Critical parameters for the heliumlike atoms: A phenomenological
									
... charge is still large enough to bind the two electrons. In the limit l→l 2 c the second local maxima reaches the same height of the first one. For l51.105.l (12) the second c maxima at large distance is getting larger and the second electron is far away from the fixed one. In this region the nuclear ...
                        	... charge is still large enough to bind the two electrons. In the limit l→l 2 c the second local maxima reaches the same height of the first one. For l51.105.l (12) the second c maxima at large distance is getting larger and the second electron is far away from the fixed one. In this region the nuclear ...
									Conservation of Energy in Classical Mechanics and Its Lack from the
									
... In result, the best examined motions could be classified as belonging to two domains. One of them concerned the periodic motions where the body returns to its original position after some period of time, another domain of mechanics considered typical progressive motions in space and time. For this s ...
                        	... In result, the best examined motions could be classified as belonging to two domains. One of them concerned the periodic motions where the body returns to its original position after some period of time, another domain of mechanics considered typical progressive motions in space and time. For this s ...
									Quantum Theory of Hydrogen
									
... Quantum Theory of the Hydrogen Atom 6.1 Schrödinger's Equation for the Hydrogen Atom We have discovered a "new" theory—quantum mechanics as exemplified by Schrödinger's equation. ...
                        	... Quantum Theory of the Hydrogen Atom 6.1 Schrödinger's Equation for the Hydrogen Atom We have discovered a "new" theory—quantum mechanics as exemplified by Schrödinger's equation. ...
									Beables for Quantum Electrodynamics
									
... of the Dirac quantum field theory, axed around the notion of negativeenergy electrons. In that approach, there are only particles of charge −e but of positive and negative energy: their total number (fermionnumber) is conserved. We will see that this approach is a convenient one to study localized pr ...
                        	... of the Dirac quantum field theory, axed around the notion of negativeenergy electrons. In that approach, there are only particles of charge −e but of positive and negative energy: their total number (fermionnumber) is conserved. We will see that this approach is a convenient one to study localized pr ...
									5.2 The Wave Equation
									
... y = A e j ( kx - ωt ) = A cos ( kx - ωt ) + j A sin ( kx - ωt ) . (A free particle is one which is not acted on by external forces, including those giving rise to a potential.) If we take the real part of y, we have the displacement of waves in a stretched string. (Beiser's equations are slightly di ...
                        	... y = A e j ( kx - ωt ) = A cos ( kx - ωt ) + j A sin ( kx - ωt ) . (A free particle is one which is not acted on by external forces, including those giving rise to a potential.) If we take the real part of y, we have the displacement of waves in a stretched string. (Beiser's equations are slightly di ...
									Overview of Atomic Structure and Collision Theory - OPEN-ADAS
									
... (antisymmetric) basis states ψν (an N -product of one-electron orbitals) with expansion coefficients aν . Spherically symmetric problem → (θ, φ) problem solved. Use standard angular algebra methods and packages are used, mostly based on Racah algebra but also Condon and Shortley (Slater-states). Onl ...
                        	... (antisymmetric) basis states ψν (an N -product of one-electron orbitals) with expansion coefficients aν . Spherically symmetric problem → (θ, φ) problem solved. Use standard angular algebra methods and packages are used, mostly based on Racah algebra but also Condon and Shortley (Slater-states). Onl ...
									Chapter 3 Symmetry in quantum mechanics
									
... Remark : for the previous statement to be valid, it is important that the eigenstates of H are non-degenerate , otherwise is does not hold. For instance, consider the hydrogen atom in the non-relativistic limit, H = T + V (r), ...
                        	... Remark : for the previous statement to be valid, it is important that the eigenstates of H are non-degenerate , otherwise is does not hold. For instance, consider the hydrogen atom in the non-relativistic limit, H = T + V (r), ...
									Holonomic Quantum Computation with Josephson Networks
									
... novel approach to quantum computation, information is encoded in a degenerate eigenspace of a parametric family of Hamiltonians. The gates are realized in terms of the non-Abelian Berry connection obtained by changing the control parameters adiabatically along closed contours in the parameter space ...
                        	... novel approach to quantum computation, information is encoded in a degenerate eigenspace of a parametric family of Hamiltonians. The gates are realized in terms of the non-Abelian Berry connection obtained by changing the control parameters adiabatically along closed contours in the parameter space ...
									of THE by 0.
									
... was first made by Bethe and published two weeks after the results of Lamb and Retherford. ...
                        	... was first made by Bethe and published two weeks after the results of Lamb and Retherford. ...