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Quantum Gravity : Motivations and Alternatives 1
Quantum Gravity : Motivations and Alternatives 1

353, 216 (2006) .
353, 216 (2006) .

Dynamic quantum vacuum and relativity
Dynamic quantum vacuum and relativity

... On the other hand, 20th century theoretical physics brought the idea of a quantum vacuum as a fundamental medium subtending the observable forms of matter, energy and space-time. As a consequence of quantum field theories and cosmology, the physical vacuum can be regarded as a unified system governi ...
Quantum Gravity as Sum over Spacetimes
Quantum Gravity as Sum over Spacetimes

Time Reversal and Unitary Symmetries
Time Reversal and Unitary Symmetries

Qualification Exam: Quantum Mechanics
Qualification Exam: Quantum Mechanics

... orbit around a helium nucleus. The atom thus formed has one electron and one µ-meson; suppose these particles are both in their lowest energy states. Give reasons why the electron wave function can be approximated as Ψe = π −1/2 ae−3/2 e−r/ae while the µ-meson wave function is approximately Ψµ = π − ...
CHAPTER 4 RIGID-ROTOR MODELS AND ANGULAR MOMENTUM
CHAPTER 4 RIGID-ROTOR MODELS AND ANGULAR MOMENTUM

... The 2D Quantum Mechanical Rigid Rotor Assume that two masses are attached by a rigid rod (i.e. ignore vibrations) at a fixed distance, r,and are free to rotate about the Center of Mass in their x-y plane. The angle  represents the angle of rotation relative to the x-axis. The 2D Schrödinger equatio ...
Quantum Computing - Department of Computing
Quantum Computing - Department of Computing

... Quantum mechanics is a very accurate description of nature as it predicts quantum effects up to an astonishing precision of 14 decimal places. But we do not know why nature works like that and why quantum mechanics gives such a good description of nature. In other words, quantum mechanics tells us h ...
PDF
PDF

Spin Flips and Quantum Information for Antiparallel Spins
Spin Flips and Quantum Information for Antiparallel Spins

... can be entangled. The huge potential of quantum information processing has renewed the interest in the foundations of two of the major scientific theories of the twentieth century: information theory and quantum mechanics [1]. Despite the very intensive recent work on quantum information, surprising ...
The Impact of Energy Band Diagram and Inhomogeneous
The Impact of Energy Band Diagram and Inhomogeneous

Photoemission studies of quantum well states in thin films
Photoemission studies of quantum well states in thin films

A Noncommutative Sigma Model by Mauritz van den Worm
A Noncommutative Sigma Model by Mauritz van den Worm

3. Generation of the Quantum Fault Table
3. Generation of the Quantum Fault Table

... quantum test theory presented here. Two new types of faults having no parallel in other types of circuit technology are presented, named and formalized in this work. We introduce and define the quantum fault table, and categorize its entries; a method is presented illustrating how to construct a cla ...
PDF of this page - Miami bulletin
PDF of this page - Miami bulletin

... prize-winning physics occurring within the lifetime of the student. Presently, the foci are the scanning tunneling microscope, high-Tc superconductivity, and the "standard model" for particle physics. Topics include quantum mechanics in three dimensions, solid state physics, quantum optics, and part ...
Three Myths About Time Reversal in Quantum Theory 1. Introduction
Three Myths About Time Reversal in Quantum Theory 1. Introduction

Universal edge information from wavefunction deformation
Universal edge information from wavefunction deformation

Strings_06 - StealthSkater
Strings_06 - StealthSkater

... [Brian Greene]: Today, this is the goal of string theory: to unify our understanding of everything from the birth of the Universe to the majestic swirl of galaxies in just one set of principles one Master equation. Newton had unified the Heavens and the Earth in a theory of gravity. Maxwell had unif ...
Quantum Chemistry Methods
Quantum Chemistry Methods

arXiv:1312.4758v2 [quant-ph] 10 Apr 2014
arXiv:1312.4758v2 [quant-ph] 10 Apr 2014

Entanglement and its Role in Shor`s Algorithm
Entanglement and its Role in Shor`s Algorithm

quantum computation of the jones polynomial - Unicam
quantum computation of the jones polynomial - Unicam

... Definition 1.1.4. We define an isotopy of the space R3 as a continuous application H : R × [0, 1] → R, such that the map ht : R → R given by x 7→ ht (x) = H(x, t) is a homomorphism for every t ∈ [0, 1] and moreover h0 is the identity of R3 Then, the concept of isotopy, allows us to define the equiva ...
Atomic Physics  - Teaching Commons Guide for MERLOT
Atomic Physics - Teaching Commons Guide for MERLOT

... of the content including the approximate time required to complete each section. A graphic organization of the whole content is presented next to the outline. All these three will assist you to picture how content is organized in the module. GENERAL OBJECTIVE(S): Clear informative, concise and under ...
Quantum Thermodynamics: A Dynamical Viewpoint
Quantum Thermodynamics: A Dynamical Viewpoint

11_abs_Fritz Riehle
11_abs_Fritz Riehle

< 1 ... 22 23 24 25 26 27 28 29 30 ... 252 >

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.
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