From evans@nevis1.nevis.columbia.edu Fri Aug 7 03:01:04 1998 Date: Fri, 7 Aug 1998 09:31:18 -0400 From: Hal Evans To: Horst Wahl Cc: Hal Evans Subject: comments on Physics Section Resent-Date: Fri, 7 Aug 1998 9:32:55 -0400 (EDT) Resent-From: wahl@FSHEB1 Resent-To: wahl Hi Horst, I looked over your draft of the physics section of the report to the PAC. It looks quite good - and addresses all the points I think we should be making. I have a few suggestions for improvements - but they are mainly cosmetic. If you don't think that any of them would be useful, don't bother putting them in. *** Section 1.2.2 (page 2): - phi0 should be defined for b<>0. You could add something like: "... B is the impact parameter [and phi0 is phi at the point of closest approach of the track to the nominal beam line.]" - It might also be worthwhile mentioning that phi(r) is an approximation and point out under what conditions it holds. *** Et/Pt for electrons at L2 (page 4): - Was 13%/sqrt(E) used as the L2 electron energy resolution as in Fig. 13? (This seems quite good to me for a L2 number, by the way). It should probably be stated. *** Section 1.3 (page 5) - Would it be worth adding to the list of benefits of the STT that it could provide stability against unforseen backgrounds? In the case where background conditions are significantly worse than predicted the signal to background behavior of STT triggers could decrease less sharply than normal triggers. I think that this is the reason why John's WH0 studies have more optimistic conclusions than Doug's SUGRA 4-b results. Doug only looks at points of high signal efficiency and low backgrounds - while John considers a broader eff/bgrd set. Section 1.6 (page 9) - If I remember correctly, the current Higgs limit from LEP as reported at ICHEP 98 is something like 89 GeV (rather than 75 from last year). Another study of the final LEP reach has also been done (and was presented at ICHEP). It indicates that the final LEP Higgs reach will be around 105 GeV. Table 5 (page 11) - What does TT mean? Is it the number of tracks with Pt>X? If so, perhaps it should be called Trks. Section 1.8 (page 13) - We should probably use l+l- instead of mu+mu- in the rare decay mode list to be as general as possible. ***** Table 11 (page 15) - Where do the background cross-section and eff1 come from? It might be clearer to quote the total background cross-section and eff1 from the trigger rejection factor, if this is possible. Reference 26 (page 19) - Refer to ICHEP 98 talks. Peter Macnamara gave the LEP Higgs talk and Daniel Treille gave the searches summary. Figure 13 caption (page 23) - "...z-vertex [assumed to be] at zero..." That's all for my comments. I hope that they're useful. As I mentioned before, I'll be out of contact for the next two weeks. I'll return on the 24th of August. Best Regards - Hal ^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v | Hal Evans | | evans@nevis1.columbia.edu | | Physics Dept. Nevis Labs | | Columbia University PO Box 137 | | 550 W 120th Mailcode 5215 136 S Broadway | | New York, NY 10027 Irvington, NY 10533 | | Tel: (212)854-3334 (914)591-2815 | | Fax: (212)854-3379 (914)591-8120 | v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^v^