Light Dark Matter experiment

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Light Dark Matter experiment Joshua Hiltbrand, University of Minnesota on behalf of the LDMX Collaboration TeVPA 2017 7-11 August 2017

A Thermal Relic Plentiful evidence for dark matter! Assuming DM has thermal origin Constrains viable mass window Sets minimum annihilation cross section Freeze out occurs Observed density 2

Looking for Light Dark Matter Amazing direct detection work has been done to explore WIMP phase space! LDM regime largely unexplored, well motivated However, SM forces cannot give observed matter density New, light forces must be present Vector mediator (dark photon) a simple, but predictive model 3

Reaching LDM Thermal Targets Current Constraints Current Constraints ~ 1010-1020 ~ 102-103 Relativistic nature of accelerators wipes out velocity dependence Significant velocity dependence for direct detection cross section leaves some targets out of reach Thermal targets are within reach! 4

LDM Accelerator Searches To maximize LDM yield, mediator production must be maximized! Largest cross section for production realized via dark bremsstrahlung Can also be off-shell 5

The Light Dark Matter experiment LDMX is an electron fixed-target, missing momentum experiment With 1016 electrons on target, LDMX can probe thermal targets over the MeV-GeV range Recoil Tracker DM Tagging Tracker 10% X Target 0 Full B X Fringe B X Electromagnetic Calorimeter 6

Dark Bremsstrahlung Recoil Energy Distribution Kinematics Recoil pt Distribution Single, low energy deposition Wide angle recoil DM With massive mediator kinematics quite different from SM bremsstrahlung No other activity in calorimeters Missing p and E carried away by DM Signal 7

Backgrounds Outgoing Incoming Irreducible neutrino backgrounds < 10-16 8

The Detector Dipole Magnet Recoil Tracker ECal Tagging Tracker HCal Target 9

Tracking System Tagging Tracker Objective: Verify incoming electron has beam energy and veto otherwise Recoil Tracker Objective: Identify low-momentum, recoiling electrons Designed with experience from HPS 10

Electromagnetic Calorimeter Objective: Make high speed energy measurements with excellent resolution and radiation hardness Hardware based on CMS forward calorimeter upgrade CERN/FNAL Testbeam 11

Trigger High signal efficiency 3 x 10-4 background rejection Primary physics trigger Total energy deposition in the first 20 layers of the ECal Trigger on low energy! Reduce beam particle rate from 46 MHz to 4 khz 12

Hadronic Calorimeter Objective: Assist ECal in vetoing photonuclear Takes advantage of CMS Phase I upgrade Neutron Flux Detection Efficiency Back HCal Side HCal 13

Physics Potential 0.1 0.3 X0 Target LDMX Phase I: 1014 EOT @ 4 GeV LDMX Phase II: 1016 EOT @ 8 GeV Sensitivity extends down to lower masses 14

Summary Accelerator-based experiments uniquely sensitive to sub-gev range Missing momentum technique has the best sensitivity LDMX has broad sensitivity over sub-gev mass range Other physics potential Displaced vertex from visibly decaying mediators Displaced electron-positron showers that result from DM co-annihalation models Dark Vectors decaying to neutrinos Photonuclear and electronuclear measurements for neutrino scattering LDMX Phase 1 LDMX Phase 1 2 (4 & 8 GeV) 15

The Collaboration Bertrand Echenard, David Hitlin Gordan Krnjaic, Nhan Tran, Andrew Whitbeck Norman Graf, Jeremy McCormick, Takashi Maruyama, Omar Moreno, Tim Nelson, Philip Schuster, Natalia Toro Owen Colegrove, Joe Incandela, Alex Patterson Josh Hiltbrand, Jeremy Mans, Reese Petersen Robert Johnson 16

Backup 17

Dealing with Photons With elastic form factor Photonuclear events Currently able to reject on the order of a few x 1013 EOT Investigating overproduction of exotic final state kinematics in Geant4 Extremely hard, backwards going hadrons Overproduced by perhaps orders of magnitude! Muon conversion Can be treated similarly to photonuclear Currently can veto all but a few in 1013 EOT Looking at Geant4 form factor implementation 18