Lorentz transform of a scalar in QM

In summary, when performing a Lorentz transform on a scalar, the function and coordinates go in opposite directions. There are two ways to describe this rotation, the active approach where the function goes first and the passive approach where the coordinates go first. Mathematically, we prefer to read from right to left, but when dealing with a function in the middle, the order of the rotations must be switched to preserve this.
  • #1
geoduck
258
2
If you Lorentz transform a scalar:

[tex]U^{-1}(\Lambda)\phi(x)U(\Lambda)=\phi(\Lambda^{-1}x) [/tex]

If you now perform another Lorentz transform, would it it look like this:

[tex]U^{-1}(\Lambda')U^{-1}(\Lambda)\phi(x)U(\Lambda)U(\Lambda')=\phi(\Lambda'^{-1}\Lambda^{-1}x) [/tex] ?

But isn't this wrong, because this expression is equal to:

[tex]U^{-1}(\Lambda\Lambda')\phi(x)U(\Lambda\Lambda')=\phi([\Lambda\Lambda']^{-1}x) [/tex]

and not:

[tex]U^{-1}(\Lambda'\Lambda)\phi(x)U(\Lambda'\Lambda)=\phi([\Lambda'\Lambda]^{-1}x) [/tex]
 
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  • #2
geoduck, There are two ways to describe a rotation: active and passive. In both methods the function gets rotated relative to the coordinates, the function goes one way and the coordinates go the other. The only distinction is which you call Λ and which you call Λ-1. What you've described is the active approach. The two methods are completely equivalent of course, but in some ways the passive approach looks more natural:

Let x → x' = Λx. Then U(Λ) φ(x) U(Λ)-1 = φ(x') = φ(Λx).

Two rotations in succession: U(Λ2)U(Λ1) φ(x) U(Λ1)-1U(Λ2)-1 = φ(Λ2Λ1x) = U(Λ2Λ1) φ(x) U(Λ2Λ1)-1
 
  • #3
Thanks. I think I see it now. As you said, function goes opposite of coordinates. So if you want them to visually go the same way, you have to inverse all the U's.

I guess what it boils down to is that mathematically, we like to read from right to left, which would look like this:

B-1A-1 φ(x) AB

Starting from the right, that should read first B, then A. And this is true if there were a ket on the right end: that's the order you'd perform A and B

But with regards to φ(x), that would read first A, then B.

Now if by default we like U(A)U(B) to mean first B, then A when operating on something to the right, then in order to preserve that when dealing with a function φ(x) in the middle (rather than a ket at the edge), you'll have to put U(A)U(B) on the left hand side, and not the right, so:

U(A)U(B)φ(x)U-1(B)U-1(A)=...

but mathematically then you'd have to invert the stuff to the right of the equal sign, so you'd get:

U(A)U(B)φ(x)U-1(B)U-1(A)=φ(ABx)
 

Related to Lorentz transform of a scalar in QM

1. What is the Lorentz transform of a scalar in Quantum Mechanics?

The Lorentz transform of a scalar in Quantum Mechanics refers to the mathematical transformation used to describe how a scalar quantity (a physical quantity that has only magnitude, not direction) changes when transitioning from one reference frame to another in special relativity.

2. Why is the Lorentz transform of a scalar important in Quantum Mechanics?

The Lorentz transform of a scalar is important in Quantum Mechanics because it allows us to accurately describe the behavior of particles moving at high speeds, close to the speed of light. It is a fundamental concept in special relativity, which is essential for understanding the behavior of particles in quantum systems.

3. How is the Lorentz transform of a scalar derived in Quantum Mechanics?

The Lorentz transform of a scalar is derived using the Lorentz transformation equations, which were first introduced by Hendrik Lorentz in 1904. These equations describe how space and time coordinates change when transitioning from one inertial reference frame to another, and they are based on the principles of special relativity.

4. Can the Lorentz transform of a scalar be applied to all scalar quantities in Quantum Mechanics?

Yes, the Lorentz transform of a scalar can be applied to all scalar quantities in Quantum Mechanics, including energy, mass, and momentum. It is a universal concept that applies to all scalar quantities that are affected by the principles of special relativity.

5. Are there any practical applications of the Lorentz transform of a scalar in Quantum Mechanics?

Yes, there are several practical applications of the Lorentz transform of a scalar in Quantum Mechanics. One example is in particle accelerators, where particles are accelerated to high speeds and their behavior must be described using special relativity and the Lorentz transform of a scalar. It is also used in the development of quantum technologies, such as quantum computing and quantum cryptography.

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