Action invariance under galilean boost

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SUMMARY

The discussion focuses on demonstrating the invariance of the action of a non-relativistic particle described by the Schrödinger density Lagrangian under a Galilean boost. The transformation of the wave function is given by ψ(x0,x)→ψ'(x0,x)=eimvx-(im/2)x0v2ψ(x0,x-vx0). The Lagrangian used is L= ihψ*\partial0ψ+h2/2m(\partialiψ*)(\partialiψ). It is established that the Lagrangian is not invariant under this transformation, necessitating the addition of a total divergence to maintain the equations of motion. The discussion emphasizes the handling of terms resulting from the transformation and suggests that a suitable total divergence is ∂i(ψ*φ*∂iψφ).

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Petraa
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Hello,

I've been spending a lot of time trying to solve this problem but I can't figure out a good solution.

I have to show that the action of a non-relativistic particle ( Schrödinger density Lagrangian ) is invariant under Galilean boost with the form

ψ(x0,x)→ψ'(x0,x)=eimvx-(im/2)x0v2ψ(x0,x-vx0)

x0= t

I've tried to find the transformed Lagrangian by replacing the wave functions and the derivatives but I'm not sure I did it correctly because I get monstrous expressions

I'm using this density Lagrangian L= ihψ*\partial0ψ+h2/2m(\partialiψ*)(\partialiψ)


If someone can give me a good tip I'll appreciate it
thank you!
 
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Ok, hints only, because this is an assignment.

Important fact: Lagrangians are not unique. You can freely add a total divergence to a Lagrangian without changing the equations of motion. And in this example the Lagrangian will not be invariant under the transformation, you will need to add a total divergence.

Let φ(x,t) be the phase factor in front you've added. You'll get three types of terms:

φ*φ x (derivatives on ψ) + ψ*ψ x (derivatives on φ) + (derivatives on both φ and ψ)

The first two types are easily handled. :smile: For terms of the third type you'll need to split off a total divergence, e.g. by throwing derivatives of ψ over onto derivatives of φ.
 
Bill_K said:
Ok, hints only, because this is an assignment.

Important fact: Lagrangians are not unique. You can freely add a total divergence to a Lagrangian without changing the equations of motion. And in this example the Lagrangian will not be invariant under the transformation, you will need to add a total divergence.

Let φ(x,t) be the phase factor in front you've added. You'll get three types of terms:

φ*φ x (derivatives on ψ) + ψ*ψ x (derivatives on φ) + (derivatives on both φ and ψ)

The first two types are easily handled. :smile: For terms of the third type you'll need to split off a total divergence, e.g. by throwing derivatives of ψ over onto derivatives of φ.

I've tried some, the "best" total divergence I've found is ∂i(ψ*φ*∂iψφ)

Fits all the terms on the equation but ( obviously ) φ*∂0φ and also leaves me a term ∂iψ∂iψ* that doesn't appear on the L'

I'm close to the solution ?
 

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