- Acharyya, A;
- Archer, A;
- Bangale, P;
- Bartkoske, JT;
- Batista, P;
- Baumgart, M;
- Benbow, W;
- Buckley, JH;
- Falcone, A;
- Feng, Q;
- Finley, JP;
- Foote, GM;
- Fortson, L;
- Furniss, A;
- Gallagher, G;
- Hanlon, WF;
- Hervet, O;
- Hoang, J;
- Holder, J;
- Humensky, TB;
- Jin, W;
- Kaaret, P;
- Kertzman, M;
- Kherlakian, M;
- Kieda, D;
- Kleiner, TK;
- Korzoun, N;
- Krennrich, F;
- Lang, MJ;
- Lundy, M;
- Maier, G;
- McGrath, CE;
- Moriarty, P;
- O’Brien, S;
- Ong, RA;
- Pfrang, K;
- Pohl, M;
- Pueschel, E;
- Quinn, J;
- Ragan, K;
- Reynolds, PT;
- Roache, E;
- Rodd, NL;
- Ryan, JL;
- Sadeh, I;
- Saha, L;
- Santander, M;
- Sembroski, GH;
- Shang, R;
- Splettstoesser, M;
- Tak, D;
- Tucci, JV;
- Vassiliev, VV;
- Williams, DA
Dark matter is a key piece of the current cosmological scenario, with weakly interacting massive particles (WIMPs) a leading dark matter candidate. WIMPs have not been detected in their conventional parameter space (100 GeV ≲M χ ≲ 100 TeV), a mass range accessible with current Imaging Atmospheric Cherenkov Telescopes. As ultraheavy dark matter (UHDM; M χ ≳ 100 TeV) has been suggested as an underexplored alternative to the WIMP paradigm, we search for an indirect dark matter annihilation signal in a higher mass range (up to 30 PeV) with the VERITAS γ-ray observatory. With 216 hr of observations of four dwarf spheroidal galaxies, we perform an unbinned likelihood analysis. We find no evidence of a γ-ray signal from UHDM annihilation above the background fluctuation for any individual dwarf galaxy nor for a joint-fit analysis, and consequently constrain the velocity-weighted annihilation cross section of UHDM for dark matter particle masses between 1 TeV and 30 PeV. We additionally set constraints on the allowed radius of a composite UHDM particle.