Determination of phase differences of transition matrix elements from Pt(110) by means of spin-resolved photoemission with circularly and linearly polarized radiation

1998 ◽  
Vol 416 (3) ◽  
pp. 396-402 ◽  
Author(s):  
S.-W. Yu ◽  
R. David ◽  
N. Irmer ◽  
B. Schmiedeskamp ◽  
N. Müller ◽  
...  
1984 ◽  
Vol 52 (21) ◽  
pp. 1876-1879 ◽  
Author(s):  
A. Saha ◽  
Kamal K. Seth ◽  
M. Artuso ◽  
B. Harris ◽  
R. Seth ◽  
...  

1982 ◽  
Vol 49 (7) ◽  
pp. 451-454 ◽  
Author(s):  
A. M. Bernstein ◽  
R. A. Miskimen ◽  
B. Quinn ◽  
S. A. Wood ◽  
M. V. Hynes ◽  
...  

2001 ◽  
Vol 08 (03n04) ◽  
pp. 321-325
Author(s):  
ŞAKIR ERKOÇ ◽  
HATICE KÖKTEN

We have performed self-consistent field (SCF) calculations of the electronic structure of GaAs/Ga 1-x Al x As superlattices with parabolic potential profile within the effective mass theory. We have calculated the optical transition matrix elements involving transitions from the hole states to the electron states, and we have also computed the oscillator strength matrix elements for the transitions among the electron states.


Photonics ◽  
2021 ◽  
Vol 8 (7) ◽  
pp. 283
Author(s):  
Andrey Ustinov ◽  
Svetlana Khonina ◽  
Alexey Porfirev

Recently, there has been increased interest in the shaping of light fields with an inverse energy flux to guide optically trapped nano- and microparticles towards a radiation source. To generate inverse energy flux, non-uniformly polarized laser beams, especially higher-order cylindrical vector beams, are widely used. Here, we demonstrate the use of conventional and so-called generalized spiral phase plates for the formation of light fields with an inverse energy flux when they are illuminated with linearly polarized radiation. We present an analytical and numerical study of the longitudinal and transverse components of the Poynting vector. The conditions for maximizing the negative value of the real part of the longitudinal component of the Poynting vector are obtained.


2017 ◽  
Vol 95 (1) ◽  
Author(s):  
B. A. Brown ◽  
A. B. Garnsworthy ◽  
T. Kibédi ◽  
A. E. Stuchbery

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