Exploring EIC Detector Concepts Exploring EIC detector concepts

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Exploring EIC Detector Concepts Exploring EIC detector concepts Rik Yoshida Temple EIC UG Meeting

Exploring EIC Detector Concepts Exploring EIC detector concepts Rik Yoshida Temple EIC UG Meeting 11/30/17

What this meeting is about • From past experience: after its establishment, the EIC

What this meeting is about • From past experience: after its establishment, the EIC laboratory will likely solicit detector proposals from the community. • Existing detector concepts will certainly play a major role in this process. • However, detector ideas will, and should, develop in the coming years. In the end, the detector(s) we will build—in my view—will be very different from the current concepts. • There is plenty of scope for new ideas and contributions—from specific sub-detectors to entire detector concepts. • I’ll compare the existing detectors first: they are based on the same concepts • Then I’ll present one way of rethinking the EIC detector. • There are likely many other ways of rethinking the detector. . the idea is to stimulate your thoughts for the discussion following—and also tomorrow. EIC Detector Concepts 2

Current Reference Detectors Jefferson Lab Concept • Vertex detectors: silicon pixel/strip • Tracking: TPC,

Current Reference Detectors Jefferson Lab Concept • Vertex detectors: silicon pixel/strip • Tracking: TPC, Drift chambers (streamer tubes? ) supplemented by GEM, Micromegas • Calorimetry: PW 0 in certain areas (electron direction, hadron direction (pi 0/e)). Sampling calorimeters elsewhere. • Particle ID: DIRC, RICH, TRD? , Hadron-blind detector, Timing (Argonne) EIC Detector Concepts 3

Far-forward Detection Extended detector: 80+ m Roman pots with position sensors. Zero Degree Calorimeter

Far-forward Detection Extended detector: 80+ m Roman pots with position sensors. Zero Degree Calorimeter EIC Detector Concepts 4

Exploring different detector technologies. . Time-of-propagation Counter (TOP) Straw tube central tracker DIRC alternative

Exploring different detector technologies. . Time-of-propagation Counter (TOP) Straw tube central tracker DIRC alternative PANDA TRD alternative Belle II (Charles Hyde short report ) Other ideas? Silicon TRD (Julia Furletova short report) EIC Detector Concepts Can we do more? Different philosophy in designing the whole detector? 5

Hadron colliders and the partonic center-of-mass system X 1 X 2 Heavy Ions (both)

Hadron colliders and the partonic center-of-mass system X 1 X 2 Heavy Ions (both) Highest Pt Events (Central) b quarks (Forward) EIC Detector Concepts X 1/X 2 determines where the final state goes. 6

What about EIC: are we optimized for the physics we want to do? Electrons

What about EIC: are we optimized for the physics we want to do? Electrons EIC Detector Concepts Struck quark 7

Low-x events at EIC Highly asymmetric collision at the parton level Eelectron_beam Since x

Low-x events at EIC Highly asymmetric collision at the parton level Eelectron_beam Since x 0, energy is tending to 0 at x = 10 -4 -5 Beam Energy ~10 Ge. V Parton energy ~ 10 Me. V Where does the final state go? EIC Detector Concepts 8

Final State Configuration for EIC Low-x events y ~ 1 (lowest x) electron energy

Final State Configuration for EIC Low-x events y ~ 1 (lowest x) electron energy < Ebeam Relatively high angle 10 Ge. V total “remnant”, p for diff. y ~ 0. 1 (same Q 2, somewhat larger x) 10 Ge. V total “remnant”, p for diff. electron energy ≈ Ebeam Low angle Left side is essentially fixed target kinematics EIC Detector Concepts 9

If we just wanted to do Low-x physics: Specialized detector CAL? Part ID? Dipole

If we just wanted to do Low-x physics: Specialized detector CAL? Part ID? Dipole Field No Field Proton (remnant) far forward det. Tracker/TRD We’re only reconstructing ~10 Ge. V worth of particles -and the diffractive forward state. EIC Detector Concepts 10

EIC High-x Configuration Highly asymmetric collision at the parton level (the other way) Parton

EIC High-x Configuration Highly asymmetric collision at the parton level (the other way) Parton carrying x. Eproton_beam Eelectron_beam Since x ->1, this is like the beam energy Parton energy ~100 Ge. V Electron Beam ~10 Ge. V Where does the final state go? EIC Detector Concepts 11

High-x measurements at EIC High-x uncertainties and LHC searches Dynamical Symmetry Breaking Pion/Kaon structure

