The Strained State Cosmology Angelo Tartaglia Politecnico di

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The Strained State Cosmology Angelo Tartaglia Politecnico di Torino and INFN

The Strained State Cosmology Angelo Tartaglia Politecnico di Torino and INFN

“Elastic” continua N+n N ξa r xμ Xa April 19 2011 r’ PONT-2011 Avignon

“Elastic” continua N+n N ξa r xμ Xa April 19 2011 r’ PONT-2011 Avignon N 2

Space-time defect Flat reference frame Curved natural frame April 19 2011 PONT-2011 Avignon 3

Space-time defect Flat reference frame Curved natural frame April 19 2011 PONT-2011 Avignon 3

Strained space-time dr 0 unstrained Strain tensor g dr strained April 19 2011 PONT-2011

Strained space-time dr 0 unstrained Strain tensor g dr strained April 19 2011 PONT-2011 Avignon 4

Physical relevance of the strain • In a continuum, strain is associated with stress

Physical relevance of the strain • In a continuum, strain is associated with stress • Strain and stress correspond to a deformation energy • Defects can fix the global symmetry • Strain is originated by the presence of matter/energy or by defects April 19 2011 PONT-2011 Avignon 5

Isotropic medium Lamé coefficients Elastic energy April 19 2011 PONT-2011 Avignon 6

Isotropic medium Lamé coefficients Elastic energy April 19 2011 PONT-2011 Avignon 6

The Lagrangian density Potential term “Kinetic” term Geometry April 19 2011 PONT-2011 Avignon 7

The Lagrangian density Potential term “Kinetic” term Geometry April 19 2011 PONT-2011 Avignon 7

Robertson-Walker symmetry l r z r l =f(r) April 19 2011 PONT-2011 Avignon 8

Robertson-Walker symmetry l r z r l =f(r) April 19 2011 PONT-2011 Avignon 8

The Hubble parameter A. Tartaglia and N. Radicella, CQG, 27, 035001 (2010) September 6,

The Hubble parameter A. Tartaglia and N. Radicella, CQG, 27, 035001 (2010) September 6, 2010 ERE 2010 - Granada 9

Fitting the data (307 Sn. Ia) April 19 2011 PONT-2011 Avignon 10 10

Fitting the data (307 Sn. Ia) April 19 2011 PONT-2011 Avignon 10 10

Other cosmological tests • Primordial nucleosynthesis (correct proportion between He, D and hydrogen) •

Other cosmological tests • Primordial nucleosynthesis (correct proportion between He, D and hydrogen) • CMB spectrum • Structure formation after the recombination era. September 6, 2010 ERE 2010 - Granada 11

Bayesian posterior probability April 19 2011 PONT-2011 Avignon 12

Bayesian posterior probability April 19 2011 PONT-2011 Avignon 12

Optimal value of the parameters N. Radicella, M. Sereno, A. Tartaglia, IJMPD, 20, n.

Optimal value of the parameters N. Radicella, M. Sereno, A. Tartaglia, IJMPD, 20, n. 3 (2011) April 19 2011 PONT-2011 Avignon 13

Schwarzschild symmetry Natural frame Reference frame (Minkowski) Gauge function April 19 2011 PONT-2011 Avignon

Schwarzschild symmetry Natural frame Reference frame (Minkowski) Gauge function April 19 2011 PONT-2011 Avignon 14

The strain tensor 15

The strain tensor 15

Weak strain April 19 2011 PONT-2011 Avignon 16

Weak strain April 19 2011 PONT-2011 Avignon 16

Approximate solutions , = functions of , ~ , April 19 2011 PONT-2011 Avignon

Approximate solutions , = functions of , ~ , April 19 2011 PONT-2011 Avignon 17

Post-Keplerian circular orbits Looks like the effect of dark matter Light rays April 19

Post-Keplerian circular orbits Looks like the effect of dark matter Light rays April 19 2011 PONT-2011 Avignon 18

Conclusion • The strained space-time theory introduces a strain energy of vacuum depending on

Conclusion • The strained space-time theory introduces a strain energy of vacuum depending on curvature • The theory accounts for the accelerated expansion of the universe and is consistent with BBN, structure formation and Sn. Ia’s • The strain affects free fall also in spherically symmetric stationary spacetimes April 19 2011 PONT-2011 Avignon 19

References • • A. Tartaglia and N. Radicella, CQG, 27, 035001 (2010) N. Radicella,

References • • A. Tartaglia and N. Radicella, CQG, 27, 035001 (2010) N. Radicella, M. Sereno, A. Tartaglia, IJMPD, 20, n. 3 (in press) 2011