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Relativistic quantum mechanics and the S matrix
Relativistic quantum mechanics and the S matrix

Black Hole Entropy: From Shannon to Bekenstein
Black Hole Entropy: From Shannon to Bekenstein

... to the entropy problem as perceived by an observer outside the BH horizon. Consider that a pair of left moving and right moving modes is created just outside the BH horizon. We would like to reduce the problem to that of a yes-no type of two state problem, that is simply whether a particle exists or ...
Quantum Spin Hall Effect and Enhanced Magnetic Response by
Quantum Spin Hall Effect and Enhanced Magnetic Response by

... for opposite directions of spins. The QSH phase can be regarded as a novel phase constrained by the Z2 topological number I [6]. It is equal to a number of Kramers pairs of helical edge states modulo two. The QSH phase has I = odd, while the spin-Hall-insulator (SHI) phase [10], topologically equiva ...
Monday, Nov. 27, 2006 - UTA High Energy Physics page.
Monday, Nov. 27, 2006 - UTA High Energy Physics page.

... Baryons and Mesons (the observed particles) are color charge neutral ...
Text and script of the play "Incredible Quantum Tablet".
Text and script of the play "Incredible Quantum Tablet".

... machine is a crane controlled by lower part. The crane serves as a one– dimensional pendulum – a robot crane. A humanoid robot is somehow attached to the crane. The connection allows for one or more additional degrees of freedom (DOF), depending on particular design. This connection depends on a par ...
A Microscopic Approach to Van-der
A Microscopic Approach to Van-der

... between nanoclusters. I will start by giving some background information on Van-der-Waals forces. In chapter 2 I will introduce the theory behind the Coupled Dipole Method. The following chapters will deal with my results. In chapter 3 I will present my results concerning the static polarizability o ...
Physics - College of William and Mary
Physics - College of William and Mary

... Vector analysis, complex variables, matrices, series solutions of differential equations, orthogonal functions and partial differential equations. 303. Classical Mechanics of Particles and Waves II. Fall (3) Carlson. Prerequisite: PHYS 208. Central force motion, scattering, systems of particles, cou ...
Interpreting Quantum Mechanics in Terms of - Philsci
Interpreting Quantum Mechanics in Terms of - Philsci

... parts of quantum mechanics. As a result, protective measurement can not only measure the physical state of a quantum system and help to unveil the meaning of the wave function, but also be used to examine the solutions to the measurement problem before experiments give the last verdict. A full expos ...
PDF - at www.arxiv.org.
PDF - at www.arxiv.org.

Solutions to Problems
Solutions to Problems

... If the force is attractive, then the charges are of opposite sign. The value used for F must then be negative. Other than that, the solution method is the same as for part (a). ...
MODULE MAPS OVER LOCALLY COMPACT QUANTUM GROUPS
MODULE MAPS OVER LOCALLY COMPACT QUANTUM GROUPS

... be the convolution quantum group algebra of G. If we let C0 (G) be the reduced C ∗ -algebra associated with G, then its operator dual M (G) is a faithful completely contractive Banach algebra containing L1 (G) as an ideal. It has been shown in the recent work [26, 27, 29] that many important results ...
Quantum simulation of disordered systems with cold atoms
Quantum simulation of disordered systems with cold atoms

Implementing Qubits with Superconducting Integrated Circuits Michel H. Devoret and John M. Martinis
Implementing Qubits with Superconducting Integrated Circuits Michel H. Devoret and John M. Martinis

Quantum Correlations in Information Theory
Quantum Correlations in Information Theory

... its content, while the last section summarises its main results. In the body of the work, the narrative voice is “we”, as I repute it to be more suitable for the scientific exposition. The content of each chapter is the following: • Chapter 1 is merely introductory. First, I review basic facts and t ...
Path Integral Formulation of Quantum Mechanics
Path Integral Formulation of Quantum Mechanics

... The exponent of (2.12) is then Scl /~ ≈ 0.5 · 1027 , i.e., a very large number. Since this number is multiplied by ‘i’, the exponent is a very large imaginary number. Any variations of Scl would then lead to strong oscillations of the contributions exp( ~i S) to the path integral and one can expect ...
Physical Foundations of Quantum Electronics
Physical Foundations of Quantum Electronics

Reversible vs. Quantum Computing
Reversible vs. Quantum Computing

... physical hardware can act as a different gate at different times. For example, after being used as an NDRAG(A:0→1) gate, the same NFET can later be used as an NDRAG(A:1→0) gate, which will undo any change to B, if G is still the same. It turns out that networks of DRAG gates, constructible using ord ...
Introduction
Introduction

... structure that is common to all physical theories of the macrocosm and to explain the origin of this common structure. The starting point of this investigation is the analysis of physical variables under a new profile: we take into consideration all those geometric features that are usually overlook ...
Interference of Bose#Einstein Condensates†
Interference of Bose#Einstein Condensates†

Frontiers in Quantum Methods and Applications in Chemistry and
Frontiers in Quantum Methods and Applications in Chemistry and

... as from initiatives from authors or translations. The basic theories of physics—classical mechanics and electromagnetism, relativity theory, quantum mechanics, statistical mechanics, quantum electrodynamics —support the theoretical apparatus which is used in molecular sciences. Quantum mechanics pla ...
Jagiellonian University M. Smoluchowski Institute of Physics Entropy
Jagiellonian University M. Smoluchowski Institute of Physics Entropy

Spectroscopic Selection Rules: The Role of Photon States
Spectroscopic Selection Rules: The Role of Photon States

ppt file - Manchester HEP
ppt file - Manchester HEP

Differential Forms and Electromagnetic Field Theory
Differential Forms and Electromagnetic Field Theory

... having an orientation. The integral of the one-form −dx over a path from (0, 0, 0) to (4, 0, 0) is −4. Thus, when we count surfaces pierced by a path, we have to compare the sign of the one-form with the direction of the path in order to determine whether the surface contributes positively or negati ...
A bound for the range of a narrow light
A bound for the range of a narrow light

... domain Dev where the waves are evanescent, as is asymptotically true for large z. Then, the spectral width WðzÞ reaches its maximum 2k if and only if jEðκ; θ; zÞj2 ∼ κ−1 δðκ − kÞjAðκ; θ; zÞj2 , where we have introduced the polar coordinates ðκ; θÞ in the spectral domain. Consequently, W ðzÞ ≤ 2k for ...
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History of quantum field theory

In particle physics, the history of quantum field theory starts with its creation by Paul Dirac, when he attempted to quantize the electromagnetic field in the late 1920s. Major advances in the theory were made in the 1950s, and led to the introduction of quantum electrodynamics (QED). QED was so successful and ""natural"" that efforts were made to use the same basic concepts for the other forces of nature. These efforts were successful in the application of gauge theory to the strong nuclear force and weak nuclear force, producing the modern standard model of particle physics. Efforts to describe gravity using the same techniques have, to date, failed. The study of quantum field theory is alive and flourishing, as are applications of this method to many physical problems. It remains one of the most vital areas of theoretical physics today, providing a common language to many branches of physics.
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