[esa-t474] more comments, chapter 3
Bino Maiheu
bino at hep.ucl.ac.uk
Thu Sep 27 14:52:24 BST 2007
Hi Mark,
Here are some more comments and suggestions from me on chapter 3 of the
paper.... Along with some general comments as well that i just put up
for discussion.
I'll send some more comments tonight and tomorrow for the rest of the
chapters.
Cheers,
bino
Some general comments
---------------------
- General question to the ATF people amongst you guys are there any
comments that were sent back to the nanoBPM paper relevant for this
paper ?
- Do we want photographs...in the paper ? I personally feel like not.
- Need to address why RF cavity BPMs are preferable to e.g. strip line
or buttons or our purposes. I think that just quoting the fact that
they can achieve higher resolutions is not enough. In other words,
why do RF cavities tend to have a higher resolution ? Is their
sensitivity ( V/mm ) typically higher than strip lines or buttons ?
Maybe quote some numbers here ??? I don't really have any experience
in this to be honest.
- Check whether we use the equations in what is coming further. If
not, don't really seed the need to derive them all. Or alternatively
we can derive them, but then not just put them in, but we need to
comment a bit more on what they physically mean !!!
e.g. :
- eq 22,23 : comment that these equations effectively indicate
that position and tilt can be found by a coordinate
system rotation from the IQ plane
- suggest "scaling factor" -> "calibration scale" ??
Comments to chapter 3
---------------------
- line 252 : don't like title
suggest : "Theory of cavity BPMs"
or something like that
- line 254 : "... the dipole fields excited in a cavity..."
suggest : "... the dipole excitation induced by the beam in the
cavity..."
- line 257 : The "(x)", "(\theta)" and "(\alpha)" are in the wrong
place !
suggest : "the beam offset $x$ from the [...], the angle
$\theta$ of the beam trajectory and the rotation $\alpha$ ..."
and don't use brackets around the variables !
- line 258 : should cite as "[14,15]", not as [14],[15] -> check
latex manual
- line 260 : "($V(t)$)" -> "$V(t)$"
- line 262 : explicitely mention what you mean with tilt signal,
refer to $V_theta$ and $V_\alpha$, the word tilt signal
wasn't mentioned before...
- line 263 : what do you mean with "single" complex oscillator ?
- line 266 : "... and $\phi$ is the relative phase."
suggest : "... and $\phi$ it's relative phase."
- line 267 -> 272 : need to stress that the second down conversion is
done in software using a down mixing and filtering algorithm.
-> rises important question for the reader... why not mix down
to base band in hardware ? Need to answer this here !!!!
- line 273 : you already defined $\omega$ and $\phi$, do they have
the same meaning here ?
- line 277 : Why Gaussian ? ... I know it had to do with the
particular phase response of this filter.. need to check
exactly what the advantages were here ....
- line 278 : might want to chose different name for $t_0$, more like
$t_s$ or $t_{ref}$
- line 281 : get rid of 2x "in MHz", this is obvious, could quote
some typical values here, or refer to a later table...
- line 285 : "power envelope"... hmm, me don't like
- line 289 : "depended" -> "depends" ... this is still the case :)
- Figure 9. : Get rid of the arrows !!, looks awful !
Rearrange plots, all 3 next to each other
You didn't mention the "DDC" abbreviation anywhere
before. Define it in the text before referring to
figure 9.
- section 3.2.2 : too much usage of the word "frequency", read very
non fluently, suggest to rephrase parts
- equations 22,23 : I suspect that the tilt signal needs to be
orthogonal to the position signal, so
something like -sin(phi_IQ)*I + cos(phi_IQ)*Q
or something like that... need to check on
coordinate rotation !!!
- line 327 : "phase advance" normally used in storage ring lattice
context, replace by "phase difference"
- line 331 : "... change in calibration." - > "... change in
calibration scale."
- line 323-325 : Maybe mention that the phase dependence is linear
having the frequency difference $\omega -
\omega_{DDC}$ as slope.... donno ??
- table 4 : Would not call this precision.
typo in table as well
Not sure whether or not this table is useful ? What do we
want to prove here ? Is it not enough to quote the RMS
noise of empty pulses ? If you want to check errors
coming from the DDC algorithm i think we need to do it on
simulated waveforms and compare generated amplitudes and
phases with DDC'ed ones.
-> goes for lines 345 -> 352
- line 358 : already defined $x$ etc... no need to redefine.
--
!!!!!
( o o )
@ -- Bino Maiheu, Dr. ;) ---------oOO----(_)----OOo------- @
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