Lorentz Invariance of the Lagrangian

In summary, QFT requires the Lagrangian to be Lorentz invariant in order for the equations of motion to hold true in all inertial reference frames. However, non-inertial reference frames, such as those in general relativity, do not accommodate accelerated linear motion. This is addressed in QFT through the use of non-inertial reference frames, but it is more complicated in quantum theory compared to classical physics. For example, in the Unruh effect, the vacuum state appears as a state with many particles in a thermal state for an accelerated observer.
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Silviu
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Hello! I started reading stuff on QFT and it seems that one of the main points is for the Lagrangian to be Lorentz invariant, so that the equations of motion remain the same in all inertial reference frames. I am not sure however i understand how do non inertial reference frames come into play. I didn't take a course on GR yet, but Lorentz group doesn't accommodate accelerated linear motion for example, so a Lorentz scalar in one frame wouldn't be scalar in another frame moving with a non zero acceleration. So how is this taken into account, such that the equations of motion hold true in all frames?
 
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As in Newtonian physics you can of course use non-inertial reference frames in SRT. You come already very close to the general tensor formalism needed in GR, and it's a good way to start into GR with this approach.

However, be warned, in QT non-inertial reference frames are not as easy as in classical physics, and particularly in QFT it's fascinating. E.g., if you just take a free field, quantize it in the usual way in an inertial frame and then ask, how the vacuum looks like for an accelerated observer, you get surprising results. E.g., taking a uniformly accelerated observer (i.e., with constant proper acceleration), you'll get the Unruh effect: The vacuum determined in the inertial frame (it's identical for all inertial frames because the vacuum is Poincare invariant) appears as a state with many particles in a thermal state for the acclerated observer (who lives in "Rindler space"). Look for "Unruh radiation".
 
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1. What is Lorentz Invariance of the Lagrangian?

The Lorentz Invariance of the Lagrangian is a fundamental principle in physics that states that the laws of nature should remain the same for all observers in uniform motion, regardless of their relative velocities.

2. Why is Lorentz Invariance important?

Lorentz Invariance is important because it is a key component of Einstein's theory of Special Relativity, which has been extensively tested and confirmed through experiments. It also allows for consistency and predictability in the laws of physics across different frames of reference.

3. How is Lorentz Invariance related to the concept of spacetime?

Lorentz Invariance is closely related to the concept of spacetime, as it describes the way in which space and time are perceived to be interconnected and can be transformed between different frames of reference. The equations of Special Relativity, which incorporate Lorentz Invariance, allow for the unification of space and time into a four-dimensional spacetime.

4. Can the Lagrangian be invariant under transformations other than Lorentz transformations?

Yes, the Lagrangian can also be invariant under Galilean transformations, which describe the laws of physics in non-relativistic situations. However, in the context of Special Relativity, the principle of Lorentz Invariance is necessary for the consistency of the theory.

5. How does Lorentz Invariance affect the equations of motion?

Lorentz Invariance does not directly affect the equations of motion, but rather it dictates how the equations should be written in order to be consistent with the principle. The equations of motion, such as the famous E=mc², are derived from the Lagrangian and are thus inherently Lorentz Invariant.

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