CHANGES TO DRAFT 2 dated january 6

This page last updated on february 23

My answers to your comments are in blue, I do not master completely the fonts…

 

 Dirk's comments

 Paolo's comments

 Frederic's comments

 John's comments

 Steve's comments

 

1- Dirk's comments:

Page 1 Section 1 Paragraph 7:

"[...] showing an excellent agreement."

c'est plutot quelque chose qui doit aller dans la discussion de l'erreur systematique. J'effacerais ces 4 mots.

OK==>done

Meme Paragraph:

"A comparison sample ...."

j'ai un petit mal avec cette phrase, je trouve mieux:

"EXCALIBUR was used to generate events with colour reconnection following the ansatz of ....."

OK==>done

Page 2 Paragraph 3:
"[...] between LEP1 or LEP2 data and Monte Carlo."

je propose:

"[...] between data and Monte Carlo."

OK==>done

Phrase suivante: pas de "final"

OK==>done

Page 2 Section 2.2 Paragraph 1:

"As the electron and muon ..."

je trouve que c'est trop tot, donc je propose "delete" ou de le mettre au debut de 2.2.3Results

The layout of this section is now changed according to John's propositions, see below. This sentence is not needed anymore==>delete.

Page 3 Section 2.2.2

"[...] the energy of the higher energy of the two quark jets [...]"

difficile a digerer, c'est mieux comme ca:

"[...] the energy of the most energetic quark jet [...]"

OK==>done

Page 4 Paragraph 3:

"[...] cut on energy around the beam for tvqq events."

pour eviter des commentaires de Wasserbaech/JFG/Patrick

"[...] and by the uncertainty introduced by the cut on energy detected close to the beam axis in the tvqq analyses."

OK==>done

Page 6 Par 2:

"[...] obtained assuming lepton universality only is:"

j'aime mieux:

"[...] obtained assuming only lepton universality is:"

OK==>done

Page 6 Section 4:

"[...] adding together the data samples collected at [...]"

plutot

"[...] combining the data samples collected at [...]"

OK==>done

Dernier commentaire: je trouve que la discussion de la deviation de la mesure par rapport a ce qu'on a mesure et les trucs DPA IBA doivent aller dans la section 3 au moment on donne des resultats et pas dans les conclusions.

OK==>done

 

2-Paolo's comments:

sect 1: page 1:

-par 3: Rather than the "measurement of cross-sections ..." I would say the "separation of WW events in all possible W decay channels allows the determination of W br...". The measurement of the total ee-->WW reaction is another test of the SM, separate from the BR measurements (if you want to say it so, before the comment on the br mesurements).

OK==>done

-par 7 (line3): "an excellent agreement" can we replace "excellent" with a quantitative xsection or efficiency difference. (or just say it is taken into account in the syst)

OK==>done

-last line: "which, for sqrt(s)=....[18], gives sigma_WW="

OK==>done

sect 2.1

-par 2: "Beam related...the beam" Sounds unclear. What about "Beam related background and detector noise that is not simulated in Monte Carlo events, affect the efficiencies of the cut which has the purpose of removing gamma-gamma events depositing energy ...the beam"

OK, much better!==>done

-par 4: "Events are classified into six di-lepton channels making use of electron and muon identification criteria. A jet or a track is classified as a tau either if no lepton identification is fulfilled or if the identified lepton has an energy lower than 25 GeV."

OK, I buy it!

sect 2.2

-par 1:"Similary to the lower energy measurements three selection procedures are applied.One selection is optimised for WW events with an electon or a muon, and requires an identified (remove energetic!) electron or muon track. The other two are designed to select other tvqq events, based on ... events. As the ... selections select efficiently tvqq events with leptonic tau decays, and the tau selections select also e/munuqq events, a reclassification of selected events is finally performed."

OK for first part, second part removed as layout of this section is changed (same comment as for Dirk)

sect 2.2.1 2.2.2 2.2.3

The probability paragraph in the results section is misleading: the prob is built ONLY for the e/mu selection and NOT for the tau ones . The e/mu analysis selects only events with electrons or muons, but the related e/mu prob is in fact separated in e-mu-tau components where the tau component accounts for leptonic tau decays (tau->e,mu nu nu).

This is not true anymore in Ann's analysis!

--Move the beginning of par 2.2.3 "The probability for ... (Fig1)." to the end of par 2.2.1 .

