the first and second most abundant natural polysaccharides on the earth, respectively [6-10]. Chitin is an aminopolysaccharide consisting of β (1g4)-linked N-acetyl-D-glucosamine residues, which has acetamido groups at the C-2 position in place of hydroxy groups of the glucose residues in cellulose (<xref ref-type="fig" rid="fig1">Figure 1</xref>). Despite its huge production in nature and easy accessibility, chitin still remains as an unutilized biomass resource primary because of its intractable bulk structure and insolubility in water and common organic solvents. Even in recent years, therefore, there is major interest in conversion into various useful materials after proper dissolution of chitin in suitable solvents.</p><p>Chitin occurs mainly in the exoskeletons of crustacean shells such as crab and shrimp shells in nature. Native chitin in crustacean shells is arranged as microfibrils embedded in a protein matrix [11,12]. The microfibril is composed of nanofibers with 2 nm - 5 nm diameters. Moreover, three types of crystalline forms, i.e., α-, β-, and γ-chitins, are known depending on the arrangement of the polymeric chains. The most abundant form is α-chitin (e.g., from crab and shrimp shells) [<xref ref-type="bibr" rid="scirp.31731-ref13">13</xref>], where the polymeric chains are aligned in an antiparallel fashion. This arrangement is favorable for the formation of</p><p>strong intermolecular hydrogen bonding, leading to the most stable form in the three types of crystalline structures. In β-chitin (e.g., from squid pen), the polymeric chains are packed in a parallel arrangement [<xref ref-type="bibr" rid="scirp.31731-ref14">14</xref>], resulting in weaker intermolecular forces. Accordingly, β-chitin is considered to be less stable than α-chitin. γ-Chitin may be a mixture of α- and β-forms.</p><p>Since Rogers et al. comprehensively reported that an ionic liquid, 1-butyl-3-methylimidazolium chloride, dissolved cellulose in relatively high concentrations [<xref ref-type="bibr" rid="scirp.31731-ref15">15</xref>], ionic liquids have began to be used in the processing of cellulose, which mainly concern with the dissolution, homogeneous derivatization and modification, and regeneration [16-19]. Therefore, ionic liquids are considered as powerful solvents and are used for material processing of cellulose. On the other hand, only the limited investigations have been reported regarding the dissolution of chitin with ionic liquids including the author’s study, in which the author found that an ionic liquid, 1-allyl-3-methylimidazolium bromide (AMIMBr), dissolved or swelled chitin to form weak gel-like materials (ion gels) (<xref ref-type="fig" rid="fig2">Figure 2</xref>) [20,21]. The other groups have also reported the dissolution of chitin with ionic liquids, 1-butyland 1-ethyl-3-methylimidazolium acetates (<xref ref-type="fig" rid="fig2">Figure 2</xref>) [22,23]. However, the dissolution of chitin with other ionic liquids having different cationic, anionic, and substituent structures has hardly been reported. The observation suggests that the aforementioned ionic liquids only having specific structures probably exhibit a potential for the dissolution of chitin [24-27].</p><p>Chemical derivatization of chitin is one of the efficient approaches to explore their potentials, giving the novel types of functional materials [28,29]. Derivatization of chitin, however, is generally difficult owing to a lack of solubility as aforementioned, and thus the reactions often take place under heterogeneous conditions, leading to low degree of substitution (DS). Even acetylation of chitin, a simplest derivatization, has been performed only under special conditions. The author has considered that ionic liquids, that dissolve chitin, act as efficient media for derivatizations of chitin with high DS, and thus investigated acetylation of chitin in AMIMBr [<xref ref-type="bibr" rid="scirp.31731-ref30">30</xref>].</p><p>On the other hand, the preparation of self-assembled fibrillar nanostructures, so-called nanofibers, is one of the most useful methods to practically utilize polymeric functional materials from native chitin sources [31-33]. Conventional approaches to the production of chitin nanofibers are mainly performed upon top-down procedures that break down the starting bulk materials from native chitin sources (<xref ref-type="fig" rid="fig3">Figure 3</xref>). As the representative techniques, acid hydrolysis [34-37], 2,2,6,6-tetramethylpiperidine-1-oxyl radical (TEMPO)-mediated oxidation [38,39], and grinding technique [40,41] have previously been performed to produce chitin nanofibers from native chitin sources. The other method accorded to self-assembling generative (bottom-up) route (<xref ref-type="fig" rid="fig3">Figure 3</xref>), in which fibrillar nanostructures were produced by regeneration from chitin solutions via appropriate process, as examples of the electrospinning equipment [42,43] and simple precipitation process [44,45]. To efficiently provide chitin nanofibers by the bottom-up technique, the author has focused on the ionic liquid, AMIMBr. Accordingly, the author successfully reported that chitin nanofiber films were facilely obtained by regeneration from the ion gels with AMIMBr using methanol, followed by filtration [<xref ref-type="bibr" rid="scirp.31731-ref46">46</xref>].