Joost B. Buijs

Fluorescence Rejection in Resonance Raman Spectroscopy Using a Picosecond-Gated Intensified Charge-Coupled Device Camera

A Raman instrument was assembled and tested that rejects typically 98–99% of background fluorescence. Use is made of short (picosecond) laser pulses and time-gated detection in order to record the Raman signals during the pulse while blocking most of the fluorescence. Our approach uses an ultrafast-gated intensified charge-coupled device (ICCD) camera as a simple and straightforward alternative to ps Kerr gating. The fluorescence rejection efficiency depends mainly on the fluorescence lifetime and on the closing speed of the gate (which is about 80 ps in our setup). A formula to calculate this rejection factor is presented. The gated intensifier can be operated at 80 MHz, so high repetition rates and low pulse energies can be used, thus minimizing photodegradation. For excitation we use a frequency-tripled or -doubled Ti: sapphire laser with a pulse width of 3 ps; it should not be shorter in view of the required spectral resolution. Other critical aspects tested include intensifier efficiency as a function of gate width, uniformity of the gate pulse across the spectrum, and spectral resolution in comparison with ungated detection. The total instrumental resolution is 7 cm−1 in the blue and 15 cm−1 in the ultraviolet (UV) region. The setup allows one to use resonance Raman spectroscopy (RRS) for extra sensitivity and selectivity, even in the case of strong background fluorescence. Excitation wavelengths in the visible or UV range no longer have to be avoided. The effectiveness of this setup is demonstrated on a test system: pyrene in the presence of toluene fluorescence (λexc = 257 nm). Furthermore, good time-gated RRS spectra are shown for a strongly fluorescent flavoprotein (λexc = 405 nm). Advantages and disadvantages of this approach for RRS are discussed.

Picosecond Raman spectroscopy with a fast intensified CCD camera for depth analysis of diffusely scattering media

A spectroscopic depth profiling approach is demonstrated for layers of non-transparent, diffusely scattering materials. The technique is based on the temporal discrimination between Raman photons emitted from the surface and Raman photons originating from a deeper layer. Excitation was carried out with a frequency-doubled, 3 ps Ti:sapphire laser system (398 nm; 76 MHz repetition rate). Time-resolved detection was carried out with an intensified CCD camera that can be gated with a 250 ps gate width. The performance of the system was assessed using 1 mm and 2 mm pathlength cuvettes with powdered PMMA and trans-stilbene (TS) crystals, respectively, or solid white polymer blocks: Arnite (polyethylene terephthalate), Delrin (polyoxymethylene), polythene (polyethylene) and Teflon (polytetrafluoroethylene). These samples were pressed together in different configurations and Raman photons were collected in backscatter mode in order to study the time difference in such media corresponding with several mm of extra net photon migration distance. We also studied the lateral contrast between two different second layers. The results demonstrate that by means of a picosecond laser system and the time discrimination of a gated intensified CCD camera, molecular spectroscopic information can be obtained through a turbid surface layer. In the case of the PMMA/TS two-layer system, time-resolved detection with a 400 ps delay improved the relative intensity of the Raman bands of the second layer with a factor of 124 in comparison with the spectrum recorded with a 100 ps delay (which is more selective for the first layer) and with a factor of 14 in comparison with a non-gated setup. Possible applications will be discussed, as well as advantages/disadvantages over other Raman techniques for diffusely scattering media.

Phosphorescence for Sensitive Enantioselective Detection in Chiral Capillary Electrophoresis

Enantioselective phosphorescence lifetime detection was combined with chiral cyclodextrin-based electrokinetic chromatography for the analysis of camphorquinone (CQ). A time-gated detection system based on a pulsed light-emitting diode for excitation at 465 nm was developed for the online lifetime determination. The background electrolyte for the chiral separation consisted of 20 mM alpha-cyclodextrin (alpha-CD), 10 mM carboxymethyl-beta-CD, and 25 mM borate buffer at pH 9.0. The separation of (+)-CQ and (-)-CQ is caused by a difference in association constants of these enantiomers with alpha-CD. Under the separation conditions, different phosphorescence lifetimes were obtained for (+)-CQ and (-)-CQ (tau = 384 +/- 8 and 143 +/- 5 micros, respectively), which could be used to distinguish the enantiomers. This selectivity in detection is based on a difference in protection of the enantiomers against phosphorescence quenching after their complexation with alpha-CD. Concentration detection limits were 2 x 10(-7) and 1 x 10(-6) M for (+)-CQ and (-)-CQ, respectively. After correction for the lifetime shortening by triplet-triplet annihilation at higher CQ concentrations, a linear dynamic range was obtained from the detection limit up to 2 mM. The system was used to determine the enantiomeric impurity levels of commercial samples of (+)-CQ and (-)-CQ; 0.2% and 0.1%, respectively.

