picoTAS는 새로 개발된 RIPT(Randomly Interleaved Pulse Train) 방식을 사용하여 기존 방식으로는 측정하기 어려운 Gap Time Region(1~20 nanoseconds)을 포함한 다양한 시간 범위에서 발생하는 변화를 측정하는 데 매우 유용합니다.
또한 형광 신호를 제거하는 기능이 있어 기존에 측정할 수 없었던 다양한 Photo-induced reactions을 측정할 수 있습니다.
Models | picoTAS-ns | picoTAS-ps | |
---|---|---|---|
Method | RIPT method (Randomly Interleaved Pulse Train method) | ||
Time Resolution (10% 90% rise time) | < 400 ps | < 100 ps | |
Delay Time resolution | 10ps, 20ps, 50ps, 100ps, 200ps, 500ps, 1ns, 2ns, 5ns, 10ns, 20ns | ||
Full scale | 100 ns-2 ms | ||
Wavelength Range | 410-1600 nm | ||
Automatic Control | wavelength scan, light intensity adjustment, shutter control | ||
Sample Holder | solution (optical path length is 2 mm), thin film | ||
Pump Light Source | Source | passive Q-SW microchip laser | picosecond mode-locked laser |
Wavelength | 532nm and/or 355nm | 532nm and/or 355nm and/or 266nm | |
Pulse Width | < 350 ps | < 25 ps | |
Pulse Energy | > 20 μJ | > 80 μJ | |
Repetition Rate | 100-1000 Hz (variable) | 1000 Hz | |
Probe Light Source | Source | picosecond Supercontinuum Light Source | |
Pulse Width | < 50-100 ps (dependent on wavelength) | ||
Repetition Rate | 20 MHz ±5% | ||
PC & Software | OS | Windows® 7/10 | |
Function | Automatic reconstruction of transient absorption temporal profile, curve fitting (nonlinear least square method), data storage in text format | ||
Installation Environment | no optical bench required | on optical bench |