![]() ![]() This limited warranty only applies to authentic Crossover Symmetry products. ![]() This limited warranty is limited as follows: The terms of this limited warranty provide the exclusive and sole remedy available to you. What Does This Limited Warranty Not Cover? 13-24 Months – After 12 months, the purchaser must pay shipping costs for repaired or replaced products.0-12 Months – Within 12 months of purchase, Crossover Symmetry will also cover domestic UPS Ground shipping costs for repaired or replaced products. ![]() It does not cover injuries or damages to third parties using the products.Īt its discretion, Crossover Symmetry will repair or replace any defective Crossover Symmetry exercise products covered by this limited warranty. ![]() This limited warranty covers the original purchaser only and lasts for Two (2) Years (“Warranty Period”), beginning from the purchase date. Who Does the Limited Warranty Cover & How Long Does The Coverage Last? This limited warranty applies to products intended solely for personal, family, or household purposes. This limited warranty covers defects in manufacture and materials with your Crossover Symmetry products purchased through Fitworks, Inc, DBA Crossover Symmetry or an authorized re-seller. S2CID 119416033.Crossover Symmetry Limited Warranty for Crossover Symmetry Products Intended Solely for the purchaser of the products. "The Electroweak Phase Transition: A Non-Perturbative Analysis". Current Topics in Astrofundamental Physics: Primordial Cosmology. "Electroweak Phase Transition in the Early Universe?". ^ Bergerhoff, Bastian Wetterich, Christof (1998).Soviet Physics Uspekhi (in Russian and English). "Violation of CP invariance, C asymmetry, and baryon asymmetry of the universe". Journal of Experimental and Theoretical Physics Letters. : CS1 maint: multiple names: authors list ( link) "Standard model cross-over on the lattice". ^ D'Onofrio, Michela and Rummukainen, Kari (2016).However many extensions to the Standard Model including supersymmetry and the two-Higgs-doublet model have a first-order electroweak phase transition (but require additional CP violation). Or the production of an observable gravitational wave background. In the minimal Standard Model, the transition during the electroweak epoch was not a first- or a second-order phase transition but a continuous crossover, preventing any baryogenesis, The electroweak phase transition is also a potential source of baryogenesis, provided the Sakharov conditions are satisfied. If first order, this could source a gravitational wave background. The electroweak epoch ended with an electroweak phase transition, the nature of which is unknown. The remaining W and Z bosons decayed quickly, and the weak interaction became a short-range force in the following quark epoch. As the universe expanded and cooled, interactions became less energetic and when the universe was about 10 −12 seconds old, W and Z bosons ceased to be created at observable rates. Particle interactions in this phase were energetic enough to create large numbers of exotic particles, including W and Z bosons and Higgs bosons. Others place it at approximately 10 −32 seconds after the Big Bang when the potential energy of the inflaton field that had driven the inflation of the universe during the inflationary epoch was released, filling the universe with a dense, hot quark–gluon plasma. The current concept of the universe has passed debate of the current academic community however, there remains a conjecture, approximately 10 −33 seconds, after the Big Bang. Some theorists suggest that this inflation is permanent, and may have created a universe that includes our parent universe or multiverse. The universe is supercooled from about 10 27 down to 10 22 kelvin. Space is subjected to inflation, expanding by a factor of the order of 10 26 over a time of the order of 10 −33 to 10 −32 seconds. Some cosmologists place the electroweak epoch at the start of the inflationary epoch, approximately 10 −36 seconds after the Big Bang. In the Standard Model of particle physics). In physical cosmology, the electroweak epoch was the period in the evolution of the early universe when the temperature of the universe had fallen enough that the strong force separated from the electroweak interaction, but was high enough for electromagnetism and the weak interaction to remain merged into a single electroweak interaction above the critical temperature for electroweak symmetry breaking (159.5☑.5 GeV ![]()
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