TECHNIQUES
Time-Resolved Fluorescence
Time-Resolved Fluorescence (or Fluorescence Lifetime) Spectroscopy is an extension of Steady State Fluorescence. When we discuss time-resolved fluorescence or fluorescence lifetimes, what we are studying is the fluorescence of a sample monitored as a function of time after excitation by a pulse of light.
Fluorescence lifetimes, occurring as emissive decays from the singlet-state, can also be approximated as those decays occurring in the time region from picoseconds to nanoseconds.
If you are conducting research on time-resolved fluorescence and would like to know how our instrumentation can help you with your research, simply contact a member of our Sales Team.
DESCRIPTION
The time-resolution can be obtained in a number of ways, depending on the required sensitivity and time regions. Edinburgh Instruments employs the technique called Time-Correlated Single Photon Counting (TCSPC), for Time-Resolved Fluorescence, which is used for the acquisition of single photons and allows for time resolutions in the range of picoseconds (ps) to nanoseconds (ns).
This technique is a digital counting technique, counting photons that are time-correlated in relation to a short excitation light pulse. In TCSPC the sample is repetitively excited using a pulsed light source with a high repetition rate. During the measurement a probability histogram builds, which relates the time between an excitation pulse (START) and the observation of the first fluorescence photon (STOP). The fact that the time at which a fluorescence photon is incident on the detector can be defined with picosecond resolution is critical to the operation and precision of TCSPC. To study lifetime decays slower than this (ns to seconds time range) please see Phosphorescence Lifetime.To find out more about what TCSPC is and why we use TCSPC, please see the technical notes provided in the resources section.
This technique is a digital counting technique, counting photons that are time-correlated in relation to a short excitation light pulse. In TCSPC the sample is repetitively excited using a pulsed light source with a high repetition rate. During the measurement a probability histogram builds, which relates the time between an excitation pulse (START) and the observation of the first fluorescence photon (STOP). The fact that the time at which a fluorescence photon is incident on the detector can be defined with picosecond resolution is critical to the operation and precision of TCSPC. To study lifetime decays slower than this (ns to seconds time range) please see Phosphorescence Lifetime.To find out more about what TCSPC is and why we use TCSPC, please see the technical notes provided in the resources section.
APPLICATIONS
- Single and Multiple Exponential Decays
- Time-Resolved Emission Spectroscopy (TRES)
- Monomer-Excimer Kinetics
- Time-Resolved Fluorescence Anisotropy
- Solvent Relaxation Dynamics
DOCUMENTS
- Download the TCC2 Lifetime Electronics Module Datasheet
- Photoluminescence Product Overview Flyer
PRODUCTS
PUBLICATIONS
| Specifications | Spectral | Phosphorescence Lifetime | Fluorescence Lifetime |
|---|---|---|---|
| Mode of Operation | Single Photon Counting | Time-Resolved Single Photon Counting (Multi Channel Scaling - MCS) | Time-Correlated Single Photon Counting (TCSPC) |
| Lifetime range | Milliseconds to hours | 10 ns - 50 s * | 5 ps - 10 µs * |
| Sensitivity | >35,000:1 ** | n/a | n/a |
| Excitation Sources | |||
| Type | 450 W ozone-free xenon arc lamp | Microsecond flashlamp | Picosecond pulsed diode lasers (EPLs, HPLs) and pulsed LEDs (EPLEDs) |
| Spectral Range | 230 nm- > 1000 nm | 200 nm - >1000 nm | Discrete wavelengths between 250 nm - 980 nm |
| Pulse width | n/a | 1 µs - 2 µs | from 60 ps |
| Options | Ozone generating lamp with spectral range 200 nm - >1000 nm | Low to medium repetition rate pulsed lasers. Variable pulse width VPL and VPLEDs | Nanosecond flashlamp 200 nm - >400 nm pulse width <1 ns |
| * source and detector dependent ** standard water Raman measurement conditions: Excitation wavelength = 350 nm, Excitation and emission bandwidths = 5 nm, step size = 1 nm, integration time = 1 s, emission wavelength = 397 nm, noise measured at 450 nm and calculation based on the SQRT method | |||
| Monochromator | Specifications |
|---|---|
| Type | Czerny-Turner with 'plug and play' triple grating turret |
| Focal Length | 325 mm (double monochromators: 2 x 325 mm) |
| Stray Light Rejection | 1:10-5 (single), 1:10-10 (double) |
| Gratings | Mounted to triple grating turret |
| Accuracy | +/- 0.2 nm * |
| Minimum Step Size | 0.01 nm * |
| Option | Spectrographs available for operations of CCDs and diode array detectors |
| * grating dependent | |
| Detectors | PMT-900 | PMT-1010 | PMT- 1400/1700 | HS-PMT | MCP-PMT | HS-HPD |
|---|---|---|---|---|---|---|
| Spectral Range | <200 nm - 870 nm | <200 nm - 1010 nm | 500 nm - 1700 nm | <230 nm - 850 nm | <200 nm - 850 nm | 220 nm - 870 nm |
| Dark Count Rate | <50 cps (-20 °C) | <200 cps (-20 °C) | <20 kcps or <200 kps | <150 cps (0 °C) | <10 cps (-20 °C) | <200 cps (10 °C) |
| Reponse Width | 600 ps | 800 ps | 400 ps or 800 ps | 180 ps | <25 ps | 20 ps |
| Options | A wide variety of other photomultipliers and analogue detectors are available up to 5,500 nm | |||||
