A femtosecond pulse-shaping apparatus containing microlens arrays for use with pixellated spatial light modulators

1996 ◽  
Vol 32 (12) ◽  
pp. 2071-2077 ◽  
Author(s):  
K.M. Mahoney ◽  
A.M. Weiner
1999 ◽  
Vol 38 (Part 1, No. 10) ◽  
pp. 5898-5904
Author(s):  
Toshiaki Hattori ◽  
Kouhei Kabuki ◽  
Yoshitsugu Kawashima ◽  
Masahiro Daikoku ◽  
Hiroki Nakatsuka

2021 ◽  
Vol 4 (4) ◽  
Author(s):  
Edoardo Carnio ◽  
Andreas Buchleitner ◽  
Frank Schlawin

We investigate how entanglement can enhance two-photon absorption in a three-level system. First, we employ the Schmidt decomposition to determine the entanglement properties of the optimal two-photon state to drive such a transition, and the maximum enhancement which can be achieved in comparison to the optimal classical pulse. We then adapt the optimization problem to realistic experimental constraints, where photon pairs from a down-conversion source are manipulated by local operations such as spatial light modulators. We derive optimal pulse shaping functions to enhance the absorption efficiency, and compare the maximal enhancement achievable by entanglement to the yield of optimally shaped, separable pulses.


Nanoscale ◽  
2019 ◽  
Vol 11 (29) ◽  
pp. 14070-14078 ◽  
Author(s):  
Qingyun Liu ◽  
Haichun Liu ◽  
Deyang Li ◽  
Wen Qiao ◽  
Guanying Chen ◽  
...  

Microlens arrays are applied as spatial light modulators to manipulate the distribution of excitation light fields in order to overcome the high excitation-intensity threshold of upconversion nanoparticles, taking advantage of their nonlinear response to excitation irradiance.


1998 ◽  
Vol 536 ◽  
Author(s):  
A. B. Pevtsov ◽  
N. A. Feoktistov ◽  
V. G. Golubev

AbstractThin (<1000 Å) hydrogenated nanocrystalline silicon films are widely used in solar cells, light emitting diodes, and spatial light modulators. In this work the conductivity of doped and undoped amorphous-nanocrystalline silicon thin films is studied as a function of film thickness: a giant anisotropy of conductivity is established. The longitudinal conductivity decreases dramatically (by a factor of 109 − 1010) as the layer thickness is reduced from 1500 Å to 200 Å, while the transverse conductivity remains close to that of a doped a- Si:H. The data obtained are interpreted in terms of the percolation theory.


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