PPT - Henry Haselgrove`s Homepage
... between the ●’s? We find that the entanglement is bounded by a function of the energy gap between ground and first exited states ...
... between the ●’s? We find that the entanglement is bounded by a function of the energy gap between ground and first exited states ...
document
... • quant-ph/0610203 (Lo, Preskill) Security of quantum key distribution using weak coherent states with nonrandom phases. Security proof that applies when key information is encoded in the relative phase of a coherent-state reference pulse and a weak coherent-state signal pulse. The proof works even ...
... • quant-ph/0610203 (Lo, Preskill) Security of quantum key distribution using weak coherent states with nonrandom phases. Security proof that applies when key information is encoded in the relative phase of a coherent-state reference pulse and a weak coherent-state signal pulse. The proof works even ...
The Yrast Spectra of Weakly Interacting Bose
... maximum alignment L = M ). Thus the relevant single particle states involve only a single non-negative quantum number, m. In the yrast state with total angular momentum h̄L, the motion in the oscillator will contribute an excitation energy Lh̄ω0 with respect to the ground state. However, this config ...
... maximum alignment L = M ). Thus the relevant single particle states involve only a single non-negative quantum number, m. In the yrast state with total angular momentum h̄L, the motion in the oscillator will contribute an excitation energy Lh̄ω0 with respect to the ground state. However, this config ...
JOYNT
... R = Σ |Re Oij – Re Oij′| and I = Σ |Im Oij – Im Oij′| R = I= 0 means that the algorithm has failed ! ...
... R = Σ |Re Oij – Re Oij′| and I = Σ |Im Oij – Im Oij′| R = I= 0 means that the algorithm has failed ! ...
CHAPTER 7: The Hydrogen Atom
... In ground state an atom cannot emit radiation. It can absorb electromagnetic radiation, or gain energy through inelastic bombardment by particles. ...
... In ground state an atom cannot emit radiation. It can absorb electromagnetic radiation, or gain energy through inelastic bombardment by particles. ...
CHEM3023: Spins, Atoms and Molecules
... • Is a fundamental law of nature: It can not be proved, but we know it works. Newton's second law of motion (F=m a) is another example of a law of nature. • Applies at the microscopic scale: electrons, atoms, molecules, etc. • What information can it provide? Every property that can be ...
... • Is a fundamental law of nature: It can not be proved, but we know it works. Newton's second law of motion (F=m a) is another example of a law of nature. • Applies at the microscopic scale: electrons, atoms, molecules, etc. • What information can it provide? Every property that can be ...
Pulsed Energy-Time Entangled Twin
... of the pulses during transmission. Moreover, polarization fluctuations and depolarization, inevitable in optical fibers, have no effect on our system, as already demonstrated by our long distance quantum correlation experiments [10,11]. Another significant advantage of our pulsed source is that the ...
... of the pulses during transmission. Moreover, polarization fluctuations and depolarization, inevitable in optical fibers, have no effect on our system, as already demonstrated by our long distance quantum correlation experiments [10,11]. Another significant advantage of our pulsed source is that the ...
In class exercises 3
... Let us see if this choice of units7 also works for the harmonic oscillator. (d) Phase-space density of states for a harmonic oscillator. Consider a harmonic oscillator with Hamiltonian H = p2 /2m + 1/2 mω 2 q 2 . Draw a picture of the energy surface with energy E, and find the volume (area) of phase ...
... Let us see if this choice of units7 also works for the harmonic oscillator. (d) Phase-space density of states for a harmonic oscillator. Consider a harmonic oscillator with Hamiltonian H = p2 /2m + 1/2 mω 2 q 2 . Draw a picture of the energy surface with energy E, and find the volume (area) of phase ...
No Slide Title
... g = 29 meV ; at n = 0.05, measured 1/T2 = 2.5 meV ; – no inhomogeneous broadening = 20 meV – with s = 6 meV reduced = 2 meV Organics? g ~ 80 meV ; T2 ?? Solid state laser materials? Dilute atomic gases (microwave cavity) ? dephasing rate ~ 10-3 x dipole coupling (reduce further by starting with ...
... g = 29 meV ; at n = 0.05, measured 1/T2 = 2.5 meV ; – no inhomogeneous broadening = 20 meV – with s = 6 meV reduced = 2 meV Organics? g ~ 80 meV ; T2 ?? Solid state laser materials? Dilute atomic gases (microwave cavity) ? dephasing rate ~ 10-3 x dipole coupling (reduce further by starting with ...
2. Atomic Structure 2.1 Historical Development of Atomic Theory
... “The more precisely the position is determined, the less precisely the momentum is known in this instant, and vice versa.” (Heisenberg, 1927) ...
... “The more precisely the position is determined, the less precisely the momentum is known in this instant, and vice versa.” (Heisenberg, 1927) ...
l - coercingmolecules
... Silberberg, M. 2010. Principles of General Chemistry. 2nd ed. New York: McGraw-Hill. ...
... Silberberg, M. 2010. Principles of General Chemistry. 2nd ed. New York: McGraw-Hill. ...
Periodic Boundary Conditions. Classical Limit ( + problems 27
... these wavepackets are almost the eignstates of the Hamiltonian, and, on the other hand, they behave like classical particles. Below we explicitly construct such packets and use them to derive classical Maxwell-Boltzmann distribution from quantum statistics. Maxwell-Boltzmann Distribution As we demo ...
... these wavepackets are almost the eignstates of the Hamiltonian, and, on the other hand, they behave like classical particles. Below we explicitly construct such packets and use them to derive classical Maxwell-Boltzmann distribution from quantum statistics. Maxwell-Boltzmann Distribution As we demo ...
What is Quantum Computation? - IC
... Measurement can only yield one classical bit • Choose basis (x/y, left/right, etc) representing orthogonal polarisations (antipodal points on Bloch sphere) • Find photon in one or other channel with certain probability ...
... Measurement can only yield one classical bit • Choose basis (x/y, left/right, etc) representing orthogonal polarisations (antipodal points on Bloch sphere) • Find photon in one or other channel with certain probability ...
Slides from lecture 4.
... Now put 18 people (electrons) in the auditorium (atom). Note that no two people (electrons) can occupy the same seat (state)! So, when one row is filled, a new row is started. This is a fundamental property of quantum mechanics, i.e., no two electrons in an atom can exist in the same state. It is ca ...
... Now put 18 people (electrons) in the auditorium (atom). Note that no two people (electrons) can occupy the same seat (state)! So, when one row is filled, a new row is started. This is a fundamental property of quantum mechanics, i.e., no two electrons in an atom can exist in the same state. It is ca ...