Skip to content

Commit

Permalink
Apply suggestions from code review
Browse files Browse the repository at this point in the history
Co-authored-by: Edoardo Pedicillo <[email protected]>
  • Loading branch information
GabrielePalazzo and Edoardo-Pedicillo authored Jan 22, 2024
1 parent 2f2cad8 commit e473c83
Showing 1 changed file with 2 additions and 2 deletions.
4 changes: 2 additions & 2 deletions doc/source/protocols/resonator_punchout.rst
Original file line number Diff line number Diff line change
Expand Up @@ -4,7 +4,7 @@ Resonator punchout

With the resonator spectroscopy at high power we found the bare resonator frequency
(also called high power frequency), but this is not the frequency that will be used to perform measurements.
We need to find the frequency in the low power regime, where the resonator is actually coupled
We need to find the frequency, where the resonator is actually coupled
to the qubit. To do that, we first have to find the correct amplitude of the readout pulse.
This experiment can be initially performed with a VNA, to check that everything is
working and to obtain a rough estimation of the parameters to be used by the control devices.
Expand Down Expand Up @@ -92,7 +92,7 @@ to reach any sensible result. To be sure that, at the given pulse amplitude, we
in the transition regime, we can repeat the standard resonator spectroscopy with a finer
scan, checking if the peak is Lorentzian.
A resonator spectroscopy is also useful to better check the resonator frequency at low
power. We can alse write down the maximum value of the peak.
power. We can also write down the maximum value of the peak.
Since we are not interacting directly with the qubit, we are effectively measuring the
amplitude of the ground state and, from now on we will not change the resonator frequency,
so we expect to always measure this amplitude for the zero state. Here it is
Expand Down

0 comments on commit e473c83

Please sign in to comment.