false vacuum decay in gauge theory
play

False vacuum decay in gauge theory ~Standard model and beyond~ - PowerPoint PPT Presentation

Mar 09, 2024 •17 likes •377 views

PPP2018@YITP , 6-10 Aug 2018 False vacuum decay in gauge theory ~Standard model and beyond~ Yutaro Shoji (KMI, Nagoya U.) Phys. Lett. B771(2017)281; M. Endo, T. Moroi, M. M. Nojiri, YS JHEP11(2017)074; M. Endo, T. Moroi, M. M. Nojiri, YS Phys.

  1. PPP2018@YITP , 6-10 Aug 2018 False vacuum decay in gauge theory ~Standard model and beyond~ Yutaro Shoji (KMI, Nagoya U.) Phys. Lett. B771(2017)281; M. Endo, T. Moroi, M. M. Nojiri, YS JHEP11(2017)074; M. Endo, T. Moroi, M. M. Nojiri, YS Phys. Rev. Lett. 119 (2017) no.21, 211801; S. Chigusa, T. Moroi, YS Phys. Rev. D97 (2018) no.11, 116012; S. Chigusa, T. Moroi, YS https://github.com/YShoji-HEP/ELVAS

  2. Introduction

  3. <latexit sha1_base64="J628e3KH6Hzd58Tl90c7NsjuWao=">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</latexit> <latexit sha1_base64="J628e3KH6Hzd58Tl90c7NsjuWao=">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</latexit> <latexit sha1_base64="J628e3KH6Hzd58Tl90c7NsjuWao=">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</latexit> <latexit sha1_base64="J628e3KH6Hzd58Tl90c7NsjuWao=">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</latexit> <latexit sha1_base64="9U8J0QXYvcn1KYg7ScAGc/Xhc=">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</latexit> <latexit sha1_base64="9U8J0QXYvcn1KYg7ScAGc/Xhc=">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</latexit> <latexit sha1_base64="9U8J0QXYvcn1KYg7ScAGc/Xhc=">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</latexit> <latexit sha1_base64="9U8J0QXYvcn1KYg7ScAGc/Xhc=">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</latexit> Vacuum decay in the standard model V ( Φ ) = λ ( Φ † Φ ) 2 − M 2 ( Φ † Φ ) Vacuum Energy ' λ ( Φ † Φ ) 2 Low energy High energy λ > 0 λ < 0 (due to RG running) ∼ 10 10 GeV Field value Tunneling EW vacuum False vacuum True vacuum

Recommend

Flowing to the Bounce Takeo Moroi (Tokyo) Refs: Chigusa, TM, Shoji, 1906.10829 [hep-ph] PPP

Flowing to the Bounce Takeo Moroi (Tokyo) Refs: Chigusa, TM, Shoji, 1906.10829 [hep-ph] PPP

Flowing to the Bounce Takeo Moroi (Tokyo) Refs: Chigusa, TM, Shoji, 1906.10829 [hep-ph] PPP Workshop @ YITP, 19.08.01 1. Introduction V The subject today: a new method to calculate the bounce False vacuum false vacuum decay True

495 views • 30 slides
Contents of this talk 1. Experimental data 2. Theory : Mesonic decay 3. Theory : Nonmesonic decay

Contents of this talk 1. Experimental data 2. Theory : Mesonic decay 3. Theory : Nonmesonic decay

Hypernuclear weak decay : -- present and future problems -- K. Itonaga Gifu University Kakenhi-kenkyukai Atami2009 Atami Feb.27-28 2009 1 Contents of this talk 1. Experimental data 2. Theory : Mesonic decay 3. Theory : Nonmesonic decay 4.

579 views • 30 slides
Towards a Towards a Gauge Theory of Gravity Gauge Theory of Gravity Ivan Debono Fundamental

Towards a Towards a Gauge Theory of Gravity Gauge Theory of Gravity Ivan Debono Fundamental

Towards a Towards a Gauge Theory of Gravity Gauge Theory of Gravity Ivan Debono Fundamental Interactions All physical interactions in nature described by 4 fundamental forces: Gravity Electromagnetism Weak nuclear force

390 views • 20 slides
False vacuum as an unstable state: possible cosmological implications Krzysztof Urbanowski 1 ,

False vacuum as an unstable state: possible cosmological implications Krzysztof Urbanowski 1 ,

False vacuum as an unstable state: possible cosmological implications Krzysztof Urbanowski 1 , University of Zielona G ora, Institute of Physics, ul. Prof. Z. Szafrana 4a, 65516 Zielona G ora, Poland. 25 th Recontres de Blois: Particle

645 views • 33 slides
Algebras of observables: a gauge theory example Owen Gwilliam Max Planck Institut f ur

Algebras of observables: a gauge theory example Owen Gwilliam Max Planck Institut f ur