</p><p>On the basis of the above backgrounds and viewpoints, this paper reviews the studies on the dissolution, acetylation, and nanofibrillation using AMIMBr. The series of the studies provide new approaches for material processing from native chitin sources.</p></sec><sec id="s2"><title>2. Dissolution of Chitin with Ionic Liquid</title><p>For the dissolution study of chitin with ionic liquids, the author noted the previous study reporting that the imidazolium-type ionic liquids having a bromide counter anion were the good solvents for synthesis of polyamides and polyimides [<xref ref-type="bibr" rid="scirp.31731-ref47">47</xref>]. The result inspired to use the same kind of ionic liquids for dissolution of chitin, because chitin has the -N-C=O groups as same as polyamides and polyimides. Thus, three ionic liquids consisting of a bromide anion were prepared, which were AMIMBr, 1-methyl-3- propylimidazolium bromide, and 1-butyl-3-methylimidazolium bromide, and the dissolution experiments were conducted as follows [<xref ref-type="bibr" rid="scirp.31731-ref21">21</xref>].</p><p>A mixture of chitin with each ionic liquid was heated at 100˚C and the heating process was simply followed by a charge coupled device (CCD) camera on glass plate. When AMIMBr was used for the dissolution experiment, the clear solutions of chitin were formed in the concentrations up to ~4.8 wt% (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a)), whereas the other ionic liquids did not show ability to dissolve chitin even in 1 wt% concentration. The disappearance of chitin powder in the solution of 4.8 wt% chitin with AMIMBr was confirmed further by the SEM measurement. The SEM image of the mixture of chitin with AMIMBr after heating it at 100˚C for 48 h did not show any solid of chitin (<xref ref-type="fig" rid="fig4">Figure 4</xref>(b)), suggesting that 4.8 wt% chitin was solvated with AMIMBr at least at the μm scale level.</p><p>It was confirmed as follows that degradation and decrease in the molecular weight of chitin did not frequently occur during dissolution with AMIMBr. The powder X-ray diffraction (XRD), thermal gravimetrical analysis (TGA), and IR results of the regenerated chitin from the solution with AMIMBr, which was prepared by addition of methanol into it, followed by filtration and dryness of the precipitate, were almost same as those of the original chitin. In addition, the hexanoyl derivative of the regenerated chitin, which was synthesized by the re-</p><p>action of the regenerated material with hexanoyl chloride [<xref ref-type="bibr" rid="scirp.31731-ref48">48</xref>], showed the exact same <sup>1</sup>H NMR pattern as that of the hexanoylated sample from the original chitin and the GPC profiles of both the derivatives were not much different from each other.</p><p>Interestingly, mixtures of higher amounts of chitin with AMIMBr gave more viscous materials, i.e., gel-like materials when 6.5 wt% - 10.7 wt% of chitin were immersed in AMIMBr at room temperature for 24 h, followed by heating at 100˚C for 48 h and cooling to room temperature. Indeed, the obtained 6.5 wt% chitin with AMIMBr did not flow upon leaning a test tube, whereas the aforementioned 4.8 wt% chitin with AMIMBr started to flow upon leaning (<xref ref-type="fig" rid="fig5">Figure 5</xref>). The dynamic rheological measurements showed that both 4.8 wt% and 6.5 wt% chitins with AMIMBr behaved as the weak gels.</p></sec><sec id="s3"><title>3. Acetylation of Chitin in Ionic Liquid</title><p>As a simplest and useful derivatization reaction of chitin, acetylation of chitin using acetic anhydride in an ionic liquid solvent, AMIMBr, was performed (<xref ref-type="fig" rid="fig6">Figure 6</xref>) [<xref ref-type="bibr" rid="scirp.31731-ref30">30</xref>]. Prior to acetylation, chitin was dissolved with AMIMBr (2.0 wt%) by heating the mixture at 100˚C for 24 h with stirring. Then, the 5 - 20 equiv. of acetic anhydride for a repeating unit was added to the solution and the mixture was heated at 60˚C - 100˚C for 24 h with stirring. The products were isolated as a fraction insoluble in methanol and the DS values of the products were estimated by comparison of the intensities of the two carbonyl absorptions due to amido I (ca. 1658 cm<sup>−</sup><sup>1</sup>) and ester (ca. 1745 cm<sup>−</sup><sup>1</sup>)</p><p>in the IR spectra (<xref ref-type="fig" rid="fig7">Figure 7</xref>). No acetylation took place under the conditions using 5 equiv. of acetic anhydride at 60˚C. While the DS values increased under the conditions using larger equiv. of acetic anhydride at higher reaction temperatures. The highest DS value (1.86) was obtained when the reaction was carried out using 20 equiv. of acetic anhydride at 80˚C.</p><p>Because the products with high DS, which were obtained by the reaction using 20 equiv. of acetic anhydride, were soluble in DMSO, the structures of these products were further confirmed by the <sup>1</sup>H NMR analysis measured in DMSO-d<sub>6</sub>. On the basis of the integrated ratios of the signals due to the acetyl protons to the signal due to the anomeric protons, the DS values were calculated, which were in good agreement with those determined by the IR spectra. The all the above results indicated that AMIMBr was the powerful media for the efficient derivatization of chitin.