OK, this is also required by John

Change "from a signal process..." to " from each of the three evqq,mvqq or tvqq signal processes...".

OKè done

I don't know exacly how the selection has been finally applied but there should be a general cut on the total lvqq probability like Prob(lvqq)>0.40 {Prob(lvqq)=prob(evqq)+Prob(mvqq)+Prob(tvqq)} to select all events. After the 3 three e-mu-tau prob components should be used only for reclassification purposes.If this is what is done we should try to state it . The global Prob(lvqq) should be stated in the 2.2.1 par and the reclassification business with partial Probs in par 2.2.3 .

It is not done like that

-page4 line3:"This classification improves .." --> "This classification reduces the electon-tau and muon-tau correlations (section 4)."

OKè done

-sect 3. last par: Bleah. sigma_WW as a simple sum is not nice !

Ok we had a lot of discussions about this ... but my personal taste is still the same. Let me say again that such a summed total xsection is built violating the consistency of W BR within the 3 samples. It is not bad because it does not have SM BR but because it just does not have a common hadronic/leptonic BR for the produced W-pairs at all.

And if we put together these 3 topologies we do need some common BR if we assume that all 3 of them come from W-pair decays. No?

I agree. For me the " simple " sum has no meaning.

3- Frederic’s comments

-Remove ALEPH 99-?... add CERN-EP

OKè done

INTRODUCTION- "...determination of the W branching ratios and, indirectly, the coupling of the W to cs pairs."

OKè doneSECTION 2.1- "...24 fb and is dominated by the MC stat. error in the subtraction of bkg and in the signal eff."

If I look at table 2 the main systematic errors are

MC stat, bkg normalization and beam bkg. I don't

understand what do you mean by signal eff.

These are stat error on efficiencies for lvlv events due to MC statistics. The MC stat line accounts for both background and signal MC stat error.

A general comment on the paper... you have chosen to mention

only what are the main systematic errors in each section.

The problem is that by looking at table 2 it is very

difficult in some cases to understand what is the meaning

of the error just looking at the tag in this table. Even

worse, nowhere is explained how in fact this errors have

been calculated, what actually has been done. This problem

is particularly relevant in section 2.3 for the 4q channel.

I think MC statistics can be understood.

The systematic error on the background due to normalization is 8.5fb, which divided by 0.64 gives 13 fb, as in table 2.

The error +-7 refers only to the background MC statistics Following Maria’s proposal, I suggest to write 131+-7(stat)+-8.5(syst). I think the beam background error is given : 8.2+-0.5% and does not need more explanation (it is not statistics limited, but there were discussions on how to weight these random triggers with instantaneous luminosity which would take some lines to explain).

However the text can be modified : " …and is dominated by the Monte Carlo statistical errors, the uncertainties on the background cross sections and the uncertainty introduced by the cut on energy detected close to the beam axis. "

- As you have decided to compare the result in section 2.3

with the SM predictions, why you don't do the same in sections

2.1 and 2.2? it would be nice to write a sentence after the

result with the SM prediction to be compared for the sake

of consistency.

OKè done

SECTION 2.2- "... and by the uncertainty coming from the cut on energy around the beam for tnqq events." Is this lepton isolation in table 2??? ... again the same problem: difficult to understand the meaning of the

errors in table 2 and what has been done to determine them.

No, this is tagged as " beam background ". It is the E12 cut and photon veto for lvlv and lvqq analyses, but there is no such cut for the 4q. However the beam background was also studied for the 4q channel. I could add a sentence like : " A model for local energy deposits due to beam background was obtained with random trigger events. Such deposits were then added to the simulated events to estimate their effect on the measurement.Another estimate of this effect was obtained by locking out from the analysis all energy deposits below a polar angle of 12 degrees. " This was done for lvqq and 4q channels.There were other estimates obtained by reweighting the probability distributions, the details of which I have forgotten : Anne Ealet is writing a Note on this.

We could simplify table 2 by merging "lepton isolation and probability discrimination" items into "background shape", thus in the same line as for the 4q. I leave it to the Ed Board.

- Same comment than in section 2.1 for the SM predictions.

OKè done

 

SECTION 2.3

- "... gives an identical result, but slighly less precise."

- why you don't simply quote the results mentioning that they

are compatible, in place of quoting 10 fb lower and 10% higuer

error? if you quote 6.74 +- 0.25, the reader does not need to

use the calculator...

