Received: from FNAL.FNAL.Gov by b0ig16.fnal.gov via ESMTP (950413.SGI.8.6.12/940406.SGI) for id KAA09550; Sat, 1 Apr 2000 10:44:55 -0600 Received: from pcnometh1.cern.ch ([137.138.242.137]) by FNAL.FNAL.GOV (PMDF V5.2-32 #36665) with ESMTP id <01JNPVX2EUPU0014S1@FNAL.FNAL.GOV> for sgeer@b0ig16.fnal.gov (ORCPT rfc822;sgeer@fnal.gov); Sat, 1 Apr 2000 10:44:55 -0600 CDT Received: from localhost (abueno@localhost) by pcnometh1.cern.ch (8.9.3/8.9.3) with ESMTP id SAA29385; Sat, 01 Apr 2000 18:44:54 +0200 Date: Sat, 01 Apr 2000 18:44:54 +0200 (CEST) From: Antonio Bueno Subject: comments to Nufact document To: sgeer@fnal.gov Cc: Andre.Rubbia@cern.ch, campanel@pcnometh3.cern.ch Message-id: MIME-version: 1.0 Content-type: TEXT/PLAIN; charset=US-ASCII Dear Steve Geer, please find below the comments and impressions I have about the "Physics at a Neutrino Factory" draft you have successfully edited. First of all, I congratulate you for the impressive and outstanding effort you've done in order to produce this document. It conveys in a most remarkable way the physics case at a neutrino factory. A few comments are due: -Inside the author list M. Campanelli is referenced as ETH Honggerberg while A. Rubbia and myself are assigned to the Institute fur Teilchenphysik at ETHZ. The correct reference, for the three of us, to our institution would be: Institut f\"ur Teilchenphysik, ETHZ, CH-8093, Z\"urich, Switzerland. >> done -Page 12, Table 1. Rates are given in kt-yr for nu_mu CC and anti-nue CC for different baselines and energies assuming 10^20 mu- decays. I understand that in order to be consistent with the numbers quoted in the table, all of the assumed 10^20 muon decay in the straight section pointing to the actual detector location. This implies that 2 x 10^20 muons are circulating in the ring. On the other hand, if only 10^20 muons are stored in the ring, the quoted rates should be divided by a factor two. In order to avoid misunderstandings and inconsistencies I think that in the caption should be clearly stated the number of muons circulating in the ring and the number of useful decays corresponding to the quoted rates. >> We can only really talk about the number of decays in the >> straight section ... the relationship between that and the >> number of muons in the ring depends on the ring design. >> To be clear we have updated the table caption to say numbers >> correspond to 10^20 "useful" decays. -Page 21, oscillation formula for nu-mu to nu-tau conversion in the one mass scale approximation is wrong. The amplitude of the oscillation in formula number 30 should read: \sin^2 (2\theta_{23}) \cos^4 (\theta_{13}) while in the paper is written \sin^2 (2\theta_{13}) \cos^2 (\theta_{13}) >> fixed -Table 5 in page 35: For the scenario labeled IB1, it is quoted that ICANOE cannot detect nu-mu to nu-e oscillations. We considered this is not correct, since the studies we performed for the ICANOE proposal showed that for a mass difference of 0.4 eV$^2$ and sin^2 2\theta_{LSND} = 0.025 (in fact quite similar to your assumptions for scenario IB1), we expect a large electron appearance signal at energies below 30 GeV when compared to background expectations due to the natural nu-e beam contamination. >> done - Page 45: reference to figure where a nu-e CC event, as detected by ICANOE, is shown. The figure itself is assigned number 20, while in the text is referred as Figure 3.4.2 >> done Also in this page the last setence reads: Electrons and photons can be identified event by event and their energies are measured ... I think it should better read: Electrons and photons can be identified and their energies are measured ... >> done -Page 46: The paragraph refering to the dimensions and active mass of the ICANOE detector should be removed, since it gives the baseline design for an ICANOE detector at the CNGS beam and therefore it is incosistent with our assumptions for the physics case at a neutrino factory, where an ICANOE detector with 10 kton fiducial mass was considered. >> Rather than remove this text it would be better to update >> the numbers to correspond to the 10 kt simulated. If we >> could get the updated numbers that would be great ! - Table 8, page 56, gives angular resolutions for the muon and hadronic shower that are not consistent with the parameterization we used in our studies. In fact we used an angular resolution of 130 mrad / sqrt(p) for each hadron and the muon >> done -Page 72: First setence reads: Fig 38 for a 10kton ICANOE ... in which there are 10^20 mu^+ decays followed by 10^20 mu^- decays. This is inconsistent with fig 38 where the sensitivity on theta_13 is shown for 10^20 and 10^21 muon decays of each polarity. Therefore the end of the setence should be erased. >> My master copy of draft 1 doesnt seem to have this for the fig. 38 >> caption ... so Im puzzled. Perhaps you can look at Drfat 2 and see >> if the problem still persists, and let me know. - Finally, page 122, reference 74 is written M. Campanelli et al., in preparation. I think that the proper reference to our work should read: A.Bueno, M. Campanelli, A. Rubbia, "Physics potential of an ICANOE-like detector at a neutrino factory", in preparation. >> done -----------------------oooooOOOOOOOOOOOOOOooooo----------------------- Thank you very much in advance for taking into account the comments and considerations I wrote. Best wishes, Antonio BUENO VILLAR CERN Inst fur Teilchenphysik CH-1211, Geneve 23, Suisse ETH-Honggerberg, 8093 Zurich e-mail: abueno@pcnometh1.cern.ch phone: 41-22-767-1793