Undergrad Momentary Co-Moving Reference Frame in SR

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In special relativity (SR), the momentary co-moving reference frame (MCRF) has the velocity four-vector U represented as (1,0,0,0). The discussion centers on whether the basis vectors associated with this velocity are zero or if the coefficients in front of these basis vectors are zero. It is clarified that basis vectors must be linearly independent and cannot be zero, with an infinite number of possible orthonormal spatial basis vectors orthogonal to U. A common choice for these vectors in the Minkowski metric is <0,1,0,0>, <0,0,1,0>, and <0,0,0,1>. Understanding this distinction is crucial for developing a Lorentz transformation to transition from one frame to the MCRF frame.
Vitani1
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What are the basis vectors?
In SR, for the momentary co-moving reference frame, U (the velocity four vector) takes the form (1,0,0,0). I'm wondering whether the basis vectors associated with this velocity are zero or if the coefficients in front of the basis vectors are zero. In classical mechanics we would say that the coefficients in front of the basis vectors are zero. I ask because the four-acceleration is defined as the proper-time derivative of this velocity and has components (0,x,y,z) hence the dot product of these two vectors is zero like in classical mechanics which makes sense. I also ask this because I'm trying to develop a lorentz transformation that takes a vector U in some frame to the MCRF frame using the lorentz matrix and if I know which it is (components or basis vectors) that cause the last 3 components of the four-velocity to be zero it would save me a lot of work.
 
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Vitani1 said:
Summary:: What are the basis vectors?

I'm wondering whether the basis vectors associated with this velocity are zero or if the coefficients in front of the basis vectors are zero.
Basis vectors must be linearly independent. So they cannot be zero.
 
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Thank you... this is what I thought.
 
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There are technically an infinite number of possible basis vectors - as other posters have mentioned, the only real requirement for the basis vecotrs is that they are linearly independent.

There are also an infinite number of possible spatial vectors that have unit length and are orthogonal to the timelike vector <1,0,0,0>. However, for the Minkowskii metric -dt^2 + dx^2 + dy^2 + dz^2, a convenient set of orthonormal spatial basis vectors ortohgonal to the vectors with components <1,0,0,0> are vectors with components <0,1,0,0>, <0,0,1,0>, <0,0,0,1>. Those are probably the vectors you are thinking of when you talk about "the" co-moving reference frame.

Note that I'm using geometrized units where c=1 for simplicity - otherwise <1,0,0,0> wouldn't be a unit length timelike vector.
 
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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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