OKè done

- "Small but significant disagreements appear for jet energy

distributions in particular. These differences can be propagated

at LEP2 by energy rescaling and all alter the shapes of the

background distributions in such a way that the resulting

W pair cross-section is lowered. The cross-section is

corrected upwards by 100 fb accordingly:"

I see that you have decided a radical change of philosophy

here, which is not what it was agreed in the W meeting. We have

agreed in the meeting that this 100 fb should be considered

as an aditional source of systematic error, and not a shift.

To conclude that this is a shift on the central value you

have to show that the error in this 100 fb is negligible. You

have to explain what are the variables not reproduced by the

MC, and if we decided our MC is not reproducing data we

have to be consistent with this in ALL our papers ( W mass

for instance). Are you sugesting that our MC does not reproduce

Jet Energies even after applying the Jet Energy corrections?

The studies done by Jullian suggest indeed that there are residual differences at the Z. ALL variables used in NN14, when looked at the Z, show these residual differences which, when transferred to LEP2 energies, all change the qqbar shapes in such a direction that the WW cross section goes up. This increase varies up to 90fb when btag and Ejetmin are reweighted

(see list below). You may notice that some of the variables are not included in the "jet corrections.

Finally I did not understand that we had decided not to correct in the meeting. I agree that the error on this effect is as large as the effect. However all variables go in the same direction. So the effect has a sign. Not correcting and putting a symmetric error is not right. Correcting with a symmetric error seems to me better. However you are right that with such a lousy determination of this effect, there is a danger that when we have more statistics or more insight, we get a different correction. If we correct for this paper, we have to also correct for the 1999 data for the coming winter conferences!

Conceptually I would prefer to correct, but it may be wiser to delay this for a final paper on lep2 cross-sections.

probe VS emin (+91 fb)

xgamma VS emin (+89 fb)

probe VS emax (+82 fb)

emax VS emin (+78 fb)

emax VS xgamma (+78 fb)

emin VS thjj23 (+77 fb)

emax VS thrust (+70 fb)

emin VS thrust (+69 fb)

emin VS emin2 (+68 fb)

emax VS sphe (+67 fb)

emin VS sphe (+65 fb)

emin VS echmax (+63 fb)

emin2 VS thjj23 (+63 fb)

emax VS emin2 (+62 fb)

emax VS thjj23 (+62 fb)

probe VS sphe (+59 fb)

thrust VS xgamma (+57 fb)

emax VS echmax (+56 fb)

probe VS thrust (+52 fb)

probe VS thjj23 (+48 fb)

probe VS emin2 (+47 fb)

emin2 VS thrust (+47 fb)

emin VS evis (+43 fb)

emin2 VS sphe (+42 fb)

sphe VS thjj23 (+42 fb)

emin VS thjj4 (+39 fb)

sphe VS echmax (+38 fb)

thjj23 VS echmax (+37 fb)

probe VS xgamma (+36 fb)

probe VS echmax (+35 fb)

xgamma VS echmax (+35 fb)

emin2 VS xgamma (+34 fb)

etc etc etc...

If, finally, you have decided this is a shift, then it is

not more a systematic error. This is in contradiction with

the next paragraph:

"The uncertainty on the variables used for the event

preselection cuts, and for the NN input is assessed by

changing jet directions and energies according to possible

residual differences between LEP1 Z data and MC..."

Here is Shan's explanation:

There is no inconsistency or double counting between what I got using Marumi's jet correction/smearing and what Julian got:

1) The jet correction and smearing from Marumi is based on 2 jet events at Z peak data. We know our MC can simulate

these events not too bad. So this smearing effect is small.

In 1999 data (192-202 GeV), the jet correction and smearing is even smaller than 1998 data (189 GeV).

So what Marumi did is mainly to check our detector performance based on the belief that our qqg generator has no big problem in

the simulation of 2 jet events at Z peak.

2) What Julian found is that when we force 2q events into 4 jets, the jet directions and energies are not well simulated

for both Z peak data and high energy data. This has little to do with the jet correction and smearing based 2 jet events.

So what Julian did is mainly to check the problem from qqg generator (may be mainly in the fragmentation).

However, it might not be easy to explain these clearly in the paper.

 

My personal opinion is: do not take this as a shift

but as a systematic error.

