Particle Production in Strong Electromagnetic Fields in Relativistic Heavy-Ion Collisions

Figure 8

Energy loss per unit length by quarks moving in constant external magnetic field as a function of (a) 𝑝_𝑇 at RHIC at 𝜂=𝜑=0, (b) 𝑝_𝑇 at LHC at 𝜂=𝜑=0, (c) azimuthal angle 𝜑 with respect to the reaction plane for 𝑝_𝑇=5 GeV and 𝜂=0,1, and (d) fractional energy loss versus rapidity 𝜂 at 𝑝_𝑇=5 GeV and 𝜑=0,𝜋/4.

(a)

(b)

(c)

(d)