Atomic Collisions and Backscattering Spectrometry
... Of all the analytical techniques, Rutherford backscattering spectrometry is perhaps the easiest to understand and to apply because it is based on classical scattering in a central-force field. Aside from the accelerator, which provides a collimated beam of MeV particles (usually 4 He+ ions), the inst ...
... Of all the analytical techniques, Rutherford backscattering spectrometry is perhaps the easiest to understand and to apply because it is based on classical scattering in a central-force field. Aside from the accelerator, which provides a collimated beam of MeV particles (usually 4 He+ ions), the inst ...
authentication with quantum smart-card
... indicates acceptance or rejection. The classical basis states of V are called a and r by convention. For any fixed key k, we denote the corresponding super-operators by Ak and Bk . ...
... indicates acceptance or rejection. The classical basis states of V are called a and r by convention. For any fixed key k, we denote the corresponding super-operators by Ak and Bk . ...
1 Correlated Electrons: Why we need Models to - cond
... point this functional gives the free energy of the system. One can use a different Legendre transform and obtain functionals of the self-energy Σ [14], or complicated functionals of two variables G and Γ [15], or a more simple functional of G and screened Coulomb interactions W [10] which is useful ...
... point this functional gives the free energy of the system. One can use a different Legendre transform and obtain functionals of the self-energy Σ [14], or complicated functionals of two variables G and Γ [15], or a more simple functional of G and screened Coulomb interactions W [10] which is useful ...
Variational method for ground-state energy of helium atom in N
... Clearly, the above equation shows that the effective nuclear charge which is seen by the electron depends on the space dimension N , and for the three-dimensional space (N = 3) it yields an effective charge Z = 27/16 = 1.6875. With the help of eq. (37), it is tempting to calculate the effective nuclear ...
... Clearly, the above equation shows that the effective nuclear charge which is seen by the electron depends on the space dimension N , and for the three-dimensional space (N = 3) it yields an effective charge Z = 27/16 = 1.6875. With the help of eq. (37), it is tempting to calculate the effective nuclear ...
Ultracold Atoms in Artificial Gauge Fields by Tobias Graß PhD Thesis
... The present thesis studies a variety of cold atomic systems in artificial gauge fields. In the first part we focus on fractional quantum Hall effects, asking whether interesting topological states can be realized with cold atoms. We start by making a close connection to solid-state systems and first ...
... The present thesis studies a variety of cold atomic systems in artificial gauge fields. In the first part we focus on fractional quantum Hall effects, asking whether interesting topological states can be realized with cold atoms. We start by making a close connection to solid-state systems and first ...
"Liquid-State NMR Quantum Computing" in
... Classical and quantum computers both represent information in the form of binary digits (bit). When we use spins for representing information, we arbitrarily assign “0” to a spin up and “1” to a spin down. As shown in Figure 1, we need a sufficiently large number of spins to store the information th ...
... Classical and quantum computers both represent information in the form of binary digits (bit). When we use spins for representing information, we arbitrarily assign “0” to a spin up and “1” to a spin down. As shown in Figure 1, we need a sufficiently large number of spins to store the information th ...
Monday, Mar. 28, 2005
... • This QN is found to be conserved in strong interactions • But not conserved in EM or Weak interactions • Third component of isospin QN is assigned to be positive for the particles with larger electric charge • Isospin is not a space-time symmetry • Cannot be assigned uniquely to leptons and photon ...
... • This QN is found to be conserved in strong interactions • But not conserved in EM or Weak interactions • Third component of isospin QN is assigned to be positive for the particles with larger electric charge • Isospin is not a space-time symmetry • Cannot be assigned uniquely to leptons and photon ...