Show that d^4k is Lorentz invariant

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Homework Statement


Show that ##d^4k## is Lorentz Invariant

Homework Equations


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Under a lorentz transformation the vector ##k^u## transforms as ##k'^u=\Lambda^u_v k^v##
where ##\Lambda^u_v## satisfies ##\eta_{uv}\Lambda^{u}_{p}\Lambda^v_{o}=\eta_{po}## , ##\eta_{uv}## (2) the Minkowski metric, invariant.

The Attempt at a Solution


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I think my main issue lies in what ##d^4k## is and writing this in terms of ##d^4k##
Once I am able to write ##d^4k## in index notation I might be ok.
For example to show ##ds^2=dx^udx_u## is invariant is pretty simple given the above identities and my initial step would be to write it as ##ds^2=\eta_{uv}dx^udx^v## in order to make use (2).
I believe ##d^4k=dk_1 dk_2 dk_3 dk_4##?
For example given a vector ##V^u = (V^0,V^1,V^2,V^3)## I don't know how I would express ##V^0V^1V^2V^3## as some sort of index expression of ##V^u## (and probably I'm guessing the Minkowski metric?). I would like to do this for ##d^4k##.
Is this the first step required and how do I go about it?

Many thanks in advance.
 
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Length contraction and time dilation "cancel" in a volume element.

For simplicity, have the moving frame be moving along the x axis.
dx = gamma dx'
dt = dt' /gamma
dy = dy'
dz = dz'

dxdydzdt = dx'dy'dz'dt' gamma/gamma = dx'dy'dz'dt'

Same applies to momentum space with k1,k2,k3,k4
 
DuckAmuck said:
Length contraction and time dilation "cancel" in a volume element.

For simplicity, have the moving frame be moving along the x axis.
dx = gamma dx'
dt = dt' /gamma
dy = dy'
dz = dz'

dxdydzdt = dx'dy'dz'dt' gamma/gamma = dx'dy'dz'dt'

Same applies to momentum space with k1,k2,k3,k4

huh? using the relevant equations please?
don't think i'd get the marks if I plucked something out of the air ...