Proving L3 is a Lorentz Transformation

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Homework Help Overview

The discussion revolves around proving that the product of two Lorentz transformations, L1 and L2, denoted as L3, is also a Lorentz transformation. Participants are exploring the properties of Lorentz transformations and their implications in the context of Minkowski space.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the invariance of the dot product under the transformation L3 and question the definition of the dot product in the context of 4-vectors. There are attempts to express the transformation mathematically and to clarify the conditions under which L3 retains the properties of a Lorentz transformation.

Discussion Status

The discussion is active, with participants providing definitions and clarifications regarding Lorentz transformations. Some guidance has been offered regarding the mathematical expressions needed to demonstrate that L3 is a Lorentz transformation, and there is acknowledgment that the approach can be validated through the properties of the metric.

Contextual Notes

Participants are working with definitions and properties of Lorentz transformations as outlined in their notes or texts, and there are indications of potential confusion regarding index notation and the formulation of the transformation equations.

martyf
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Homework Statement



L1 and L2 are two lorentz trasformation.
show that L3=L1 L2 is a lorentz trasformation too.


Homework Equations





The Attempt at a Solution

 
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I could be wrong but I think it would be enough to show the invariance of the dot product under L3.
 
what is the dot product?
 
The scalar product, or inner product or whatever it's called of 4-vectors. In Minkowski space it's r_1 \cdot r_2 = c^2 t_1 t_2 - x_1 x_2 - y_1 y_2 - z_1 z_1 or with the signs reversed depending on the convention. But if you haven't yet done the Minkowski notation then you could write L1 and L2 as Lorentz transformations with some velocities and show by applying them consecutively that L3 has the same form.
 
I write better :

I have: \Lambda ^{\mu}_{\nu} and \Lambda\widetilde{} ^{\mu}_{\nu} : lorentz trasformations.

Show that \Lambda\overline{} ^{\sigma}_{\rho} = \Lambda\widetilde{} ^{\sigma}_{\mu} \Lambda ^{\mu}_{\rho} is a lorentz trasformation
 
What is the definition of Lorentz transformation given in your notes and/or text?
 
a trasfonmation that not change the space-time distance of a point to the origin.
 
martyf said:
a trasfonmation that not change the space-time distance of a point to the origin.

Can you write a definition in terms of mathematics, i.e., \Lambda^\mu{}_\nu[/itex] is a Lorentz transformation iff ... ?
 
...if :

x^{2}_{0} - r ^{2}= (\Lambda ^{0}_{\nu} x_{0})^{2} -( \Lambda ^{\mu}_{\nu} r_{\mu})^{2}
 
  • #10
is it right?
 
  • #11
You don't have the indices right, your right hand side depends on on \nu whereas the left hand side doesn't. It should be:

(x^0)^2 - r^2 = (\Lambda^0{}_\nu x^\nu)^2 - (\Lambda^j{}_\nu x^\nu)^2

Where j goes from 1 to 3. More compactly:

g_\alpha_\beta x^\alpha x^\beta = g_\mu_\nu \Lambda^\mu{}_\alpha \Lambda^\nu{}_\beta x^\alpha x^\beta

Where g is the metric. Use the fact that L1 and L2 satisfy this to show that L3 satisfies it as well.
 
  • #12
L1 and L2 are two generical lorents tranformation. I must demostrate that their product is also a lorentz transormation.
Can I demostrate :

g_\alpha_\beta x^\alpha x^\beta = g_\mu_\nu \Lambda^\mu{}_\alpha \Lambda^\nu{}_\beta x^\alpha x^\beta

with \Lambda =L3= L1 L2 ?
 
  • #13
Yes you can.
 

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