- #1

Joella Kait

- 5

- 0

## Homework Statement

Consider a point in the intergalactic medium at some cosmic time ## t_{obs}##, the time of arrival of a photon of wavelength ##λ_{obs}## as seen by a hydrogen atom at that location. The source of this photon a comoving distance ##r## away emitted it at wavelength ##λ_{em}## at time ##t_{em}##. Assume the scale factor at present ##a_0= 1##.

(a) Express ##r## as a function of ##t_{obs}##, ##t_{em}## and the scale factor ##a(t)##.

(b) Solve for the dependence of ##a(t)## on ##t## for a universe in which the Hubble constant varies with time according to

[tex]\ H(t)=\frac{2}{3t}. [/tex]

(c) What is the ratio of ##λ_{em}## to ##λ_{obs}## in terms of ##t_{em}## and ##t_{obs}##, in a universe described in (b)?

(d) The same photon will later reach a telescope on Earth today at ##λ_0=3645 Angstroms##. Suppose ##λ_{obs}=1215 Angstroms##, the H atom Lyman-alpha line transition. What is ##λ_{em}## if the source is located a comoving distance ##r=500 Mpc## (in present-day units) away from the H atom? Assume ##H_0=70 km s^{-1} Mpc^{-1}##.

I mainly just want help with part (d).

## Homework Equations

[/B]

## ds^2=-c^2dt^2+a(t)^2[dr^2+s_k(r)^2d\Omega^2## but ##ds=0## and ##d\Omega=0##

##H(t)=\frac{1}{a}*\frac{da}{dt}##

##\frac{\lambda_{em}}{a(t_{em})}=\frac{\lambda_{obs}}{a(t_{obs})}##

## The Attempt at a Solution

[/B]

For part (a) I intergrated and got ## r=c\int\limits_{t_{em}}^{t_{obs}} \frac{1}{a(t)} \ dt ##.

For part (b) I used the second equation to get ##a(t)=t^{2/3}##

For part (c) I used the third equation to get ##\frac{\lambda_{em}}{\lambda_{obs}}=\frac{t_{em}^{2/3}}{t_{obs}^{2/3}}##

I'm really lost on part (d) though. I was told that I'm supposed to integrate my answer from (a), but I am not quite sure how to go about that.

##r=c\int\limits_{t_{em}}^{t_{obs}} \frac{1}{t^{2/3}} \ dt = 3c(t_{obs}^{1/3}-t_{em}^{1/3})##

I'm not sure how to get ##\lambda's## from this, and I'm also not sure how to include ##t_0/\lambda_0##

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