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Mikhail Shaposhnikov

Researcher at École Polytechnique Fédérale de Lausanne

Publications -  298
Citations -  34138

Mikhail Shaposhnikov is an academic researcher from École Polytechnique Fédérale de Lausanne. The author has contributed to research in topics: Baryon asymmetry & Higgs boson. The author has an hindex of 76, co-authored 281 publications receiving 30085 citations. Previous affiliations of Mikhail Shaposhnikov include Aspen Center For Physics & University of Copenhagen.

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The statistical theory of anomalous fermion number non-conservation

TL;DR: In this article, the authors present a non-equilibrium method for studying anomalous B -nonconservation in the electroweak theory at finite temperature, and derive formally the equation of B -evolution advocated previously on physical grounds.
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The Electroweak Phase Transition: A Non-Perturbative Analysis

TL;DR: In this article, the 3D SU(2)+Higgs model is studied on the lattice and the 3-loop correction to the effective potential of the scalar field is determined.
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Generic rules for high temperature dimensional reduction and their application to the Standard Model

TL;DR: In this article, the authors formulate the rules for dimensional reduction of a generic finite temperature gauge theory to a simpler three-dimensional effective bosonic theory in terms of a matching of Green functions in the full and the effective theory, and present a computable set of 1-and 2-loop graphs needed for the application of these rules.
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FCC Physics Opportunities: Future Circular Collider Conceptual Design Report Volume 1

A. Abada, +1504 more
TL;DR: In this article, the physics opportunities of the Future Circular Collider (FC) were reviewed, covering its e+e-, pp, ep and heavy ion programs, and the measurement capabilities of each FCC component, addressing the study of electroweak, Higgs and strong interactions.
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Asymptotic safety of gravity and the Higgs boson mass

TL;DR: For a positive gravity induced anomalous dimension A λ > 0, the running of the quartic scalar self interaction at scales beyond the Planck mass is determined by a fixed point at zero as mentioned in this paper.