Measuring Observables in 3+1 Formalism

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    Measuring observables
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Discussion Overview

The discussion revolves around the challenges of extracting observables from a Hamiltonian approximation of gravitational interactions in a simulation involving mass particles and photons. Participants explore the implications of not having a metric and the methods to measure properties such as proper time for test particles in a curved spacetime context.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes a Hamiltonian approximation for simulating gravitational interactions but lacks a metric to extract observables from the simulation.
  • Another participant suggests using the stress-energy tensor to solve the Einstein equations, questioning what specific observables the original poster intends to measure.
  • A clarification is made that the participant cannot solve the Einstein equations analytically due to the complexity of the configuration and would need to derive the metric numerically from the simulation.
  • A method is proposed to measure proper time for a test particle by relating coordinate time to proper time using the Lorentz factor, although concerns are raised about the simplicity of this approach in a gravitational field.
  • Discussion includes acknowledgment of the general problem in numerical relativity regarding the determination of initial data that corresponds to a matter distribution.
  • One participant mentions familiarity with the ADM formalism but expresses the difficulty of applying it practically without examples.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the best approach to extract observables or the implications of the lack of a metric. Multiple competing views and uncertainties remain regarding the methods and challenges involved.

Contextual Notes

Participants note limitations in their understanding of practical applications of the ADM formalism and the complexities involved in numerical relativity, particularly in deriving metrics from simulations.

tendor
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Hello,

lets say I have Hamiltonian aproximation [itex]H(\vec{x}_a,\vec{p}_a)[/itex] of gravitational interaction that can be used for n-body simulation of mass particles and photons. Spacetime curved by simulated particles would be asymptoticly flat. But I don't have a metric etc. All I have is evolution of particles based on coordinate time, so I have masses, momenta and coordinates of particles.

My problem is I can't find materials that would told me how to use test particles and photons in order to extract observables etc. from such simulation...
 
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You have particles, and so you have the stress energy tensor. Solving the Einstein equations for a given stress energy tensor is typically what's done anyway--we don't start off with the metric, we solve for it.

I'm not sure what observables you're planning on figuring out, though. Could you elaborate on what information it is you want from this system?
 
I'm sorry for poor description of the problem. When I've said I don't have a metric I have meant that I can't solve E.e. analyticly because configuration is too complex. If anything, I would have to get information about the metric numerically from the simulation itself.

Lets say I would like to measure a proper time of test particle located in studied area. Simulation is "ticking" with coordinate time which can be seen as a proper time of distant observer.
 
I see. Well, if you already have this simulation working, you can drop the test particle in, and at each time step, you say that [itex]\Delta \tau = \Delta t/\gamma[/itex] and just look at the particle's coordinate velocity at every time step to figure out [itex]\gamma[/itex].
 
Thank you Muphrid. :) That would cover time dilation due to the relative velocity. I just wonder if its really so simple in the presence of gravitation field.

I'll think about that in some better hour when my mind will working...
 
Oh, of course, silly me, your problem is that you don't know the metric, so the metric that would be involved in the GR case is at issue.

I mean, this is a general problem for numerical relativity--finding the initial data (metric, etc.) that corresponds to a starting matter distribution. You talk about a Hamiltonian approximation--is this something you already have? Are you familiar with the ADM formalism?
 
I'm playing with http://arxiv.org/abs/1003.0561 It works fine for things like perihelion precession, bending of light etc.

I've read about ADM formalism in general but practical usage without examples or practice and experience is another thing.
 

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