"Nuclear Stopping and Rapidity Loss in Au+Au collisions at ~s = 62.4 GeV"

Phys. Lett. B677, 267-271 (2009)

• Tables of data for fig.1-fig3
  
  
• Tables of data for fig.4 3 datasets
  
  
• Tables of data for fig.5 3 datasets
  
  
• Figure 1: Spectra of idented protons and anti-protons for y ~ 0, y ~ 0.65, y ~ 2.3 and y ~ 3 respectively. The solid drawn lines are the fit functions used to determine the yield. Vertical bars show statistical errors only
  
• Figure 2Top: rapidity densities of protons and anti-protons. Bottom: rapidity densities of net protons. The statistical errors are smaller than the marker sizes. The vertical brackets shows the estimated systematic errors due the extrapolation of yields, and the horizontal bars indicate the width of the rapidity interval for each data point. The histograms are from HIJING/BB(v2.1).
  
• Figure 3Rapidity losses for heavy systems (Au,Pb) from AGS, SPS and RHIC as a function of beam rapidity. The solid line is a fit to SPS and RHIC data, and the band is the statistical uncertainty of this fit. The LHC beam rapidity is y = 8.67. The dashed line is a linear fit to AGS and SPS data from [16]. The lower rapidity points from NA49 are preliminary data from [17].
  
• Figure 4 The top left panel shows (1/Npart /2)dN (P-Pbar)/dy vs. y ~ yb for SPS and RHIC energies. No scaling is observed. The three other panels show data from SPS and RHIC drawn together with the ~target~ net-baryon contribution from [21]. The triangles represent data from NA49, the squares BRAHMS data from 62 GeV and the circles BRAHMS 200 GeV data.
  
• Figure 5 Projectile net-baryon rapidity density from SPS and RHIC after subtraction of the target net-baryon contribution(see Fig. 4)