- My blog
- Post new blog entry
- Top bloggers
- Recent posts
Towards a Run 6 Pion Cross Section
Updated on Wed, 2009-08-05 16:24. Originally created by stevens4 on 2009-07-30 11:02.Here is an Introduction to Cross Section Calculation I wrote up to remind myself how we get from experimentally measured qu
Eta-averaged BSMD slopes
Updated on Thu, 2009-07-30 10:18. Originally created by wleight on 2009-07-30 10:18.The pdf slopeSummary_1_120.pdf has a plot of slopes vs. eta, with averages over eta, for both eta and phi planes.
EEMC simulation studies
Updated on Thu, 2009-07-30 09:47. Originally created by jwebb on 2009-07-30 09:47.EEMC simulation studies
Updated on Thu, 2009-07-30 09:47. Originally created by jwebb on 2009-07-30 09:47.Energy and pseudorapidity dependence of sampling fraction in the EEMC
Updated on Thu, 2009-07-30 07:46. Originally created by jwebb on 2009-07-30 07:46.Figure 1 -- Sampling fraction vs. incident energy for an electron normally incident on the EEMC. The fit is to a 3rd degree polynomial in x=log(E).
2005 Dijet Cross Section Figure
Updated on Wed, 2009-08-05 12:05. Originally created by mattheww on 2009-07-29 15:47.Attached to this post is a copy of the 2005 Dijet Cross Section Figure. The systematic analysis is not quite complete, but this figure shows approximately what it will look like.
30 GeV Energy particle energy deposit in FMS and FHC compare
I studied the 30 GeV n, p, pion0, pion+ and pion- energy deposit in FMS and FHC. The particles are shot from (0,0,0) to (100,0,850).
Virtual Machine note pad.
Below are various notes regarding Virtual Machines as I introduce myself to them. Most notes will likely be relevant to Xen and/or RHEL 5 -- my first reference source is:
Lambda decay vertex recreating through proton pion-
I looked at the Lambda decay into proton and pion- channel using FHC and FMS, and try to recreate the Lambda decay v
FGT thermal model
Updated on Mon, 2009-08-10 17:06. Originally created by jphw on 2009-07-28 14:04.I've just completed the first set of thermal model measurements, which have included two new channels: temperature measurements of the input and exhaust.