Interactive Graphics Lecture 18: Slide 3. Computer Aids to Animation. Fully
automatic animation has not proved successful. However computer tools to
support ...
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... Teknik sipil: studi struktur, simulasi (banyak metode numerik).
Natural Computing 20/09/2011 J. M. Herrmann .... G. Rozenberg, T. Bäck, J. N.
Kok (Editors) Handbook of Natural. Computing Springer Verlag, 2010.
Feb 6, 2013 ... Embryology of female lower genital tract. Embryology ... Netter's Atlas of Human
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Semua contoh slide dalam buku ini memiliki hak cipta dan dirancang ....
Menggunakan PowerPoint, pilih outline mode dan tuliskan dalam kalimat
lengkap inti.
Strategy designed by Doug Cooper. – Professor at Berkeley who wrote "Oh
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1-6. Preface. Iron-Carbon Alloys I. Elemental Iron. The Fe-FeBC Alloy System. Fe
-Fe3C Phase Diagram / Solid Phases in the Fe-FeHC Phase. Diagram ...
Setelah mengikuti kuliah, peserta dapat membedakan antara baris dan deret,
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1077. 10. J. ailantifolia. 0. 1200 J. cinerea. 1000. 800. 600. 400. 2000 2 1. 0. A. 3. 1. 10. 4. 26. 2. N. 0 ooo 1 0 o. 0.75. 0.8. 0.85. 0.9. 0.95 0.97 0.99 >0.99 u. 11.
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Altri testi consigliati: G. Pighizzini, M. Ferrari, Dai fondamenti agli oggetti Addison
Wesley, 2005. • Introduzione a Java (dispensa) (www.dimi.uniud.it/demis).
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Equatorial Guinea:
Aug 20, 2013 ... 2nd slow-roll condition ... Universe enters 2nd Slow-Roll Regime. → Settles
down to ... Universe leaves MPS before T.P. grows sufficiently.
Review on EiBI Inflation: Discussion on Tensor Perturbation Inyong Cho
(Seoul National University of Science & Technology)
The CMB and theories of the primordial universe Yukawa Institute for Theoretical Physics, Aug. 20, 2013 - Phys. Rev. Lett. 111, 071301 (2013) I.C., Hyeong-Chan Kim (KNUT) & Taeyoon Moon (Inje Univ.)
Outline 1. Introduction to EiBI Gravity 2. Chaotic Inflation in GR
3. Scalar Field in EiBI Gravity 4. MPS (Maximal Pressure Solution)
5. Inflation in EiBI gravity 6. Conclusions
7. Discussion on Tensor Perturbation
Eddington-inspired Born-Infeld Gravity Formalism Einstein Gravity
Field:
Palatini
GR
Eddington Gravity (1924)
Field:
Varying S, Integrating by parts, Eliminating a vanishing trace, we get
Therefore, Eddington’s action :- viable and alternative starting point to GR ::- dual to GR However, incomplete : NOT including MATTER Later attempts to couple matter with :- start with Palatini gravitational action coupled to matter -- no derivatives in g :- EOM for g
back into
can eliminate g :-
: complicated, but Dynamics is fully equivalent to the original metric theory
Eddington-inspired Born-Infeld Gravity
(MERIT 1) One parameter (k) theory
(Vollick 2004, Banados-Ferreira 2010) :-
: independent
:- Matter is in usual way (Not in sqrt) :- For large
:- For small
-limit Eddington limit
-limit Einstein limit
Field Equations
EOM1:
: Relation b/t g and q via T
EOM2:
:- Auxiliary Metric :- Dynamical Equation : Connection is defined by q
: EOM for matter : Energy-Momentum Conservation Matter plays in the background metric
Some Immediacies (Banados-Ferreira 2010) Equivalence to GR in Vacuum
: EOM1
EOM2: (MERIT 2) EiBI in vacuum or with only CC is the same with EH
Black Hole Solutions Schwartzchild-de Sitter BH SAME with Einstein Solution
Charged BH : non-vacuum
: electric field
Poisson Equation Nonrelativistic Limit w/ the lowest-order correction
Metric : with
and : Poisson Equation Implies repulsive nature of EiBI gravity
Nonsingular Universe driven by Perfect Fluid
Metric & Auxiliary Metric
Matter-Stress Tensor
: same with GR
Banados & Ferreira for w=1/3 (2010) IC, Kim and Moon for all w (2012)
EOM 1
we get
: relation b/w q and g via matter field
EOM 2 Friedmann Equations Volume Part :
1) w>0
Banados & Ferreira for w=1/3 (2010) IC, Kim and Moon for all w (2012)
Bouncing Universe
Non-Singular Universe
: Maximal Pressure/Density Limit
Early Times
At a=
, H=0 :
Expand near a=
:
Then we have
:- t -infty : origin of Universe :- finite size :- Non-Singular Universe
Chaotic Inflation in GR Action & Metric
Field Equations & Slow-Roll Conditions : 1st slow-roll condition : 2nd slow-roll condition Chaotic :- large fluctuation
Inflation :- slow roll
Inflaton decay :- reheating
Attractor Solution for Slow-Roll Inflation
Quantum Gravity Regime
The curvature scale is determined mainly by H
When H > Mp , Gravity Part requires quantum treatment :- In GR, large curvature is inevitable
:- In EiBI gravity, curvature scale is NOT directly related with energy scale maybe Quantum Gravity is avoidable in describing the high-energy state of the scalar field
Scalar Field in EiBI Gravity
EOM1:
: Relation b/t g and q via T
EOM2:
:- Auxiliary Metric :- Dynamical Equation : Connection is defined by q
: EOM for matter : Energy-Momentum Conservation Matter plays in the background metric
Field Equations
Puts an upper limit on pressure
H in Phase Space
for
Contour gradient :
forbidden
H=0
H=1 Quantum Gravity Regime
forbidden
Slow-Roll Evolution : Same both for GR and EiBI
1st Slow-Roll Condition : same as in GR
integrated
2nd Slow-Roll Condition
: usual chaotic inflation attractor
Backward in Time
Only 1st Slow-Roll Cond’s Satisfied jumps rapidly