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Profile Documents Logout
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Chapter 1 Introduction
Chapter 1 Introduction

Quantum Control in Cold Atom Systems
Quantum Control in Cold Atom Systems

... Hole-like Goldstino is an excited state with one more boson and one fewer fermion; hard to couple to. However in the presence of Bose condensate, boson number NOT fixed in the first place; can couple to it by creating single fermion hole: ...
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Scientific Poster Example/Template

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Group Problems #27 - Solutions Wednesday, November 2 Problem 1

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Quantum Numbers (6.5-9)
Quantum Numbers (6.5-9)

... 2s orbital is not degenerate (e.g., the same energy) with a 2p or a 1s orbital. The ml values are entirely dependent on the l values; each type of orbital has a set degeneracy. For an s-orbital, ml = 0, and degeneracy = 1. For a p-orbital, ml = -1, 0, +1, and degeneracy = 3. For a d-orbital, ml = -2 ...
Quantum Numbers
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... 2s orbital is not degenerate (e.g., the same energy) with a 2p or a 1s orbital. The ml values are entirely dependent on the l values; each type of orbital has a set degeneracy. For an s-orbital, ml = 0, and degeneracy = 1. For a p-orbital, ml = -1, 0, +1, and degeneracy = 3. For a d-orbital, ml = -2 ...
What is Time in Quantum Mechanics?
What is Time in Quantum Mechanics?

... repertoire of geometrical tools, a few other tools that have already been developed in differential geometry, although for a different reason. 2.2. Time of arrival according to EEQT In EEQT a detector is characterized by a sensitivity parameter κ > 0. Here let us compare time of arrival obtained form ...
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... Tiny quantum tornadoes observed in ultracold gases of fermionic atoms provide definitive evidence of superfluidity, and open up new vistas in the modelling of quantum many-body systems. transport of electrons in superconductors in terms of composites known as Cooper pairs. The great interest in ultr ...
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Quantum Numbers Activity

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... between electrons must be accounted for in the energy levels. • A neutral atom has Z electrons, as well as Z protons in its nucleus. Z is called the atomic number. • Four quantum numbers: n, l, ml , ms can be used to describe an electron in atom. • The energy depends mainly on n and l. ...
Properties, Statistics and the Identity of Quantum Particles
Properties, Statistics and the Identity of Quantum Particles

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From ancient Greece to Nobel prize: a Higgs timeline

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Field extension of real values of physical observables in classical
Field extension of real values of physical observables in classical

... eigenvalues by somehow measuring separately its real and pure imaginary parts could lead to problems in the quantum formalism, as two observations may “interfere” with one another. Inspite of having complex eigenvalues, nonhermitian operators have found several applications [23–33] in studying open ...
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... • Energy levels depend on n and l, except in hydrogen. The other quantum numbers also result in small energy differences • Pauli exclusion principle: no two electrons in the same atom can be in the same quantum state • Electrons are grouped into shells and subshells • Periodic table reflects shell s ...
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Course Outline Template Word Document - Physics for All

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Density operators and quantum operations
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... states. If two particles become entangled then information can be transmitted between them. ...
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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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