Sub-second liquid chromatographic separations by means of shear-driven chromatography.

Utilizing the concept of shear-driven chromatography, we have been able to realize reversed-phase LC separations in flat rectangular nano-channels coated with a C8 monolayer and being as thin as 100 nm. At this scale, the separation kinetics are strongly enhanced, as is witnessed by the extremely short time (< 0.1 s) needed to separate a mixture of coumarin dyes. The observed plate numbers are still relatively small, because the experiments were conducted in ultra-short columns (< or = 1 mm) and under injection band width-limiting conditions.

Noninvasive detection of concealed explosives: depth profiling through opaque plastics by time-resolved Raman spectroscopy.

The detection of explosives concealed behind opaque, diffusely scattering materials is a challenge that requires noninvasive analytical techniques for identification without having to manipulate the package. In this context, this study focuses on the application of time-resolved Raman spectroscopy (TRRS) with a picosecond pulsed laser and an intensified charge-coupled device (ICCD) detector for the noninvasive identification of explosive materials through several millimeters of opaque polymers or plastic packaging materials. By means of a short (250 ps) gate which can be delayed several hundred picoseconds after the laser pulse, the ICCD detector allows for the temporal discrimination between photons from the surface of a sample and those from deeper layers. TRRS was applied for the detection of the two main isomers of dinitrotoluene, 2,4-dinitrotoluene, and 2,6-dinitrotoluene as well as for various other components of explosive mixtures, including akardite II, diphenylamine, and ethyl centralite. Spectra were obtained through different diffuse scattering white polymer materials: polytetrafluoroethylene (PTFE), polyoxymethylene (POM), and polyethylene (PE). Common packaging materials of various thicknesses were also selected, including polystyrene (PS) and polyvinyl chloride (PVC). With the demonstration of the ability to detect concealed, explosives-related compounds through an opaque first layer, this study may have important applications in the security and forensic fields.

Sensitized enantioselective laser-induced phosphorescence detection in chiral capillary electrophoresis.

The sensitivity of enantioselective cyclodextrin-induced room-temperature phosphorescence detection of camphorquinone (CQ) is enhanced using sensitization via a donor with a high extinction coefficient. The enantiomeric distinction is based on the different phosphorescence lifetimes of (+)-CQ and (-)-CQ after their complexation with α-cyclodextrin (α-CD). The collisional Dexter energy transfer from the selected donor 2,6-naphthalenedisulfonic acid (2,6-NS) to the acceptor CQ is still very efficient despite the inclusion of the acceptor into CD. For coupling to the chiral separation of (±)-CQ in cyclodextrin-based electrokinetic chromatography, the donor was added to the deoxygenated background electrolyte that consisted of 20 mM α-CD, 10 mM carboxymethyl-β-CD, and 25 mM borate buffer at pH 9.0. Time-resolved batch studies on sensitized phosphorescence show a significant enantioselectivity for (+)- and (-)-CQ in the presence of both α-CD and CM-β-CD although the lifetime difference is somewhat reduced with respect to direct excitation. The enantiomers were distinguished after their separation using an online time-resolved detection system. Excitation was performed at 266 nm with a pulsed, small-sized, quadrupled Nd:YAG laser. With 1 × 10(-5) M 2,6-NS, limits of detection of 4.1 × 10(-8) M and 5.2 × 10(-8) M were found for (+)-CQ and (-)-CQ, respectively. The online measured lifetimes were 238 ± 8 μs for (+)-CQ and 126 ± 10 μs for (-)-CQ. The method was used to determine the concentration of (±)-CQ leaching from a cured dental resin into water. The extracts contained 4.7 ± 0.1 × 10(-7) M of both (+)-CQ and (-)-CQ.

