Proving that the scalar product is invariant

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SUMMARY

The discussion centers on proving the invariance of the scalar product defined as xuxu = (x0)² - (x1)² - (x2)² - (x3)² under Lorentz transformations. It establishes that a Lorentz transformation can be defined as a linear map x → Λx: ℝ⁴ → ℝ⁴, satisfying the condition ΛᵀηΛ = η, where η is the Minkowski metric. The scalar product is defined as = xᵀηy, and it is demonstrated that <Λx,Λy> = holds true for Lorentz transformations, confirming the scalar product's invariance.

PREREQUISITES
  • Understanding of Lorentz transformations and their properties
  • Familiarity with the Minkowski metric in special relativity
  • Basic knowledge of linear algebra, particularly matrix operations
  • Concept of scalar products in vector spaces
NEXT STEPS
  • Study the derivation of Lorentz transformations in various reference frames
  • Explore the implications of the Minkowski metric in physics
  • Learn about linear transformations and their applications in physics
  • Investigate the role of invariance in different physical theories
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Physicists, mathematicians, and students studying special relativity or linear algebra, particularly those interested in the properties of Lorentz transformations and their applications in theoretical physics.

Someone1987
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Is there a general way of proving that the scalar product
xuxu = (x0)2 - (x1)2 - (x2)2 - (x3)2
is invariant under a Lorentz transformation that applies no matter the explicit form of the transformation.
 
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First derive the form of a Lorentz transform in an arbitrary direction.
Then check that the scalar product is invariant.
 
You could take the requirement that this "scalar product" is invariant (and the requirement that a Lorentz transformation is a linear transformation) as the definition of a Lorentz transformation. If you do, you don't have to prove that it's invariant.

An alternative is to define a (homogeneous) Lorentz transformation as a linear map [itex]x\mapsto\Lambda x:\mathbb R^4\rightarrow\mathbb R^4[/itex] such that [itex]\Lambda^T\eta\Lambda=\eta[/itex] (where ^T is the transpose of the 4x4 matrix). The "scalar product" <x,y> of x and y is then defined by [itex]\langle x,y\rangle=x^T\eta y[/itex]. If you know anything about matrices you should find it easy to prove that [itex]\langle\Lambda x,\Lambda y\rangle=\langle x,y\rangle[/itex] when [itex]\Lambda[/itex] is a Lorentz transformation.
 

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