Three-dimensional electromagnetic breathers in carbon
... kn ¼ k ¼ 1 (equivalent to the pulse half-width along the axes Ox and Oy equal to Ly ¼ Lx ¼ kn c=x0 3 104 cm). Figure 1 presents the field intensity distribution in the array of CNTs in the planes nOf andpOf ffiffi at different instants of the dimensionless time s ¼ x0 t= e. The field intensity is ...
... kn ¼ k ¼ 1 (equivalent to the pulse half-width along the axes Ox and Oy equal to Ly ¼ Lx ¼ kn c=x0 3 104 cm). Figure 1 presents the field intensity distribution in the array of CNTs in the planes nOf andpOf ffiffi at different instants of the dimensionless time s ¼ x0 t= e. The field intensity is ...
Electromagnetic Wave Propagation in Periodic Porous Structures I
... incident light and the thickness of the structure are again of the same order, but they are only a factor of three times larger than the period. Although the theory developed in this paper requires these scales to be disparate, our results may offer some qualitative information about these devices. ...
... incident light and the thickness of the structure are again of the same order, but they are only a factor of three times larger than the period. Although the theory developed in this paper requires these scales to be disparate, our results may offer some qualitative information about these devices. ...
Notes for Solid State Theory FFF051/FYST25
... of solid state physics, such as Snoke (2008), Hofmann (2008), Ibach and Lüth (2003) or Kittel (1996), to which is frequently referred. Solid state theory is a large field and thus a 7.5 point course must restrict the material. E.g., important issues such as calculation schemes for the electronic st ...
... of solid state physics, such as Snoke (2008), Hofmann (2008), Ibach and Lüth (2003) or Kittel (1996), to which is frequently referred. Solid state theory is a large field and thus a 7.5 point course must restrict the material. E.g., important issues such as calculation schemes for the electronic st ...
ELECTRONS: THE HIGH ENERGY DISTRIBUTION S.
... spectrum permit the particle distribution function to attain a steady state. Electron runaway to infinite momentum occurs only on the column axis while at other radii, the distribution is cut off by the friction from th unstable waves. ...
... spectrum permit the particle distribution function to attain a steady state. Electron runaway to infinite momentum occurs only on the column axis while at other radii, the distribution is cut off by the friction from th unstable waves. ...
Using analogies to explain electrical relationships
... For example, the comparison between the G and k allows deeper understanding of the relationship between Fg and Fe. In the next table, is the relationship between gravitational field strength and electric field strength. Students have difficulty seeing that “little g” is a measurement of field streng ...
... For example, the comparison between the G and k allows deeper understanding of the relationship between Fg and Fe. In the next table, is the relationship between gravitational field strength and electric field strength. Students have difficulty seeing that “little g” is a measurement of field streng ...
Coherent whistler emissions in the magnetosphere
... features, a coherency and a wave packet structure, are difficult to explain in terms of linear theories of cyclotron resonant instability fed by a temperature anisotropy, since the theory predicts a broader frequency range of excited waves with random phases. We suggest that the coherent structure o ...
... features, a coherency and a wave packet structure, are difficult to explain in terms of linear theories of cyclotron resonant instability fed by a temperature anisotropy, since the theory predicts a broader frequency range of excited waves with random phases. We suggest that the coherent structure o ...
Spin and photophysics of carbon-antisite potential quantum bit Linköping University Post Print
... case, a closed shell singlet with a fully occupied a1 state and an empty e state forms. Since there is a gap between the a1 and e states one might consider the closed-shell singlet as the ground state. In this Rapid Communication, we show that the S = 1 state should be also considered, where the a1 ...
... case, a closed shell singlet with a fully occupied a1 state and an empty e state forms. Since there is a gap between the a1 and e states one might consider the closed-shell singlet as the ground state. In this Rapid Communication, we show that the S = 1 state should be also considered, where the a1 ...
Document
... Fig. 21.15 A charged body creates an electric field. Coulomb force of repulsion between two charged bodies at A and B, (having charges Q and qo respectively) has magnitude: ...
... Fig. 21.15 A charged body creates an electric field. Coulomb force of repulsion between two charged bodies at A and B, (having charges Q and qo respectively) has magnitude: ...
Physics
... recognise that, for a perfectly elastic collision between two bodies, the relative speed of approach is equal to the relative speed of separation ...
... recognise that, for a perfectly elastic collision between two bodies, the relative speed of approach is equal to the relative speed of separation ...
chapter2
... the model. Therefore we test the dependence on the field model by calculating L* for electrons at a range of radial distance and input Dst values. Figure 3 plots L* values calculated for electrons at X=-8-8, Y=0, and Z=0 in magnetic coordinates using Dst values from 20nT to –100 nT at 10nT interval ...
... the model. Therefore we test the dependence on the field model by calculating L* for electrons at a range of radial distance and input Dst values. Figure 3 plots L* values calculated for electrons at X=-8-8, Y=0, and Z=0 in magnetic coordinates using Dst values from 20nT to –100 nT at 10nT interval ...
