Recent experiments show that Δy,an observable designed to detect the chiral magnetic effect(CME),in small collision systems(p+A) is similar to that in heavy ion collisions(A+A).This introduces a challenge to the exis...Recent experiments show that Δy,an observable designed to detect the chiral magnetic effect(CME),in small collision systems(p+A) is similar to that in heavy ion collisions(A+A).This introduces a challenge to the existence of the CME because it is believed that no azimuthal correlation exists between the orientation of the magnetic field(Φ_(B)) and participant plane(Φ_(2)) in small collision systems.In this work,we introduce three charge density models to describe the inner charge distributions of protons and neutrons and calculate the electric and magnetic fields produced in small p+A collisions at both RHIC and LHC energies.Our results show that the contribution of the single projectile proton is the main contributor to the magnetic field after averaging over all participants.The azimuthal correlation between Φ_(B) and Φ_(2) is small but not vanished.Additionally,owing to the large fluctuation in field strength,the magnetic-field contribution to Δγ may be large.展开更多
文摘Recent experiments show that Δy,an observable designed to detect the chiral magnetic effect(CME),in small collision systems(p+A) is similar to that in heavy ion collisions(A+A).This introduces a challenge to the existence of the CME because it is believed that no azimuthal correlation exists between the orientation of the magnetic field(Φ_(B)) and participant plane(Φ_(2)) in small collision systems.In this work,we introduce three charge density models to describe the inner charge distributions of protons and neutrons and calculate the electric and magnetic fields produced in small p+A collisions at both RHIC and LHC energies.Our results show that the contribution of the single projectile proton is the main contributor to the magnetic field after averaging over all participants.The azimuthal correlation between Φ_(B) and Φ_(2) is small but not vanished.Additionally,owing to the large fluctuation in field strength,the magnetic-field contribution to Δγ may be large.