Algebras of observables: a gauge theory example Owen Gwilliam Max Planck Institut f ur Mathematik, Bonn 9 December 2017 Owen Gwilliam Algebras of observables: a gauge theory example A basic challenge with gauge theory The usual kinematics

434 views • 28 slides
SU(2) with six flavors A new kind of gauge theory George T. Fleming (Yale) for the LSD

SU(2) with six flavors A new kind of gauge theory George T. Fleming (Yale) for the LSD

SU(2) with six flavors A new kind of gauge theory George T. Fleming (Yale) for the LSD Collaboration Two-Color Gauge Theories Perturbatively, SU(2) gauge theories behave like any other SU(N c ) gauge theory. Non-perturbatively, SU(2)

384 views • 16 slides
Decay Tube &amp; Windows Decay Tube &amp; Windows Introduction (Location, Planning) Decay Tube

Decay Tube &amp; Windows Decay Tube &amp; Windows Introduction (Location, Planning) Decay Tube

Decay Tube &amp; Windows Decay Tube &amp; Windows Introduction (Location, Planning) Decay Tube Entrance Window Exit Window Vacuum System NBI 2003 - Decay Tube and Windows 11/ 11/ 2003 1 1 Present at ion by Ans Pardons Location

323 views • 21 slides
Set Theory: doubtful: This statement is false. Russell Paradox is it true or false?

Set Theory: doubtful: This statement is false. Russell Paradox is it true or false?

Mathematics for Computer Science Self application MIT 6.042J/18.062J Self application is notoriously Set Theory: doubtful: This statement is false. Russell Paradox is it true or false? Albert R Meyer, March 4, 2015 Albert R

62 views • 5 slides
Fate of a recent conformal fixed point and -function in the SU (3) BSM gauge theory with ten

Fate of a recent conformal fixed point and -function in the SU (3) BSM gauge theory with ten

Fate of a recent conformal fixed point and -function in the SU (3) BSM gauge theory with ten massless flavors Daniel Nogradi in collaboration with Zoltan Fodor, Kieran Holland Julius Kuti, Chik Him Wong What, why and how? SU (3) gauge

476 views • 43 slides
Insightful D-branes Albion Lawrence Brandeis University 1 Outline I. Introduction II. A

Insightful D-branes Albion Lawrence Brandeis University 1 Outline I. Introduction II. A

Insightful D-branes Albion Lawrence Brandeis University 1 Outline I. Introduction II. A singularity with a gauge theory dual III. Gauge theory vs. spacetime coordinate transformations IV. Gauge theory dynamics and hyperbolic black holes V.

478 views • 33 slides
What is theory? Theory is when you make claims that are either True or False, but not

What is theory? Theory is when you make claims that are either True or False, but not

What is theory? Theory is when you make claims that are either True or False, but not both Example of claims: 1+1 = 2 there is a graph with &gt; 56 edges all prime numbers are between 57 and 59 all regular languages are context-free

489 views • 28 slides
Gauge&amp;theory&amp;of&amp;states&amp;of&amp;matter&amp; /&amp;old&amp;and&amp;new&amp;

Gauge&amp;theory&amp;of&amp;states&amp;of&amp;matter&amp; /&amp;old&amp;and&amp;new&amp;

Gauge&amp;theory&amp;of&amp;states&amp;of&amp;matter&amp; /&amp;old&amp;and&amp;new&amp; Jrg%Frhlich% Em.,%ETH%Zurich% Vienna,%Sept.%2014% Dedicated%to%the%memory%of% Edward&amp;Nelson % Credits(

848 views • 20 slides
Discrete Gauge Symmetry and Aharonov-Bohm Radiation in String Theory Yutaka Ookouchi (Kyushu U.)

Discrete Gauge Symmetry and Aharonov-Bohm Radiation in String Theory Yutaka Ookouchi (Kyushu U.)

Discrete Gauge Symmetry and Aharonov-Bohm Radiation in String Theory Yutaka Ookouchi (Kyushu U.) 1310.4026 [hep-th], Published in JHEP String theory Aharonov-Bohm effect Discrete Gauge Theory Discrete gauge sym. is ubiquitous Consider

553 views • 22 slides
On gauge theory phase diagrams at zero and finite temperature K. Tuominen University of

On gauge theory phase diagrams at zero and finite temperature K. Tuominen University of

On gauge theory phase diagrams at zero and finite temperature K. Tuominen University of Jyvskyl &amp; Helsinki Institute of Physics SCGT 2012, Nagoya. Outline: SU( N c ) gauge + fund rep. matter x f x f N f H L N c 7 6 1.

794 views • 58 slides
Vacuum decay rate in the standard model and beyond Yutaro Shoji (KMI, Nagoya U.) Phys. Lett.

Vacuum decay rate in the standard model and beyond Yutaro Shoji (KMI, Nagoya U.) Phys. Lett.

