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Complexity in cosmic structures. Francesco Sylos Labini . Enrico Fermi Center & Institute for Complex Systems (ISC-CNR) Rome Italy . A.Gabrielli, FSL, M. Joyce, L. Pietronero Statistical physics for cosmic structures Springer Verlag 2005. Early times density fields . COBE DMR, 1992. - PowerPoint PPT Presentation
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Complexity in cosmic structures
Francesco Sylos Labini
Enrico Fermi Center &
Institute for Complex Systems (ISC-CNR)
Rome Italy
A.Gabrielli, FSL, M. Joyce, L. Pietronero Statistical physics for cosmic structures
Springer Verlag 2005
Early times density fields
WMAP satellite 2006
COBE DMR, 1992
150 Mpc/h(1990)
300 Mpc/h(2006)
5 Mpc/h
Late times density fields
The problem of cosmological structure formation
Initial conditions: Uniform distribution (small amplitude fluctuations)
Final conditions: Stronlgy clustered,
power-law correlations
Dynamics: infinite self-gravitating system
Cosmological energy budget: the “standard model”
Non baryonic dark matter (e.g. CDM): -never detected on Earth-needed to make structures compatible with
anisotropies Dark Energy-never detected on Earth-needed to explain SN data
What do we know about dark matter ?Fundamental and observational constraints
Substantially Poisson (finite correlation length)
Super-Poisson (infinite correlation length)
Sub-Poisson (ordered or super-homogeneous)
Classification of uniform structures
€
<ΔM(r)2 > <∝ M(r) >
< M(r) >∝ r3
€
<ΔM(r)2 > <∝ M(r) >β 1 < β < 2
Extremely fine-tuned distributions
€
<ΔM(r)2 > <∝ M(r) >β
2/3 < β <1 < ΔM(r)2 >∝ r2
Gas
Critical system
€
σφ2(r) ≈ const.
HZ tail
CMBR: results
Angular correlation function vanishes at > 60 deg (COBE/WMAP teamsand Schwartz et al. 2004)
Small quadrupole/octupole (COBE/WMAP teams)
€
<ΔM 2(r) >≈ r2 ⇒ C(l) ≈ l(l +1)[ ]−1
Super-homogeneous
Poisson-like
Critical
€
< n >=< n(r) >p= const
Statistically isotropic and homogeneous
Fractals: isotropic but not homogeneous
€
< n(r) >p ≈ r−γ
< n >= 0
Extendend Classification of homogeneous structures
Conditional correlation properties
€
N(r)P
= N i(r) = BrDi=1
M
∑ 0 < D ≤ 3
€
n(r)P
=N(r)
p
V (r)= 3B
4πrD−3
Galaxy correlations: results
Sylos Labini, F., Montuori M. & Pietronero L. Phys Rep, 293, 66 (1998)Hogg et al. (SDSS Collaboration). ApJ, 624, 54 (2005)
Discrete gravitational N body problem
From order to complex structures:A Toy model
GravitationalDynamics
generates
Complex Structures
Power law correlationsNon Gaussian velocity distributionsProbability distributions with “fat tails”(In)dipendence on IC and universal properties….
Structure formation: the cosmological problem
Summary
HZ tail: the only distinctive feature of FRW-IC in matter distribution is the behavior of the large scales tail of the real space correlation function Note yet observed in galaxy distributions Problem with large angle CMBR anisotropies
Homogeneity scale: not yet identified in galaxy distributions
Structures in N-Body simulations: too small and maybe different in nature from galaxy structures
Basic propeerties of SGS