What is the Connection Between the Hubble Constant and Scalar Field Dynamics?

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SUMMARY

The discussion centers on the relationship between the Hubble constant (H) and scalar field dynamics, specifically in the context of the Klein-Gordon equation for a massless scalar field in curved spacetime. The equation H\dot{\phi}=-\partial^2\phi/{\partial x^2} is analyzed, with emphasis on the omission of the \ddot{\phi} term, which is crucial for accurate representation in Friedmann-Robertson-Walker (FRW) spacetime. Participants highlight the need to derive expressions from first principles to fully understand the dynamics involved.

PREREQUISITES
  • Understanding of the Hubble constant (H) in cosmology
  • Familiarity with scalar fields and their dynamics
  • Knowledge of the Klein-Gordon equation in curved spacetime
  • Basic concepts of Friedmann-Robertson-Walker (FRW) cosmological models
NEXT STEPS
  • Study the derivation of the Klein-Gordon equation in curved spacetime
  • Learn about the role of the \ddot{\phi} term in scalar field dynamics
  • Explore the implications of the Hubble constant in cosmological models
  • Investigate the mathematical formulation of FRW spacetime
USEFUL FOR

Researchers in cosmology, theoretical physicists, and students studying scalar field theory and its applications in cosmological models will benefit from this discussion.

nikhilb1997
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1. Homework Statement
If \phi is a usual field is it possible that
H\dot{\phi}=-\partial^2\phi/{\partial x^2}
Where H is the Hubble constant and the dot denotes time derivative

2. Homework Equations
H\dot{\phi}=-\partial^2\phi/{\partial x^2}

3. The Attempt at a Solution
I tried different ways but am not able to find the particular expression for Hubble constant used here.
 
Last edited:
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On a curved spacetime, the Klein-Gordon equation for a massless scalar field is ##\nabla^\mu \nabla_\mu \phi =0##. If the spacetime is of the FRW type, then there will be a term proportional to ##H\dot{\phi}##. You seem to have missed the ##\ddot{\phi}## term in your expression, so you might want to go through the exercise of working this out from first principles.
 
fzero said:
On a curved spacetime, the Klein-Gordon equation for a massless scalar field is ##\nabla^\mu \nabla_\mu \phi =0##. If the spacetime is of the FRW type, then there will be a term proportional to ##H\dot{\phi}##. You seem to have missed the ##\ddot{\phi}## term in your expression, so you might want to go through the exercise of working this out from first principles.

Thanks a lot. I did miss that term because this was the part i was confused about but i guess that was important too.
 

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