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Finsler Geometry vs. Dark Matter and Dark Energy Hyp othesis CHANG Zhe Institute of High Energy Physics Chinese Academy of Sciences 17/11/2009 at ITP

I. Experimental observations

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Finsler Geometry vs. Dark Matter and Dark Energy Hypothesis CHANG Zhe Institute of High Energy Physics Chinese Academy of Sciences 17/11/2009 at ITP. I. Experimental observations. 1. Galactic rotation curves 2. Velocity dispersions of galaxies 3. Missing matter in clusters of galaxies - PowerPoint PPT Presentation

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Page 1: I. Experimental observations

Finsler Geometry vs.

Dark Matter and Dark Energy Hypothesis

CHANG ZheInstitute of High Energy Physics

Chinese Academy of Sciences

17/11/2009 at ITP

Page 2: I. Experimental observations

I. Experimental observations

1. Galactic rotation curves

2. Velocity dispersions of galaxies

3. Missing matter in clusters of galaxies

4. Large scale structure formation

5. Accelerated expanding Universe

Page 3: I. Experimental observations

6. Pioneer anomaly

7. Anomalous increase of the Astronomical Unit

8. Anomalous orbital-energy changes during spacecraft flyby of earth

9 ……

Page 4: I. Experimental observations

1. Galactic rotation curves

In the late 1960s and early 1970s

V. Rubin

from Carnegie Institution of Washington

presented that most stars in spiral galaxies orbit at

roughly the same speed.

Page 5: I. Experimental observations

Rotation curve of a typical spiral galaxy: predicted (A) and observed (B).

Page 6: I. Experimental observations

2. Velocity dispersions of galaxies

Rubin's pioneering work has stood the test of time.

Measurements of velocity curves in spiral galaxies were soon followed up with velocity dispersions of elliptical galaxies. While sometimes appearing with lower mass-to-light ratios, measurements of ellipticals still indicate a relatively high dark matter content.

Page 7: I. Experimental observations

3. Missing matter in clusters of galaxies

X-ray measurements of hot intracluster gas correspond closely to Zwicky's observations of mass-to-light ratios for large clusters of nearly 10 to 1. Many of the experiments of the Chandra X-ray Observatory use this technique to independently determine the mass of clusters.

Page 9: I. Experimental observations

4. Large scale structure formationObservations suggest that structure formation i

n the universe proceeds hierarchically, with the smallest structures collapsing first and followed by galaxies and then clusters of galaxies. As the structures collapse in the evolving universe, they begin to "light up" as the baryonic matter heats up through gravitational contraction and the object approaches hydrostatic pressure balance.

Page 11: I. Experimental observations

Pioneer 10 (also called Pioneer F) was the first spacecraft to travel through the asteroid belt, which it entered on July 15, 1972, and to make direct observations of Jupiter, which it passed by on December 3, 1973. It was launched from Cape Canaveral Air Force Station's Launch Complex 36A on March 3, 1972 at 01:49:00 UTC. Pioneer 10 is heading in the direction of Aldebaran, located in Taurus. By some definitions, Pioneer 10 has become the first artificial object to leave the solar system. It is the first human-built object to have been set upon a trajectory leading out of the solar system.

Page 12: I. Experimental observations

– The Pioneer anomaly is the observed deviation from pre

dicted trajectories and velocities of various

unmanned spacecraft visiting the outer solar system, mos

t notably Pioneer 10 and Pioneer 11.

– Both Pioneer spacecraft are escaping from the solar sys

tem, and are slowing down under the influence of the S

un's gravity. Upon very close examination, however, the

y are slowing down slightly more than expected.

Page 13: I. Experimental observations

6. Anomalous increase of the Astronomical unit

Transits of Venus across the face of the Sun were for long the best method of measuring the astronomical unit

Page 14: I. Experimental observations

The latest planetary ephemerides gave the accurate value of AU

Reports from Krasingky and Brumberg Celest. Mech. Dyn. Astrn. 90, 267 (2004).

Standish Proc. IAU Colloq. 196, 163 (2005)

Page 15: I. Experimental observations

7. Accelerated expanding Universe

• Cosmology is the scientific study of the large scale properties of the Universe as a whole.

• It endeavors to use the scientific method to understand the origin, evolution and ultimate fate of the entire Universe.

• Cosmology involves the formation of theories or hypotheses about the universe which make specific predictions for phenomena that can be tested with observations.

• Depending on the outcome of the observations, the theories will need to be abandoned, revised or extended to accommodate the data.

Page 16: I. Experimental observations

Ricci tensor

By making use of the energy-momentum tensor, the Einstein equation reads Time-time component:Space-space components:

The space-time components give 0=0Friedmann equation

Page 17: I. Experimental observations
Page 18: I. Experimental observations
Page 19: I. Experimental observations

II.Finsler geometryIn 1854 Riemann saw the difference between the q

uadratic differential form--Riemannian geometry and the general case.

The study of the metric which is the Fourth root of a quartic differential form is quite time--consuming and does not throw new light to the problem." Happily, interest in the general case was revived in 1918 by Paul Finsler's thesis, written under the direction of Caratheodory.

