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Magnetic Field and Pressure Induced Quantum Phase Transitions in the Spin Liquid TlCuCl3 Ch. Rüegga , A. Furrerb , K. Krämerc, H.-U. Güdelc , and H. Tanakad a London Centre for Nanotechnology, University College London, London WC1E 6BT, UK Laboratory for Neutron Scattering, ETH Zurich, 5232 Villigen PSI, Switzerland c Department of Chemistry and Biochemistry, University of Bern, 3000 Bern 9, Switzerland d Department of Physics, Tokyo Institute of Technology, 152-8551 Tokyo, Japan b The generic low-temperature phase diagram of gapped dimer spin liquids is investigated by neutron scattering in high magnetic fields and under hydrostatic pressure. The model compound TlCuCl 3 with a non–magnetic singlet ground state (S = 0) shows quantum phase transitions at H c = 5.7 T and pc = 1.07 kbar. The ground states above these transitions are characterized by condensates of magnetic quasi-particles and result from a softening of the elementary triplet excitations (S = 1) by Zeeman splitting in a magnetic field or by a pressure induced increase of the triplet bandwidth. We have measured the parameter dependence of the excitation spectrum at ”T=0” across the quantum phase transitions as well as at finite temperatures in the quantum critical region1 . The results will be discussed in the context of magnetization plateaus and BEC of magnons as recently discovered in the related dimer-based spin systems BaCuSi6 O6 , SrCu2 (BO3 )2 , and NH4 CuCl3 . 1 Ch. Rüegg et al., Nature 423, 62 (2003); Phys. Rev. Lett. 93, 037207 (2004); Phys. Rev. Lett. 93, 257201 (2004). Sorting category: Ce Magnetism and properties of solids Keywords: quantum phase transitions, neutron scattering, dimer spin systems, magnetic excitations INVITED PAPER LT2340