... | @@ -74,15 +74,31 @@ considerations: |
... | @@ -74,15 +74,31 @@ considerations: |
|
|
|
|
|
### What does the BCT measure?
|
|
### What does the BCT measure?
|
|
|
|
|
|
### Why is the BCT cabling delay so large?
|
|
The BCT is made of a toroidal magnetic core with a winding around it
|
|
|
|
that delivers a voltage when the beam goes through the center of the
|
|
### You have calibrated using an LHC beam. How do those measurements apply to the CNGS beam?
|
|
toroid. It's a bit like a conventional transformer, with the beam
|
|
|
|
playing the role of the primary winding and its effect being observed in
|
|
|
|
the secondary winding.
|
|
|
|
|
|
## Measurement set up.
|
|
### Why is the BCT cabling delay so large?
|
|
|
|
|
|
### How do you measure the neutrino speed?
|
|
There are no electronics near the beam pipe for radiation reasons. The
|
|
|
|
original mission of that BCT was to make sure the beam had the required
|
|
|
|
characteristics for CERN Neutrinos to Gran Sasso (CNGS) operation. Using
|
|
|
|
it as a means to provide a time-stamped acquisition for neutrino time of
|
|
|
|
flight experiments was an afterthought. In any case, the cable length
|
|
|
|
and the amplifier combined with the BCT still provide a bandwidth of
|
|
|
|
several hundreds of MHz so there is no appreciable distortion in the
|
|
|
|
waveform.
|
|
|
|
|
|
### How could you remove any systematics errors?
|
|
### You have calibrated using an LHC beam. How do those measurements apply to the CNGS beam?
|
|
|
|
|
|
### Is there anyone else measuring the neutrino velocity?
|
|
Lab measurements indicate that there is a variation in beam-to-output
|
|
|
|
delay with respect to transverse beam position. We measured an effect of
|
|
|
|
almost 10 ns for a 10 cm transverse displacement. But the different in
|
|
|
|
transverse position between an LHC beam and a CNGS beam is less than 2
|
|
|
|
mm. So this effect is not a problem. Also, for the purpose of measuring
|
|
|
|
BCT delay, the actual time structure of the beam is irrelevant. This is
|
|
|
|
why we chose the LHC beam, with its properly separated bunches that make
|
|
|
|
analysis of the delay much simpler.
|
|
|
|
|