
Quantum Information and Quantum Computation
... Professor Seth Lloyd, Professor Jeffrey H. Shapiro, Professor Scott Aaronson, Professor Edward Farhi, Professor Jeffrey Goldstone, Professor Leonya Levitov, Professor Sanjoy Mitter, Professor Jean-Jacques Slotine, Professor Peter Shor Over the last half century, the components of computers have gott ...
... Professor Seth Lloyd, Professor Jeffrey H. Shapiro, Professor Scott Aaronson, Professor Edward Farhi, Professor Jeffrey Goldstone, Professor Leonya Levitov, Professor Sanjoy Mitter, Professor Jean-Jacques Slotine, Professor Peter Shor Over the last half century, the components of computers have gott ...
Quantum Superpositions and Causality: On the Multiple Paths to the
... which exists within rational potentiality is then characterized as being capable of both contrary effects.3 This also means that potentiality is capable of being and not being at one and the same time.4 The contradiction of being and not being present in rational potentiality is only dissolved when ...
... which exists within rational potentiality is then characterized as being capable of both contrary effects.3 This also means that potentiality is capable of being and not being at one and the same time.4 The contradiction of being and not being present in rational potentiality is only dissolved when ...
A Spin Chain Primer - University of Miami Physics
... R matrices, one can construct anisotropic (XXZ and XYZ) chains, chains with spins in higher-dimensional representations (S = 1 , 3/2 , . . .) or with combinations of different spins, and chains with spins in representations of higher-rank algebras (su(N ) , . . .). Using also so-called K matrices, o ...
... R matrices, one can construct anisotropic (XXZ and XYZ) chains, chains with spins in higher-dimensional representations (S = 1 , 3/2 , . . .) or with combinations of different spins, and chains with spins in representations of higher-rank algebras (su(N ) , . . .). Using also so-called K matrices, o ...
Velocity of sound in liquids
... To determine the wavelength of sound in liquids, and from this calucate the sound velocity, from the structure of the centrally projected image. Set-up and procedure Fig. 1 shows the experiment set-up. The glass cell is 2/3 full of liquid, and the sound head is immersed in it to a depth of a few mil ...
... To determine the wavelength of sound in liquids, and from this calucate the sound velocity, from the structure of the centrally projected image. Set-up and procedure Fig. 1 shows the experiment set-up. The glass cell is 2/3 full of liquid, and the sound head is immersed in it to a depth of a few mil ...
Document
... • Single instances of non-orthogonal quantum states cannot be distinguished with certainty. Obviously, ensembles can. ...
... • Single instances of non-orthogonal quantum states cannot be distinguished with certainty. Obviously, ensembles can. ...
1 QED: Its state and its problems (Version 160815) The aim of this
... The aim of this introductory part is to gain an overview on the conceptual and mathematical problems in the current formulation of QED. We start by recalling some key ideas that led to the method of second quantization and discuss the resulting difficulties in finding an equation of motion. The abse ...
... The aim of this introductory part is to gain an overview on the conceptual and mathematical problems in the current formulation of QED. We start by recalling some key ideas that led to the method of second quantization and discuss the resulting difficulties in finding an equation of motion. The abse ...
Tina Bilban Epistemic and ontic interpretation of quantum
... Epistemic and ontic interpretation of quantum mechanics – further derivations Based on the presented possibility of ontic-epistemic interpretations of quantum mechanics some further philosophical-physical issues can be detailed. Beside the relationship between the observation and the observed, also ...
... Epistemic and ontic interpretation of quantum mechanics – further derivations Based on the presented possibility of ontic-epistemic interpretations of quantum mechanics some further philosophical-physical issues can be detailed. Beside the relationship between the observation and the observed, also ...
Postulates of Quantum Mechanics
... • Usually, the form of the matrix H needs to be either derived by a physicist or obtained via direct measurement of the properties of the computer. ...
... • Usually, the form of the matrix H needs to be either derived by a physicist or obtained via direct measurement of the properties of the computer. ...
A commentary on Eric Scerri`s paper “Has Quantum Mechanics
... The correspondence between the spectral properties of atoms and their chemistry was used by Niels Bohr to “deduce” the periodic table (see, e.g., Pais, 1991). In what follows, we’ll concentrate on the electronic properties of atoms as revealed by their spectra. In quantum mechanics, only few problem ...
... The correspondence between the spectral properties of atoms and their chemistry was used by Niels Bohr to “deduce” the periodic table (see, e.g., Pais, 1991). In what follows, we’ll concentrate on the electronic properties of atoms as revealed by their spectra. In quantum mechanics, only few problem ...
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.