Towards a Quantum Programming Language
... for the classical hardware and the quantum device to be in the same physical location; it is even possible for several classical controllers to share access to a single quantum device. In quantum complexity theory, algorithms are often presented in a certain normal form: a quantum computation consis ...
... for the classical hardware and the quantum device to be in the same physical location; it is even possible for several classical controllers to share access to a single quantum device. In quantum complexity theory, algorithms are often presented in a certain normal form: a quantum computation consis ...
A continued fraction resummation form of bath
... QKE rates of the first three orders are numerically computed in a quantum Debye bath. In Sec. III, the continued fraction resummation form is developed, and the RQKE rates are numerically compared with the exact results of both unbiased and biased systems. In this paper, all the exact quantities are ...
... QKE rates of the first three orders are numerically computed in a quantum Debye bath. In Sec. III, the continued fraction resummation form is developed, and the RQKE rates are numerically compared with the exact results of both unbiased and biased systems. In this paper, all the exact quantities are ...
UTEP - The University of Texas at El Paso
... Step 3 – The pair whose sum is –11 is –5 and –6. Therefore, the critical integers are –5 and –6, 5 6 11 . Factoring Trinomials of the Form x 2 bx c To factor trinomials of the form x 2 bx c follow the same principle described above. Find two integers whose sum equals the middle term ...
... Step 3 – The pair whose sum is –11 is –5 and –6. Therefore, the critical integers are –5 and –6, 5 6 11 . Factoring Trinomials of the Form x 2 bx c To factor trinomials of the form x 2 bx c follow the same principle described above. Find two integers whose sum equals the middle term ...
Compendium of Theoretical Physics
... In the first chapter, Mechanics, we present the often overemphasized Newtonian approach to mechanics next to the Lagrange and Hamilton formulations. Each of these equivalent representations distinguishes itself by specific advantages: whereas Newton’s approach is most easily accessible using the conce ...
... In the first chapter, Mechanics, we present the often overemphasized Newtonian approach to mechanics next to the Lagrange and Hamilton formulations. Each of these equivalent representations distinguishes itself by specific advantages: whereas Newton’s approach is most easily accessible using the conce ...
Calculation of the integral magnetic field of a star - ewald
... variables with respect to the line of sight - without any relation to the cartographic coordinates of the star’s globe. The surface field is described by spherical harmonics. This makes the calculation of the phase curve rather difficult, because the rotation axis is tilted to the perpendicularly ar ...
... variables with respect to the line of sight - without any relation to the cartographic coordinates of the star’s globe. The surface field is described by spherical harmonics. This makes the calculation of the phase curve rather difficult, because the rotation axis is tilted to the perpendicularly ar ...
Fractionally charged impurity states of a fractional quantum Hall system
... e.g. s- or d-wave. Similarly, a fractional quantum Hall (FQH) system can support exotic quasiparticles that carry a fractional charge. These quasi-particles, predicted by Laughlin [3], were first observed in the nonequilibrium shot-noise of the current carrying FQH edge states [4]. More recently, ex ...
... e.g. s- or d-wave. Similarly, a fractional quantum Hall (FQH) system can support exotic quasiparticles that carry a fractional charge. These quasi-particles, predicted by Laughlin [3], were first observed in the nonequilibrium shot-noise of the current carrying FQH edge states [4]. More recently, ex ...
Experimental Implementation of Adiabatic Passage between
... limit corresponds to T; M → ∞; τ → 0. Using M ¼ 31, the optimized sweep reaches a theoretical fidelity > 99.5% of the final state with respect to the true ground state. For each step of the adiabatic passage, we designed the NMR pulse sequence to create an effective Hamiltonian, i.e., Ĥtol ½J m ( ...
... limit corresponds to T; M → ∞; τ → 0. Using M ¼ 31, the optimized sweep reaches a theoretical fidelity > 99.5% of the final state with respect to the true ground state. For each step of the adiabatic passage, we designed the NMR pulse sequence to create an effective Hamiltonian, i.e., Ĥtol ½J m ( ...
