Presentation is loading. Please wait.

Presentation is loading. Please wait.

Ariel Caticha From Information Geometry to Newtonian Dynamics

Similar presentations


Presentation on theme: "Ariel Caticha From Information Geometry to Newtonian Dynamics"— Presentation transcript:

1 Ariel Caticha From Information Geometry to Newtonian Dynamics
July 8, 2007 (62)

2 E. T. Jaynes “Information Theory and Statistical Mechanics” Physical Review, 1957

3 From Information Geometry to Newtonian Dynamics
Ariel Caticha and Carlo Cafaro Department of Physics University at Albany - SUNY MaxEnt 2007

4 The laws of Physics are not laws of Nature;
they are rules for processing information about nature. Outrageous!! But the evidence accumulates... Statistical Mechanics Quantum Mechanics This is where we specify the interpretation. Geometry Our objective: Classical Mechanics

5 Objective: To derive from principles of inference. Challenge: To codify the relevant prior information into an appropriate statistical model. To derive the dynamics without appealing to additional postulates from physics.

6 Configuration Space: a single particle
The particle lives in a 3-dimensional space. Positions are uncertain: space is fuzzy. (Small uncertainties.)

7 To each “point” we associate a probability distribution.
A “point” is not just a dot. These “points” have structure. Configuration Space is a statistical manifold. The degree to which a point can be distinguished from a neighbor is a measure of distance. The induced “information” geometry is unique.

8 Information geometry:

9 To each “point” we associate a probability distribution:
Given we can find , and vice versa! In fact, caution!! Information distance is measured in units of the local uncertainty

10 Entropic Dynamics: ?? The entropic dynamics trajectory is a geodesic.

11 The trajectory minimizes the length
We are done, but ... does it look like classical mechanics? Yes ... it is identical to Jacobi’s action principle: where

12 The parameter is quite arbitrary.
Define time t so that motion looks simple, then, and Quite impressive, but...

13 Objections: The energy is a fixed constant: the particle is isolated. Is t really a universal time? Or just a parameter for one specific particle? Solution: Apply the theory to the whole universe.

14 The whole Universe: N = 2 particles To each “point” in configuration space, we associate a probability distribution, ... a product: are independent, but...

15 For particle 1, a spherically symmetric Gaussian Each particle has its own mass. A single conformal factor affects all particles equally.

16 For the whole Universe, where mass matrix Information metric: Entropic Dynamics:

17 Define time t so that motion looks simple,
then, Newton’s equation for interacting particles!! and

18 Conclusions and remarks:
On mass and interactions: On time: There is no external time. Internal time: Ephemerides time The universe is the ultimate clock. It measures universal time. This is just a model... ...but it is a statistical model!

19

20 Statistical manifolds or statistical fiber bundles?
9-dim space of Gaussians: Standard information metric: But we want the metric induced on a 3-dim submanifold.

21 On the 9-dim manifold On the 3-dim submanifold: Substitute ? No: not covariant!! better: Therefore Given find Solution:

22 Entropic Dynamics: ?? The entropic dynamics trajectory is a geodesic.

23 We only need to consider very short steps.

24 Entropic Dynamics: and form a straight line. The entropic dynamics trajectory is a geodesic.

25 Information Theory and Classical Mechanics
Ariel Caticha and Carlo Cafaro Department of Physics University at Albany - SUNY MaxEnt 2007


Download ppt "Ariel Caticha From Information Geometry to Newtonian Dynamics"

Similar presentations


Ads by Google