Abstracts - QCMC 2016 - Centre for Quantum Technologies
... Quan Quan P1-23 - Suppression law of quantum states in a 3D photonic fast Fourier transform chip Niko Viggianiello P1-28 - Quantum dot based simultaneous classical logic gates Ronny A. Christin and Duncan L. MacFarlane P1-29 - Error probability in quantum-dot based quantum circuits Ronny A. Christin ...
... Quan Quan P1-23 - Suppression law of quantum states in a 3D photonic fast Fourier transform chip Niko Viggianiello P1-28 - Quantum dot based simultaneous classical logic gates Ronny A. Christin and Duncan L. MacFarlane P1-29 - Error probability in quantum-dot based quantum circuits Ronny A. Christin ...
Teaching Theoretical Physics: the cases of Enrico Fermi and Ettore
... issues of Fermi’s 1927-28 course. The same holds for his 1926-27 course where, although the Compton effect was explicitly reported, the relativistic kinematics was not discussed. Therefore, one might even wonder how Fermi could lecture on the Compton effect at all. Remarkably, he carried out his cal ...
... issues of Fermi’s 1927-28 course. The same holds for his 1926-27 course where, although the Compton effect was explicitly reported, the relativistic kinematics was not discussed. Therefore, one might even wonder how Fermi could lecture on the Compton effect at all. Remarkably, he carried out his cal ...
8 Momentum
... 8.4 Conservation of Momentum The force or impulse that changes momentum must be exerted on the object by something outside the object. • Molecular forces within a basketball have no effect on the momentum of the basketball. • A push against the dashboard from inside does not affect the momentum of a ...
... 8.4 Conservation of Momentum The force or impulse that changes momentum must be exerted on the object by something outside the object. • Molecular forces within a basketball have no effect on the momentum of the basketball. • A push against the dashboard from inside does not affect the momentum of a ...
Vibration Dynamics
... in which, x is a column array of describing coordinates of the system, and f is a column array of the associated applied forces. The square matrices [m], [c], [k] are the mass, damping, and stiffness matrices. Example 30 (The one, two, and three DOF model of vehicles) The one, two, and three DOF mod ...
... in which, x is a column array of describing coordinates of the system, and f is a column array of the associated applied forces. The square matrices [m], [c], [k] are the mass, damping, and stiffness matrices. Example 30 (The one, two, and three DOF model of vehicles) The one, two, and three DOF mod ...
Orthogonal metals: The simplest non-Fermi liquids
... Fermi surface with a critical Fermi surface appearing right at the critical point. We present exactly soluble models that realize an orthogonal metal phase, and the phase transition to the Fermi liquid. These models thus provide valuable solvable examples for phase transitions associated with the de ...
... Fermi surface with a critical Fermi surface appearing right at the critical point. We present exactly soluble models that realize an orthogonal metal phase, and the phase transition to the Fermi liquid. These models thus provide valuable solvable examples for phase transitions associated with the de ...