</p></sec><sec id="s4"><title>4. Preparation of Nanofiber Films from Chitin Ion Gel with Ionic Liquid</title><p>The author has reported that chitin nanofiber films were formed by regeneration from the aforementioned ion gels with AMIMBr using methanol, followed by filtration (<xref ref-type="fig" rid="fig8">Figure 8</xref>, Route A) [<xref ref-type="bibr" rid="scirp.31731-ref46">46</xref>]. First, chitin was swollen with AMIMBr according to the procedure as aforementioned to give the chitin ion gels with AMIMBr (9.1 wt% - 10.7 wt%). It was found that chitin dispersions were obtained when the gels were immersed in methanol at room temperature for 24 h to slowly regenerate chitin, followed by sonication. The resulting dispersion was diluted with methanol, which was subjected to the SEM measure-</p><p>ment. The morphology of nanofibers with ca. 20 nm - 60 nm in width and several hundred nanometers in length was observed in the SEM image of the sample from the dispersion (<xref ref-type="fig" rid="fig9">Figure 9</xref>(a)), indicating the formation of the self-assembled chitin nanofibers by the above regeneration approach from the ion gel according to the bottomup process. When the dispersion was filtered, the residue formed a film, which was further purified by Soxhlet extraction with methanol. The SEM image of the resulting film was also measured to confirm the nanoscaled morphology of chitin, which showed the pattern of highly entangled nanofibers (<xref ref-type="fig" rid="fig9">Figure 9</xref>(b)). This suggested that such entangled structure of the nanofibers contributed to formability of the film. The XRD pattern of the chitin nanofiber film mainly showed the diffraction peaks corresponding to crystalline structure of α-chitin and is in good agreement with that of an original chitin powder. The result indicated that the crystalline structure of α- chitin was reconstructed by the above regeneration procedure during the formation of the nanofibers.</p><p>As one of the possible applications of the present chitin nanofiber film, the preparation of the chitin nanofiberpoly(vinyl alcohol) (PVA) composite films was investigated (<xref ref-type="fig" rid="fig8">Figure 8</xref>, Route B) [<xref ref-type="bibr" rid="scirp.31731-ref46">46</xref>]. First, the 9.1 wt% chitin ion gel with AMIMBr was prepared according to the aforementioned procedure and a solution of PVA (DP = ca. 4300) in a small amount of hot water was added to the gel (the feed weight ratio of chitin to PVA = 1:0.30). Then, the co-regeneration using methanol was conducted, followed by filtration and Soxhlet extraction with methanol same as the aforementioned procedure to produce the chitin nanofiber-PVA composite film. It was confirmed that a small amount of AMIMBr was remained in the composite. The SEM image of the composite showed that the nanofiber-like morphology was maintained and PVA components probably filled in spaces among the fibers (<xref ref-type="fig" rid="fig9">Figure 9</xref>(c)), indicating relative immiscibility of chitin and PVA in the composite. Indeed, the DSC profile of the composite film exhibited an endothermic peak attributed to the melting point of PVA, suggesting some immiscibility of PVA toward chitin in the composite. However, the melting point peak of PVA in the composite film was broadened, indicating that the crystallinity of PVA decreased in the composite film. The DSC result suggested that chitin and PVA might be partially misci-</p><p>ble at the interfacial area between the two polymers in the composite film by the formation of hydrogen bonding between them or by the presence of a small amount of AMIMBr.</p></sec><sec id="s5"><title>5. Conclusion</title><p>This article reviewed the dissolution, derivatization, and nanomaterial processing of chitin using the ionic liquid, AMIMBr. Because the author found that AMIMBr dissolved chitin in the concentrations up to 4.8 wt% by heating and further the chitin ion gels were obtained from the mixture of the higher amounts of chitin with AMIMBr, acetylation of chitin using acetic anhydride was performed in the AMIMBr solvent to give the acetylated chitins with the high DS values. Chitin-based nanomaterials such as chitin nanofibers and nanocomposites with synthetic polymer were also fabricated using AMIMBr. Immersing the ion gel in methanol and subsequent sonication gave the chitin dispersion. The SEM image of the dispersion showed the formation of the self-assembled chitin nanofibers. Then, filtration of the dispersion was carried out to give the chitin nanofiber film. The composite film of the chitin nanofibers with PVA was prepared by a similar procedure as that for the chitin nanofiber film. The present methods using the ionic liquid, AMIMBr, provide new chitin-based functional and composite materials which have a highly potential to apply to practical material research filed in the future. Finally, the author would like to state that this review has especially presented to the readers how the ionic liquid media are useful for new approaches in the chitin research field, which will be increasingly developed with attracting much attention on the further technological interests in the efficient use of chitin as the abundant biomass resource.</p></sec><sec id="s6"><title>6. 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