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Development of a Silicon Semiconductor Quantum Dot Qubit with
... Schematic showing the coupling of the double quantum dot and an electrical resonator . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Top: Schematic diagram showing the quantum dot capacitively coupled to the microwave resonator (green, shown as a lumped element LC circuit), ...
... Schematic showing the coupling of the double quantum dot and an electrical resonator . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Top: Schematic diagram showing the quantum dot capacitively coupled to the microwave resonator (green, shown as a lumped element LC circuit), ...
Development of a Silicon Semiconductor Quantum Dot Qubit with
... Schematic showing the coupling of the double quantum dot and an electrical resonator . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Top: Schematic diagram showing the quantum dot capacitively coupled to the microwave resonator (green, shown as a lumped element LC circuit), ...
... Schematic showing the coupling of the double quantum dot and an electrical resonator . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Top: Schematic diagram showing the quantum dot capacitively coupled to the microwave resonator (green, shown as a lumped element LC circuit), ...
Engineering a Robust Quantum Spin Hall State in Graphene via
... C0 ; remarkably, the components with Dirac-point momenta Q vanish identically. More physically, electrons near the Dirac points interfere destructively when hopping onto the m ¼ 0 adatom orbital. (See Appendixes A and D for complementary perspectives.) We stress that this argument holds only for p ...
... C0 ; remarkably, the components with Dirac-point momenta Q vanish identically. More physically, electrons near the Dirac points interfere destructively when hopping onto the m ¼ 0 adatom orbital. (See Appendixes A and D for complementary perspectives.) We stress that this argument holds only for p ...
Semiclassical Green`s functions and an instanton formulation of
... Other instanton approaches are well known from adiabatic rate23–29 and tunnelling splitting30,31 calculations, where in both cases the Born-Oppenheimer approximation is first applied to obtain a single-surface Hamiltonian. The Im F method32 can be used to derive the instanton approximation to the ad ...
... Other instanton approaches are well known from adiabatic rate23–29 and tunnelling splitting30,31 calculations, where in both cases the Born-Oppenheimer approximation is first applied to obtain a single-surface Hamiltonian. The Im F method32 can be used to derive the instanton approximation to the ad ...
Quasi Classical Trajectory Binning: A Systematic
... valuable because they can provide a more intuitive description of dynamics, as classical processes dominate the macroscopic scale. As a result, there is a high demand for methods of classical calculation that are able to provide a good representation of systems with quantum features. Since it is imp ...
... valuable because they can provide a more intuitive description of dynamics, as classical processes dominate the macroscopic scale. As a result, there is a high demand for methods of classical calculation that are able to provide a good representation of systems with quantum features. Since it is imp ...
Ph.D. Thesis Chirag Dhara
... Quantum mechanics was developed as a response to the inadequacy of classical physics in explaining certain physical phenomena. While it has proved immensely successful, it also presents several features that severely challenge our classicality based intuition. Randomness in quantum theory is one suc ...
... Quantum mechanics was developed as a response to the inadequacy of classical physics in explaining certain physical phenomena. While it has proved immensely successful, it also presents several features that severely challenge our classicality based intuition. Randomness in quantum theory is one suc ...
Chapter 1 Similarity Judgments: From Classical to Complex Vector
... as opposed to another? Tversky’s [1977] assumption was that when assessing Sim(A, B) then A is the subject and B is the referent and so “...the features of the subject are weighted more heavily than the features of the referent” [p. 333, Tversky, 1977]. This allows one to set ↵ > , which enables pos ...
... as opposed to another? Tversky’s [1977] assumption was that when assessing Sim(A, B) then A is the subject and B is the referent and so “...the features of the subject are weighted more heavily than the features of the referent” [p. 333, Tversky, 1977]. This allows one to set ↵ > , which enables pos ...
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(Never) Mind your p`s and q`s: Von Neumann versus Jordan on the
... This is the special case of Jordan’s interpretation that Pauli had hit upon (in f dimensions). Jordan also recognized that in quantum mechanics the usual addition and multiplication rules of probability apply to the probability amplitudes rather than to the probabilities themselves. Again crediting ...
... This is the special case of Jordan’s interpretation that Pauli had hit upon (in f dimensions). Jordan also recognized that in quantum mechanics the usual addition and multiplication rules of probability apply to the probability amplitudes rather than to the probabilities themselves. Again crediting ...
Quantum Nonlinear Optics in Lossy Coupled-Cavities in Photonic Crystal Slabs
... loss difference between signal and idler channels plays an important role in minimizing the number of unpaired photon in the system. Also, there is a trade-off between source brightness and higher order generation depending on the losses in the system. This is important, because both the number of u ...
... loss difference between signal and idler channels plays an important role in minimizing the number of unpaired photon in the system. Also, there is a trade-off between source brightness and higher order generation depending on the losses in the system. This is important, because both the number of u ...
lecture notes - Analysis Group TU Delft
... theorem for unbounded selfadjoint operators in Hilbert spaces, and some applications to elementary quantum mechanics. The main focus will be on the decomposition of a selfadjoint operator onto its family of spectral projections. Some elements of functional calculus will also be given. We will start ...
... theorem for unbounded selfadjoint operators in Hilbert spaces, and some applications to elementary quantum mechanics. The main focus will be on the decomposition of a selfadjoint operator onto its family of spectral projections. Some elements of functional calculus will also be given. We will start ...
Some New Classical and Semiclassical Models for Describing
... that explore complex-valued regions of phase space.1-6 For example, in the 1-d WKB approximation for barrier tunneling, the momentum of the particle is imaginary when it is inside the barrier. Recent work by Kay7 and Heller and co-workers8,9 reemphasizes this fact. For practical reasons, however, fo ...
... that explore complex-valued regions of phase space.1-6 For example, in the 1-d WKB approximation for barrier tunneling, the momentum of the particle is imaginary when it is inside the barrier. Recent work by Kay7 and Heller and co-workers8,9 reemphasizes this fact. For practical reasons, however, fo ...
Infinitely Disordered Critical Behavior in Higher Dimensional
... of collective phenomena. In this thesis we are going to study continuous quantum phase transitions, driven by quantum, rather than thermal fluctuations, originating from Heisenberg’s uncertainty principle at T = 0. The most impressive property of continuous phase transitions is their universality: t ...
... of collective phenomena. In this thesis we are going to study continuous quantum phase transitions, driven by quantum, rather than thermal fluctuations, originating from Heisenberg’s uncertainty principle at T = 0. The most impressive property of continuous phase transitions is their universality: t ...
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... is useful for understanding low energy (≈ 1 GeV) strong interaction scattering cross sections. Consider the two reactions (d = deuterium): pp → dπ+ pn → dπ0 ◆ Deuterium is an “iso-singlet”, |0,0>. ◆ In terms of isospin states we have: pp = |1/2,1/2>|1/2,1/2> dπ+ = |0,0>|1,1> pn = |1/2,1/2>|1/2,-1 ...
... is useful for understanding low energy (≈ 1 GeV) strong interaction scattering cross sections. Consider the two reactions (d = deuterium): pp → dπ+ pn → dπ0 ◆ Deuterium is an “iso-singlet”, |0,0>. ◆ In terms of isospin states we have: pp = |1/2,1/2>|1/2,1/2> dπ+ = |0,0>|1,1> pn = |1/2,1/2>|1/2,-1 ...
