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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 71 (2000), S. 437-443 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Factors leading to a decrease in the resonance quality (the Q factor) of quartz microtuning fork/optical fiber assemblies used as sensing elements in near-field scanning optical microscopes were considered using a simple elastomechanical analysis. Experiments to test the predictions of the analysis were carried out and strategies for recovering high Q factors were proposed and tested. Three major factors affecting the magnitude of the Q factor are discussed. The first is the stiffness imparted to the tine of the microtuning fork by the optical fiber attached to it; the second is the location of the attachment point of the fiber along the tine; the third is the resonant vibrational excitation of the fiber tip which acts as an energy dissipative channel. For tapping mode operation using a standard 125 μm diameter fiber, the large longitudinal stiffness of the fiber results in a dramatic Q-factor degradation. This effect can be overcome by reducing the diameter of the fiber cladding, d, and by slightly bending the fiber. Under these conditions, bending rather than longitudinal stretching dominates the fiber dynamics. The effective bending force constant for a thinned fiber is predicted to be proportional to d4. A sharp upturn in the Q factor is observed for d≤25 μm, consistent with this prediction. The effective stiffness and mass of the fiber are also expected to scale approximately as x3, where x is the distance from the point of attachment of the fiber to the fork's base. Hence, the Q factor can be improved further by attaching the fiber closer to the tuning fork's base. Vibrational coupling between the tuning fork and the probe tip can result in a substantial Q-factor degradation for tips of a certain size. By taking these insights into consideration, we were able to construct tapping mode tuning fork/optical fiber assemblies with Q factors of up to 9000. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 71 (1992), S. 5401-5409 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Scanning the scanning tunneling microscopy (STM) tip on a Au(111) (22±1)×(square root of)3 reconstructed surface causes monatomic stripes to grow preferentially on the fcc portions of the surface. Stripes several 100 nm's in length, ∼4 nm wide, and separated by spaces ranging from 2 to ∼4 nm (the hcp regions of the reconstructed surface) can be grown. Stripe formation only takes place when the scan direction corresponds, more or less, with the [1,1,−2] primary direction of the reconstruction. Growth occurs much more rapidly than can be accounted for by diffusion alone, leading to the conclusion that the STM tip transports gold, previously picked up from other portions of the surface, to the growing ends of the stripes. Stripes grown in this way may serve as convenient templates for subsequent growth of quantum wire structures by molecular beam epitaxy.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Accounts of chemical research 12 (1979), S. 229-236 
    ISSN: 1520-4898
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 4492-4492 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 6668-6679 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The adsorption of CO2 on clean silver films, oxygen treated silver films and alkali metal predosed silver films has been studied with surface enhanced Raman spectroscopy (SERS) and work function measurements. At 50 K, CO2 was observed to adsorb on vapor deposited silver films with downward vibrational frequency shifts of (approximate)15 cm−1 from the corresponding gas phase values. On oxygen pretreated films, CO2 reacts to form a surface carbonate. Isotope studies with C18 O2 show that the carbonate is formed from the reaction of CO2 with oxygen, and not from the disproportionation of CO2 . Based on the observed intensities of the vibrational bands, an orientation of the carbonate is suggested in which the molecule's plane is perpendicular to the surface. On silver films dosed with submonolayer amounts of potassium, CO2 reacts to form the C2v isomer of a K+CO−2 surface complex. Bands at 755 and 1220 cm-1 observed with potassium dosed surfaces were assigned to the νs and δ vibrational modes of CO−2. The orientation of the CO−2. ion is likely with its molecular plane perpendicular to the surface and bonded to the alkali metal through the O atoms. Experiments on lithium and cesium dosed silver surfaces led to similar conclusions. The similarity of these vibrational spectra to those reported in our recent study of CO adsorption on potassium predosed silver in which we proposed that a KOC surface complex was formed [K.J. Maynard and M. Moskovits, Chem. Phys. Lett. 142, 298 (1987)] lead us to the conclusion that K+CO−2 was formed, in that case also, from the reaction of CO with residual oxygen. The SERS band intensities associated with CO−2 showed an amonotonic dependence on CO2 exposure. This has been ascribed to depolarization by the induced dipole fields of the adsorbate molecules upon one another. Experiments with varying potassium coverage imply that the K+CO−2 ion pairs are not randomly distributed on the surface but are aggregated into islands. A Monte Carlo simulation confirmed the conclusion that only island formation could adequately account for the observed results.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 4600-4608 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The intensity of the surface enhanced Raman scattering signal from an organic molecule (usually pyrazine) adsorbed on a rough, coldly deposited Ag surface was monitored as a function of dose. The interference maxima observed in the SERS signal as a function of film thickness are not of constant intensity. Model calculations were performed assuming that the organic film adsorbed on the Ag surface is a stratified three phase medium and the modulation in SERS intensity to be the result of interference effects both in the incident and Raman scattered light. Simulations of experimental results using this model give semiquantitative agreement between the experimental and calculated SERS intensity modulation obtained with pyrazine films as a function of increasing film thickness. Experiments and model calculations were also performed for benzene, iodobenzene, and ethylene films and a method for determining the (nonbulk) values of the densities of these films is described. The implications of this interference effect on the photodecomposition of pyrazine at and near rough Ag surfaces is discussed. We reinterpret the increase in photochemical reaction rate observed with increasing pyrazine doses as being due to interference effects in the intensity incident at the Ag surface and not due to a tuning of the surface plasmon as suggested in a previous study [Wolkow and Moskovits, J. Chem. Phys. 87, 5858 (1987)].
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  • 7
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 102 (1980), S. 495-500 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 94 (1972), S. 4750-4751 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 92 (1988), S. 2957-2960 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 92 (1988), S. 6081-6085 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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