
PDF of this page - Kettering University Catalog
... physics and engineering. The first part of this course will introduce students to the basics of vibration, including the effects of real damping, response to driving forces, nonlinear oscillation and application to several acoustical, optical, electrical, and mechanical systems. After this introduct ...
... physics and engineering. The first part of this course will introduce students to the basics of vibration, including the effects of real damping, response to driving forces, nonlinear oscillation and application to several acoustical, optical, electrical, and mechanical systems. After this introduct ...
Physics
... Phy 340. Optics. Theoretical and experimental study of the properties of light: wave motion, propagation of light in media, geometrical optics, polarization, interference, diffraction, Fourier optics and coherence theory. Prerequisite:185. Phy 341. Advanced Physics Laboratory. Experiments in upper- ...
... Phy 340. Optics. Theoretical and experimental study of the properties of light: wave motion, propagation of light in media, geometrical optics, polarization, interference, diffraction, Fourier optics and coherence theory. Prerequisite:185. Phy 341. Advanced Physics Laboratory. Experiments in upper- ...
Využití Kr laseru ve SLO UP a AVČR
... entangled photon pairs, Phys. Lett. A 319, 251 (2003). J. Soubusta et al, Experimental realization of a programmable quantum-state discriminator and a phase-covariant quantum multimeter, Phys. Rev. A 69, 052321 (2004). R. Filip et al, How quantum correlations enhance prediction of ...
... entangled photon pairs, Phys. Lett. A 319, 251 (2003). J. Soubusta et al, Experimental realization of a programmable quantum-state discriminator and a phase-covariant quantum multimeter, Phys. Rev. A 69, 052321 (2004). R. Filip et al, How quantum correlations enhance prediction of ...
Document
... number. The actual spin angular momentum is S s(s 1) Electrons are s = ½ (spin one-half) particles. Since this never changes, it is often not specified. ms = z-component of spin angular momentum and can have values of ms = −s, −s+1, … s−1, s. The actual z-component of spin angular momentum is S ...
... number. The actual spin angular momentum is S s(s 1) Electrons are s = ½ (spin one-half) particles. Since this never changes, it is often not specified. ms = z-component of spin angular momentum and can have values of ms = −s, −s+1, … s−1, s. The actual z-component of spin angular momentum is S ...
Lecture 1
... Moore’s Law: The number of transistors that can be placed on a chip doubles every two years I.e., the computational power doubles This trend has been approximately true for more than 50 years Main way to achieve this is by making smaller transistors! Even today quantum mechanical effects are importa ...
... Moore’s Law: The number of transistors that can be placed on a chip doubles every two years I.e., the computational power doubles This trend has been approximately true for more than 50 years Main way to achieve this is by making smaller transistors! Even today quantum mechanical effects are importa ...
Quantum Condensed Matter Field Theory
... formation of an electron “solid phase” — out of which a magnetic state emerges. This application in turn motivates the investigation of the hydrodynamic or spin-wave spectrum of the quantum Heisenberg spin (anti)ferromagnet. We then close this section with a discussion of the weakly interacting dilu ...
... formation of an electron “solid phase” — out of which a magnetic state emerges. This application in turn motivates the investigation of the hydrodynamic or spin-wave spectrum of the quantum Heisenberg spin (anti)ferromagnet. We then close this section with a discussion of the weakly interacting dilu ...
Integration via a Quantum Information Processor
... that can process information in a way that preserves quantum coherence. Unlike a classical bit, a qubit can be in a superposition of states 0 and 1 at the same time. In addition, quantum bits may become entangled, that is, there may arise correlations between quantum bits that are not allowed classi ...
... that can process information in a way that preserves quantum coherence. Unlike a classical bit, a qubit can be in a superposition of states 0 and 1 at the same time. In addition, quantum bits may become entangled, that is, there may arise correlations between quantum bits that are not allowed classi ...
WP1
... discovered the wave nature of electrons - the ironies of history!! This wave-particle duality is an important part of quantum physics! ...
... discovered the wave nature of electrons - the ironies of history!! This wave-particle duality is an important part of quantum physics! ...
fn1_1h_qm2_cr
... If two particles become entangled then information can be transmitted between them. ...
... If two particles become entangled then information can be transmitted between them. ...
Max Born

Max Born (German: [bɔɐ̯n]; 11 December 1882 – 5 January 1970) was a German physicist and mathematician who was instrumental in the development of quantum mechanics. He also made contributions to solid-state physics and optics and supervised the work of a number of notable physicists in the 1920s and 30s. Born won the 1954 Nobel Prize in Physics for his ""fundamental research in Quantum Mechanics, especially in the statistical interpretation of the wave function"".Born was born in 1882 in Breslau, then in Germany, now in Poland and known as Wrocław. He entered the University of Göttingen in 1904, where he found the three renowned mathematicians, Felix Klein, David Hilbert and Hermann Minkowski. He wrote his Ph.D. thesis on the subject of ""Stability of Elastica in a Plane and Space"", winning the University's Philosophy Faculty Prize. In 1905, he began researching special relativity with Minkowski, and subsequently wrote his habilitation thesis on the Thomson model of the atom. A chance meeting with Fritz Haber in Berlin in 1918 led to discussion of the manner in which an ionic compound is formed when a metal reacts with a halogen, which is today known as the Born–Haber cycle.In the First World War after originally being placed as a radio operator, due to his specialist knowledge he was moved to research duties regarding sound ranging. In 1921, Born returned to Göttingen, arranging another chair for his long-time friend and colleague James Franck. Under Born, Göttingen became one of the world's foremost centres for physics. In 1925, Born and Werner Heisenberg formulated the matrix mechanics representation of quantum mechanics. The following year, he formulated the now-standard interpretation of the probability density function for ψ*ψ in the Schrödinger equation, for which he was awarded the Nobel Prize in 1954. His influence extended far beyond his own research. Max Delbrück, Siegfried Flügge, Friedrich Hund, Pascual Jordan, Maria Goeppert-Mayer, Lothar Wolfgang Nordheim, Robert Oppenheimer, and Victor Weisskopf all received their Ph.D. degrees under Born at Göttingen, and his assistants included Enrico Fermi, Werner Heisenberg, Gerhard Herzberg, Friedrich Hund, Pascual Jordan, Wolfgang Pauli, Léon Rosenfeld, Edward Teller, and Eugene Wigner.In January 1933, the Nazi Party came to power in Germany, and Born, who was Jewish, was suspended. He emigrated to Britain, where he took a job at St John's College, Cambridge, and wrote a popular science book, The Restless Universe, as well as Atomic Physics, which soon became a standard text book. In October 1936, he became the Tait Professor of Natural Philosophy at the University of Edinburgh, where, working with German-born assistants E. Walter Kellermann and Klaus Fuchs, he continued his research into physics. Max Born became a naturalised British subject on 31 August 1939, one day before World War II broke out in Europe. He remained at Edinburgh until 1952. He retired to Bad Pyrmont, in West Germany. He died in hospital in Göttingen on 5 January 1970.