827 resultados para Welland
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Map of measurements of lot no.186, Dec. 19, 1855.
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Map of measurements of lots no.185 and 186 by George Strohan, Dec. 29, 1855.
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Power of water discharged over breach of weir (1 page, handwritten), n.d.
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Totals of free goods up – class 3 and class 4 (1 page, handwritten), n.d.
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Sketch in the lock of the new canal above St. Catharines. The sketch is unsigned, Aug. 18, 1899
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List of prices (2 pages, handwritten) for items such as furniture, curtains, pictures, carpets and glassware. This is embossed with the Welland Canal stamp, Dec. 1855.
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Indenture of deed of quit claim (original copy and memorial of) between Walter H. and Charlotte Dickson of Guelph and Joseph A. Woodruff of Niagara for land in the Town of Clifton, Stamford and Welland, Aug. 10, 1863.
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Letter to Henry Nelles from S.B. Ritchie (1 page, double-sided) wondering what the prospects for the Welland Canal will be in the next season. This letter is somewhat stained. This does not affect the text. This is accompanied by an envelope, Feb. 3, 1834.
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Broadside advertising the appearance of the Prince of Wales, Albert Edward, who was Queen Victoria’s eldest son. He was to become Edward VII. The visit took place on Tuesday, the 18th of September in 1860. The broadside measures 20 cm. x 17.5 cm. The Royal Coat of Arms is featured on the top. Different typefaces are used throughout the broadside. The Broadside reads: "The Prince's Visit to St. Catharines. His Royal Highness will be at St. Catharines on Tuesday, the 18th Sept. 1860. The Committee of Management express the earnest hope that the Inhabitants of the Counties of Lincoln & Welland Generally, will manifest their Loyalty by joining in an enthusiastic demonstration to the Prince. Come Early to get Seats! As the accommodation in the Amphitheatre will be limited. A Grand Procession Of Firemen and other Public Bodies will be formed, accompanied by Bands of Music. A Royal Salute Will be fired by the St. Catharines Volunteer Artillery Company; and British Cheers will be given by the assembled assembled thousands. A General Illumination in the Evening! God Save The Queen! C.P. Camp, Sec'y to Committee. St. Catharines, September 15, 1860."
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Among the range of materials used in bioengineering, parylene-C has been used in combination with silicon oxide and in presence of the serum proteins, in cell patterning. However, the structural properties of adsorbed serum proteins on these substrates still remain elusive. In this study, we use an optical biosensing technique to decipher the properties of fibronectin (Fn) and serum albumin adsorbed on parylene-C and silicon oxide substrates. Our results show the formation of layers with distinct structural and adhesive properties. Thin, dense layers are formed on parylene-C, whereas thicker, more diffuse layers are formed on silicon oxide. These results suggest that Fn acquires a compact structure on parylene-C and a more extended structure on silicon oxide. Nonetheless, parylene-C and silicon oxide substrates coated with Fn host cell populations that exhibit focal adhesion complexes and good cell attachment. Albumin adopts a deformed structure on parylene-C and a globular structure on silicon oxide, and does not support significant cell attachment on either surface. Interestingly, the co-incubation of Fn and albumin at the ratio found in serum, results in the preferential adsorption of albumin on parylene-C and Fn on silicon oxide. This finding is supported by the exclusive formation of focal adhesion complexes in differentiated mouse embryonic stem cells (CGR8), cultured on Fn/albumin coated silicon oxide, but not on parylene-C. The detailed information provided in this study on the distinct properties of layers of serum proteins on substrates such as parylene-C and silicon oxide is highly significant in developing methods for cell patterning.
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Mode of access: Internet.
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Multiple emission peaks have been observed from surface passivated PbS nanocrystals displaying strong quantum confinement. The emission spectra are shown to be strongly dependent on the excited-state parity. We also find that intraband energy relaxation from initial states excited far above the band-edge is nearly three orders of magnitude slower than that found in other nanocrystal quantum dots, providing evidence of inefficient energy relaxation via phonon emission. The initial-state parity dependence of the photoluminescent emission properties suggests that energy relaxation from the higher excited states occurs via a radiative cascade, analogous to energy relaxation in atomic systems. Such radiative cascade emission is possible from ideal zero-dimensional semiconductors, where electronic transitions can be decoupled from phonon modes.
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Photoluminescent emission is observed from surface-passivated PbS nanocrystals following the two-photon excitation of high-energy excitonic states. The emission appears directly at the excitation energy with no detectable Stokes-shift for a wide range of excitation energies. The observation of direct emission from states excited by two-photon absorption indicates that the parity of the excited states of surface-passivated PbS nanocrystals is partially mixed.
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PbS nanocrystals were synthesized directly in the conducting polymer, poly (3 -hexylthiophene-2,5-diyl). Transmission electron microscopy shows that the PbS nanocrystals are faceted and relatively uniform in size with a mean size of 10 nm. FFT analysis of the atomic lattice planes observed in TEM and selected area electron diffraction confirm that the nanocrystals have the PbS rock salt structure. The synthesis conditions are explored to show control over the aggregation of PbS nanocrystals in the thiophene conducting polymer.
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PbS nanocrystals are synthesized using colloidal techniques and have their surfaces capped with oleic acid. The absorption band edge of the PbS nanocrystals is tuned between 900 and 580 nm. The PbS nanocrystals exhibit tuneable photoluminescence with large non-resonant Stokes shifts of up to 500 mcV. The magnitude of the Stokes shift is found to be dependent upon the size of PbS nanocrystals. Time-resolved photoluminescence spectroscopy of the PbS nanocrystals reveals that the photouminescence has an extraordinarily long lifetime of 1 mus. This long fluorescence lifetime is attributed to the effect of dielectric screening similar to that observed in other IV-VI semiconductor nanocrystals.