Design and Analysis of A Complete Full Adder Based On Metal-Insulator-Metal (MIM) Waveguide-Based Plasmonic Waves

Design and Analysis of A Complete Full Adder Based On Metal-Insulator-Metal (MIM) Waveguide-Based Plasmonic Waves | Research Square window.SnipcartSettings = { analytics: { enabled: false } }; (function() { var accessVector = localStorage.getItem('access_vector') || ''; window.dataLayer = window.dataLayer || []; if (accessVector) { window.dataLayer.push({ user: { profile: { profileInfo: { snid: accessVector } } } }); } })(); (function(w,d,s,l,i){w[l]=w[l]||[];w[l].push({'gtm.start':new Date().getTime(),event:'gtm.js'});var f=d.getElementsByTagName(s)[0],j=d.createElement(s),dl=l!='dataLayer'?'&l='+l:'';j.async=true;j.src='https://www.googletagmanager.com/gtm.js?id='+i+dl;f.parentNode.insertBefore(j,f);})(window,document,'script','dataLayer','GTM-K279D39R'); Browse Preprints In Review Journals COVID-19 Preprints AJE Video Bytes Research Tools Research Promotion AJE Professional Editing AJE Rubriq About Preprint Platform In Review Editorial Policies Our Team Advisory Board Help Center Sign In Submit a Preprint Cite Share Download PDF Research Design and Analysis of A Complete Full Adder Based On Metal-Insulator-Metal (MIM) Waveguide-Based Plasmonic Waves oraman yoosefi, Angel Rodríguez This is a preprint; it has not been peer reviewed by a journal. https://doi.org/ 10.21203/rs.3.rs-34397/v1 This work is licensed under a CC BY 4.0 License Status: Posted Version 1 posted You are reading this latest preprint version Abstract In this paper, metal-insulator-metal (MIM) plasmonic waveguide structures and a rectangular cavity resonator at a central frequency of 1550 nm were used to propose a complete full adder. Under this circumstances, the system has a fast function with slight variations in real- time or near real-time manner, and this led to its minimum power consumption, while serving in various situations. In this full adder, we benefited from the property of combining resonant waves in the first and second modes, and we managed to obtain a high transmission coefficient in states where the output must be active. This complete full adder operates through designing 4-input AND, XOR, OR, and NOT logic gates, resulting in the design of a complete full adder with low manufacturing complexity and cost relative to ones designed through combining the conventional 2-input AND and OR gates. In comparison of three computational methods, finite‐difference time‐domain (FDTD) is a simple and versatile method. This method directly discretizes the time‐domain partial differential form of Maxwell's equations in various dimensions while using analytical solution in the remaining direction and solving the 3D scattering problem. Therefore, necessary simulations were conducted using FDTD software, and showed a good fit to the results predicted through approximations intended for theoretical relations. Optical Materials and Devices Full adder OR gate Plasmonic waves Resonance wavelength MIM Waveguide Figures Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Full Text Supplementary Files comments.docx Cite Share Download PDF Status: Posted Version 1 posted You are reading this latest preprint version Research Square lets you share your work early, gain feedback from the community, and start making changes to your manuscript prior to peer review in a journal. As a division of Research Square Company, we’re committed to making research communication faster, fairer, and more useful. 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Also discoverable on Platform About Our Team In Review Editorial Policies Advisory Board Help Center Resources Author Services Accessibility API Access RSS feed Manage Cookie Preferences © Research Square 2026 | ISSN 2693-5015 (online) Privacy Policy Terms of Service Do Not Sell My Personal Information {"props":{"pageProps":{"initialData":{"identity":"rs-34397","acceptedTermsAndConditions":true,"allowDirectSubmit":true,"archivedVersions":[],"articleType":"Research","associatedPublications":[],"authors":[{"id":659389,"identity":"8165f86b-917c-4a92-8a64-f6ca473560da","order_by":0,"name":"oraman yoosefi","email":"data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAAZAAAAAyAQMAAABI0h/eAAAABlBMVEX///8AAABVwtN+AAAACXBIWXMAAA7EAAAOxAGVKw4bAAAA8UlEQVRIiWNgGAWjYNCDCgMbIMnYeIB4LWcM0kBaGkjRwnAYTOPVwi99+OmGnzsYEvvZ2x8+OFBw3m5t+2GgLTU20bi0SPalmd3sPcOQOLPnjLHBAYPbydvOJAK1HEvLbcChxeAMg9kN3jaGxA03ctikPwC1mB0AamFsOIxHC/u3m3/BWtKf/zhgcC7Z7PxDQlp4zG5DbEkwYzhgcMDO7AYBWyR7eMpuy7ZJGIP8InHAIDnB7AbQlgQ8fuHnYd92822bjSwoxD4c+GNnb3Y+/eGDDzU2OLVAgYQjTEEimJGAXzkY2GMwRsEoGAWjYBTAAAAHmWhZl0e9fgAAAABJRU5ErkJggg==","orcid":"https://orcid.org/0000-0002-1872-8054","institution":"Universitat Politecnica de Catalunya","correspondingAuthor":true,"prefix":"","firstName":"oraman","middleName":"","lastName":"yoosefi","suffix":""},{"id":659390,"identity":"0b75c226-24ee-43cf-9e39-3dd39988543b","order_by":1,"name":"Angel