Theoretical and experimental status of magnetic monopoles
... observation that the phase unobservability in quantum mechanics permits singularities manifested as sources of magnetic fields, just as point electric monopoles are sources of electric fields. This was only possible if the product of electric and magnetic charges was quantized. This prediction was an ...
... observation that the phase unobservability in quantum mechanics permits singularities manifested as sources of magnetic fields, just as point electric monopoles are sources of electric fields. This was only possible if the product of electric and magnetic charges was quantized. This prediction was an ...
Coherent Spin Dynamics of a Spin-1 Bose-Einstein
... F.1 BEC radius vs. expansion time. . . . . . . . . . . . . . . . . . . . . . . . . . ...
... F.1 BEC radius vs. expansion time. . . . . . . . . . . . . . . . . . . . . . . . . . ...
The general theory of first-order spatio-temporal
... Ultrashort laser pulses are usually expressed separately in terms of the temporal and spatial dependences of their electric field. In this formalism, it is implicitly assumed that the spatial or spatial frequency dependence of the pulse is completely separable from time or frequency dependence. Howe ...
... Ultrashort laser pulses are usually expressed separately in terms of the temporal and spatial dependences of their electric field. In this formalism, it is implicitly assumed that the spatial or spatial frequency dependence of the pulse is completely separable from time or frequency dependence. Howe ...
Efimov Trimers under Strong Confinement
... three-body potential VðRÞ, where the hyperradius R2 ¼ r21 þ r22 þ r23 is defined in terms of the atom positions ri at a vanishing center-of-mass coordinate. The potential appears in an effective hyperradial Schrödinger equation ½−ð1=2mÞ∂ 2 =∂R2 þ VðRÞf 0 ðRÞ ¼ ðE3 þ ωz Þf 0 ðRÞ, where we ignore all ...
... three-body potential VðRÞ, where the hyperradius R2 ¼ r21 þ r22 þ r23 is defined in terms of the atom positions ri at a vanishing center-of-mass coordinate. The potential appears in an effective hyperradial Schrödinger equation ½−ð1=2mÞ∂ 2 =∂R2 þ VðRÞf 0 ðRÞ ¼ ðE3 þ ωz Þf 0 ðRÞ, where we ignore all ...
E vac Space Charge - MSU College of Engineering
... Streetman explanation brings out scattering and group ...
... Streetman explanation brings out scattering and group ...
Ultracold atoms in optical lattices with long- PhD Thesis
... In most theoretical descriptions, the atoms are treated as simple, structureless quantum particles (see section 2.1 for more details on the type of theoretical description that will be relevant for this thesis). That does not mean that their internal structure is irrelevant: there are many proposals ...
... In most theoretical descriptions, the atoms are treated as simple, structureless quantum particles (see section 2.1 for more details on the type of theoretical description that will be relevant for this thesis). That does not mean that their internal structure is irrelevant: there are many proposals ...
Quantum-dot lithium in zero magnetic field: Electronic properties
... E th and the number of many-body quantum states N mbs involved in the expansion 共7兲. One sees that including about 1000 many-body states leads to very accurate results for the energy at ⭐20. Notice that below I present results for the energy in the interval ⭐10, where the method is practically exa ...
... E th and the number of many-body quantum states N mbs involved in the expansion 共7兲. One sees that including about 1000 many-body states leads to very accurate results for the energy at ⭐20. Notice that below I present results for the energy in the interval ⭐10, where the method is practically exa ...
Rigid Body Dynamics
... is called the Coriolis force. Notice that it is greatest if the velocity is perpendicular to the axis of rotation. This corresponds to motion which, for positive vbody , moves the particle further from the axis of rotation. Since the velocity required to stay above a point on a rotating body increas ...
... is called the Coriolis force. Notice that it is greatest if the velocity is perpendicular to the axis of rotation. This corresponds to motion which, for positive vbody , moves the particle further from the axis of rotation. Since the velocity required to stay above a point on a rotating body increas ...
Chapter 9 Rotational Motion
... notwithstanding any contrary hypothesis that may be imagined, till such time as other phenomena occur, by which they may either be made more accurate, or liable to exceptions. Isaac Newton ...
... notwithstanding any contrary hypothesis that may be imagined, till such time as other phenomena occur, by which they may either be made more accurate, or liable to exceptions. Isaac Newton ...
Model Four
... or imaginary) about which the object spins is referred to as the rotation axis. Note that all points that lie on the rotation axis do not move. All other points on the object, however, exhibit circular motion around the rotation axis. If the object, in addition to spinning, is also moving, this mode ...
... or imaginary) about which the object spins is referred to as the rotation axis. Note that all points that lie on the rotation axis do not move. All other points on the object, however, exhibit circular motion around the rotation axis. If the object, in addition to spinning, is also moving, this mode ...