epub |eng | 2015-06-14 | Author:Richard P. Feynman & Robert B. Leighton & Matthew Sands

epub |eng | | Author:Masud Chaichian & Hugo Perez Rojas & Anca Tureanu

epub |eng | 2021-04-09 | Author:Max Diem [Diem, Max]

epub |eng | | Author:Kaden Richard Alan Hazzard

35. D. Jaksch, C. Bruder, J.I. Cirac, C.W. Gardiner, P. Zoller, Phys. Rev. Lett. 81, 3108 (1998)CrossRefADS 36. I.M. Khalatnikov, An Introduction to the Theory of Superfluidity. (Westview Press, USA, ...

epub |eng | 2019-10-08 | Author:John Gribbin [Gribbin, John]

Nearly every result [the quantum theorist] pronounces is about the probability of this or that or that ... happening—with usually a great many alternatives. The idea that they may not ...

epub |eng | | Author:Wolfgang Demtröder

(7.106) which become increasingly dense with increasing principal quantum number n. They are caused by transitions from level into bound Rydberg levels. The series converges for towards the ionization limit ...

epub |eng | | Author:Jacob (Theo) Kloprogge

In soils, kaolinite is formed at pressure-temperature conditions of the Earth’s surface (i.e., 25–30 °C and atmospheric pressure). However, kaolinite also persists until late diagenesis at temperatures lower than 200 ...

epub |eng | 2017-04-20 | Author:Baggott, Jim; [Baggott, Jim]

The exchanged photon carries momentum from one electron to the other, thereby changing the momentum of both. The result is recoil, with both electrons changing speed and direction and moving ...

epub |eng | | Author:R Paul Drake

(7.73) This would not admit a self-similar solution if all the terms in c V were important. However, for T e > 10 eV, the terms of highest order in ...

epub |eng | | Author:Harald Friedrich

a finite scattering length does not exist even for l = 0. The leading near-threshold behaviour of the s-wave phase shift is [LK63], (4.110) so, towards threshold, the s-wave partial-wave ...

epub |eng | 2015-07-14 | Author:Richard P. Feynman & Robert B. Leighton & Matthew Sands

epub |eng | | Author:George Rawitscher & Victo dos Santos Filho & Thiago Carvalho Peixoto

8.3.1 The Iterative Method of Seaton and Peach The iterative method of Seaton and Peach [1] consists in rewriting Eq. (8.5) in the form (8.7) where (8.8) and calculating the ...

epub |eng | | Author:José J. C. Teixeira-Dias

E43. Use Mathematica to show that the trace of the polarizability tensor and its anisotropy, whose square is given by γ 2 = [(α xx − α yy )2 + ...

epub |eng | | Author:Ingvar Lindgren

Multireference Model Space We shall now investigate the time dependence of the Green’s operator in a general, quasi-degenerate model space. We can express the relation (6.96), using the general perturbation, ...

epub |eng | | Author:Bogdan Povh & Mitja Rosina

Energy conservation implies that (10.1) where is the speed after the production of the excitation. Momentum conservation additionally requires (10.2) It is easy to see that the phonon excitation first ...