Rodríguez","email":"","orcid":"","institution":"Universitat Politecnica de Catalunya","correspondingAuthor":false,"prefix":"","firstName":"Angel","middleName":"","lastName":"Rodríguez","suffix":""}],"badges":[],"createdAt":"2020-06-08 22:22:41","currentVersionCode":1,"declarations":"","doi":"10.21203/rs.3.rs-34397/v1","doiUrl":"https://doi.org/10.21203/rs.3.rs-34397/v1","draftVersion":[],"editorialEvents":[],"editorialNote":"","failedWorkflow":false,"files":[{"id":1317524,"identity":"2a06658f-4de7-46fa-a8d6-4f39c687aad8","added_by":"auto","created_at":"2020-06-12 19:16:07","extension":"jpg","order_by":1,"title":"Figure 1","display":"","copyAsset":false,"role":"figure","size":30684,"visible":true,"origin":"","legend":"The structure and dimensions of a 4-input OR logic gate","description":"","filename":"Fig1.jpg","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/Fig1.jpg"},{"id":1317525,"identity":"2e7f3411-e40e-4131-a51b-a2ebc4c43c57","added_by":"auto","created_at":"2020-06-12 19:16:07","extension":"jpg","order_by":2,"title":"Figure 2","display":"","copyAsset":false,"role":"figure","size":11839,"visible":true,"origin":"","legend":"The resonance wavelengths for the structure","description":"","filename":"Fig2.jpg","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/Fig2.jpg"},{"id":1317526,"identity":"5e20f9fe-d81a-40e1-9bb1-b50bf34cb0c2","added_by":"auto","created_at":"2020-06-12 19:16:07","extension":"jpg","order_by":3,"title":"Figure 3","display":"","copyAsset":false,"role":"figure","size":31388,"visible":true,"origin":"","legend":"The structure of the designed 4-input OR gate: (a) The state where all four input ports are stimulated;(b) The electric field amplitude at a wavelength of 1490 nm at the output port; (c) Shows the fields in the gate structure at a wavelength of 1490 nm.","description":"","filename":"Fig3.jpg","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/Fig3.jpg"},{"id":1317527,"identity":"1bcbee43-0b1b-4aa5-b685-2075a61f70bc","added_by":"auto","created_at":"2020-06-12 19:16:07","extension":"jpg","order_by":4,"title":"Figure 4","display":"","copyAsset":false,"role":"figure","size":32522,"visible":true,"origin":"","legend":"The structure of the designed 4-input OR gate: (a) The stimulation state where Input-1 = 0, Input-2 = 1, Input-3 = 0, and Input-4 = 1; (b) The electric field amplitude at a wavelength of 1490 nm at the output port; (c) Shows the fields in the gate structure at a wavelength of 1490 nm.","description":"","filename":"Fig4.jpg","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/Fig4.jpg"},{"id":1317528,"identity":"ef8f67fe-9a1c-4289-b0fd-6ce3655bdd9d","added_by":"auto","created_at":"2020-06-12 19:16:07","extension":"jpg","order_by":5,"title":"Figure 5","display":"","copyAsset":false,"role":"figure","size":27854,"visible":true,"origin":"","legend":"The structure of the designed 4-input OR gate: (a) The stimulation state where Input-1 = 1, Input-2 = 1, Input-3 = 0, and Input-0 = 0; (b) The electric field amplitude at a wavelength of 1490 nm at the output port; (c) Shows the fields in the gate structure at a wavelength of 1490 nm.","description":"","filename":"Fig5.jpg","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/Fig5.jpg"},{"id":1317529,"identity":"e7e9010a-bdc4-427b-8ebd-705bc70b6747","added_by":"auto","created_at":"2020-06-12 19:16:07","extension":"jpg","order_by":6,"title":"Figure 6","display":"","copyAsset":false,"role":"figure","size":25384,"visible":true,"origin":"","legend":"The structure of the designed 4-input OR gate: (a) The stimulation state where Input-1 = 1, Input-2 = 0, Input-3 = 0, and Input-0 = 0; (b) The electric field amplitude at a wavelength of 1490 nm at the output port; (c) Shows the fields in the gate structure at a wavelength of 1490 nm.","description":"","filename":"Fig6.jpg","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/Fig6.jpg"},{"id":1317531,"identity":"3cd0f031-f103-4167-8dc7-6515353b3165","added_by":"auto","created_at":"2020-06-12 19:16:09","extension":"pdf","order_by":0,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":764811,"visible":true,"origin":"","legend":"","description":"","filename":"DesignandAnalysisofaCompleteFullAdder.jadid.pdf","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1_stamped.pdf"},{"id":1317530,"identity":"a244a8bc-5e63-4684-9388-cf385799214b","added_by":"auto","created_at":"2020-06-12 19:16:08","extension":"pdf","order_by":0,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":691762,"visible":true,"origin":"","legend":"","description":"","filename":"DesignandAnalysisofaCompleteFullAdder.jadid.pdf","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/DesignandAnalysisofaCompleteFullAdder.jadid.pdf"},{"id":13509130,"identity":"59d59da1-082f-4684-a7d2-5bf452efd30b","added_by":"auto","created_at":"2021-09-16 