Orthochronous subspace of Lorentz group.

In summary: The equations with sums over the matrix indices don't use orthogonality. They use the definitions of matrix multiplication and matrix transposition. Do you know what those definitions are? It would help me if you could write them down for me. I won't be able to respond any more today, but I will check tomorrow.
  • #1
LayMuon
149
1
In a Lorentz group we say there is a proper orthochronous subspace. How can I prove that the product of two orthchronous Lorentz matrices is orthochronous? Thanks. Would appreciate clear proofs.
 
Physics news on Phys.org
  • #2
Sounds like homework...

As a start, what is your definition of orthochronous?
 
  • #3
[itex] \Lambda^0_0 \geq 1 [/itex]
 
  • #4
LayMuon said:
In a Lorentz group we say there is a proper orthochronous subspace. How can I prove that the product of two orthchronous Lorentz matrices is orthochronous? Thanks. Would appreciate clear proofs.

Consider two such matrices, [itex]A[/itex] and [itex]B[/itex], call their product [itex]C[/itex]. Now take the [itex](0,0)[/itex] entries of the following matrix equations
[tex]A B = C , \ \ \ A \ \eta \ A^{ T } = B^{ T } \eta \ B = \eta .[/tex]
Now, if you use the Schwarz inequality
[tex]
- \sqrt{ ( A^{ 0 }{}_{ i } )^{ 2 } ( B^{ i }{}_{ 0 } )^{ 2 } } \leq A^{ 0 }{}_{ i } \ B^{ i }{}_{ 0 } ,
[/tex]
and
[tex]A^{ 0 }{}_{ 0 } \geq 1 , \ \ B^{ 0 }{}_{ 0 } \geq 1 ,[/tex]
you should be able to show that [itex]C^{ 0 }{}_{ 0 } \geq 1[/itex]
 
  • #5
Thanks for reply. Why is there a minus sign in Schwartz inequality? Isn't it [itex] \sqrt{ ( A^{ 0 }{}_{ i } )^{ 2 } ( B^{ i }{}_{ 0 } )^{ 2 } } \geq |A^{ 0 }{}_{ i } \ B^{ i }{}_{ 0 }| [/itex]?

[tex]

C^0 {}_0 - A^0 {}_0 B^0 {}_0 = A^{ 0 }{}_{ i } \ B^{ i }{}_{ 0 }

[/tex]

How to proceed?
 
  • #6
I don't (yet) see what Sam is doing there. But what you wrote isn't the standard Cauchy-Schwarz inequality either. I think what you're looking for is
$$\left|\sum_i A^0{}_i B^i{}_0\right|\leq \sqrt{\sum_i(A^0{}_i)^2}\sqrt{\sum_j(B^j{}_0)^2}.$$ Do you know how to prove that if ##\Lambda## is orthochronous, its 00 component is either ##\geq 1## or ##\leq -1##? If you have proved that, it will be sufficient to prove that the 00 component of the product transformation is ##\geq 0##. I think that makes the problem much easier. One approach is to try to show that (in a notation with all indices of matrix components written downstairs) ##(\bar\Lambda\Lambda)_{00}=\bar\Lambda_{00} \Lambda_{00} X,## where X is a non-negative real number.
 
Last edited:
  • #7
So how does it work out?
 
  • #8
Have you tried this approach? (I have, so I know that it works). What do you get?
 
  • #9
Moved to homework since it is a homework type question.

LayMuon said:
So how does it work out?

Please provide an attempt at the solution.
 
  • #10
[tex] |C^0 {}_0 - A^0 {}_0 B^0 {}_0 | \leq \sqrt{\sum_i(1-B^0{}_0{}^2)}\sqrt{\sum_j(A^0{}_i)^2} [/tex]. I don't know how to express $$ A^0{}_i^2$$ in terms of A00
 
Last edited:
  • #11
I don't see what you're doing there.

I worked through the solution by my method again. I had to use Cauchy-Schwartz, the familiar version for vectors on ##\mathbb R^3##, but not until the very end.

You didn't answer if you have already proved that the 00 component of a Lorentz transformation can't be in the interval (-1,1). You should start with that, because it makes your task easier. You will find that result if you look at the 00 component of the matrix equation ##\Lambda^T\eta\Lambda=\eta##. (Use the definition of matrix multiplication). The next step is to use the definition of matrix multiplication on the 00 component of ##\bar\Lambda\Lambda##. Feel free to use the notation AB instead of ##\bar\Lambda\Lambda## if you prefer.
 
  • #12
Fredrik said:
You didn't answer if you have already proved that the 00 component of a Lorentz transformation can't be in the interval (-1,1).

Yes, that's clear.
 
  • #13
OK, I should also mention that I find it useful to know that if ##\Lambda## is the transformation from the coordinate system S to the coordinate system S', then (in my notation, where all matrix indices are downstairs), ##\Lambda_{i0}/\Lambda_{00}## is the velocity of S in S'. It's not absolutely necessary to know that, but it makes some steps easier to see.
 
  • #14
LayMuon said:
Thanks for reply. Why is there a minus sign in Schwartz inequality? Isn't it [itex] \sqrt{ ( A^{ 0 }{}_{ i } )^{ 2 } ( B^{ i }{}_{ 0 } )^{ 2 } } \geq |A^{ 0 }{}_{ i } \ B^{ i }{}_{ 0 }| [/itex]?
Ok, doesn’t this imply that
[tex]- \sqrt{ ( A^{ 0 }{}_{ i } )^{ 2 } ( B^{ j }{}_{ 0 } )^{ 2 } } \leq A^{ 0 }{}_{ i } \ B^{ i }{}_{ 0 } .[/tex]

[tex]

C^0 {}_0 - A^0 {}_0 B^0 {}_0 = A^{ 0 }{}_{ i } \ B^{ i }{}_{ 0 }

[/tex]

How to proceed?

