The Klein-Gordon equation at background level for a scalar field φ is given by (found in image below) where H is the Hubble parameter, V the potential of the scalar field, and V′ = dV/dφ. Assume a flat Friedmann-Robertson-Walker universe, dominated by the scalar field. i) State the conditions for slow-roll inflation. Write down the Friedmann equation and the Klein-Gordon equation valid for slow-roll inflation. ii) For a scalar field potential V =1/2m^2φ^2, where m is the mass of the field, calculate the time evolution of the field φ in the case of slow-roll inflation.
Stellar evolution
We may see thousands of stars in the dark sky. Our universe consists of billions of stars. Stars may appear tiny to us but they are huge balls of gasses. Sun is a star of average size. Some stars are even a thousand times larger than the sun. The stars do not exist forever they have a certain lifetime. The life span of the sun is about 10 billion years. The star undergoes various changes during its lifetime, this process is called stellar evolution. The structure of the sun-like star is shown below.
Red Shift
It is an astronomical phenomenon. In this phenomenon, increase in wavelength with corresponding decrease in photon energy and frequency of radiation of light. It is the displacement of spectrum of any kind of astronomical object to the longer wavelengths (red) side.
The Klein-Gordon equation at background level for a scalar field φ is given by
(found in image below)
where H is the Hubble parameter, V the potential of the scalar field, and V′ = dV/dφ.
Assume a flat Friedmann-Robertson-Walker universe, dominated by the scalar field.
i) State the conditions for slow-roll inflation. Write down the Friedmann equation and the
Klein-Gordon equation valid for slow-roll inflation.
ii) For a scalar field potential V =1/2m^2φ^2, where m is the mass of the field, calculate the
time evolution of the field φ in the case of slow-roll inflation.
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