Для дальнейшего исследования спектр

Для дальнейшего исследования спектров ФЛ чешуек графена были произведены дополнительные измерения с использованием в качестве детектора кремниевого болометра. При этом в качестве накачки использовался как импульсный лазер Solar, так и непрерывный лазер мощностью~ 300 мВт с длиной волны 808 нм. При работе с непрерывным источником использовалась методика синхронного детектирования с помощью синхродетектора StanfordSR830.
К сожалению, в ходе дополнительных измерений не было обнаружено сигнала ФЛ от чешуек графена.

Results (English) 1:

For further study of the spectra of Graphene flakes were made INDIVIDUAL additional measurements using a Silicon bolometer as a detector. The pump was used as a Pulse Laser Solar and continuous laser ~ 300 MW wavelength 808 nm. When you work with a continuous source of methodology of synchronous detection using sinhrodetektora StanfordSR830.Unfortunately, there was no additional measurements of the signal from INDIVIDUAL Graphene flakes.

Results (English) 2:

To further investigate the photoluminescence spectra of graphene flakes additional measurements were made ​​using a silicon detector bolometer. Thus as the pumping laser used as a pulse Solar, and continuous laser power from about 300 mW, a wavelength of 808 nm. When working with a continuous source of the synchronous detection technique used via sync detector StanfordSR830.
Unfortunately, in the course of further measurements it was found from the PL signal graphene flakes.

Results (English) 3:

to further study the spectra of 3 графена flakes were made additional measurements using a detector кремниевого болометра. the as (used as a pulse laser and continuous laser power solar, ~ 300 mw with a wavelength of 808 nm. when working with a continuous source of methodology followed by simultaneous detection of синхродетектора StanfordSR830.unfortunately, the extra dimensions was found графена signal 3 from the flakes.