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Has elasticity anything to do with cosmology?. Angelo Tartaglia RELGRAV. r. r’. X a. “Elastic” continua. N+n. N. ξ a. x μ. N. Geometry and elasticity. In a strained medium each point is in one to one correspondence with points in the unstrained state.
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Has elasticity anything to do with cosmology? Angelo Tartaglia RELGRAV
r r’ Xa “Elastic” continua N+n N ξa xμ N RELGRAV
Geometry and elasticity In a strained medium each point is in one to one correspondence with points in the unstrained state u, r and r’ are (N+n)-vectors in the flat embedding space RELGRAV
The strain is described by the differential change of u RELGRAV
Metricity RELGRAV
What about space-time? Space-time/Matter-energy What is this? RELGRAV
What is space-time? • Is it a mathematical artifact to describe the gravitational field and the global properties of the universe? • Is it something real endowed with physical properties? RELGRAV
A four-dimensional manifold Minkowski (flat) space-time General (curved) space-time RELGRAV
Defects in continua Flat reference frame Curved natural frame RELGRAV
What consequences from a defect? • The defect fixes the global symmetry • A spontaneous strain tensor εμν(or displacement vector field ua) appears • All this must show up in the Lagrangian of the strained manifold (space-time) RELGRAV
Strained space-time unstrained dr0 Strain tensor g dr strained RELGRAV
Hooke’s law The “elastic” approach Stress tensor Elastic modulus tensor RELGRAV
Isotropic medium Lamé coefficients Elastic energy RELGRAV
The Lagrangian density Potential term “Kinetic”term Geometry RELGRAV
l r z l r Robertson-Walker symmetry =f(r) RELGRAV
Has the universe a R-W symmetry? RELGRAV
The Hubble parameter from the Einstein equations A. Tartaglia and N. Radicella, CQG, 27, 035001 (2010) RELGRAV
The distance modulus of bright objects Observed magnitude Absolute magnitude Hubble parameter Distances in Mpc RELGRAV
Fitting the data (307 SnIa) RELGRAV 19
Other cosmological tests • Primordial nucleosynthesis (correct proportion between He, D and hydrogen) • CMB acoustic horizon • Structure formation after the recombination era. RELGRAV
Nucleosynthesis In the early stages the universe is radiation-dominated XBoost
Large Scale Stractures Particle horizon at the equality epoch (z=3150) Constraint from LSS: Ωm0 : matter density in units of h: Hubble constant in units of km/(sMpc)
Acoustic scale of the CMB The power spectrum of the CMB depends on the expansion rate of the universe zls 1090 last scattering DA:angular diameter distance rs:sound horizon
Bayesian posterior probability RELGRAV
Optimal value of the parameters N. Radicella, M. Sereno, A. Tartaglia RELGRAV
Schwarzschild symmetry Natural frame Reference frame (Minkowski) Gauge function RELGRAV
The strain tensor RELGRAV
Three field equations RELGRAV
Weak strain RELGRAV
Approximate solutions , = functions of , ~ , RELGRAV
Post-Keplerian circular orbits Looks like the effect of dark matter Light rays RELGRAV
Conclusion • The strained space-time theory introduces a strain energy of vacuum depending on curvature • The idea of a cosmic defect explains why the symmetry of the universe should be R-W (or anything else) • The theory accounts for the accelerated expansion of the universe and is consistent with BBN, structure formation, acoustic scale of the CMB and SnIa’s luminosity RELGRAV