The 24th regular meeting of the NHWG, Dec 21-22 2018 Vacuum decay rate in the standard model and beyond Yutaro Shoji (KMI, Nagoya U.) Phys. Lett. B771(2017)281; M. Endo, T. Moroi, M. M. Nojiri, YS JHEP11(2017)074; M. Endo, T. Moroi, M. M.

906 views • 31 slides
Curvature perturbation spectrum from false vacuum inflation Jinn-Ouk Gong University of

Curvature perturbation spectrum from false vacuum inflation Jinn-Ouk Gong University of

Curvature perturbation spectrum from false vacuum inflation Jinn-Ouk Gong University of Wisconsin-Madison 1150 University Avenue, Madison WI 53706-1390 USA Cosmo 08 University of Wisconsin-Madison, USA 26th August, 2008 Based on JG and M.

497 views • 22 slides
Supergravity Gravity: on-shell Einstein gravity gauge theory of local Lorentz/translation

Supergravity Gravity: on-shell Einstein gravity gauge theory of local Lorentz/translation

Supergravity Gravity: on-shell Einstein gravity gauge theory of local Lorentz/translation symmetry generators M ab , P a gauge fields ab , spin connection, e a vierbein where a, b = 0 , . . . , 3 are Lorentz gauge group

408 views • 39 slides
Rethinking Gauge Theory through Connes Noncommutative Geometry Chen Sun Virginia Tech

Rethinking Gauge Theory through Connes Noncommutative Geometry Chen Sun Virginia Tech

Rethinking Gauge Theory through Connes Noncommutative Geometry Chen Sun Virginia Tech October 24, 2015 Chen Sun @ Duke Gauge Theory through NCG October 24, 2015 1 / 44 Work with Ufuk Aydemir, Djordje Minic, Tatsu Takeuchi: Phys. Rev. D

1.27k views • 108 slides
Abstract and Outline We are investigating the dynamics of a new Poincar e gauge theory of

Abstract and Outline We are investigating the dynamics of a new Poincar e gauge theory of

Poincar e Gauge Theory with Coupled Even and Odd Parity Dynamic Spin- 0 Modes: Dynamical Isotropic Bianchi Cosmologies Fei-hung Ho Department of Physics, National Cheng Kung University, Tainan Taiwan Work with James M. Nester 2012-03-01 @YITP

612 views • 29 slides
Getting Something Out of Nothing: Implications of a Future Information Theory Based on Vacuum

Getting Something Out of Nothing: Implications of a Future Information Theory Based on Vacuum

Getting Something Out of Nothing: Implications of a Future Information Theory Based on Vacuum Microtopology International Association of Nanotechnology Conference San Fransisco, CA November 2, 2005 William Michael Kallfelz Committee for

404 views • 25 slides
Seiberg-Witten Theory and AGT Relation Tohru Eguchi We consider N = 2 supersymmetric gauge

Seiberg-Witten Theory and AGT Relation Tohru Eguchi We consider N = 2 supersymmetric gauge

Seiberg-Witten Theory and AGT Relation Tohru Eguchi We consider N = 2 supersymmetric gauge theories in 4- dimensions and study the case when the theory possesses the conformal invariance. Simplest example of a conformal invariant theory:

904 views • 38 slides
Large-Nc gauge theory and Chiral Random matrix theory Masanori Hanada Hana Da Masa Nori (KEK

Large-Nc gauge theory and Chiral Random matrix theory Masanori Hanada Hana Da Masa Nori (KEK

Large-Nc gauge theory and Chiral Random matrix theory Masanori Hanada Hana Da Masa Nori (KEK Theory Center YITP , Kyoto U.) April 2013 M.H., J.-W. Lee and N. Yamada, 1212.****[hep-lat] 7 Dec 2012 @Nagoya U. SU( ),

510 views • 16 slides
Gauge invariant regularization for perturbative chiral gauge theory Yu Hamada Kyoto Univ.

Gauge invariant regularization for perturbative chiral gauge theory Yu Hamada Kyoto Univ.

Gauge invariant regularization for perturbative chiral gauge theory Yu Hamada Kyoto Univ. 2018/7/30 @Strings and Fields 2018 Based on YH, H. Kawai, arXiv:1705.01317, YH, H. Kawai, K. Sakai, arXiv:1806.00349 YH, H. Kawai, K. Sakai, to appear

465 views • 22 slides
Gravity in three dimensions as a noncommutative gauge theory George Manolakos ESI workshop MM

Gravity in three dimensions as a noncommutative gauge theory George Manolakos ESI workshop MM

Gravity in three dimensions as a noncommutative gauge theory George Manolakos ESI workshop MM for NCG and string theory July 10, 2018 Joint work with: A. Chatzistavrakidis, L. Jonke, D. Jurman, P. Manousselis, G. Zoupanos NTUA

229 views • 20 slides

More recommend