Topos logic in measurement-based quantum computation
... magic states [8], contextuality is necessary for both quantum computational universality and the hardness of classical simulation of quantum computation [9,10]. Contextuality also plays a role in measurement-based quantum computation (MBQC). If an MBQC on qubits evaluates a nonlinear Boolean functio ...
... magic states [8], contextuality is necessary for both quantum computational universality and the hardness of classical simulation of quantum computation [9,10]. Contextuality also plays a role in measurement-based quantum computation (MBQC). If an MBQC on qubits evaluates a nonlinear Boolean functio ...
Quantum error correction
... have no correspondence in classical information theory. These phenomena include decoherence, as a consequence of entanglement. Decoherence can also be understood as “information leakage”, i.e., knowledge of an event is transferred to the reservoir – an effect that in general destroys superpositions ...
... have no correspondence in classical information theory. These phenomena include decoherence, as a consequence of entanglement. Decoherence can also be understood as “information leakage”, i.e., knowledge of an event is transferred to the reservoir – an effect that in general destroys superpositions ...
Landau Gauge Quark Propagator with External Magnetic Fields
... field theory already long time ago, consolidating and deepening the significant insights into quantum physics that Quantum Electrodynamics (QED) had just given a few years before. The feature of asymptotic freedom [1] makes QCD behave like a free theory at small distances, making it easily treatable ...
... field theory already long time ago, consolidating and deepening the significant insights into quantum physics that Quantum Electrodynamics (QED) had just given a few years before. The feature of asymptotic freedom [1] makes QCD behave like a free theory at small distances, making it easily treatable ...
Lecture 1: Review of Quantum Mechanics, Introduction to Statistical
... Time Averages and State Averages Many microscopic states ⇔ one macroscopic / thermodynamic state (e.g., fixed E; V , N .) Our particles in a box can be in many, many degenerate states ∼ 10N . ...
... Time Averages and State Averages Many microscopic states ⇔ one macroscopic / thermodynamic state (e.g., fixed E; V , N .) Our particles in a box can be in many, many degenerate states ∼ 10N . ...
Some identities of Laguerre polynomials arising from differential
... is remarkable that a new family of generalized Laguerre polynomials are introduced in applying spectral methods for numerical treatments of FDEs in unbounded domains. They can also be used in solving some differential equations (see [–]). Also, it should be mentioned that the modified generalized ...
... is remarkable that a new family of generalized Laguerre polynomials are introduced in applying spectral methods for numerical treatments of FDEs in unbounded domains. They can also be used in solving some differential equations (see [–]). Also, it should be mentioned that the modified generalized ...
Calculating Floquet states of large quantum systems: A
... of the eigenvalue problem for the system Hamiltonian H. When the Hamiltonian is time-independent, this task can be executed by performing full diagonalization of the Hamiltonian matrix. When the system becomes too large the size of the matrix may not allow any longer for its full diagonalization. Th ...
... of the eigenvalue problem for the system Hamiltonian H. When the Hamiltonian is time-independent, this task can be executed by performing full diagonalization of the Hamiltonian matrix. When the system becomes too large the size of the matrix may not allow any longer for its full diagonalization. Th ...
Nonequilibrium entropy production in open and closed quantum
... quantum system to its thermal surroundings. Therefore, we start with an introductory chapter 2, in which we summarize the main developments in recent statistical physics for classical systems arbitrarily far from equilibrium. In particular, we will briefly summarize the notion of fluctuation theorem ...
... quantum system to its thermal surroundings. Therefore, we start with an introductory chapter 2, in which we summarize the main developments in recent statistical physics for classical systems arbitrarily far from equilibrium. In particular, we will briefly summarize the notion of fluctuation theorem ...
CDM article on quantum chaos - Department of Mathematics
... confirm this conjecture in the special case of arithmetic surfaces and Hecke eigenfunctions, but correct it with an extra arithmetic factor. A final direction we survey is the applications of quantum ergodicity to problems in nodal geometry. Given the large amount of work on matrix elements hAϕj , ϕ ...
... confirm this conjecture in the special case of arithmetic surfaces and Hecke eigenfunctions, but correct it with an extra arithmetic factor. A final direction we survey is the applications of quantum ergodicity to problems in nodal geometry. Given the large amount of work on matrix elements hAϕj , ϕ ...