High-x measurements at EIC High-x uncertainties and LHC searches Dynamical Symmetry Breaking Pion/Kaon structure at high-x and origin of mass Many other reasons to do high-x at EIC Detector Concepts 12

EIC Final State at High-x Need a very precise measurement to get x Most

EIC Final State at High-x Need a very precise measurement to get x Most of the time: Eelectron ≅ Eelectron_beam θ ~ Q 2 beamline E jet Eproton_beam This is hard to measure: a jet close to beam pipe This is why HERA measurement have big bins for high-x Can we do better at LHe. C and EIC? Yes. . in principle. . EIC Detector Concepts 13 =X

Improve Hadron side measurement? High Granularity Particle-flow Calorimeter No Field Dipole Field Pb-Sci calorimeter

Improve Hadron side measurement? High Granularity Particle-flow Calorimeter No Field Dipole Field Pb-Sci calorimeter electron Θ Proton beam electron beam Ejet Tracker/TRD Electron is “always” 10 Ge. V: use TRD to ID, use conventional calorimeter. Measure angle to get Q 2. Jet energy needs to be measured as well as possible for x: use particle flow. 30%/root(E)? If so 3 -5% resolution on x (0. 5 to 1) EIC Detector Concepts 14

Electron Solution? How well does the electron need to be measured? Tracking? “Dipole” PWO

Electron Solution? How well does the electron need to be measured? Tracking? “Dipole” PWO calorimeter? electron Θ electron beam Proton beam Ejet Tracking solutions? For L = 1. 5 m, B = 1 T and p= 10 Ge. V s ≈ 10 mm so 100 um measurement of s gives a ~1% measurement of p at 10 Ge. V. (Needs checking!) Tracker/TRD Calorimeter solution? Pb. W ~ 3%/√E and 1 -2% constant term? Absolute calibration? Difficult but not impossible? EIC Detector Concepts 15

“Caldwell Detector” 2004 Proposal for Lox-x/High-x detector for EIC https: //arxiv. org/pdf/hep-ex/0407053. pdf EIC

“Caldwell Detector” 2004 Proposal for Lox-x/High-x detector for EIC https: //arxiv. org/pdf/hep-ex/0407053. pdf EIC Detector Concepts 16

Low-x/High-x detector for EIC (second interaction point? ) PWO Part ID Proton (remnant) far

Low-x/High-x detector for EIC (second interaction point? ) PWO Part ID Proton (remnant) far forward det. VXD? Tracker/TRD Probably could be built inexpensively Dipole Field Background rejection? How does the electron beam get through the dipole field? ~2 Tm EIC Detector Concepts 17

Specialized detectors at 2 nd interaction point? Or perhaps improve a general detector using

Specialized detectors at 2 nd interaction point? Or perhaps improve a general detector using high/low-x detector concepts? EIC Detector Concepts 18

LHe. C Detector LHe. C detector adds the central and high/low-x detector together. Can

LHe. C Detector LHe. C detector adds the central and high/low-x detector together. Can we do the same at the EIC? EIC Detector Concepts 19

Adding High/Low-x Enhancement to the main detector? HCAL dipole solenoid EM VTX +Tracking EM

Adding High/Low-x Enhancement to the main detector? HCAL dipole solenoid EM VTX +Tracking EM TOP GEM Tracker HCAL EIC Detector Concepts 20

A Couple of Obvious Issues Can we live with the smaller central tracking volume?

A Couple of Obvious Issues Can we live with the smaller central tracking volume? Can we get the electron beam though the dipoles? For L = 0. 5 m, B = 1. 5 T and p= 10 Ge. V s ≈ 5 mm so 50 um measurement of s gives a ~1% measurement of p at 10 Ge. V. Mg. B 2 Shield Prototype Statera et al. Doesn’t sound impossible. EIC Detector Concepts 21 Stony Brook Magnetic Cloak N. Feege et al.

Discussion • Detector development for EIC is really just starting. • I just discussed

Discussion • Detector development for EIC is really just starting. • I just discussed one different way of thinking about the requirements of the EIC detector than has been done so far. • Probably there are many other ideas that should be brought up and discussed. -At the level of sub-detectors, detector technologies, etc. -But also at the detector concept level. • Availability of the 2 nd interaction point should be kept in mind. -A general detector with different philosophy? -Specialized detector(s)? • What are your ideas? • What is the best way to develop these ideas in the Users Group. -Working groups? How should they be organized? EIC Detector Concepts 22