
Summary
... With the realization of coherent, laser-like atoms in the form of Bose-Einstein condensates it has become possible to explore matter-wave amplification, a process in which the number of atoms in a quantum state is amplified due to bosonic stimulation. In previous amplifiers based on superradiant Ray ...
... With the realization of coherent, laser-like atoms in the form of Bose-Einstein condensates it has become possible to explore matter-wave amplification, a process in which the number of atoms in a quantum state is amplified due to bosonic stimulation. In previous amplifiers based on superradiant Ray ...
Lecture 5
... • We are interested in the behavior of electronic energy levels in crystalline materials (any, not just semiconductors!) as a function of wavevector k or momentum p = ħk ...
... • We are interested in the behavior of electronic energy levels in crystalline materials (any, not just semiconductors!) as a function of wavevector k or momentum p = ħk ...
Chapter 10 • We want to complete our discussion of quantum Schr
... gets smaller, the momentum gets smaller. If we somehow want to hold onto the de Broglie relation even for quanta that are not free. The “wavelength” must be getting larger as E – V gets smaller (i.e. smaller p). The wave function, which is an energy eigenfunction, must look something like the follow ...
... gets smaller, the momentum gets smaller. If we somehow want to hold onto the de Broglie relation even for quanta that are not free. The “wavelength” must be getting larger as E – V gets smaller (i.e. smaller p). The wave function, which is an energy eigenfunction, must look something like the follow ...
General Properties of Electromagnetic Radiation
... 1. The cathode was connected to the positive terminal of the variable voltage source, where it is more difficult to release electrons from cathode surface. 2. The anode was connected to the negative terminal of the voltage source which makes it more difficult for the electron to collide with the ano ...
... 1. The cathode was connected to the positive terminal of the variable voltage source, where it is more difficult to release electrons from cathode surface. 2. The anode was connected to the negative terminal of the voltage source which makes it more difficult for the electron to collide with the ano ...
From Billiard Balls to Quantum Computing: Geoff Sharman
... energy required per computational step - showed that at least kT log2 energy is expended when 1 bit is discarded (known as the Landauer limit) - where k is Boltzmann's constant and T is temperature ...
... energy required per computational step - showed that at least kT log2 energy is expended when 1 bit is discarded (known as the Landauer limit) - where k is Boltzmann's constant and T is temperature ...
Honors Chemistry Midterm Review 2008
... c. John Dalton- First atomic theory; Atoms solid spheres; Law of Multiple Proportions d. Eugene Goldstein- Cathode rays; lead to the discovery of the electrons 1886; discovered protons e. JJ Thompson- “ Plum Pudding model of the atom f. Werner Heisenberg- quantum mechanics; uncertainty principle ; m ...
... c. John Dalton- First atomic theory; Atoms solid spheres; Law of Multiple Proportions d. Eugene Goldstein- Cathode rays; lead to the discovery of the electrons 1886; discovered protons e. JJ Thompson- “ Plum Pudding model of the atom f. Werner Heisenberg- quantum mechanics; uncertainty principle ; m ...
III. Quantum Model of the Atom
... Orientation of orbital Specifies the exact orbital within each sublevel ...
... Orientation of orbital Specifies the exact orbital within each sublevel ...
are WAVES. PARTICLES!
... unthinkable. But what end?” “There is the great standing perennial problem to which human reason is as far from an answer as ever.” ...
... unthinkable. But what end?” “There is the great standing perennial problem to which human reason is as far from an answer as ever.” ...
Preprint
... their smaller mass. (2) Use stronger coupling than second-order tunneling in the form of electrostatic interactions. This can be realized with Rydberg admixtures, or polar molecules which interact via strong electric dipole moments. (3) A third possibility is to realize magnetic ordering not with sp ...
... their smaller mass. (2) Use stronger coupling than second-order tunneling in the form of electrostatic interactions. This can be realized with Rydberg admixtures, or polar molecules which interact via strong electric dipole moments. (3) A third possibility is to realize magnetic ordering not with sp ...
Experiments in “Quantum Erasure” and “Delayed
... chance of being in any of the set of two trajectories that exit the slits and impact at one point on the screen. At the screen, it has no chance of passing it. It therefore “descends” out of higher dimensional reality and “chooses” probabilistically any point where the double-slit pattern can fo ...
... chance of being in any of the set of two trajectories that exit the slits and impact at one point on the screen. At the screen, it has no chance of passing it. It therefore “descends” out of higher dimensional reality and “chooses” probabilistically any point where the double-slit pattern can fo ...
Atoms: Some Basics
... a product of symbols of the form nk which represents k electrons in the orbital n, . n is the principal quantum number, which characterizes the radial motion and has the largest influence on the energy. n and m are written numerically, but the spdf ... coding is used for . An example of the configu ...
... a product of symbols of the form nk which represents k electrons in the orbital n, . n is the principal quantum number, which characterizes the radial motion and has the largest influence on the energy. n and m are written numerically, but the spdf ... coding is used for . An example of the configu ...
Canonical quantization of scalar fields
... Recall, in classical mechanics, starting with lagrangian as a function of coordinates and their time derivatives we define conjugate ...
... Recall, in classical mechanics, starting with lagrangian as a function of coordinates and their time derivatives we define conjugate ...
Quantum Disentanglement Eraser
... • ‘Clicks’ at D1 or D2 erase the which path information (Fringes!!) • absence or restoration of interference can be arranged via an appropriately contrived photon correlation experiment. ...
... • ‘Clicks’ at D1 or D2 erase the which path information (Fringes!!) • absence or restoration of interference can be arranged via an appropriately contrived photon correlation experiment. ...
Chapter 7 Atomic Structure and Periodicity Study Guide
... (2) frequency (ν)- a number of waves (cycles) per sec that pass a give point in space, measured in Hertz (which is cycles per sec = 1/sec = sec-1) ...
... (2) frequency (ν)- a number of waves (cycles) per sec that pass a give point in space, measured in Hertz (which is cycles per sec = 1/sec = sec-1) ...
1 Chemical kinetics
... • InfraRed waves (frequency: THz, wavelength ≈ micrometer), can exchange energy with the vibrational levels of molecules, givin informations about the kind of atoms and bounds present. Due to quantum selection rules, only some modes can interact direcltly with the EMF; still the others can be invest ...
... • InfraRed waves (frequency: THz, wavelength ≈ micrometer), can exchange energy with the vibrational levels of molecules, givin informations about the kind of atoms and bounds present. Due to quantum selection rules, only some modes can interact direcltly with the EMF; still the others can be invest ...
powerpoint
... be determined exactly simultaneously. One component cannot exhaust the total momentum (because of “+1” in l(l +1) ). The angular momentum is quantized in both its length and orientation – it cannot point at any arbitrary direction (space quantization). ...
... be determined exactly simultaneously. One component cannot exhaust the total momentum (because of “+1” in l(l +1) ). The angular momentum is quantized in both its length and orientation – it cannot point at any arbitrary direction (space quantization). ...
Problem set 6
... Show that we can always define a new real function of time h(t) and a new hermitian operator H such that H(t) = h(t)H . Express h(t) and H in terms of c(t) and K and any other appropriate quantities. 2. Consider the functional equation for a complex-valued function of one real variable f (t + s) = f ...
... Show that we can always define a new real function of time h(t) and a new hermitian operator H such that H(t) = h(t)H . Express h(t) and H in terms of c(t) and K and any other appropriate quantities. 2. Consider the functional equation for a complex-valued function of one real variable f (t + s) = f ...