Page 20: I. Experimental observations

Mathematical ProblemsLecture delivered before the International

Congress of Mathematicians at Paris in 1900

By Professor David Hilbert

• 4. Problem of the straight line as the shortest distance between two points• 23. Further development of the methods of the calculus of variations

Page 21: I. Experimental observations

1926, L. Berwald: Berwald connection Torsion f

ree: yes g-compatibility: no

1934, E. Cartan: Cartan connection

Torsion free: no g-compatibility: yes

1948, S. S. Chern: Chern connection

Torsion free: yes g-compatibility: no

Chern connection differs from that of Berwald's

by an À term

Page 22: I. Experimental observations

Finsler structure of M.

with the following properties:(i) Regularity: F is C on the entire slit tangent bundle TM\ 0(ii) Positive homogeneity : F(x, y)= F(x,y), for all >0(iii) Strong convexity: the Hessian matrix

Is positive-definite at every point of TM\0

Page 23: I. Experimental observations

The symmetric Cartan tensor

Cartan tensor Aijk=0 if and only if gij has no y-de

pendence

A measurement of deviation from Riemannian M

anifold

Page 24: I. Experimental observations

Euler's theorem on homogenous function gives

Where li=yi/F

Page 25: I. Experimental observations

1. Chern connection

transform like

The nonlinear connection Nij on TM\0

where ijk is the formal Christoffel symbols of the second kind

Page 26: I. Experimental observations

Chern Theorem guarantees the uniqueness of Chern connection.

S. S. Chern, Sci. Rep. Nat. Tsing Hua Univ. Ser. A 5, 95 (1948); or Selected Papers, vol. II, 194, Springer 1989.

Torsion freeness

Almost g-compatibility

Page 27: I. Experimental observations

Torsion freeness is equivalent to the absence of dyi terms in i

j

together with the symmetry

Almost g-compatibility implies that

where

Page 28: I. Experimental observations

2.CurvatureThe curvature 2-forms of Chern connection are

The expressionof ijin terms of the natural basis

is of the form

where R, P and Q are the hh-, hv-, vv-curvature tensors of the Chern connection, respectively.

Page 29: I. Experimental observations

III.Gravity and large scale structure

The tangent spaces (TxM, Fx) of an arbitrary Finsler manifolds typically not isometric to each other.

Given a Berwald space, all its tangent spaces are linearly isometric to a common Minkowski space

A Finsler structure F is said to be of Berwald type if the Chern connection coefficients i

jk in natural coordinates have no y dependence. A direct proposition on Berwald space is that hv--part of the Chern curvature vanishes identically

Page 30: I. Experimental observations

X. Li and Z. Chang, Toward a Gravitation Theory in Berwald--Finsler Space ,gr-qc/0711.1934.

Gravitational field equation on Berwald space

Page 31: I. Experimental observations

Z. Chang and X. Li, Modified Newton’s gravity in Finsler space as a possible alternative to dark matter hypothesis, Phys. Lett. B668, 453(2008).

To get a modified Newton's gravity, we consider a particle moving slowl

y in a week stationary gravitational field. Suppose that the metric is close

to the locally Minkowskian metric

A modified Newton's gravity is obtained as the weak field

approximation of the Einstein's equation

Page 32: I. Experimental observations

Limit the metric to be the form

a0is the deformation parameter of Finsler geometry

The deformation of Finsler space should have cosmological significance.

One wishes naturally the deformation parameter relates with the cosmological constant ,

Page 33: I. Experimental observations

The geometrical factor of the density of baryons

In the zero limit of the deformation parameter, familiar results on Riemann geometry are recovered

The acceleration a of a particle in spiral galaxiesis

Page 34: I. Experimental observations

M. Milgrom, Astrophys. J. 270, 365 (1983).

G. Gentile, MOND and the universal rotation curve: similar phenomenologies, astro-ph/0805.1731

The MOND

M. Milgrom, The MOND paradigm, astro-ph/0801.3133.

Universal Rotation Curves

Page 35: I. Experimental observations

IV.Possible model of accelerated expanding Universe

Z. Chang and X. Li,

Robertson-Walker metric satisfies the requirements of

homogeneity, isotropy and closure

Modified Friedmann model in Randers-Finsler space of approximate Berwald type as a possible alternative to dark energy hypothesis, Phys. Lett. B676 (2009) 173,arXiv 0901.1023

Page 36: I. Experimental observations

• Ricci tensor

By making use of the energy-momentum tensor, the Einstein equation reads Time-time component:Space-space components:

The space-time components give 0=0Friedmann equation

Page 37: I. Experimental observations

The Randers-Finsler metric

The Friedmann equation

Let to be the Robertson-Walker type

Page 38: I. Experimental observations

Omitting the O(b2) term and combining with the the space-space component of the field equations, we obtain

One can see clearly that the accelerated expanding universe is guaranteed by the constraint

Page 39: I. Experimental observations

So that the complete constraint on Randers-Finsler structure to support accelerated expanding universe is

It means that a negative provides an effective repulsive force in the course of universe expanding.

Page 40: I. Experimental observations

V. Conlusions

A possible unified scenario for large structure

• Secular increase of astronomical unit• Pioneer anomaly• Galactic rotation curves• Missing matter in clusters of galaxies• Large scale structure formation• Accelerated expanding Universe

Finsler geometry may really supply a framework of astronomy and cosmology without invoking dark

matter and dark energy hypothesis.

Page 41: I. Experimental observations

Thanks for your attention!