DIS: What is important
This page describes the important considerations to experimentally realize the physics program described in the EIC White Paper.
The measurements that comprise the EIC physics program divide into four classes of scattering reaction:
The following sections discuss the requirements placed on a DIS detector in order to measure these reactions, and how each reaction relates to the key physics measurements at an EIC.
Inclusive scattering
Inclusive DIS refers to measurements that involve only the scattered lepton.
The requirements for detecting the scattered lepton are critical, and remain the same for semi-inclusive, exclusive and diffractive reactions, as the scattered lepton defines the parton kinematics (through x and Q2) for all reaction types. Key Physics MeasurementsBelow is a list of measurements from the EIC WP are that rely only on the measurement of the scattered lepton. These measurements are based on the polarised spin structure function g1 and the unpolarised structure functions F2 and FL. ep:
eA:
Kinematics describing inclusive DISDetails of the scattered lepton kinematics can be found here Detector Design Requirements following from inclusive DISDetails of the requirements imposed on detector performance can be found here Performance Studies for inclusive DISDetails can be found here |
Semi-inclusive scattering
Semi-inclusive DIS (SIDIS) involves measuring one or more (in the case of correlation measurements) final-state particles in addition to the detection of the scattered lepton. A schematic view of a SIDIS event is shown in the figure.
All the requirements for detection of the scattered lepton apply in SIDIS as for inclusive reactions. However further requirements are posed by the need to detect the final state hadron(s). A measured hadron is typically characterised by its transverse momentum, pT, with respect to the virtual photon (not the incident beams) and its energy fraction, z; see the section on kinematics for further details and definitions. Key Physics MeasurementsThe following is a list of measurements that rely on the measurement of a hadron or hadrons in addition to the scattered lepton. References are given to the relevant sections of the EIC white paper (WP) for further details. ep:
eA:
Kinematics describing semi-inclusive DISDetails of the kinematics of the hadronic final state in coincidence with the scattered lepton can be found here Detector Design Requirements following from semi-inclusive DISDetails of the requirements imposed on detector performance can be found here Performance Studies for semi-inclusive DISDetails can be found here |
Exclusive scattering
Exclusive DIS describes measurements that involve the measurement of the scattered lepton, the scattered proton (either intact or dissociated into a hadronic final state) and the reconstruction of the final particle produced in the interaction.
For low-x events the proton scatters at such a small angle that very often it escapes the main detector through the beam pipe hole, and its measurement requires forward detectors ("Roman Pots") installed along the beam pipe. The reconstruction of the produced particle, such as a photon or a vector meson decaying into leptons, imposes extra detector requirements, mainly on tracking and calorimetry. The accelerator and detector requirements are discussed on the EIC WP chapter 2.4.4 A note on terminology:
Key Physics MeasurementsBelow is a list of measurements from the EIC WP are that rely only on the reconstruction of the entire final state. ep:
eA:
Kinematics describing exclusive DISDetails of the kinematics of the final state and the forward scattered proton and nuclei in coincidence with the scattered lepton can be found here Detector Design Requirements following from exclusive DISDetails of the requirements imposed on detector performance can be found here Performance Studies for exclusive DISDetails can be found here |
Diffractive scattering
Hard diffractive events, e(k) + N(p) → e′(k′) + N(p′) + X, are events where the proton/nucleus remains intact and the highly virtual photon fragments into a final state, X, that is separated from the scattered proton/nucleus by a large rapidity gap without any particles.
These events are indicative of a color neutral exchange in the t-channel between the virtual photon and the proton over several units in rapidity. A note on terminology:
Key MeasurementsBelow is a list of measurements from the EIC WP are that use diffractive events. ep:
eA:
Kinematics describing diffractive physicsDetails of the kinematics of the final state and the forward scattered nucleus/proton in coincidence with the scattered lepton can be found here Detector Design Requirements following from diffractive eventsDetails of the requirements imposed on detector performance can be found here Performance Studies for diffractive eventsDetails can be found here |