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Quantum blockade and loop currents in graphene with topological defects
Quantum blockade and loop currents in graphene with topological defects

... Graphene is a single layer of graphite with a honeycomb lattice consisting of two triangular sublattices. This peculiar structure of graphene gives rise to two linear “Dirac-type” energy dispersion spectra around two degenerate and inequivalent points K and K⬘ at the corner of the Brillouin zone.1,2 ...
Propagation of electromagnetic waves in the plasma near electron
Propagation of electromagnetic waves in the plasma near electron

HS-SCI-CP -- Chapter 19- Magnetism
HS-SCI-CP -- Chapter 19- Magnetism

Electron dephasing scattering rate in two
Electron dephasing scattering rate in two

Print - Science Advances
Print - Science Advances

... the switching of multiple nano-antiferromagnets via a substrate-mediated interaction (Fig. 1A). Both the trimer and the nano-antiferromagnets are assembled using a low-temperature STM with Fe atoms on a monolayer copper nitride (Cu2N) surface on a Cu(100) substrate (17, 25). The nanoantiferromagnets ...
Aspects of the Quantum Hall Effect
Aspects of the Quantum Hall Effect

85, 155302 (2012)
85, 155302 (2012)

... Frequently, the quantum state on the topological side of a TQCP can be distinguished by certain nontrivial statistical properties of its excitations,4–7 as well as a novel ground state quantum degeneracy which is not associated with any symmetry in the underlying Hamiltonian.7 An example is provided ...
Superradiance, subradiance, and suppressed superradiance of
Superradiance, subradiance, and suppressed superradiance of

Can the Wave Function in Configuration Space Be Replaced by
Can the Wave Function in Configuration Space Be Replaced by

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Exam 1

... ____ 10. A proton and electon are in a constant E-field as shown. You release an electron and proton at a point equidistant between the plates. Which particle has more kinetic energy when they strike the plates? ...
Stationary Solutions of the Klein-Gordon Equation in a Potential Field
Stationary Solutions of the Klein-Gordon Equation in a Potential Field

... wave functions in two inertial frames of reference. If we define the stationary state wave functions as special solutions like Ψ(r, t) = ψ(r)e−iEt/h̄ , and define m = E/c2 , which is called the mass of the system, then the Klein-Gordon equation can clearly be expressed in a better form when compared ...
Differentiation of vectors
Differentiation of vectors

... that the result of applying such a function is a real number, which is a scalar quantity. We now wish to consider vector-valued functions f : D → Rm . In principal, m can be any positive integer, but we will only consider the cases where m = 2 or 3, and the results of applying the function is either ...
Problems on Propagation
Problems on Propagation

... In the region defined by y < 0, filled with a nonmagnetic material (medium 1), is propagating a plane wave of frequency 1.5 GHz that is characterized by the phasor ~ i (x, y) = ẑE0 e−j4π(4x+3y) (V/m). E This wave impinges obliquely on the interface with the region y > 0, that is filled with air. (a ...
Introduction to NMR spectroscopy Nuclei of isotopes which possess
Introduction to NMR spectroscopy Nuclei of isotopes which possess

... In this scale TMS is arbitrarily assigned a value of zero. TMS is used because its protons are more highly shielded than those observed in most common organic molecules and because it is chemically inert. For 1 H NMR, the δ scale generally extends from 0-12 ppm and then each chemically inequivalent ...
Magnetic structure and hysteresis in hard magnetic nanocrystalline film: Computer simulation
Magnetic structure and hysteresis in hard magnetic nanocrystalline film: Computer simulation

This resource provides guidance for teaching the Interactions
This resource provides guidance for teaching the Interactions

Gauge Field Theory - High Energy Physics Group
Gauge Field Theory - High Energy Physics Group

Chapter 11 The Uniform Plane Wave
Chapter 11 The Uniform Plane Wave

... direction. Both the electric and magnetic fields are perpendicular to the direction of propagation, or both lie in a plane that is transverse to the direction of propagation; the uniform plane wave is a transverse electromagnetic wave, or a TEM wave. Some feeling for the way in which the fields vary ...
Quantum control of a Landau-quantized two
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Photorefractive quantum  wells:  transverse Franz-Keldysh  geometry
Photorefractive quantum wells: transverse Franz-Keldysh geometry

... Franz-Keldysh geometry are addressed, and the onedimensional transport equations are solved. The respective roles of carrier diffusion and drift are described, with an emphasis on new behavior related to interband photoexcitation. Limitations of the one-dimensional transport model are discussed, wit ...
Gauge Field Theory - High Energy Physics Group
Gauge Field Theory - High Energy Physics Group

... In particular, ψ ∗ ψ integrated over all space, is constant in time. This is a notion which is probably familiar to you from classical mechanics and electromagnetism. It says that ψ ∗ ψ, which we interpret as the probability density in QM, is conserved, meaning that the probability interpretation is ...
Coherence of atomic matter-wave fields - IAP TU
Coherence of atomic matter-wave fields - IAP TU

Atomic Parity Non-Conservation in Francium: The FrPNC Ex
Atomic Parity Non-Conservation in Francium: The FrPNC Ex

Spacetime physics with geometric algebra
Spacetime physics with geometric algebra

... Dirac matrices. In view of what we know about STA, this correspondence reveals the physical significance of the Dirac matrices, appearing so mysteriously in relativistic quantum mechanics: The Dirac matrices are no more and no less than matrix representations of an orthonormal frame of spacetime vec ...
Ultracold Atoms in Line-World: Bose
Ultracold Atoms in Line-World: Bose

... of matter predated those experiments by some 70 years [5]. From first principle, Bose derived the statistical behavior of photons. Upon receiving his draft, Einstein personally translated it into German to be published in the Zeitschrift für Physik [6], and then he extended the idea to matter [7]. ...
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Aharonov–Bohm effect

The Aharonov–Bohm effect, sometimes called the Ehrenberg–Siday–Aharonov–Bohm effect, is a quantum mechanical phenomenon in which an electrically charged particle is affected by an electromagnetic field (E, B), despite being confined to a region in which both the magnetic field B and electric field E are zero. The underlying mechanism is the coupling of the electromagnetic potential with the complex phase of a charged particle's wavefunction, and the Aharonov–Bohm effect is accordingly illustrated by interference experiments.The most commonly described case, sometimes called the Aharonov–Bohm solenoid effect, takes place when the wave function of a charged particle passing around a long solenoid experiences a phase shift as a result of the enclosed magnetic field, despite the magnetic field being negligible in the region through which the particle passes and the particle's wavefunction being negligible inside the solenoid. This phase shift has been observed experimentally. There are also magnetic Aharonov–Bohm effects on bound energies and scattering cross sections, but these cases have not been experimentally tested. An electric Aharonov–Bohm phenomenon was also predicted, in which a charged particle is affected by regions with different electrical potentials but zero electric field, but this has no experimental confirmation yet. A separate ""molecular"" Aharonov–Bohm effect was proposed for nuclear motion in multiply connected regions, but this has been argued to be a different kind of geometric phase as it is ""neither nonlocal nor topological"", depending only on local quantities along the nuclear path.Werner Ehrenberg and Raymond E. Siday first predicted the effect in 1949, and similar effects were later published by Yakir Aharonov and David Bohm in 1959. After publication of the 1959 paper, Bohm was informed of Ehrenberg and Siday's work, which was acknowledged and credited in Bohm and Aharonov's subsequent 1961 paper.Subsequently, the effect was confirmed experimentally by several authors; a general review can be found in Peshkin and Tonomura (1989).
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