ccm08-bazeia.ppt [modo de compatibilidade]ccm08/abstract/bazeia.pdf · 2008. 4. 7. · microsoft...
TRANSCRIPT
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CCM08, Dresden, 5CCM08, Dresden, 5--8.03.20088.03.2008
SCALARSCALAR--FIELD MODELS:FIELD MODELS:BIFURCATION DEFORMATION ANDBIFURCATION DEFORMATION ANDBIFURCATION, DEFORMATION ANDBIFURCATION, DEFORMATION AND
NETWORK OF TOPOLOGICAL DEFECTSNETWORK OF TOPOLOGICAL DEFECTS
Dionísio BazeiaDionísio BazeiaDepartamento de FísicaDepartamento de FísicaDepartamento de FísicaDepartamento de Física
Universidade Federal da ParaíbaUniversidade Federal da Paraíba
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Outlook:
1 1 & 2 scalar fields1. 1 & 2 scalar fields
2. Bifurcation
3. Deformation
4. Network of defects
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1: Single fieldR l ti i ti t 1+1 di iRelativistic systems, 1+1 dimensions
non-negative
kinetic … gradient … potential
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1: Single field
non-negative
kinetic … gradient … potential
Bogomol’nyi bound:
Energy minimized to:
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1: Single fieldsolutionpotential
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1: Single fieldsolutionpotential
It may be used to describe this:
or this:or this:
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1: Single fieldsolutionpotential
Applications:Applications:Magnetic systems…Pattern formation…AlAlso:Cosmology: DB,Gomes, Losano, RMenezes PLB(2006)Braneworld: Afonso, DB, Losano PLB (2006)Brane/cosmology: DB, Brito, Costa PLB(2008)
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1: Two or more fields
non-negativenon-negative
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1: Two or more fields
non-negative
Door to DS
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1: Two or more fields
Good way to describe junctions
Fi t d f kFirst-order framework:Abraham, Townsend NPB(1991)DB, JMenezes, Santos PLB(2001); NPB(2002)
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1: Two or more fieldsGood way to describe junctions
roots of unit
nice discretesymmetry appearssymmetry appearsvery naturally…
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1: Two or more fieldsGood way to describe junctions
3 4
Gibbons, Townsend, PRL99DB, Brito, PRL2000
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2: Bifurcationinteraction
Elphick, Hagberg, Meron, PRL (1998)h f i bili i GL d lphase front instability in a GL model
W id th
DB, Brito, Losano, EPL, 2006 …but it breaks first-order structure
We consider the case
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2: Bifurcationgreen
εεIllustration:
redyellow
orange
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3: Deformation
DB, Losano, Malbouisson, PRD(R), 2002Theorem:
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3: Deformation p odd integerp g
kink2-kink,p=3
DB, JMenezes,RMenezes, PRL(2003)
Direction: 3-kink, 4-kink,…, to build a stair… In preparation Another direction: deformation with 2 fields PRD 2007;Another direction: deformation with 2 fields, PRD, 2007;Network of defects, PLB(2008)
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3: Deformation
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4: Network
One field, in the line…
Consider the model:
and the deformation:
Then, we get:Sine-GordonSine Gordon
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4: Network Complex field, in the plane
The Z3 case:Afonso, DB,GonzalezLeon,Losano,MateosGuilarte,PRD(2007); PLB(2008)
freedom to choosefreedom to choosedeformation function
0 1
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4: Network
The Z3 case:
0 1
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4: NetworkThe deformed potential is:
It is depicted as:
Hexagonal structure- U
Hexagonal structureof minima around singularity
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4: Network
Thus:
We had to addWe had to addsingularities:
But niceorbits and network:
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4: Network
ZZ3: Weierstrass Z4: elliptic Jacobi
Z4 is similar:
singularities
and orbits…
We can also make asymmetric patterns: in preparation…
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Th k tTh k tThanks to:Thanks to:
# The organizers
# Collaborators & Students, Brazil
# Juan Mateos Guilarte# Jua ateos Gu a teMiguel Angel Gonzalez Leon, Salamanca U
Sponsored by:
# CAPES# CNPq# PRONEX CNP /FAPESQ# PRONEX-CNPq/FAPESQ