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Chapter 7 Linear Momentum
Chapter 7 Linear Momentum

The noncommutative geometry of the quantum Hall effect
The noncommutative geometry of the quantum Hall effect

... C. Localization in physical models. .......................................... VI. APPLICATIONS AND COMPLEMENTS. ................................... A. Low-lying states do not contribute to the IQHE. ............................. B. Where and how does the localization length diverge?. .............. ...
Basic Atomic Physics
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Quiet Readout of Superconducting Flux States

... decoherence due to environmental noise, but back action from the required measuring device and intrinsic noise in the qubit itself results in decoherence that must be quantified and reduced. A dc Superconducting QUantum Interference Device (SQUID), which involves two Josephson junctions connected i ...
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Finite Element Approach of Electronic Structures THÈSE

... to be coupled with larger scales models, the accuracy of their solutions, and their ability to handle large systems. This evaluation hints at using the finite element method. The core of this chapter deals with the details of the numerical strategy that we propose. • Chapter 4 presents the results o ...
Broad Feshbach Resonance in the 6Li-40K Mixture
Broad Feshbach Resonance in the 6Li-40K Mixture

... Our procedure to create an ultracold mixture of 6 Li and 40 K is described in detail elsewhere [26,27]. Here we briefly summarize the procedure. We perform forced evaporative cooling on both species in an optically plugged magnetic quadrupole trap [28]. A small amount of spinpolarized 6 Li in the j3 ...
Lecture 1. Newton`s Laws
Lecture 1. Newton`s Laws

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introduction to quantum field theory

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Wavefunctions and carrier-carrier interactions in InAs quantum dots

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... with the wavelength of several metres for seismic waves). SAWs can be generated electrically in a piezoelectric medium using interdigital transducers (IDTs). As illustrated in Figure 2, the IDTs consist of two interlocking arrays of metal electrodes deposited on the surface of the material, which is ...
Spin Algebra, Spin Eigenvalues, Pauli Matrices Lecture 10
Spin Algebra, Spin Eigenvalues, Pauli Matrices Lecture 10

... But bbot (a) must be smaller than btop (a), so only the second solution works. Therefore bbot (a) = −btop (a). Hence b, which is the eigenvalue of Sz , ranges from −btop (a) to btop (a). Furthermore, since S− lowers this value by ~ each time it is applied, these two values must differ by an integer ...
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Quantum Chemistry for Spectroscopy – A Tale of Three Spins (S = 0

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... 2. A company offers a 2% discount if you buy 1–5 of their products. If you buy 6–10 of their products, you earn a 3.5% discount. Buying 11–15 products will earn you a 5% discount. If the pattern continues, what discount would be offered for buying 33 products? ...
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Electronic structure, plane waves and pseudopotentials

... Finding the Ground State ...
Quantum information with continuous variables
Quantum information with continuous variables

Electronic Correlations in Transport through Coupled Quantum Dots V 82, N 17
Electronic Correlations in Transport through Coupled Quantum Dots V 82, N 17

... problem. The phase shift d is an increasing function of J, which starts at the value given above Eq. (2), and increases until it saturates at d ­ p at a scale J p . From the above estimate of TK the ratio J p yTK0 increases exponentially with tyG. These considerations, and the knowledge of the cross ...
Atomic Quantum Metrology with Narrowband Entangled and Squeezed States of Light DISSERTATION
Atomic Quantum Metrology with Narrowband Entangled and Squeezed States of Light DISSERTATION

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Review of the Safety of LHC Collisions

... surrounding any black hole. Some particles (or antiparticles) disappear into the black hole itself, and the corresponding antiparticles (or particles) must escape as radiation. There is broad consensus among physicists on the reality of Hawking radiation, but so far no experiment has had the sensiti ...
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T-symmetry

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