 

SECTION 3

OKè done

- Table 2 cannot be understood unless somewhere in the text is

explained what is the meaning of the tags, and what has been

done to compute the systematic errors. For instance, I'm afraid

that what is called FSI only corresponds to BE, and so on…

OK, I give some more details. (BE and CR are included)

SECTION 5

- I believe the discussion on the new calculations should fit

better in section 3, and to have in section 5 only a summary

of the results.

OKè done

REMOVE PRELIMINARY FROM ALL FIGURES

OKè done

 

4-John’s comments:

1) Abstract 3rd sentence:

Replace 'Under Standard....and decay' by something like

'Combining all final states and assuming lepton universality, the total

W-pair cross section is measured ....'

I do not agree to quote the lepton universality number for the cross section in the abstract as it is customary between LEP experiments to give the cross section assuming all SM branching fractions.

2) sect 1 page 1:

KORALW > KORALW version 1.21 (first time it is mentioned)

OKè done

3) sect 2.1 page 2:

The 3 main sources of syst error in the total

24fb are not clearly explained and referred to in Table 2. MC stats does not appear to account entirely for the 'background normalisation' error (this is 7fb in the text). Is 'MC stats' the error in the signal

efficiencies part of which comes from the 0.5% uncertainty in the random triggers? The 11fb 'beam bkgd' is not explained.

Please see my answers to Frederic on the same topic.

4) sect 2.2.1 page 3:

'With increased sqrt (s), the two W's..."

OKè done

Remove the sentence ' For this purpose the topology....'

OKè done

Is it true that the e/mu ID criteria are applied

AFTER the candidate lepton is chosen - seems quite inefficient?

Yes it is done this way. Another way would be to find an electron/muon and then take the one which maximizes pl**2(1-costheta). This is not equivalent to what is done. I think what is done is optimal. What do you think Paolo?

5) sect 2.2.3 page 3:

The 1st two sentences 'The probability for an

event....' and 'If an event is...' should be transferred to the end of

section 2.2.1.

OKè done

However, the second sentence can be re-worded: 'If the

probability is greater than 0.40 the event is kept in its corresponding channel otherwise it is considered by the tvqq selection.

This is now reworded after more precisions from Anne.

Then, it would be better to transfer the rest of the 1st paragraph

in section 2.2.3 to the end of sec 2.2.2

OKè done

6) sect 2.2.3

Starts with 'Table 1 gives......'

Remove 'combined' from 2nd sentence.

OKè done

Again the description of the systematics listed in Table 2 is not clear.

If 'MC stat' is really the error in the subtraction of bkgds it should be relabelled 'Bkgd subtraction'. The origin of the 'Beam bkgd' could be stated as well as the bkgd normalisation etc.

No, the 'MC stat' contains stat errors on efficiencies of signal (4f and cc3) and background. I have reworded somewhat. Maybe I could add something on Anne's reweighting.

7) sect 2.3 page 4:

Put an error on the the MC predicted number of evts (3593).

OKè done

8) sect 2.3 page 5:

I propose the following text to replace everything after the first paragraph:

'The cross section is extracted by means of a binned maximum likelihood fit to the full NN output distribution of data events where only the normalisation of the MC signal is allowed to vary. The mainly QCD background is kept fixed in shape and normalisation. The fit result is \sigma(WW>4q)=6.84+-0.23(stat) pb. (Note: no special spacing but simply embedded in the text). However, systematic studies at the Z show that small but significant discrepancies exist between data and MC in the description of hadronic 4-jet events(ref). They are in fact hadronic events forced to four jets

These differences are quantified using the 14 NN variables taking correlations and energy rescaling to 189 GeV into account. For example, Fig~\ref{Ejetmax} shows the effect of these adjustments in the case of the maximum jet energy distribution from 4-jet events at 189 GeV where the agreement with data is improved where the QCD background dominates. Assuming that these adjustments are independent of\sqrt(s), the MC events in the background NN distribution are reweighted accordingly. The corrected fit result is:

\sigma(WW>4q) = 6.89 +- 0.23 (stat) +- 0.13(syst) pb

If only events with a NN output > 0.3 are kept a value of ?+-? is found showing no significant bias due to the QCD background. The measured cross section is 2.5 standard deviations lower than the Standard Model expectation of 7.59 pb [21].

