Read (too quickly) the paper from arXiv.
My first comment is that I'd strongly prefer the propagation time to be measured between two neutrino detectors, one at Cern and the other at Gran Sasso. Presently it's measured between a proton beam current detector at Cern and a neutrino detector at Gran Sasso. As the neutrino beam is 3km*3km wide at arrival, a small detector at the source would provide as many event there for a more direct comparison - err... IF the mu neutrinos can be detected with the same inefficiency as the tau neutrinos are, which I ignore to a high degree of precision.
GPS signals are jammed but many techniques, especially differential GPS, overcome it. From the comments in the paper, scientists there obviously know that better than I do and took care of these clock and position measurements, end of paragraph.
The signal from the proton beam intensity shows a decline instead of a steady plateau. Could it be that a fuzzy signal from the neutrino detector correlates better with the inclined reference if it's shifted forward, just as a result of the waveforms?
Now, things I'm easier with.
The 200MHz modulation of the proton beam brings no certainty at all to the discussed 30ns. If the slower beam current envelope, lasting 2µs, could be measured with 5ns certainty, then the 200MHz modulation would improve the correlation precision to about 10ps, which isn't the case here. The measurement relies only on the 2µs envelope.
I believe to understand that 200MHz is the frequency of the accelerator cavities, and modulate the beam intensity fully, something like 0% to 200% of the mean intensity. Though, the diagrams on page 6 show only +-15% modulation depth at 200MHz, so even though the beam current transformer and supposedly the acquisition device have a broader bandpass than 200MHz, something attenuates the 200MHz component, be it a medium to long cable or something else.
Unfortunately, the thing that attenuates at 200MHz is probably dispersive, that is, it introduces a propagation delay that depends on the frequency. A cable for instance delays precisely at 200MHz by its known speed but gets slower at lower frequency as its series resistance adds to the inductance, and here we're talking about 30ns precision over a 2µs waveform with 500ns transitions - that is, the measurement results from a rather strong statistical interpolation.
Hence I wish this possible dispersion be eliminated. Fortunately, this looks easy, thanks to the 200MHz modulation. It just needs to suppress the DC and LF components of the signals, both at Cern and at Gran Sasso, and compare only the tone-burst envelope. It needs a filter around 200MHz, a broad one like 100-300MHz to minimize its propagation time. Over this favourable and limited frequency band, all cables and transformers will show their normal delay. Maybe these filters can be made by the same piece of software, introducing the same delay. The correlation will oscillate at 5ns, but this is meaningless. The envelope of the correlation will be meaningful and independent of LF dispersion.
Marc Schaefer, aka Enthalpy