Sensitized phosphorescence as detection method for the enantioseparation of bupropion by capillary electrophoresis

A new CE detection method was developed for the chiral drug bupropion (a second‐generation antidepressant), based on phosphorescence both in the direct and in the sensitized mode using pulsed laser excitation at 266 nm. Electrokinetic chromatography using 5 mM sulfated‐α‐CD as chiral selector in 25 mM phosphate buffer at pH 3 allowed the separation of bupropion enantiomers with a high chiral resolution (Rs>3). In the sensitized phosphorescence detection mode, excitation energy is transferred from the analyte to an acceptor (1‐bromo‐4‐napthhalenesulfonic acid or biacetyl) followed by time‐resolved phosphorescence detection under deoxygenated buffer conditions. Using 2×10−4 M biacetyl as the acceptor an LOD of 2×10−7 M was obtained for each enantiomer, about 40 times better than in the direct mode. Under these separation conditions, no significantly different phosphorescence lifetimes (measured on‐line) were obtained for the two bupropion enantiomers. The suitability of the method was demonstrated with the quantification of bupropion in a pharmaceutical formulation and its determination in a spiked urine sample.

High resolution slice imaging of a molecular speed distribution

High resolution slice imaging experiments are reported measuring the speed distribution of molecular fragments, recoiling at a most probable speed v(mp), with a full-width-half-maximum (FWHM) speed resolution near the permille level: FWHM(v)/v(mp) = 1.9 x 10(-3). We implemented a high resolution single-particle slice imaging detector and used a two-colour resonance-enhanced multi-photon ionisation (REMPI) scheme to reduce broadening of the speed distribution due to the electron kick. The results on the measurement of the CD(3) speed distribution from photolysis of CD(3)I show that it is possible to image the three-dimensional speed distribution at a resolution down to FWHM(v) = 6.7 m s(-1), when the fragment has an absolute speed of v(mp) = 3473 m s(-1). The new experiments demonstrate the potential of slice imaging to measure with high resolution the three-dimensional speed distribution of a cloud of molecules.

Evanescent-Wave Cavity Ring-Down Spectroscopy for Enhanced Detection of Surface Binding Under Flow Injection Analysis Conditions

The feasibility of liquid-phase evanescent-wave cavity ring-down spectroscopy (EW-CRDS) for surface-binding studies under flow-injection analysis (FIA) conditions is demonstrated. The EW-CRDS setup consists of an anti-reflection coated Dove prism inside a linear cavity (with standard or super-polishing of the total internal reflective (TIR) surface). A teflon spacer with an elliptical hole clamped on this surface acts as a 20 μL sized flow cell. The baseline noise of this system is of the order of 10−4 absorbance units; the baseline remains stable over a prolonged time and the prism surface does not become contaminated during repeated injections of the reversibly adsorbing test dyes Crystal Violet (CV) and Direct Red 10 (DR10). At typical FIA or liquid chromatography (LC) flow rates, the system has sufficient specificity to discriminate between species with different surface affinities. For CV a much stronger decrease in ring-down time is observed than calculated based on its bulk concentration and the effective depth probed by the evanescent wave, indicating binding of this positively charged dye to the negatively charged prism surface. The amount of adsorption can be influenced by adjusting the flow rate or the eluent composition. At a flow rate of 0.5 mL/min, an enrichment factor of 60 was calculated for CV; for the poorly adsorbing dye DR10 it is 5. Super-polishing of the already polished TIR surface works counter-productively. The adsorbing dye Crystal Violet has a detection limit of 3 μM for the standard polished surface; less binding occurs on the super-polished surface and the detection limit is 5 μM. Possible applications of EW-CRDS for studying surface binding or the development of bio-assays are discussed.

Fast-Gated Intensified Charge-Coupled Device Camera to Record Time-Resolved Fluorescence Spectra of Tryptophan

The possibilities of a 200 ps gated intensified charge-coupled device (CCD) camera to record time-resolved fluorescence were explored using the fluorescing amino acid tryptophan and its derivative N-acetyl-tryptophan amide (NATA) as model compounds. The results were compared to complementary data from time-correlated single-photon counting (TCSPC) experiments. If a spectral resolution of 1–2 nm is desired, the fast-gated intensified CCD (ICCD) camera is the method of choice. For a 10−5 M tryptophan solution, time-resolved emission spectra and intensity decays (measured over 12 ns at 25 ps resolution) could be obtained in typically 10 minutes, giving the well-known lifetimes of 0.5 and 3 ns. In addition, a longer lifetime of 7 ns was found at the red edge of the spectrum. The very short gate time of the ICCD camera allowed us to observe a shift in the emission maximum of tryptophan even within the first nanosecond of decay of the fluorescence emission. As expected from the tryptophan rotamer model, such a shift is not observed in NATA. Using amplitudes obtained by global analysis, decay-associated spectra of these lifetimes were constructed.