Question

How to calculate mean frequency in time resolved emission spectrum?

Answer 1

Explanation:

Explanation:Measurements of time-resolved emission spectra and emission lifetimes

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the fundamental of a mode-locked Ti:sapphire laser (Tsunami, Spectra Physics, 808 nm,

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the fundamental of a mode-locked Ti:sapphire laser (Tsunami, Spectra Physics, 808 nm, 1W, 80 MHz repetition rate) was generated using BBO crystals (1mm thickness) and

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the fundamental of a mode-locked Ti:sapphire laser (Tsunami, Spectra Physics, 808 nm, 1W, 80 MHz repetition rate) was generated using BBO crystals (1mm thickness) and separated with a CaF2 equilateral dispersive prism. The 269-nm mplified with preamplifiers

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the fundamental of a mode-locked Ti:sapphire laser (Tsunami, Spectra Physics, 808 nm, 1W, 80 MHz repetition rate) was generated using BBO crystals (1mm thickness) and separated with a CaF2 equilateral dispersive prism. The 269-nm mplified with preamplifiers (EG&G Ortec VT120B and Hamamatsu C5594, respectively) and then discriminated

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the fundamental of a mode-locked Ti:sapphire laser (Tsunami, Spectra Physics, 808 nm, 1W, 80 MHz repetition rate) was generated using BBO crystals (1mm thickness) and separated with a CaF2 equilateral dispersive prism. The 269-nm mplified with preamplifiers (EG&G Ortec VT120B and Hamamatsu C5594, respectively) and then discriminated with ps-timing discriminators (EG&G Ortec 9307). Those output pulses ta were

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the fundamental of a mode-locked Ti:sapphire laser (Tsunami, Spectra Physics, 808 nm, 1W, 80 MHz repetition rate) was generated using BBO crystals (1mm thickness) and separated with a CaF2 equilateral dispersive prism. The 269-nm mplified with preamplifiers (EG&G Ortec VT120B and Hamamatsu C5594, respectively) and then discriminated with ps-timing discriminators (EG&G Ortec 9307). Those output pulses ta were recorded at every 5 nm in the range of 300–400 nm, and they were used to reconstruct

Explanation:Measurements of time-resolved emission spectra and emission lifetimes Picosecond time-resolved emission data were nm) of the fundamental of a mode-locked Ti:sapphire laser (Tsunami, Spectra Physics, 808 nm, 1W, 80 MHz repetition rate) was generated using BBO crystals (1mm thickness) and separated with a CaF2 equilateral dispersive prism. The 269-nm mplified with preamplifiers (EG&G Ortec VT120B and Hamamatsu C5594, respectively) and then discriminated with ps-timing discriminators (EG&G Ortec 9307). Those output pulses ta were recorded at every 5 nm in the range of 300–400 nm, and they were used to reconstruct time-resolved emission spectra at each delay.