Replusz
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- 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?
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?