| Th. Jacobs, S. O. Katterwe, H. Motzkau, A. Rydh, A. Maljuk, T. Helm, C. Putzke, E. Kampert, M. V. Kartsovnik, V. M. Krasnov
| Martin Leib, Frank Deppe, Achim Marx, Rudolf Gross, Michael Hartmann
| M.V. Kartsovnik, W. Biberacher, D. Andres, S. Jakob, M. Kunz, K. Neumaier, H. Müller, N.D. Kushch
| N. Munnikes, B. Muschler, F. Venturini, L. Tassini, W. Prestel, Shimpei Ono, Yoichi Ando, D. C. Peets, W. N. Hardy, Ruixing Liang, D. A. Bonn, A. Damascelli, H. Eisaki, M. Greven, A. Erb, and R.
| S. Bosma, S. Weyeneth, R. Puzniak, A. Erb, A. Schilling, and H. Keller
| E. Hoffmann, F. Deppe, T. Niemczyk, T. Wirth, E. P. Menzel, G. Wild, H. Huebl, M. Mariantoni, T. Weißl, A. Lukashenko, A. P. Zhuravel, A. V. Ustinov, A. Marx, R. Gross
| A. Pashkin, M. Porer, M. Beyer, K. W. Kim, A. Dubroka, C. Bernhard, X. Yao, Y. Dagan, R. Hackl, A. Erb, J. Demsar, R. Huber, and A. Leitenstorfer
| B. G. U. Englert, G. Mangano, M. Mariantoni, R. Gross, J. Siewert, E. Solano
| B. Muschler, W. Prestel, R. Hackl, T. P. Devereaux, J. G. Analytis, Jiun-Haw Chu, I. R. Fisher
| Ferdinand Helmer, Matteo Mariantoni, Austin G. Fowler, Jan von Delft, Enrique Solano & Florian Marquardt,
| T. Niemczyk, F. Deppe, M. Mariantoni, E.P. Menzel, E. Hoffmann, G. Wild, L. Eggenstein, A. Marx, R. Gross
| M. Mariantoni, F. Deppe, A. Marx, F.K. Wilhelm, R. Gross & E. Solano,
| M.J. Storcz, M. Mariantoni, H. Christ, A. Emmert, A. Marx, W.D. Oliver, R. Gross, F.K. Wilhelm & E. Solano
| F. Deppe, M. Mariantoni, E.P. Menzel, S. Saito, K. Kakuyanagi, T. Meno, K. Semba, H. Takayanagi & R. Gross
| K. Kakuyanagi, T. Meno, S. Saito, H. Nakano, K. Semba, H. Takayanagi, F. Deppe & A. Shnirman
| V. B. Zabolotnyy, S. V. Borisenko, A. A. Kordyuk, J. Fink, J. Geck, A. Koitzsch, M. Knupfer, B. Buchner, H. Berger, A. Erb, C. T. Lin, B. Keimer & R. Follath
| M. Ganzhorn, G. Salis, D. J. Egger, A. Fuhrer, M. Mergenthaler, C. Müller, P. Müller, S. Paredes, M. Pechal, M. Werninghaus, and S. Filipp
Reaching high speed, high fidelity qubit operations requires precise control over the shape of the underlying pulses. For weakly anharmonic systems, such as superconducting transmon qubits, short
| Andreas Fuhrer and Andreas Kuhlmann and Ute Drechsler and Veeresh V Deshpande and Stefan Filipp and Marc Ganzhorn
A typical goal of a quantum simulation is to find the energy levels and eigenstates of a given Hamiltonian. This can be realized by adiabatically varying the system control parameters to steer an
We propose a quantum simulator based on driven superconducting qubits where the interactions are generated parametrically by a bichromatic magnetic flux modulation of a tunable bus element. Using a
Increasing coherence times of quantum bits is a fundamental challenge in the field of quantum computing. With long-lived qubits it is, however, inefficient to wait until the qubits have relaxed to
We investigate a nonadiabatic holonomic operation that enables us to entangle two fixed-frequency superconducting transmon qubits attached to a common bus resonator. Two coherent microwave tones are
| O Viyuela and A Rivas and S Gasparinetti and A Wallraff and S Filipp and M A Martin-Delgado
| Marco Roth and Marc Ganzhorn and Nikolaj Moll and Stefan Filipp and Gian Salis and Sebastian Schmidt
| S Berger and M Pechal and P Kurpiers and A A Abdumalikov and C Eichler and J A Mlynek and A Shnirman and Y Gefen and A Wallraff and S Filipp
| U Las Heras and A Mezzacapo and L Lamata and S Filipp and A Wallraff and E Solano
We make use of a superconducting qubit to study the effects of noise on adiabatic geometric phases. The state of the system, an effective spin one-half particle, is adiabatically guided along a
| C Eichler and C Lang and J M Fink and J Govenius and S Filipp and A Wallraff
Geometric phases, which accompany the evolution of a quantum system and depend only on its trajectory in state space, are commonly studied in two-level systems. Here, however, we study the adiabatic
| M Baur and A Fedorov and L Steffen and S Filipp and M P da Silva and A Wallraff
Superconducting circuits have been successfully established as systems to prepare and investigate microwave light fields at the quantum level. In contrast to optical experiments where light is
| R Bianchetti and S Filipp and M Baur and J M Fink and C Lang and L Steffen and M Boissonneault and A Blais and A Wallraff
| M Baur and S Filipp and R Bianchetti and J M Fink and M Göppl and L Steffen and P J Leek and A Blais and A Wallraff
| P ~J Leek and S Filipp and P Maurer and M Baur and R Bianchetti and J ~M Fink and M Göppl and L Steffen and A Wallraff
| Harshman, DR; Kossler, WJ; Wan, X; Fiory, AT; Greer, AJ; Noakes, DR; Stronach, CE; Koster, E; Erb, A; Dow, JD
| L. Alff, B. Welter, S.Kleefisch, A. Marx, R. Gross
| Schlicht, A; Schwenker, M; Biberacher, W; Lerf, A
| Schuberth, EA; Schottl, S; Flachbart, K; Sasaki, T
| F. Venturini, U. Michelucci, T.P. Devereaux, A.P. Kampf
| M. Opel, F. Venturini, R. Hackl, B. Revaz, H. Berger, L. Forro
| Schottl, S; Schuberth, EA; Kycia, JB; Halperin, WP
We describe the results of electronic Raman-scattering experiments in differently doped single crystals of YBCO and BiSCCO. The data in antiferromagnetic insulating samples suggest that at least the
| M. Opel, M. Gotzinger, C. Hoffmann, R. Nemetschek, R. Philipp, F. Venturini, R. Hackl, A. Erb, E. Walker
| Opel, M; Nemetschek, R; Venturini, F; Hackl, R; Erb, A; Walker, E; Berger, H; Forro, L
| Schottl, S; Schuberth, EA; Flachbart, K; Kycia, JB; Hong, JI; Seidman, DN; Halperin, WP
