4-derivative kinetic term Lagrangian

In summary, the conversation discusses the generation of negative energy density by the Lagrangian L=phi*Box^2*phi. The attempt at a solution involves finding the energy density using the divergence theorem, but it is incorrect due to the presence of the d'Alembertian. The correct expression for the energy density is phi*Box*phi = partial_mu(phi*partial^mu*phi) - (partial_mu(phi))*(partial^mu*phi).
  • #1
kelly0303
561
33

Homework Statement


Show that $$L=\phi\Box^2\phi$$ generates negative energy density.

Homework Equations

The Attempt at a Solution


The energy density is $$E=\frac{\partial L}{\partial \dot{\phi}}\dot{\phi}-L$$ Also the Lagrangian can be rewritten (using divergence theorem) as $$L=-\partial_\mu\phi\partial_\mu(\Box\phi)$$ So I would get $$E=-\partial_0\phi\partial_0(\Box\phi)+\partial_\mu\phi\partial_\mu(\Box\phi)$$ $$E=-\partial_x\phi\partial_x(\Box\phi)-\partial_y\phi\partial_y(\Box\phi)-\partial_z\phi\partial_z(\Box\phi)$$. Why is this negative necessarily? Thank you!
 
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  • #2
kelly0303 said:
Also the Lagrangian can be rewritten (using divergence theorem) as
L=−∂μϕ∂μ(□ϕ)​
No, it cannot. You need to remove the d’Alembertian from this expression.
 
  • #3
Orodruin said:
No, it cannot. You need to remove the d’Alembertian from this expression.
I am not sure what you mean. I used $$\int(\phi\Box^2\phi)=\int\partial_\mu(\phi\partial_\mu \Box \phi)-\int(\partial_\mu\phi\partial_\mu \Box \phi)$$ What is wrong? What do you mean by getting rid of the d'Alembertian?
 
  • #4
kelly0303 said:
I am not sure what you mean. I used $$\int(\phi\Box^2\phi)=\int\partial_\mu(\phi\partial_\mu \Box \phi)-\int(\partial_\mu\phi\partial_\mu \Box \phi)$$ What is wrong? What do you mean by getting rid of the d'Alembertian?
This is simply not true. What you are looking for is
$$
\phi \Box \phi = \partial_\mu (\phi \partial^\mu \phi) - (\partial_\mu \phi)(\partial^\mu\phi)
$$
 
  • #5
Ah, sorry. You have ##\Box^2##, not ##\Box##. In that case you cannot use the expression for the energy that you have given since your Lagrangian will contain derivatives of order higher than one.
 

1. What is a 4-derivative kinetic term Lagrangian?

A 4-derivative kinetic term Lagrangian is a term in a mathematical equation that describes the motion of a physical system. It is used in theoretical physics to calculate the energy and momentum of a system, as well as how it will evolve over time.

2. How is the 4-derivative kinetic term Lagrangian different from other Lagrangians?

The 4-derivative kinetic term Lagrangian is different from other Lagrangians because it includes fourth-order derivatives of the system's coordinates. This allows for a more accurate and detailed description of the system's motion.

3. What physical systems can be described using the 4-derivative kinetic term Lagrangian?

The 4-derivative kinetic term Lagrangian can be used to describe a wide range of physical systems, including particles, fields, and fluids. It is commonly used in theories of gravity, such as general relativity, to describe the motion of massive objects.

4. What are the advantages of using a 4-derivative kinetic term Lagrangian?

The 4-derivative kinetic term Lagrangian has several advantages over other Lagrangians. It allows for a more precise description of the system's motion, particularly at high energies or in strong fields. It also leads to more consistent and stable mathematical equations.

5. Are there any limitations or drawbacks to using the 4-derivative kinetic term Lagrangian?

One limitation of the 4-derivative kinetic term Lagrangian is that it can be more difficult to work with mathematically compared to simpler Lagrangians. It also may not accurately describe certain physical systems, such as those involving quantum mechanics, and may need to be modified or combined with other equations to fully describe a system.

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