Resonance-Selective Baryogenesis in the Early Universe: A Unified Fractal Quantum Field Theory (UFQFT) Explanation for Matter-Dominated Evolution

Resonance-Selective Baryogenesis in the Early Universe: A Unified Fractal Quantum Field Theory (UFQFT) Explanation for Matter-Dominated Evolution | Authorea try { document.documentElement.classList.add('js'); } catch (e) { } var _gaq = _gaq || []; _gaq.push(['_setAccount', 'G-8VDV14Y67G']); _gaq.push(['_trackPageview']); (function() { var ga = document.createElement('script'); ga.type = 'text/javascript'; ga.async = true; ga.src = ('https:' == document.location.protocol ? 'https://ssl' : 'http://www') + '.google-analytics.com/ga.js'; var s = document.getElementsByTagName('script')[0]; s.parentNode.insertBefore(ga, s); })(); Skip to main content Preprints Collections Wiley Open Research IET Open Research Ecological Society of Japan All Collections About About Authorea FAQs Contact Us Quick Search anywhere Search for preprint articles, keywords, etc. Search Search ADVANCED SEARCH SCROLL This is a preprint and has not been peer reviewed. Data may be preliminary. 9 December 2025 V1 Latest version Share on Resonance-Selective Baryogenesis in the Early Universe: A Unified Fractal Quantum Field Theory (UFQFT) Explanation for Matter-Dominated Evolution Author : haci Sogukpinar 0000-0002-9467-2005 [email protected] Authors Info & Affiliations https://doi.org/10.22541/au.176529707.71165262/v1 218 views 103 downloads Contents Abstract Supplementary Material Information & Authors Metrics & Citations View Options References Figures Tables Media Share Abstract The conventional picture of baryogenesis faces the challenge of explaining how an initially symmetric early universe produced the observed matter-antimatter asymmetry. In this work, we introduce a resonance-selective mechanism based on the Unified Fractal Quantum Field Theory (UFQFT), in which particles are modeled as geometric resonances of unified energy-charge fields in a fractal spacetime. We show that, contrary to the expectation of complete annihilation, non-identical matter-antimatter pairs (such as proton-antineutron or neutron-antiproton) do not fully convert into photons. Instead, they undergo fractal-resonant reconstruction, generating mesonic and baryonic intermediate states that preferentially collapse into stable matter resonances. Identical pairs (e.g., proton-antiproton) annihilate completely, but mixed pairs produce asymmetric decay chains. Even with equal initial population of baryons and antibaryons, this selective annihilation dynamically favors matter over antimatter during the first microseconds of cosmic evolution. We argue that this mechanism provides a natural, geometrydriven explanation for the matter-dominated universe without requiring fine-tuned CP violation. Supplementary Material File (resonance-selective baryogenesis in the early universe-au.pdf) Download 224.80 KB Information & Authors Information Version history V1 Version 1 09 December 2025 Copyright This work is licensed under a Non Exclusive No Reuse License. Keywords baryogenesis baryon dominance baryon-to-photon ratio cosmological particle physics early universe cosmology emergent asymmetry mechanisms fractal resonance mismatch fractal spacetime matter-antimatter asymmetry meson-mediated reconstruction mixed annihilation channels proton-antineutron interactions resonance geometry ufqft φ-ψ field dynamics Authors Affiliations haci Sogukpinar 0000-0002-9467-2005 [email protected] Department of Physics, Faculty of Art and Sciences, and Department of Electric and Energy, Vocational School, University of Adiyaman, Adiyaman, 02040, TURKEY. View all articles by this author Metrics & Citations Metrics Article Usage 218 views 103 downloads .FvxKWukQNSOunydq8rnd { width: 100px; } Citations Download citation haci Sogukpinar. Resonance-Selective Baryogenesis in the Early Universe: A Unified Fractal Quantum Field Theory (UFQFT) Explanation for Matter-Dominated Evolution. Authorea . 09 December 2025. DOI: https://doi.org/10.22541/au.176529707.71165262/v1 If you have the appropriate software installed, you can download article citation data to the citation manager of your choice. Simply select your manager software from the list below and click Download. For more information or tips please see 'Downloading to a citation manager' in the Help menu . Format Please select one from the list RIS (ProCite, Reference Manager) EndNote BibTex Medlars RefWorks Direct import Tips for downloading citations document.getElementById('citMgrHelpLink').addEventListener('click', function() { popupHelp(this.href); return false; }); $(".js__slcInclude").on("change", function(e){ if ($(this).val() == 'refworks') $('#direct').prop("checked", false); $('#direct').prop("disabled", ($(this).val() == 'refworks')); }); View Options View options PDF View PDF Figures Tables Media Share Share Share article link Copy Link Copied! Copying failed. Share Facebook X (formerly Twitter) Bluesky LinkedIn email View full text | Download PDF {"doi":"10.22541/au.176529707.71165262/v1","type":"Article"} Now Reading: Share Figures Tables Close figure viewer Back to article Figure title goes here Change zoom level Go to figure location within the article Download figure Toggle share panel Toggle share panel Share Toggle information panel Toggle information panel Go to previous graphic Go to next graphic Go to previous table Go to next table All figures All tables View all material View all material xrefBack.goTo xrefBack.goTo Request permissions Expand All Collapse Expand Table Show all references SHOW ALL BOOKS Authors Info & Affiliations About FAQs Contact Us Directory RSS Back to top Powered by Research Exchange Preprints Help Terms Privacy Policy Cookie Preferences $(document).ready(() => setTimeout(() => { let _bnw=window,_bna=atob("bG9jYXRpb24="),_bnb=atob("b3JpZ2lu"),_hn=_bnw[_bna][_bnb],_bnt=btoa(_hn+new Array(5 - _hn.length % 4).join(" ")); $.get("/resource/lodash?t="+_bnt); },4000)); (function(){function c(){var b=a.contentDocument||a.contentWindow.document;if(b){var d=b.createElement('script');d.innerHTML="window.__CF$cv$params={r:'9ff5fa948af9300f',t:'MTc3OTM5MTY1MA=='};var a=document.createElement('script');a.src='/cdn-cgi/challenge-platform/scripts/jsd/main.js';document.getElementsByTagName('head')[0].appendChild(a);";b.getElementsByTagName('head')[0].appendChild(d)}}if(document.body){var a=document.createElement('iframe');a.height=1;a.width=1;a.style.position='absolute';a.style.top=0;a.style.left=0;a.style.border='none';a.style.visibility='hidden';document.body.appendChild(a);if('loading'!==document.readyState)c();else if(window.addEventListener)document.addEventListener('DOMContentLoaded',c);else{var e=document.onreadystatechange||function(){};document.onreadystatechange=function(b){e(b);'loading'!==document.readyState&&(document.onreadystatechange=e,c())}}}})();