Special Relativity 4-tensor

In summary, the zero component lemma for any anti-symmetric 4-tensor states that if any of its off-diagonal components is zero in all inertial coordinate systems, then the entire tensor is zero. This can be proven using Lorentz Transformation in different directions, as in the case of 4-vectors. In special relativity, off-diagonal components of an anti-symmetric 4-tensor involve 3 vectors, and if any component of these vectors is zero under LT, the 4-vector is also zero, leading to all off-diagonal terms being zero. However, the expression of this in mathematical language is still unclear and requires further investigation.
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jeckster
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Homework Statement


prove the zero component lemma for any anti-symmetric 4-tensor: If anyone of its 0ff-diagonal component is zero in all inertial coordinate system, then the entire tensor is zero.


Homework Equations





The Attempt at a Solution



in case of 4-vector, if a particular component is zero in all inertial frame then by Lorentz Transformation in different direction, it can be proved that the 4-vector is zero in all inertial frame.
Here, i m confusing in how to prove it in case of anti-symmetric 4-tensor

Any help would be highly appreciated. thank
 
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  • #2
I have the same problem. No answers yet.
off diagonal components of the antisymmetric 4 tensors in special relativity involves 3 vectors and we can form 4 vectors from them. If any component of that 3 vector is zero under LT the 4-vector is zero then all the off-diagonal terms are zero. This is what I thought but how can I express this in Mathematical Language?
If I'm wrong can you give me a clue about it?
 

1. What is a 4-tensor in the context of Special Relativity?

A 4-tensor in Special Relativity is a mathematical object that represents a physical quantity with both magnitude and direction in the four-dimensional spacetime. It is commonly used to describe the properties of spacetime and the behavior of particles in it.

2. How is a 4-tensor different from a regular tensor?

A 4-tensor is different from a regular tensor in that it has four indices instead of the usual two or three. This allows it to represent quantities that are dependent on both space and time, making it a fundamental tool in the theory of Special Relativity.

3. What are the components of a 4-tensor in Special Relativity?

The components of a 4-tensor in Special Relativity are typically represented by a matrix with four rows and four columns. These components can represent various physical quantities, such as energy, momentum, and stress, in relation to the four dimensions of spacetime (x, y, z, and t).

4. How is the 4-tensor used in the theory of relativity?

The 4-tensor is used in the theory of Special Relativity to describe the behavior of particles in spacetime. It is used to calculate and predict various physical quantities, such as time dilation, length contraction, and relativistic momentum, which are essential to understanding the principles of relativity.

5. What are some real-world applications of the 4-tensor in Special Relativity?

The 4-tensor has many practical applications in the field of physics, including particle accelerators, nuclear reactors, and astrophysics. It is also used in the development of technologies, such as GPS systems, that rely on the principles of Special Relativity for accurate measurements and calculations.

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