Holonomic quantum computation with neutral atoms
... The standard paradigm of quantum computation (QC) [1] is a dynamical one: in order to manipulate the quantum state of systems encoding information, local interactions between low dimensional subsystems (qubits) are switched on and off in such a way to enact a sequence of quantum gates. On the other h ...
... The standard paradigm of quantum computation (QC) [1] is a dynamical one: in order to manipulate the quantum state of systems encoding information, local interactions between low dimensional subsystems (qubits) are switched on and off in such a way to enact a sequence of quantum gates. On the other h ...
Heisenberg, Matrix Mechanics, and the Uncertainty Principle Genesis
... coefficients. It is like saying that in a coin toss experiment whose outcome is a “head”, the coin could have been in a state which was a combination of head and tail before it was tossed! Of course, this would never be the case for actual coins, governed as they are by the laws of classical physics ...
... coefficients. It is like saying that in a coin toss experiment whose outcome is a “head”, the coin could have been in a state which was a combination of head and tail before it was tossed! Of course, this would never be the case for actual coins, governed as they are by the laws of classical physics ...
Titles and Abstracts
... Abstract: The Bethe ansatz is a key tool in the area of quantum integrable and exactly solvable models. For each such model, understanding the nature of the roots of the Bethe ansatz equations is central to understanding the mathematical physics underpinning the model’s behaviour. Here we analyse an ...
... Abstract: The Bethe ansatz is a key tool in the area of quantum integrable and exactly solvable models. For each such model, understanding the nature of the roots of the Bethe ansatz equations is central to understanding the mathematical physics underpinning the model’s behaviour. Here we analyse an ...
Slides - WFU Physics
... 2. Solve Green’s function equations in curved spacetime S x, x 4 x x ' 3. Use Green’s functions to calculate expectation value of T ...
... 2. Solve Green’s function equations in curved spacetime S x, x 4 x x ' 3. Use Green’s functions to calculate expectation value of T ...
2.4. Quantum Mechanical description of hydrogen atom
... We want to prove that in the ground state of hydrogen atom l=0: we put it into the magnetic field. We assume one beam: ...
... We want to prove that in the ground state of hydrogen atom l=0: we put it into the magnetic field. We assume one beam: ...
Quantum Physics 2005 Notes-6 Solving the Time Independent Schrodinger Equation
... If we know the values of ! j and ! j #1 near some point, we can solve for ! j+1. We can usually get ! j and ! j #1 from the continuity or symmetry conditions at a point. The only parameter with which to achieve agreement of the wavefunction with expected behavior is % . Notes 6 ...
... If we know the values of ! j and ! j #1 near some point, we can solve for ! j+1. We can usually get ! j and ! j #1 from the continuity or symmetry conditions at a point. The only parameter with which to achieve agreement of the wavefunction with expected behavior is % . Notes 6 ...
Copenhagen Interpretation
... There exist paired quantities… the combined uncertainty of which will remain above a set level. MOMENTUM vs. POSITION ENERGY CONTENT vs. TIME ...
... There exist paired quantities… the combined uncertainty of which will remain above a set level. MOMENTUM vs. POSITION ENERGY CONTENT vs. TIME ...
Exact reduced dynamics and
... techniques is mathematically simple and physically clear, and allows us to treat systems and environments that could all be strongly coupled ...
... techniques is mathematically simple and physically clear, and allows us to treat systems and environments that could all be strongly coupled ...
The statistical interpretation of quantum mechanics
... For a brief period at the beginning of 1926, it looked as though there were, suddenly, two self-contained but quite distinct systems of explanation extant: matrix mechanics and wave mechanics. But Schrödinger himself soon demonstrated their complete equivalence. Wave mechanics enjoyed a very great d ...
... For a brief period at the beginning of 1926, it looked as though there were, suddenly, two self-contained but quite distinct systems of explanation extant: matrix mechanics and wave mechanics. But Schrödinger himself soon demonstrated their complete equivalence. Wave mechanics enjoyed a very great d ...
