Abstract
... The radio isotope thorium-229 is predicted to possess a unique, extremely low-energy metastable excited state of the nucleus in the range of 7.8 ± 0.5 eV, offering the chance to coherently manipulate a nucleus by (VUV) laser light for the first time. Apart from exciting fundamental research question ...
... The radio isotope thorium-229 is predicted to possess a unique, extremely low-energy metastable excited state of the nucleus in the range of 7.8 ± 0.5 eV, offering the chance to coherently manipulate a nucleus by (VUV) laser light for the first time. Apart from exciting fundamental research question ...
PH4027 - Optoelectronics & Nonlinear Optics
... a large number of everyday applications, ranging from the ubiquitous LED, televisions and computer displays, as well as lasers in CD players, to sophisticated equipment for high-speed telecommunications applications that form the backbone of the internet. While classical optics is concerned with lin ...
... a large number of everyday applications, ranging from the ubiquitous LED, televisions and computer displays, as well as lasers in CD players, to sophisticated equipment for high-speed telecommunications applications that form the backbone of the internet. While classical optics is concerned with lin ...
( NONLINEAR OPTICS PHYC/ECE 568) Homework #4, Due Thu Sept. 24
... a. Calculate the bandwidth associated with a phase-matched SHG process in terms of the group velocities vg( 1) and vg(2 1). In the low-depletion approximation, this corresponds to the width of the Sinc2 function which is taken to be (kL)=2 with L denoting the length of the nonlinear crystal ...
... a. Calculate the bandwidth associated with a phase-matched SHG process in terms of the group velocities vg( 1) and vg(2 1). In the low-depletion approximation, this corresponds to the width of the Sinc2 function which is taken to be (kL)=2 with L denoting the length of the nonlinear crystal ...
Title: Noncollinear phase matching in nonlinear optics Author
... In the practical section, we determined the tuning curve (dependence of the optimal orientation of the crystal on I,he luminescence wavelength) of the non-linear BBO crystal. The crystal was exposed to luminescence radiation and to switching laser beam. Both waves in the crystal propagate like ordin ...
... In the practical section, we determined the tuning curve (dependence of the optimal orientation of the crystal on I,he luminescence wavelength) of the non-linear BBO crystal. The crystal was exposed to luminescence radiation and to switching laser beam. Both waves in the crystal propagate like ordin ...
( NONLINEAR OPTICS PHYC/ECE 568) Homework #5, Due Thu, Oct. 1
... The above process (i.e. the intensity-dependent phase variation of the fundamental wave) has been termed (2):(2) cascading nonlinearity. It mimics a third order (3) process where (3)eff(2)(;2,-)(2)(2;,) is effectively a cascade of two second order effects. The cascading nonlinearity has ...
... The above process (i.e. the intensity-dependent phase variation of the fundamental wave) has been termed (2):(2) cascading nonlinearity. It mimics a third order (3) process where (3)eff(2)(;2,-)(2)(2;,) is effectively a cascade of two second order effects. The cascading nonlinearity has ...
10NonlinearOptics.pdf
... polarization densities oscillating at 2ω1, 2ω2, ω1+ω2 , and ω1-ω2 , representing the sources for second harmonic generation of ω1 and ω2 , sum and difference frequency generation. Note the for second harmonic generation, only one wave is needed. Pockels effect A special case is when one of the waves ...
... polarization densities oscillating at 2ω1, 2ω2, ω1+ω2 , and ω1-ω2 , representing the sources for second harmonic generation of ω1 and ω2 , sum and difference frequency generation. Note the for second harmonic generation, only one wave is needed. Pockels effect A special case is when one of the waves ...