WebMar 5, 2024 · Generally, scattering is a complex problem. However, in many cases it allows the so-called Born approximation, 14 in which scattered wave field’s effect on the scattering object is assumed to be much weaker than that of the incident wave, and is neglected. Fig. 8.4. Scattering (schematically). As the first example of this approach, let us ... WebApr 7, 2012 · We use collective oscillations of a two-component Bose-Einstein condensate (2CBEC) of \Rb atoms prepared in the internal states $\ket{1}\equiv\ket{F=1, m_F=-1}$ …
What is physical explanation of a scattering length?
Webfor which the Pauli exclusion principle prohibits s-wave in-teractions at all, at least for identical spin states. The rich variety of ultracold gases grows when we con-sider mixtures of different species. For instance, again in 87Rb, mixtures of the total spin states uf,m&5u2,1& and u1,21& have a positive mutual scattering length @2#, making WebJul 24, 2014 · Through the use of a Feshbach resonance, the s-wave scattering length of the Rb85 atoms is tuned to a small negative value. ... We present a Ramsey-type atom interferometer operating with an optically trapped sample of 10^6 Bose-condensed Rb-87 atoms. The optical trap allows us to couple the F =1, mF =0>\rightarrow ... inc sweaters macy\\u0027s
Photonics Free Full-Text An Ultra-Low-Loss Waveguide Based …
WebIn particular we determine the interspecies s-wave singlet and triplet scattering lengths for the 40K-87Rb mixture as -111 +/- 5 Bohr and -215 +/- 10 Bohr respectively. We also predict accurate scattering lengths and position of Feshbach resonances for the other K … Webto ionize a 87Rb atom; this value is taken from Ref. [5]. The optical properties of the 87Rb D line are given in Tables 3 and 4. The properties are given separately for each of the two D-line components; the D 2 line (the 5 2S 1/2 −→ 5 P 3/2 transition) properties are given in Table 3, and the optical properties of the D 1 line (the 5 2S 1/ ... WebThe scattering length in quantum mechanics describes low-energy scattering.For potentials that decay faster than / as , it is defined as the following low-energy limit: =, where is the scattering length, is the wave number, and () is the phase shift of the outgoing spherical wave. The elastic cross section, , at low energies is determined solely by the scattering … inc style glides bold pen