With a cut on NN>0.3 we find 6.85+-0.23 which is as good as using the full distribution. One may ask then why keep the first bins as they improve marginally the stat error but buy you quite some systematics! I find 2.3 std

The sources contributing to the systematic error are summarised in Table 2 ..........(Here we should relabelled 'qqgg jet' as 'background shape' changed to 90(?) MeV); relabel 'jet correction' as 'jet energy calibration';

point out that the bkgd normalisation assumes a 5%(?) variation in its

xsection; say what beam background is and separate 'MC stats' into

'efficiency' and '4f-cc03 correction'. So, the text should refer to the list of specific tags used in Table 2 where some clarification is needed.)

the 4f-cc3 correction is not available directly due to the fit to the NN distribution

Uncertainties with the WW generator have been evaluated...... coupled to the parton level of KORALW signal events (all in the same paragraph).

Several cross checks have been performed on the fit result to search

for possible biases arising in the selection and full simulation of the WW events. The previous version of the NN [1],..... from 6.65 to 6.77pb (stop at this point).

OKè done

9) sect 3 page 5:

I am in favour of our quoted result being derived from a fit to all the channel cross sections assuming lepton universality. If the precision gained in making this assumption is quite marginal then even this could be dropped. We might mention that the fit does not allow for any variation in the fraction of semileptonic WW's selected in the 4q channel.

We should then give the fit result obtained assuming SM branching ratios for comparison.

Anne has performed 3 fits with the following results:

SM Br

Universality only

No assumption

15.71 +/- 0.34

15.75+/-0.35

15.70 +/-0.35

All LEP experiments give the first number which has a precise meaning. I could see some interest in quoting the 3rd number which is obtained with the sum of Br=1 and assumes, for instance, that the same Br(qq) is used for evqq and µvqq.

 

10) sect 4:

Please check that the 4 total xsections used come from the 'simple' fits which don't assume anything other than lepton universality.

5-Steve’s comments

General comments:

  1. No hyphen in "cross section".

Done

2. Use an italic "s" in \sqrt{s}.

Done

3. For consistency, make the particle symbols "Z", "q", and "e" roman,

not italic.

I hope I got all of them now!

4. Be consistent: use $l$ or $\ell$ for leptons (including in subscripts,tables, etc.).

Found only the figures labels with this defect, will have to be changed when figures remade in b&w

5. Because there is only one appendix, it doesn't need a letter ("A").

E.g., try "\section*{Appendix: Hadronic...}".

Done

6. Move the figures and tables earlier so they appear near the places

they are mentioned.

I will do that for the final paper as I do not control this positioning. LateX does!

7. Do we really want to have italic table and figure captions? I don't see any advantage over roman; I guess it is a matter of taste. But it does have the disadvantage that half of the symbols and numerical stuff come out roman(!) and it would take some additional effort to make everything italic (including material that is now made roman by your macros). See table 1 and fig 3 for examples.

Done

8. Remove "PRELIMINARY" from all figures!

Done

9. Concerning colors in figures: I have no evidence that they will cause problems, but do we know for sure what the color figures will look like when they are rendered in black and white in the journal? I think it would be prudent to prepare truly black and white versions for the journal, and use the color ones for the preprint, etc.

I agree, will do this for the final version

Specific comments:

abstract, 3rd sentence: it is peculiar to say we measure the WW cross

section while assuming Standard Model WW production. I think we have

to be more specific about what we assume if we want this sentence to

make sense.

"assumptions for W-pair" (delete "the").

This sentence is now changed (see John's comment)

p 1.3:

No comma between "recorded" and "at".

next sentence: delete "the" between "in" and "t-channel".

"exchange, referred to as the CC03 diagrams~[7]."

next sentence: don't start a new paragraph.

"The measured cross sections are corrected for the difference, denoted

the "4f-CC03 correction", in the accepted cross sections for CC03

processes and all Standard Model four-fermion final states consistent

with W-pair decays."

two sentences later: "Comparison samples generated with".

Hyphen in "four-fermion".

"diagrams show excellent agreement."

Done

p 1.7:

How about "$\gamma\gamma$" instead of "gamma-gamma"?

Insert "and" between "production," and "BHWIDE".

next sentence: "which gives sigma_WW = blech for sqrt{s} = blech

and m_W = blech."

Use one pair of $$ around each of these equations in order to get the

spacing correct.

two sentences later: "of the cut that removes".

How about "$\gamma\gamma$" instead of "gamma-gamma"?

"depositing energy within 12degrees of the beam axis."

Done

p 2.0:

$8.2 \pm 0.5\%$ to get the spacing correct.

