The FLS1000 Spectrometer sets the standard in both steady state and time-resolved photoluminescence spectroscopy for both fundamental research and routine laboratory applications.
The system is a modular fluorescence and phosphorescence spectrometer for measuring spectra from the ultraviolet to the mid-infrared spectral range (up to 5,500 nm), and lifetimes spanning from picoseconds to seconds. All of this can be achieved through various upgrade routes, either at the time of order or in the future.
Whether you are studying photophysics, photochemistry, biophysics, biochemistry, material or life sciences, the FLS1000 will enable you to reliably and accurately measure luminescence spectra and kinetics using state-of-the-art sources, detectors, acquisition techniques, quality optics and precision mechanics. The large sample chamber will house practically any type of sample accessory.
High sensitivity is a prerequisite for measurements of low sample concentrations, small sample volumes or low sample quantum yields. The instrument’s guaranteed sensitivity of >30,000:1 (optional >35,000:1) for the standard water Raman measurement using the SQRT method is unmatched in the industry.
The FL1000 has a USB interface and all modes of operation are controlled by ONE data acquisition module and ONE all-inclusive Fluoracle software package for data acquisition and analysis. Light source, detector, grating, slits, polarisers are all computer-controlled for accurate and precise measurements.
The FL1000 comes standard with a 450 W ozone free xenon arc lamp that covers a range of 230 nm to >1000 nm for steady state measurements. A variety of other sources can be integrated including microsecond flashlamps, nanosecond flashlamp, pulsed diode lasers (EPL Series), pulsed light emitting diodes (EPLED Series), supercontinuum lasers, Ti:sapphire lasers, Q-switched solid state lasers and OPOs, dye lasers, and infrared CW and pulsed lasers for upconversion measurements.
Single and double grating Czerny-Turner monochromators are available in the FLS1000 with 325 mm (or 2 x 325 mm) focal length, high optical throughput, excellent stray light rejection and low temporal dispersion. The monochromators feature ‘plug-and-play’ triple grating turrets with up to three gratings on each turret and computer-controlled slits.
A full range of detector options are available to enhance the range of spectral coverage and/ or to reduce the instrumental response width for lifetime measurements. The instrument comes standard with a PMT-900 detector in a cooled housing which covers a range from 185 nm – 900 nm, in TCSPC mode the instrumental response width is approximately 600 ps. Optional detectors include: high speed PMTs in a cooled housing with instrument response <200 ps, MCP-PMT in cooled housings with a response <25 ps, NIR-PMTs to cover spectral ranges out to 1700 nm with photon counting sensitivity and speed, InGaAs detectors with spectral coverage up to ~1.65 μm, 2.05 um and 2.55 μm, InAs and InSb detectors to cover up to 5.50 μm.
At the heart of the FLS1000 is an exceptionally large sample chamber that allows access to the sample from all sides, top and bottom. This ensures compatibility and simplifies access to a variety of sample holders.
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 - 50 µs * Sensitivity >30,000:1 ** n/a n/a Excitation Sources Type 450 W ozone-free xenon arc lamp Microsecond flashlamp Picosecond pulsed diode lasers (EPLs) 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 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) Slits 0 mm - 11 mm, fully computer-controlled, bandpass is grating dependent 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 Spectral graphs available for operations of CCDs and diode array detectors * grating dependent Detectors PMT-900 PMT-1010 PMT- 1400/1700 HS-PMT MCP-PMT Spectral Range 185 nm - 900 nm 300 nm - 1010 nm 300 nm - 1700 nm 230 nm - 870 nm 200 nm - 850 nm Dark Count Rate <50 cps (-20 °C) <100 cps (-20 °C) <200 cps (-80 °C) <100 cps (-20 °C) <50 cps (-20 °C) Reponse Width 600 ps 600 ps 800 ps 200 ps <25 ps Options A wide variety of other photomultipliers and analogue detectors are available up to 5,500 nm
Fluoracle spectrometer operating software is at the heart of all our fluorescence spectrometers and is a fully comprehensive, user-friendly data analysis software package. Irrespective of system configurations, this software provides the user with complete control of the instrument and of most third-party accessories.
Fluoracle is Windows compatible and is based on a data centred design that enables the user to focus on their measurement. This guarantees ease-of-use in the operation of a modular and potentially complex spectrometer.
Measurement set-up and data acquisition is made through an intuitive menu system. Key spectroscopic parameters are easily accessed through functional groupings, while common measurement routines can be saved as method files to allow previous experiments to be easily repeated. Tabbed dialogue boxes and particular scan parameters are always visible during set-up. The current status of the instrument is also continuously displayed.
