- #1
Replusz
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- TL;DR Summary
- I am not sure how to get the second line from the first.
It looks like he is expanding the exponential as a Taylor series, but what is happening to all those integrals?
Replusz said:It looks like he is expanding
I assume its just this:Defining the exponential of an operator as a power series, and supposing that the operator ##\int dt H\left(t\right)## exists, what are the first three terms of
$$\exp \left( \int dt H\left(t\right) \right) ?$$
I was actually thinking the same thing, I assume the d3^x term is just there to normalize something - I might be completely wrong though.hilbert2 said:That looks like the same as when an evolution operator ##U(t,t')## in nonrelativistic QM is written as a Dyson series, but it's not completely the same because the integrals are not only over the time coordinate.
Replusz said:I assume its just this:
View attachment 260571
This corresponds to the first three terms of the 2nd line in eq. 7.1
I think I see where I went wrong.
Where it says in the 2nd line in 7.1 "..." those only mean measures right? No integrands. So it is only the very last part that is being integrated n times.
If ##H\left(t\right)## is a Hamiltonian, what is ##\int dt H\left(t\right)## in terms of a Hamiltonian density?Replusz said:I was actually thinking the same thing, I assume the d3^x
George Jones said:I am not quite sure what you mean, as there two instances of "..." in (7.1), one for the integration variables, and one for the integrand. Write the second-order term above as
$$\int dt_1 H\left(t_1\right) \int dt_2 H\left(t_2\right) =\int dt_1 \int dt_2 H\left(t_1\right) H\left(t_2\right) ,$$
so the nth-order term is
$$ \int dt_1 \int dt_2 ... \int dt_n H\left(t_1\right) H\left(t_2\right)... H\left(t_n\right). $$
If ##H\left(t\right)## is a Hamiltonian, what is ##\int dt H\left(t\right)## in terms of a Hamiltonian density?
The vacuum amplitude in phi^4 theory is a mathematical quantity that represents the probability of a vacuum state in a quantum field theory. It is calculated using the path integral formalism and is an important concept in understanding the behavior of particles in a vacuum state.
The vacuum amplitude in phi^4 theory is calculated using the Feynman diagrams, which are graphical representations of the possible interactions between particles. The contribution of each Feynman diagram is then summed up to obtain the total vacuum amplitude.
Vacuum amplitudes in phi^4 theory are important because they provide a way to calculate the probability of particle interactions and the behavior of particles in a vacuum state. They also play a crucial role in understanding the properties of quantum field theories and their predictions.
Vacuum amplitudes in phi^4 theory are directly related to particle interactions as they represent the probability of these interactions occurring. The higher the vacuum amplitude, the more likely it is for particles to interact with each other.
Yes, vacuum amplitudes in phi^4 theory have various applications in theoretical physics, particularly in the study of quantum field theories and their predictions. They are also used in calculations for high-energy particle collisions and in understanding the behavior of particles in a vacuum state.