Charge degrees of freedom on the kagome lattice
... Within condensed matter physics, systems with strong electronic correlations give rise to fascinating phenomena which characteristically require a physical description beyond a one-electron theory, such as high temperature superconductivity, or Mott metal-insulator transitions. In this thesis, a cla ...
... Within condensed matter physics, systems with strong electronic correlations give rise to fascinating phenomena which characteristically require a physical description beyond a one-electron theory, such as high temperature superconductivity, or Mott metal-insulator transitions. In this thesis, a cla ...
The search for magnetic monopoles
... that they are already fully understood and no longer pose unanswered fundamental physics questions. Indeed, for most practical purposes they are perfectly well described by classical electrodynamics, as formulated by James Clerk Maxwell in 1864. At a deeper level, a consistent quantum mechanical acc ...
... that they are already fully understood and no longer pose unanswered fundamental physics questions. Indeed, for most practical purposes they are perfectly well described by classical electrodynamics, as formulated by James Clerk Maxwell in 1864. At a deeper level, a consistent quantum mechanical acc ...
Molecular Modelling for Beginners
... concepts and ideas are difficult ones, and you will have to think long and hard about them; if it’s any consolation, so did the pioneers in our subject. I have given many of the derivations in full, and tried to avoid the dreaded phrase ‘it can be shown that’. There are various strands to our studies ...
... concepts and ideas are difficult ones, and you will have to think long and hard about them; if it’s any consolation, so did the pioneers in our subject. I have given many of the derivations in full, and tried to avoid the dreaded phrase ‘it can be shown that’. There are various strands to our studies ...
RADIATION REACTION AND SELF-FORCE IN CURVED SPACETIME IN A FIELD THEORY APPROACH
... the post-Newtonian (PN) formalism, which assumes that the two bodies, possibly spinning, are weakly gravitating sources moving at slow velocities under their mutual gravitational influences. Recently, the equations of motion for the two bodies and the radiation these emit have been computed using th ...
... the post-Newtonian (PN) formalism, which assumes that the two bodies, possibly spinning, are weakly gravitating sources moving at slow velocities under their mutual gravitational influences. Recently, the equations of motion for the two bodies and the radiation these emit have been computed using th ...
Chapter 7. Statistical Mechanics
... most probable energy E*. This, in turn, suggests that we may be able to model, aside from infrequent fluctuations, the behavior of systems with many molecules by focusing on the most probable situation (i.e., having the energy E*) and ignoring deviations from this case. It is for the reasons just sh ...
... most probable energy E*. This, in turn, suggests that we may be able to model, aside from infrequent fluctuations, the behavior of systems with many molecules by focusing on the most probable situation (i.e., having the energy E*) and ignoring deviations from this case. It is for the reasons just sh ...
Lecture 1
... – ρ(770): Γee = Γµµ = 7.0 keV – ω(780): Γee = Γµµ = 0.60 keV (actually dimuon mode is not that well measured.) – Φ(1020): Γee = Γµµ = 1.2 keV Can we understand the relative magnitudes? Just as for J/ψ, decay involves coupling to virtual photon. The φ is ssbar: electric charge factor (-1/3)2 Both ρ a ...
... – ρ(770): Γee = Γµµ = 7.0 keV – ω(780): Γee = Γµµ = 0.60 keV (actually dimuon mode is not that well measured.) – Φ(1020): Γee = Γµµ = 1.2 keV Can we understand the relative magnitudes? Just as for J/ψ, decay involves coupling to virtual photon. The φ is ssbar: electric charge factor (-1/3)2 Both ρ a ...
Spin-Resolved Spectroscopic Studies of Topologically Ordered Materials
... by Anderson localization [9] due to the inevitable presence of random impurities. Therefore no current carrying states exist in the sample bulk. Instead, building upon Laughlin’s arguments [4], Halperin showed that for a system with Hall conductivity σxy = ne2 /h, there must exist exactly n branches ...
... by Anderson localization [9] due to the inevitable presence of random impurities. Therefore no current carrying states exist in the sample bulk. Instead, building upon Laughlin’s arguments [4], Halperin showed that for a system with Hall conductivity σxy = ne2 /h, there must exist exactly n branches ...
ABSTRACT PHOTON PAIR PRODUCTION FROM A HOT ATOMIC ENSEMBLE IN THE DIAMOND CONFIGURATION
... mechanically correlated photon pair source. The generation medium used here is a laser pumped vapor cell of warm rubidium. The scheme takes advantage of a spontaneous four wave-mixing (4WM) interaction in the atoms to create photon pairs that are correlated in direction, frequency, polarization, and ...
... mechanically correlated photon pair source. The generation medium used here is a laser pumped vapor cell of warm rubidium. The scheme takes advantage of a spontaneous four wave-mixing (4WM) interaction in the atoms to create photon pairs that are correlated in direction, frequency, polarization, and ...
Parameterization and orbital angular momentum of anisotropic
... the amplitude factor becomes a bb. Alternatively, if we add a global phase of py4, we obtain ...
... the amplitude factor becomes a bb. Alternatively, if we add a global phase of py4, we obtain ...
80, 032307 (2009)
... applications. In this paper, we consider the suppression of the phase decoherence in an atomic qubit, which is composed of a single neutral atom confined in a far-detuned optical dipole trap. The qubit is defined by two hyperfine states of the atom. This system is an excellent candidate for quantum ...
... applications. In this paper, we consider the suppression of the phase decoherence in an atomic qubit, which is composed of a single neutral atom confined in a far-detuned optical dipole trap. The qubit is defined by two hyperfine states of the atom. This system is an excellent candidate for quantum ...
Photon trapping and transfer with solitons *
... fiber is characterized, ideally, by undistorted propagation and elastic collisions. It arises because of an intensity-dependent change in the fiber’s refractive index. For a temporal soliton, this refractive index change creates a traveling potential, which can serve as a waveguide for another optic ...
... fiber is characterized, ideally, by undistorted propagation and elastic collisions. It arises because of an intensity-dependent change in the fiber’s refractive index. For a temporal soliton, this refractive index change creates a traveling potential, which can serve as a waveguide for another optic ...