A unique feature of the Fluoracle is that all modes of data acquisition, including spectral scanning and lifetime acquisition in both MCS and TCSPC modes, are controlled from within one software package. Modern light sources, detectors, complex sample holders (plate reader, XY sample stages, titrator) and cooler options (thermostated sample holders and cryostats) are supported and fully software controlled.
Fluoracle offers the “FAST” add on for the advanced analysis of fluorescence and phosphorescence decay kinetics.
Excitation and emission spectra are standard measurements in fluorescence spectroscopy. The figure demonstrates a measurement of a well documented standard test solution of anthracene in degassed cyclohexane.
Sample: Anthracene in cyclohexane (10-5M). Measurement conditions: λex = 358 nm for emission scan, λem = 400 nm for corrected excitation scan, Δλex = Δλem = 0.4 nm, step size = 1 nm, integration time = 1 s.
In synchronous scans, both excitation and emission monochromators are scanned synchronously with a pre-set offset. The figure demonstrates a sample of five different aromatic hydrocarbons dissolved in cyclohexane, measured with a conventional emission scan (red) and a synchronous scan with zero offset (green). The five hydrocarbons are resolved by the synchronous scan.
Sample: Five aromatic hydrocarbons dissolved in cyclohexane. Measurement conditions: λex = 280 nm for emission scan, Δλex = Δλem = 0.5 nm, step size = 0.5 nm, integration time = 1 s, offset = 0 nm.
Kinetic scans reveal temporal changes of the sample fluorescence at fixed excitation and emission wavelengths. Luminescence emission in the milliseconds to seconds range, such as long phosphorescence, chemical reactions or chemical migration in cells, can be studied. As an example, using the FLS1000 in T-geometry for dual wavelength detection, simultaneous measurements of the Ca2+ active fluorophore Indo-1 can be made with both emission arms set to different wavelengths.
Sample: Human platelets cells loaded with Indo-1 in 1 mM Ca2+. Measurement conditions: λex = 340 nm, λem1 = 485 nm, λem2 = 410 nm, Δλex = Δλem = 1 nm, integration time = 0.5 s.
The variety of measurement, display and analysis options allows easy and fast investigation of unknown luminescent samples or samples which contain different fluorophores. One method is to measure a series of emission scans within a selected range of excitation. The result is then demonstrated either in a 3D plot or in a contour plot.
Sample: Three organic dyes in solution: naphtalene, anthracene perylene. Measurement conditions: Xe1, PMT-900, 280 nm ≤ λex ≤ 460 nm, 310 nm ≤ λem ≤ 620 nm, Δλex = Δλem = 2 nm, integration time = 0.5 s, repeats per scan = 1.
The F1000 software can communicate with liquid nitrogen and liquid helium cryostats (along with TE controlled sample holders). Temperature maps can be made by acquiring a series of emission, excitation or synchronous scans for a predefined temperature range. The individual measurements are automatically started when the target temperatures are reached.
Sample: CuInSe2 (a material used for photovoltaic cells). Measurement conditions: Fluoracle-controlled Cryostat, Xe2, PMT-1700, λex = 694 nm, Δλex = 10 nm, Δλem = 5 nm, step size = 1 nm, integration time = 0.2 s. Temperature range: 6 K – 106 K, step 20 K.
The absolute method for fluorescence quantum yield measurements is becoming more widely used than the relative method, as it does not require a quantum yield standard. This is readily applicable to liquids, films and powders and can be extended into the near infrared spectral range.
The picture shows the independence of the fluorescence quantum yield from the wavelength of excitation for a standard organic dye. The graph shows the area of absorption for eight different excitation wavelengths on the left, while on the right it shows the corresponding emission spectra, scaled by a factor of 5. The inset shows the calculated quantum yields.
Sample: Quinine bisulphate in perchloric acid. Measurement conditions: integrating sphere, Δλex = 5.0 nm, Δλem = 0.5 nm, integration time = 0.3 s.
The emission of singlet oxygen is known to be very weak and, historically, powerful laser excitation has been used to monitor this. However, both excitation and emission spectra of singlet oxygen can be measured using the FLS1000 with a broadband xenon lamp. The figure demonstrates a measurement of singlet oxygen luminescence generated from erythrosine B in ethanol detected by NIR-PMT (green), and InGaAs (blue) detectors.
