ELECTROWEAK ANOMALY AND LEPTON ASYMMETRY
Edward W. Kolb, Michael S. Turner
Abstract
Edward W. Kolb, Michael S. Turner
Abstract
It has recently been pointed out that shortly after the electroweak phase transition (t≃10−11 sec , T≃100–200 GeV ) there was a period of very effective baryon (and lepton) number violation driven by non-perturbative effects arising from the electroweak anomaly. Here we argue that as a result of these electroweak interactions the total asymmetry in leptons must be equal and opposite to the baryon asymmetry: L≡∑iLi=Le+Lμ+Lr=−B. Since the individual lepton numbers can be positive or negative, this does not preclude any large individual contribution, i.e., |Li|>B. This fact has important consequences for primordial nucleosynthesis if |Li|≳1.
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It has recently been pointed out that shortly after the electroweak phase transition (t≃10−11 sec , T≃100–200 GeV ) there was a period of very effective baryon (and lepton) number violation driven by non-perturbative effects arising from the electroweak anomaly. Here we argue that as a result of these electroweak interactions the total asymmetry in leptons must be equal and opposite to the baryon asymmetry: L≡∑iLi=Le+Lμ+Lr=−B. Since the individual lepton numbers can be positive or negative, this does not preclude any large individual contribution, i.e., |Li|>B. This fact has important consequences for primordial nucleosynthesis if |Li|≳1.
Key concepts: Physics, Electroweak interaction, Particle physics, Lepton, Asymmetry, Anomaly (physics), Lepton number, Baryon asymmetry