Electromagnetic Tensor in (-+++) Convention

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The discussion focuses on the confusion surrounding the electromagnetic tensor in the (-+++) convention compared to the more commonly used (+---) convention. It highlights that while the matrix representation of the tensor changes between conventions, the definition of each component in terms of the vector potential remains consistent. The user expresses difficulty in deriving the relativistic Lorentz force from the Lagrangian, noting that their results contradict the expected definition of the electromagnetic tensor. There is a suggestion that the Lagrangian may need to be adjusted to align with the (-+++) convention. Clarification on these points is sought to resolve the discrepancies encountered.
tomdodd4598
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Hi there,

Over the last couple of weeks, I have been learning about the relativistic description of electromagnetism through Leonard Susskind's Theoretical Minimum lectures, and although I have managed to follow it, there are some parts which I am becoming increasingly confused by, not helped by the fact Susskind uses the (-+++) convention rather than the seemingly more popular (+---).

Is the definition of the electromagnetic tensor different depending on the convention? I am aware that the matrix changes (the contravariant and covariant forms are multiplied by -1 when moving between conventions), but does the definition of each component in terms of the vector potential change?

The reason I ask this is because when deriving the relativistic Lorentz force from the Lagrangian:
L=-m√(-dXϑ/dt dXϑ/dt)-qAϑ dXϑ/dt
I always seem to get the following answer (using the (-+++) convention):
SguMBOIh.jpg

Which is the negative of what I would expect from the definition of the Electromagnetic Tensor.

Any help would be appreciated, and thanks in advance.
 
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Note that there are also conventions regarding the index structure of F...
the ;-notation vs the ∇-notation.
 
Maybe the Lagrangian should be:
L=-m√(-dXϑ/dt dXϑ/dt)+qAϑ dXϑ/dt
when using the (-+++) convention?
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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