Sample: Singlet oxygen generated from erythrosine B in ethanol
The electronic configuration of lanthanides enables a wide variety of Stokes and anti-Stokes transitions from the ultraviolet to the mid-infrared. This makes them versatile materials that find widespread use in lasers, solar cells, bio-photonics and sensors. Their intra-4f transitions shielded by the external sub-shell are very sharp and narrow requiring high resolution instruments, as can be seen in the graph below for an erbium-ytterbium doped fluoride. Especially for non-linear processes such as upconversion, powerful lasers are fully integrated with the FLS1000.
Sample: YTa7O19: Er3+-Yb3+ powder phosphor
Other steady state measurement examples: Steady state fluorescence anisotropy, contour plots, water quality assessments, excimer equilibrium, reflection, absorption and quantum yield measurements of phosphor powders, chromaticity and much more.
Fluoracle provides analysis tools for standard decay tail fitting and numerical reconvolution. With numerical reconvolution, short lifetime components can be extracted from the raw decay data which would otherwise be distorted or masked by the instrumental profile.
The analysis routine provided is based on the Marquardt- Levenberg algorithm. Up to four exponential decay components can be fitted, with shift and offset fitting as standard. The algorithm is robust, delivers results in a blink of an eye, and is presented in a user-friendly interface.
Additional fit quality parameters are available for quality assessment, such as autocorrelation functions, the Durbin-Watson parameter and standard deviations.
The example shows two measurement results of the same homogeneous solution, taken at two different emission wavelengths. The decay at the shorter wavelength is clearly a single exponential, the decay at the longer wavelength is best characterised by three exponential components.
Sample: Hematoporphyrin IX in phosphate buffer (pH 7.2)
Measurement conditions: EPL 405, MCP-PMT, λex = 398 nm, Δλem = 1.0 nm, rep rate = 1 MHz, λem = 620 nm (left and right graph)
Data analysis: Multi-exponential reconvolution, confidence intervals verified by support plane analysis (FAST). τ1 = 15.02 ± 0.03 ns (left). τ2 = 14.80 ± 0.20 ns, τ2 = 4.62 ± 0.55 ns, τ3 = 0.81 ± 0.20 ns (right).
By exciting the sample with vertically polarised light and recording the emission in both the vertical and horizontal plane, one can calculate the fluorescence anisotropy of a homogeneous sample. The fluorescence anisotropy reveals the average rotational diffusion time of the molecules.
The measurement example shows that rotational diffusion in the picosecond time scale can be accurately measured. Most samples show rotational diffusion. To avoid this effect when precise fluorescence lifetime measurements are required, the emission polariser must be set to magic angle conditions, 54.7º (and vertically polarised excitation used).
Sample: POPOP in cyclohexane (left plot: IRF-black, decays with parallel-blue and crossed polariser-red), fluorescence anisotropy (right plot: raw data-green and fit-red). Measurement conditions: EPL 375, MCP-PMT, λex = 375 nm, Δλex = 2.0 nm, λem = 390 nm, Δλem = 2.0 nm.
Data analysis: Full anisotropy reconvolution (FAST) with ellipsoidal rotor model. The rotation diffusion times are 110 ps, 150 ps and 620 ps respectively. A spherical rotor model results in a fit with significantly increased chi-square. POPOP is a rod like molecule.
Other TCSPC measurement examples: Time-resolved emission spectroscopy (TRES), monomer-excimer kinetics, solvent relaxation dynamics and much more.
The photoluminescence emission lifetime of lanthanides extends over a large time range from nanoseconds to seconds where the method of choice for time-resolved measurements is the MCS technique. Due to the high dynamic range and the accuracy resulting from counting statistics, complex decay analysis can be performed.
The pictures show time resolved measurements from a lanthanide doped glass sample at two different emission wavelengths. At the shorter wavelength the decay is best fitted with three exponential terms, while at the longer emission wavelength the initial rise is followed by a millisecond decay.
Sample: Rare-earthed doped glass
Measurement conditions: μF2, λex = 370 nm, Δλex = Δλem = 2.5 nm, rep rate 100 Hz, step size = 10 nm, spectra produced for every 50 μs (Top Left). μF2, λex = 370 nm, λem = 430 nm, Δλex = Δλem = 2.5 nm, rep rate 100 Hz, step size = 10 nm, measurement time = 2 min (Top Right). μF2, λex = 370 nm, λem = 612 nm, Δλex = Δλem = 1.7 nm, rep rate 20 Hz, measurement time = 8 min (Bottom Left).
Data Analysis: Multi-exponential reconvoltution. Good fit results were achieved with four exponential decay model (Top Right) and model comprising two exponential rise and one decay function (Bottom Left).
Other MCS measurement examples: Time-resolved singlet oxygen measurements, time-resolved FRET measurements and much more.