Done

p 2.2:

I don't think the "resp." is used in English. Until I joined ALEPH I had never read such a thing. [If you insist on using it, please write

"resp.\ " to get the spacing correct.]

Changed it

p 2.3:

"assigned to a tau" is a bit awkward.

changed

next sentence: "A maximum likelihood fit is applied to determine the

cross section for each individual fully leptonic...". [Each channel

has one cross section.]

OK

p 2.5:

How about this? "The results of the fit are" [no colon after "are" or

"yield".]

Period at the end of the last equation.

OK

p 2.8:

"The three lnuqq selection procedures".

two sentences later: "selections have sizeable efficiencies for taunuqq events, as does the tau selection for e/munuqq events, a reclassification is performed."

This is now out

p 3.1:

Remove "energy" between "sqrt{s}" and "the".

next sentence: "In this analysis, the selection of the lepton track

therefore relies...".

OK

p 3.2:

"theta_lh the angle of the track to".

two sentences later: "so that taunuqq events where...will also be".

two sentences later: no comma between "direction" and "that".

[If you want to keep that comma, you need to add one after "cone".

But I recommend no comma.]

Space between "5" and "GeV".

two sentences later: "were described in detail in previous papers~[1],".

"energy-based cut values".

Get rid of the spurious space after sqrt{s}.

OK done

p 4.1:

"Table~1 gives the efficiencies for each selection."

next sentence: no space between "0.5" and "%".

Done

p 4.7:

"network" instead of "net".

Done

p 4.8:

"where a four-jet event becomes a three-jet event".

next sentence: "contain" instead of "contains". [subjunctive!]

next sentence: hyphen in "Four-fermion".

Done

p 5.0:

"are described in the appendix and are" [no comma].

next sentence: "simplified with respect to that used".

"with fewer input variables".

Done

p 5.2:

Don't start a new paragraph at the sentence "The fit result is...".

OK

p 5.3:

"gives" instead of "has given".

"with an 18%".

two sentences later: "non" is not a word (in English!), so it must be

attached to other stuff, at least by a hyphen: "non-four-quark".

"output" is misspelled.

"are kept, yielding a value".

This sentence is now changed

p 5.5:

"propagated to LEP2" or "taken into account at LEP2".

next sentence: space between "100" and "fb".

next sentence: don't start a new paragraph.

two sentences later: "The uncertainties related to the variables".

No comma after "cuts".

"the NN input are assessed".

Spell out "Monte Carlo".

No hyphen in "miscalibration".

next sentence: "Uncertainties in the WW generator" [or "associated with"

or...].

"are evaluated by comparing".

Spell out "Monte Carlo".

Semicolon instead of comma after "samples".

"EXCALIBUR is also used to".

next sentence: "non-b".

OK

table 1 (p 6):

Caption: don't capitalize "data".

two sentences later: no space between "0.3" and the period.

The column headings (especially "qqqq") aren't centered above the numbers.

Units: don't write "in"; write "(%)" and "(fb)".

Don't let the \hlines hit the words in the first column (bottom few rows).

[I can provide TeXnical help if you wish.]

Thanks, I can't center qqqq

p 6.5:

"previous sections and uses the". [no comma]

next sentence: no colon after "is".

Use one pair of $$ around this equation.

next sentence: "of the centre-of-mass energy."

next sentence: "performed adding" is bad grammar.

OK

table 2 (p 7):

Caption: "error" instead of "errors".

In the table:

Don't capitalize "state interactions".

Spell out "Monte Carlo" and "identification".

OK

p 7.5:

"taunu versus enu or munu," is evidently a spurious sentence fragment.

Sure!

p 7.8:

Period at the end of eq 1.

Do we want to mention "to first order in alpha_s"?

I think it is evident from the formula.

p 7.9:

Make the "cs" roman in the displayed equation.

OK

fig 1 (p 8):

The vertical axis labels should be something like "Events / 0.04".

The vertical axis values are too close to the axis.

Use a symbol font for the axis values, in order to get minus signs

instead of hyphens.

There are too many tick marks and values on the horizontal axes.

(Don't need two ticks per bin or one value every 2.5 bins.)

The HIGZ fonts (in the keys) are UGLY!

The text in the keys is too small, as are the labels "a)", "b)", "c)".

I don't think Phys Lett will appreciate all the empty space in this

figure; if you stack the three parts with no space in between you can

save a lot of room. The aspect ratio of the plots could also be

changed so the stacked version doesn't come out too narrow when it

is placed in one column of the journal.