23:42:17","extension":"pdf","order_by":1,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":615106,"visible":true,"origin":"","legend":"","description":"","filename":"DesignandAnalysisofaCompleteFullAdder.jadid.pdf","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1_covered.pdf"},{"id":1491282,"identity":"0a216d18-20a3-4587-8cf1-bf5dee6db44e","added_by":"auto","created_at":"2020-07-04 17:12:47","extension":"docx","order_by":1,"title":"","display":"","copyAsset":false,"role":"supplement","size":50365,"visible":true,"origin":"","legend":"","description":"","filename":"comments.docx","url":"https://assets-eu.researchsquare.com/files/rs-34397/v1/comments.docx"}],"financialInterests":"","formattedTitle":"\u003cp\u003eDesign and Analysis of A Complete Full Adder Based On Metal-Insulator-Metal (MIM) Waveguide-Based Plasmonic Waves\u003c/p\u003e","fulltext":[{"header":"Full Text","content":"\u003cp\u003eThis preprint is available for \u003ca href='/article/rs-34397/latest.pdf' target='_blank'\u003edownload as a PDF\u003c/a\u003e.\u003c/p\u003e"}],"fulltextSource":"","fullText":"","funders":[],"hasAdminPriorityOnWorkflow":false,"hasManuscriptDocX":false,"hasOptedInToPreprint":true,"hasPassedJournalQc":"","hasAnyPriority":false,"hideJournal":true,"highlight":"","institution":"","isAcceptedByJournal":false,"isAuthorSuppliedPdf":true,"isDeskRejected":"","isHiddenFromSearch":false,"isInQc":false,"isInWorkflow":false,"isPdf":false,"isPdfUpToDate":true,"isWithdrawnOrRetracted":false,"journal":{"display":true,"email":"[email protected]","identity":"researchsquare","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":true,"externalIdentity":"","sideBox":"","snPcode":"","submissionUrl":"/submission","title":"Research Square","twitterHandle":"researchsquare","acdcEnabled":true,"dfaEnabled":false,"editorialSystem":"","reportingPortfolio":"","inReviewEnabled":false,"inReviewRevisionsEnabled":true},"keywords":"Full adder, OR gate, Plasmonic waves, Resonance wavelength, MIM Waveguide","lastPublishedDoi":"10.21203/rs.3.rs-34397/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-34397/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eIn this paper, metal-insulator-metal (MIM) plasmonic waveguide structures and a rectangular cavity resonator at a central frequency of 1550 nm were used to propose a complete full adder. Under this circumstances, the system has a fast function with slight variations in real- time or near real-time manner, and this led to its minimum power consumption, while serving in various situations. In this full adder, we benefited from the property of combining resonant waves in the first and second modes, and we managed to obtain a high transmission coefficient in states where the output must be active. This complete full adder operates through designing 4-input AND, XOR, OR, and NOT logic gates, resulting in the design of a complete full adder with low manufacturing complexity and cost relative to ones designed through combining the conventional 2-input AND and OR gates. \u003c/p\u003e\u003cp\u003eIn comparison of three computational methods, finite‐difference time‐domain (FDTD) is \u0026nbsp;a simple and versatile method. This method directly discretizes the time‐domain partial differential form of Maxwell's equations\u0026nbsp;in various dimensions while using analytical solution in the remaining direction and solving the 3D scattering problem. Therefore, necessary simulations were conducted using FDTD software, and showed a good fit to the results predicted through approximations intended for theoretical relations.\u003c/p\u003e","manuscriptTitle":"Design and Analysis of A Complete Full Adder Based On Metal-Insulator-Metal (MIM) Waveguide-Based Plasmonic Waves","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2020-06-12 19:16:06","doi":"10.21203/rs.3.rs-34397/v1","editorialEvents":[{"type":"communityComments","content":0}],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"researchsquare","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":true,"externalIdentity":"","sideBox":"","snPcode":"","submissionUrl":"/submission","title":"Research Square","twitterHandle":"researchsquare","acdcEnabled":true,"dfaEnabled":false,"editorialSystem":"","reportingPortfolio":"","inReviewEnabled":false,"inReviewRevisionsEnabled":true}}],"origin":"","ownerIdentity":"0dc3fd6f-6e75-4c19-8771-1b0ac86512de","owner":[],"postedDate":"June 12th, 2020","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"posted","subjectAreas":[{"id":118852,"name":"Optical Materials and Devices"}],"tags":[],"updatedAt":"2020-07-04T17:12:46+00:00","versionOfRecord":[],"versionCreatedAt":"2020-06-12 19:16:06","video":"","vorDoi":"","vorDoiUrl":"","workflowStages":[]},"version":"v1","identity":"rs-34397","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-34397","identity":"rs-34397","version":["v1"]},"buildId":"J0_U0BvcaRcwD8yVFaRlm","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}