Measurement of the effective focal shift in an optical trap

The focus of an oil-immersion microscope objective is shifted because of the refractive-index mismatch between the cover glass and the aqueous sample. We present a procedure with which to determine the focal shift by use of an inverted microscope equipped with optical tweezers. As the position of the sample chamber is scanned vertically, we measure the axial displacement of an optically trapped bead; the relative motion of the bead with respect to the surface supplies the effective focal shift. Measurements of this quantity deviate from electromagnetic calculations of the focal shift, a discrepancy attributable to the depth-dependent decrease in axial trap stiffness that arises from spherical aberration.     

Crystal structure of a second modification of the mercury oxychloride Hg3O2Cl2

The crystal structure of a monoclinic mercury oxychloride of composition Hg₃ O₂ Cl₂ has been described. A crystallographically different mercury oxychloride of the same composition was reported. The crystal structure of this second modification, called the -form, has been established through a single-crystal x-ray diffraction study. The -form is also monoclinic, with space groupP2₁/c andZ = 8. The unit-cell at 25 ° C hasa = 10.826(5),b = 9.310(4),c = 11.5 15(5) Å and = 71.04(8) °. The density is calculated to be 8.53 g cm^–3, that observed by displacement being 8.53(2) g cm^–3. Diffraction data were obtained using the -2 scanning mode on a Picker four-circle automatic diffractometer with CuK radiation. This apparently unsuitable radiation was chosen in order to test rigorously an absorption correction procedure. The structure was refined toR ₁ = 4.0% through conventional least-squares reduction basedF. The structure of -Hg₃ O₂ Cl₂ is found to be markedly different from that of the earlier-determined -Hg₃O₂Cl₂; distorted Hg₄O tetrahedra are linked into a three-dimensional array, terminated at four locations within the cell by covalent Hg-Cl bonds.     

Planar micro sensors for in vivo myocardial pH measurements

Potentiometric responses of microelectronically fabricated planar pH sensors based on both TDDA or ETH 5294 proton neutral carriers, in aminated PVC matrix, were evaluated with respect to main analytical parameters (linear ranges, slopes, reproducibility of potential measurements, potential drift and membrane resistance). In order to increase the electrode life time, increased amounts of membrane material were applied on the Ag/AgCl-poly-HEMA active spots of the polyimide substrate. The electrodes were implanted into an in situ porcine beating heart preparation at a midmyocardial depth in order to monitor H(+) concentration changes during the course of coronary artery occlusion.     

Aliphatic polyurethane as a matrix for pH sensors: effects of native sites and added proton carrier on electrical and potentiometric properties

The potentiometric and impedance characteristics of polymeric membranes, based on aliphatic polyurethane (Tecoflex) as a matrix, are described and interpreted by theory and experiments for H(+) and alkali metal ion-sensitive sensors. Both dummy plasticized membranes and proton carrier-loaded membranes can show pH response. The pH response of dummy membranes is due to protonated natural negative sites in the polyurethane matrix. The electrodes with added proton carrier show improved rejection of Li(+), Na(+), and K(+) responses and give useful analytical responses. Optimal performance requires control of negative site concentration by addition of lipophilic salt (e.g. tetraphenylborate derivatives). Impedance analyses show surface-rate semicircles and, depending on the bathing electrolyte solution, appearance of a diffusional Warburg impedance. In addition to these time-dependence surface region effects, changes in the bulk membrane resistance with soaking time can be well correlated with equilibrium water content of plasticized membranes.     

Quantum dot fluorescence quenching pathways with Cr(III) complexes. photosensitized NO production from trans-Cr(cyclam)(ONO)2+

Described is the photoluminescence (PL) of water-soluble CdSe/ZnS core/shell quantum dots (QDs) as perturbed by salts of the chromium(III) complexes trans-Cr(cyclam)Cl2+ (1), trans-Cr(cyclam)(ONO)2+ (2), and trans-Cr(cyclam)(CN)2+ (3) (cyclam = 1,4,8,11-tetraazacyclo-tetradecane). The purpose is to probe the characteristics of such QDs as antennae for photosensitized release of bioactive agents (in the present case, the bioregulatory molecule NO) from transition metal centers. Addition of 1 or 2 to a QD solution results in concentration-dependent quenching of the band edge emission, but 3 has a minimal effect. Added KCl strongly attenuates the quenching by 1, and this suggests that the Cr(III) cations and the QDs form electrostatic assemblies via ion pairing on the negatively charged QD surfaces. Quenching by 2, a known photochemical NO precursor, was accompanied by photosensitized NO release. All three, however, do quench the broad red emission ( approximately 650-850 nm) attributed to radiative decay of surface trapped carriers. The effect of various concentrations of 1 on time-resolved PL and absorbance were explored using ultrafast spectroscopic methods. These observations are interpreted in terms of the F?rster resonance energy-transfer mechanism for quenching of the band edge PL by multiple units of 1 or 2 at the QD surface, whereas quenching of the low-energy trap emission occurs via a charge-transfer pathway.     

Raman and resonance-Raman spectra of CsI/I−3

Raman and resonance-Raman spectra of the I^?₃ ion isolated within CsI crystals have been studied using 647 nm and 488 nm exciting radiation. Sample temperatures between 300 and 20 K have been used. Eleven overtones of the symmetric stretching mode (nν₁) have been observed in the resonance-Raman spectrum excited by the 488 nm Ar⁺ laser line. Bands centred at 153, 170, 264 and 304 cm^?1 have been assigned as ν₃, 2ν₂, ν₁+ν₃ and 2ν₃(Σ⁺) respectively. The remaining structure between the nν₁ lines has been assigned as due to combinations of these lines with the lattice vibrations of the CsI crystal.     

Amperometric microcells for alkaline phosphatase assay

To develop simple electrochemical immunoassays, a screen printed amperometric microcell with graphite working and Ag/AgCl reference electrodes was tested for the determination of alkaline phosphatase enzyme (ALP) and anti-humanIgG conjugated ALP (alpha-hIgG-ALP) activity in 5-10 microl samples. To ensure reproducible, steady state conditions, the working electrode surface was coated with mass-transport controlling hydrogel layer. The kinetic response curves of the hydrogel coated electrodes were linear. In addition, the hydrogel layer reduced the nonspecific adsorption of the alpha-hIgG-ALP conjugate on the working electrode surface. The measurements were made in the range of 2 divided by 4000 mU ml(-1) enzyme activities using ascorbic acid 2-phosphate (AAP) as the enzyme substrate. AAP is commercially available, non-toxic and has excellent stability. The sensitivity of the determinations was about 71% of the sensitivity which could be achieved using p-aminophenylphosphate (PAPP), a not easily accessible and unstable enzyme substrate. The experimentally determined kinetic parameters of the ALP enzyme catalyzed reactions were the same with the bare and hydrogel layer coated electrodes.