about
Keeping a Quantum Bit Alive by Optimized π -Pulse SequencesCoupling of Higgs and Leggett modes in non-equilibrium superconductors.Field-induced Tomonaga-Luttinger liquid phase of a two-leg spin-1/2 ladder with strong leg interactions.Charge-order-induced sharp Raman peak in Sr14Cu24O41.Landau's quasiparticle mapping: Fermi liquid approach and Luttinger liquid behavior.Unifying Magnons and Triplons in Stripe-Ordered Cuprate SuperconductorsConcatenated Control Sequences Based on Optimized Dynamic DecouplingObservation of Two-Magnon Bound States in the Two-Leg Ladders of(Ca,La)14Cu24O41Zero-Field Incommensurate Spin-Peierls Phase with Interchain Frustration in TiOClStrong Damping of Phononic Heat Current by Magnetic Excitations inSrCu2(BO3)2Exact demonstration of magnetization plateaus and first-order dimer-Neel phase transitions in a modified shastry-sutherland model for SrCu2(BO3)(2)Excitations in one-dimensional S = 1/2 quantum antiferromagnetsNonexistence of planar magnetic order in the one- and two-dimensional generalized Hubbard model at finite temperaturesFermionic lattice models with internally competing symmetries: Nontrivial algebraic corrections in the Hartree-Fock ground-state energyInhibition of phase separation and appearance of new phases for interacting spinless fermionsExact Single Spin Flip for the Hubbard Model in d=Dynamic structure factor of the two-dimensional Shastry-Sutherland modelFractional and integer excitations in quantum antiferromagnetic spin 1/2 laddersMagnetic excitation spectrum of dimerized antiferromagnetic chainsConductivity in a symmetry-broken phase: Spinless fermions with 1/d correctionsEmergent collective modes and kinks in electronic dispersionsRoton Minimum as a Fingerprint of Magnon-Higgs Scattering in Ordered Quantum AntiferromagnetsAnomalous behavior of control pulses in presence of noise with singular autocorrelationPositivity of the Spectral Densities of Retarded Floquet Green FunctionsClassification and characterization of nonequilibrium Higgs modes in unconventional superconductors
P50
Q27454486-42257D0C-78C8-4A9D-8069-A7BF69EFCF25Q37034575-C5A748BF-1BB4-4170-83E2-10AB9B7450B5Q49526474-C4860566-4982-4B53-9046-9F644B16F9C2Q53763244-3C9F4261-C71B-4AB8-B9BB-CACF8F48F90CQ53875501-69219CDA-841A-4799-B570-2A75956159E4Q59480054-7BF63B50-1955-4623-BF5F-F1648A0E0856Q61157749-F82F2731-0A06-461C-A58B-2BE23B77D010Q62383420-F05CB441-0A4B-4BA5-A604-085CE2AF2704Q62678602-89ED87A1-CCEE-4AEB-BC3A-4AAF842B9686Q62678622-2DD69CE2-0B06-436B-83D5-1BCD2E7D80CCQ73037311-7ED949A1-2816-475C-BACD-19C625A79A42Q73662528-0945A1C2-A246-4437-85B5-7F912D94DA70Q74361261-2FDDC2F0-019E-4E89-BA30-B77E4E8289E0Q74364724-5779E66D-A37B-410C-AA8F-6970FEC3F716Q74541063-FA2E455A-76CF-4D59-A221-20B6687DF279Q74572143-B8BBD866-2D18-4926-B0C7-ED1EFF43A0DEQ75375137-995D53A8-F6B6-4A88-AD2F-18FD9B187FC8Q77108401-9801AB1B-3795-452D-A5AE-F9D255F51CACQ78154873-66E060B7-3596-41A0-A2CE-C4743ACC24D7Q78155132-43EBDB7D-922B-47D1-876F-DD149DEFD8F9Q83420166-7B6E742C-421D-47CB-8CCD-06B5C1B6888FQ86821274-1EE7280B-0B24-4BCD-8377-701C72EAA5ECQ87410289-4B6AA15D-7548-4D2D-AF68-5A38EADDC4B5Q90226431-3B2732E5-7E58-4D5D-87AB-F5CFBDB5836EQ92668706-410F38A7-31B2-4A61-B3C1-8CC23390B9BD
P50
description
researcher
@en
wetenschapper
@nl
name
Götz S. Uhrig
@en
Uhrig GS
@nl
type
label
Götz S. Uhrig
@en
Uhrig GS
@nl
altLabel
Uhrig GS
@en
prefLabel
Götz S. Uhrig
@en
Uhrig GS
@nl
P106
P108
P31
P496
0000-0003-1961-0346