I will forward this to the picture makers!

Caption: "for the (a) enuqq, (b) munuqq, and (c) taunuqq selections."

two sentences later: combine sentences: "background contribution, the

dark shaded histogram..."

OK

fig 2 (p 9):

Needs a vertical axis label.

The vertical axis values are too close to the axis.

Space instead of hyphen in the horizontal axis label.

There are too many tick marks and values on the horizontal axis.

Caption: hyphen in "four-quark".

OK

fig 3 (p 10):

Can we use the same style (font, location of axis labels) as for the

other figures?

Space between "sigma_WW" and "(pb)".

Space between "E_cm" and "(GeV)". [How about sqrt{s} instead of E_cm?]

We use lower case "m" for mass elsewhere...

While you are at it, we could use a space before and after the "="

in the m_W equation on the plot.

Caption: remove the spurious spaces after "MeV/c^2" and "m_W".

Same comment as above

p 11.0:

"Using" is bad because the subject of the sentence ("cross section")

isn't using.

Hyphen in "W-pair" for consistency.

OK

p 11.1:

"New calculations with the double pole approximation (DPA)~[24] have

recently appeared, and two Monte Carlo programs, YFSWW~[25] and

RacoonWW~[26], are being developed."

two sentences later: no space between "0.5" and "%".

next sentence: "It is currently thought [believed] that the...".

No space between "2" and "%".

next sentence: "After adding" is bad. How about this?

"After inclusion of the data collected at centre-of-mass energies

of 161, 172, and 183 GeV, the hadronic decay branching ratio is

found to be blech%, [comma] which is used...".

Roman "cs" in that last equation.

OK

p 11.7:

Need more vertical space and no indentation before "Global event

properties".

I can't make it! (help!)

p 11.9:

"Confidence level" instead of "probability".

p 12.0:

Space between "WW" and "kinematics".

Do you really want a roman "WW"?!

Last two \items: "smallest" instead of "minimum".

OK

references:

general comments:

1. It is nonstandard to give the titles of published papers. (It

is certainly not part of the journal's specifications.) And when

you put them in italics, you get the same problems I mentioned at

the beginning. For example, in [1] we have "e+e-" with one italic

"e" and one roman.

I can see other ALEPH papers with the title in the references. OPAL and L3 do as you say. I can skip the titles easily!

2. Use a backslash to prevent a big inter-sentence spacing after

abbreviated words: Phys.\ Lett.\ B453.

3. Be consistent: bold or not bold volume numbers?

OK all bold

 

specific comments:

[1] Delete the 2nd and 3rd occurrences of "ALEPH Collaboration"--it

isn't necessary to repeat the author(s) if they are the same for

consecutive papers within one \bibitem.

Semicolon instead of period after "435".

[5] "...(1992) 305; S.~Jadach..."

Period at the end.

[17] Nucl.\ Phys.\ (Proc.\ Suppl.)

[18] Capitalize "Group".

Unlike a preprint, the web page will not necessarily still say

"80.39 GeV" in one month, one year, or 100 years, and the reader

will not be able to find out how the number was obtained (e.g.,

which experiments). I think we should refer to a real document.

I agree, I found the CERN-EP-2000-016 preprint. It only quotes 80.35 for the W mass not taking into account Fermilab results. As it is the only printed document I could find, we use this mass value as the reference.

[20] Remove the extra space after "e+e-". This paper is unpublished,

so it is OK to leave in the title, in my opinion. But we need to

have two italic e's in "e+e-"!

Comma after the title, and don't necessarily capitalize the next

word.

Refer to a contributed paper, not to an abstract. And say which

conference!

I find that this reference is not really needed!

[21] et al.,

[22] G.~Marchesini

[23] et al.\ (Particle

[25] Writing out four author names is pushing it. Five is going too

far! Use et al.

[26] Here we have the title in roman, with quotation marks. Be

consistent.

[27] Bohm instead of Bhm.

"...(1992) 29; B391 (1993) 483 (erratum)."

 

Added the mention that Jetset is used for hadronisation in section 1.

Changed branching ratios to branching fractions consistently

Added error to efficiency of semi-leptonic selection in section 2.2.3

Added stat and syst error to the background to be consistent with lvqq

Changed ref mW from 80.39+-0.42 to 80.35+-0.56