Exploring the Origins of Inflation: The Significance of 10^-36 Seconds

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In summary, inflation models assume a GUT that is spontaneously broken around 10^15 GeV, corresponding to 10^-36 s. This timing is crucial as it solves the monopole problem and allows for baryogenesis. Additionally, specific inflationary models require an energy density of approximately (10^15 GeV)^4 to produce the observed density perturbations. The period of inflation needs to be long enough to flatten the universe, making 10^-36 s a lower bound for its onset.
  • #1
zeebo17
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I've seen in many places that inflation is believed to begin around [tex]10^{-36}[/tex] s corresponding to the end of the grand unification epoch. Why do we believe that this is the time that it started? Isn't the only requirement that it start sometime after Planck time [tex]10^{-44}[/tex] s?

Thanks!
 
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I'm not an expert on inflation, but here's my understanding.

Inflation models assume some kind of GUT (perhaps a variation of SU(5)) which is spontaneously broken around 10^15 GeV, which corresponds to 10^-36 s.

If inflation occurs before GUT symmetry breaking, it does not solve the monopole problem (we should see lots of magnetic monopoles but we don't).

If inflation occurs too late after GUT symmetry breaking, we have a problem of baryogenesis. Baryogenesis requires the availability of baryon number changing interactions, we know that there aren't any in the explored region of energies, but most GUTs allow such process near GUT scale. Problem is, inflation wipes any traces of baryogenesis that occurs before its onset, just as it scatters magnetic monopoles.

Therefore the solution is to have inflation right around the GUT scale, it spreads out magnetic monopoles sufficiently to make them virtually unobservable, and then, when inflation is over, the system experiences reheating and gets close enough to the GUT scale again to generate baryons.
 
  • #3
You can also fix the energy scale on some specific inflationary models. For example, a free inflaton field [tex] V \sim \phi^2 [/tex] produces density perturbations of the order of [tex] \delta \rho / \rho \sim 10^{-5} [/tex] (which is what we observe from the CMB) if and only if the energy density of the field is approximately [tex] (10^{15} \mathrm{GeV})^4 [/tex].
 
  • #4
Only a certain period of expansion is required to flatten the universe to the present degree, so my understanding is that 10^-36 is a lower bound on the period
 

Related to Exploring the Origins of Inflation: The Significance of 10^-36 Seconds

1. What is the significance of 10^-36 seconds in the study of time?

10^-36 seconds is an incredibly short unit of time known as a "Planck time." It is the smallest unit of time that can be measured and is often used in theoretical physics to study the behavior of particles at the smallest scales, such as during the Big Bang.

2. How does 10^-36 seconds compare to other units of time?

10^-36 seconds is significantly shorter than other units of time, such as a nanosecond, which is equal to 10^-9 seconds. To put it into perspective, 10^-36 seconds is to a second as a second is to 31.7 billion years.

3. Can we observe events that occur in 10^-36 seconds?

No, it is currently impossible for humans to observe events that occur in 10^-36 seconds. This unit of time is far too short for any technology or measurement tools to capture.

4. Why is it important to study events that occur in 10^-36 seconds?

Studying events that occur in 10^-36 seconds can give scientists valuable insights into the fundamental laws of nature and the behavior of particles at the smallest scales. It can also help us understand the origins of the universe and the nature of time itself.

5. Can anything travel faster than 10^-36 seconds?

No, 10^-36 seconds is the smallest unit of time and cannot be subdivided. Therefore, nothing can travel faster than this unit of time. However, particles such as photons, which have no mass, can travel at the speed of light, which is approximately 299,792,458 meters per second.

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