Now, from the other two equations, you have (sums over indices are implies)
[tex]( A^{ 0 }{}_{ i } )^{ 2 } = ( A^{ 0 }{}_{ 0 } )^{ 2 } - 1 ,[/tex]
[tex]( B^{ j }{}_{ 0 } )^{ 2 } = ( B^{ 0 }{}_{ 0 } )^{ 2 } - 1 .[/tex]
Using these, the Schwarz inequality becomes equivalent to
[tex]0 \leq | A^{ 0 }{}_{ 0 } | \ | B^{ 0 }{}_{ 0 } | \left( 1 - \sqrt{ ( 1 - | A^{ 0 }{}_{ 0 } |^{ - 2 } ) ( 1 - | B^{ 0 }{}_{ 0 } |^{ - 2 } ) } \right) \leq C^{ 0 }{}_{ 0 } .[/tex]
Now you can check that [itex]C^{ 0 }{}_{ 0 } \geq 1[/itex].
 
  • #15
How did you get this: [itex] ( A^{ 0 }{}_{ i } )^{ 2 } = ( A^{ 0 }{}_{ 0 } )^{ 2 } - 1 [/itex]? I understand it for B. how are [itex] A^0{}_j [/itex] and [itex] A^j{}_0 [/itex] related?
 
  • #16
Lower indices number the rows in the matrix. Choose any convention you like and stick with it.
 
  • #17
samalkhaiat said:
Lower indices number the rows in the matrix. Choose any convention you like and stick with it.

I still don't understand. They are different parts of lorentz matrix. One can only use the definition of lorentz group, I.e. orthogonality.
 
  • #18
LayMuon said:
I still don't understand. They are different parts of lorentz matrix. One can only use the definition of lorentz group, I.e. orthogonality.

I don't really do homework. Any way, orthogonality is what I used in writing the matrix equations
[tex]\eta = A \eta A^{ T }, \ \ \eta = B^{ T } \eta B[/tex]
Now, forget about upper and lower indices, Can you find the first matrix element, i.e. the [itex](0,0)[/itex] entry in each of the above equations?
 
  • #19
LayMuon said:
Thanks for reply. Why is there a minus sign in Schwartz inequality? Isn't it [itex] \sqrt{ ( A^{ 0 }{}_{ i } )^{ 2 } ( B^{ i }{}_{ 0 } )^{ 2 } } \geq |A^{ 0 }{}_{ i } \ B^{ i }{}_{ 0 }| [/itex]?
OK, I see now that I got confused by the notation. The inequality that samalkhaiat wrote down is an almost immediate consequence of Cauchy-Schwartz for vectors in ##\mathbb R^3##. If we use your inequality from the quote above, and then use that ##|x|\geq -x## for all real numbers x,...

Regarding notational conventions: Some people would write ##x_i x_i## rather than ##(x_i)^2## to ensure that the index to be summed over explicitly appears twice, but I suppose that can be weird too when we use a convention that typically has one of the indices upstairs and the other downstairs. I would denote the component on row ##\mu##, column ##\nu## of an arbitrary matrix X by ##X_{\mu\nu}##, ##X^\mu_\nu## or ##X^\mu{}_\nu##. Samalkhaiat apparently uses ##X^\nu{}_\mu##. That's fine too. As he said, "choose any convention you like and stick with it".
 

1. What is the Orthochronous subspace of Lorentz group?

The Orthochronous subspace of Lorentz group refers to a subset of the larger Lorentz group, which is a mathematical description of the symmetries of special relativity. This subset includes transformations that result in a positive time orientation, meaning that events occur in a specific order in time.

2. How is the Orthochronous subspace different from the full Lorentz group?

The full Lorentz group includes transformations that result in both positive and negative time orientations, while the Orthochronous subspace only includes positive time orientations. This makes it a more restricted subset of the full Lorentz group.

3. What is the significance of the Orthochronous subspace in physics?

The Orthochronous subspace has important implications in physics, particularly in special relativity. It allows us to mathematically describe the symmetries of physical laws and phenomena, and helps us understand the connection between space and time.

4. How is the Orthochronous subspace related to causality?

The Orthochronous subspace is closely related to causality, as it describes the ordering of events in time. Causality is a fundamental principle in physics, stating that an event must occur before its effects, and the Orthochronous subspace helps us understand and mathematically describe this concept.

5. Can you give an example of an Orthochronous transformation?

One example of an Orthochronous transformation is a boost, which is a change in velocity between two reference frames. A boost can result in a positive or negative time orientation, but an Orthochronous boost would only result in a positive time orientation, preserving the order of events in time.

Similar threads

  • High Energy, Nuclear, Particle Physics
Replies
27
Views
3K
Replies
3
Views
1K
  • Calculus and Beyond Homework Help
Replies
15
Views
2K
  • Calculus and Beyond Homework Help
Replies
1
Views
457
  • Calculus and Beyond Homework Help
Replies
4
Views
1K
  • Quantum Physics
3
Replies
87
Views
5K
  • Calculus and Beyond Homework Help
Replies
14
Views
1K
Replies
31
Views
3K
  • Calculus and Beyond Homework Help
Replies
4
Views
1K
  • Calculus and Beyond Homework Help
Replies
4
Views
2K
Back
Top