reciprocal lattice vector वाक्य
उदाहरण वाक्य
मोबाइल
- .. . is a reciprocal lattice vector of the reciprocal lattice.
- Another helpful ingredient in the proof is the " reciprocal lattice vectors ".
- These reciprocal lattice vectors of the FCC represent the basis vectors of a BCC real lattice.
- E are energies, k and q are wave vectors and G denotes a reciprocal lattice vector.
- An arbitrary vector, G, defines the reciprocal lattice vector between the ends of any two k vectors.
- Consider what happens when the lattice vectors are varied, resulting in a change in the reciprocal lattice vectors.
- The dispersion relations show conics of the free-electron energy dispersion parabolas for all possible reciprocal lattice vectors.
- Physically, the reciprocal lattice vectors act as additional chunks of momentum which the lattice can impart to the phonon.
- Measuring the momentum of one electronic state gives a distribution of momenta which are all separated by reciprocal lattice vectors.
- In accordance with Bragg's law, each ring corresponds to a particular reciprocal lattice vector G in the sample crystal.
- The electric or magnetic fields are expanded for each field component in terms of the Fourier series components along the reciprocal lattice vector.
- Phonon quasimomentum is defined as ! q and differs from normal momentum because it is only defined within an arbitrary reciprocal lattice vector.
- Similarly, the dielectric permittivity ( which is periodic along reciprocal lattice vector for photonic crystals ) is also expanded through Fourier series components.
- A 2D data point is defined by the length of a reciprocal lattice vector and its ( acute ) angle with another reciprocal lattice vector.
- A 2D data point is defined by the length of a reciprocal lattice vector and its ( acute ) angle with another reciprocal lattice vector.
- The magnitude of the reciprocal lattice vector is given in reciprocal length and is equal to the reciprocal of the interplanar spacing of the real space planes.
- With the Fourier series coefficients being the K numbers subscripted by m, n respectively, and the reciprocal lattice vector given by \ vec { G }.
- The third parameter specifying the reciprocal lattice vector is the angle \ phi formed by the X-ray beam and the plane containing \ zeta and \ xi.
- When the values of the off-diagonal elements U _ { \ bold { G } } between the reciprocal lattice vectors in the Hamiltonian almost go to zero.
- As a result the aggregate will be split in high and low energy components when the kinetic energy increases and the wave vector approaches the length of the reciprocal lattice vectors.
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