Replusz
- 141
- 14
- TL;DR
- 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?
The discussion revolves around the expansion of the exponential of an operator in the context of quantum field theory, specifically within the framework of \(\phi^4\) theory. Participants explore the relationship between this expansion and the Dyson series in nonrelativistic quantum mechanics, while also addressing the implications of integrating over time and space in these expressions.
Participants express varying interpretations of the notation and structure of the equations discussed, indicating that there is no consensus on certain aspects of the expansion and its implications. Some participants agree on the relationship between the Hamiltonian and the Hamiltonian density, while others remain uncertain about specific details.
Participants reference specific equations and notations from a PDF document, which may contain assumptions or definitions that are not fully explored in the discussion. The discussion also highlights the complexity of integrating over multiple variables in the context of quantum field theory.
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?