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  • 1
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    PANGAEA
    In:  British Oceanographic Data Center
    Publication Date: 2023-04-28
    Keywords: Attenuation, optical beam transmission; Attenuation, optical beam transmission, potential; Calculated; CH125B; Challenger; Chlorophyll a; CP100; CP101; CP102; CP103; CP104; CP105; CP106; CP107; CP108; CP109; CP110; CP111; CP112; CP113; CP114; CP115; CP116; CP117; CP118; CP119; CP120; CP121; CP122; CP123; CP124; CP125; CP126; CP127; CP128; CP129; CP130; CP131; CP132; CP133; CP134; CP135; CP136; CP137; CP138; CP139; CP140; CP142; CP143; CP144; CP145; CP146; CP147; CP148; CP149; CP150; CP151; CP152; CP153; CP154; CP155; CP156; CP157; CP158; CP159; CP160; CP161; CP162; CP163; CP164; CP165; CP166; CP167; CP168; CP169; CP170; CP171; CP172; CP173; CP174; CP175; CP176; CP177; CP178; CP179; CP180; CP48; CP49; CP50; CP51; CP52; CP53; CP54; CP55; CP56; CP57; CP58; CP60; CP61; CP62; CP63; CP64; CP65; CP66; CP67; CP68; CP69; CP70; CP71; CP72; CP73; CP74; CP75; CP76; CP77; CP78; CP79; CP80; CP81; CP82; CP83; CP84; CP85; CP86; CP87; CP88; CP89; CP90; CP91; CP92; CP93; CP94; CP95; CP96; CP97; CP98; CP99; CTD, Neil Brown, Mark III B; CTD/Rosette; CTD-RO; Date/Time of event; Density, sigma-theta (0); DEPTH, water; Event label; Hebridean Slope; Irradiance, downward PAR; Irradiance, upward PAR; Land-Ocean Interaction Study; Latitude of event; LOIS; LOIS-79874; LOIS-79876; LOIS-79878; LOIS-79880; LOIS-79882; LOIS-79884; LOIS-79886; LOIS-79888; LOIS-79890; LOIS-79892; LOIS-79894; LOIS-79896; LOIS-79898; LOIS-79900; LOIS-79902; LOIS-79904; LOIS-79906; LOIS-79908; LOIS-79910; LOIS-79912; LOIS-79914; LOIS-79916; LOIS-79918; LOIS-79920; LOIS-79922; LOIS-79924; LOIS-79926; LOIS-79928; LOIS-79930; LOIS-79932; LOIS-79934; LOIS-79936; LOIS-79938; LOIS-79940; LOIS-79942; LOIS-79944; LOIS-79946; LOIS-79948; LOIS-79950; LOIS-79952; LOIS-79954; LOIS-79956; LOIS-79958; LOIS-79960; LOIS-79962; LOIS-79964; LOIS-79966; LOIS-79968; LOIS-79970; LOIS-79972; LOIS-79974; LOIS-79976; LOIS-79978; LOIS-79980; LOIS-79982; LOIS-79984; LOIS-79986; LOIS-79988; LOIS-79990; LOIS-79992; LOIS-79994; LOIS-79996; LOIS-79998; LOIS-80000; LOIS-80002; LOIS-80004; LOIS-80006; LOIS-80008; LOIS-80010; LOIS-80012; LOIS-80014; LOIS-80016; LOIS-80018; LOIS-80020; LOIS-80022; LOIS-80024; LOIS-80026; LOIS-80028; LOIS-80030; LOIS-80032; LOIS-80034; LOIS-80036; LOIS-80038; LOIS-80040; LOIS-80042; LOIS-80044; LOIS-80046; LOIS-80048; LOIS-80050; LOIS-80052; LOIS-80054; LOIS-80056; LOIS-80058; LOIS-80060; LOIS-80062; LOIS-80064; LOIS-80066; LOIS-80068; LOIS-80070; LOIS-80072; LOIS-80074; LOIS-80076; LOIS-80078; LOIS-80080; LOIS-80082; LOIS-80084; LOIS-80086; LOIS-80088; LOIS-80090; LOIS-80092; LOIS-80094; LOIS-80096; LOIS-80098; LOIS-80100; LOIS-80102; LOIS-80104; LOIS-80106; LOIS-80108; LOIS-80110; LOIS-80112; LOIS-80114; LOIS-80116; LOIS-80118; LOIS-80120; LOIS-80122; LOIS-80124; LOIS-80126; LOIS-80128; LOIS-80130; LOIS-80132; LOIS-80134; Longitude of event; Optional event label; Oxygen; Oxygen probe, Beckmann Instruments; Oxygen saturation; PML 2pi PAR (photosynthetically available radiation) sensor; Pressure, water; Salinity; Temperature, water; Temperature, water, potential; UV AquaTracka Fluorometer, Chelsea Instruments
    Type: Dataset
    Format: text/tab-separated-values, 309325 data points
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 729-735 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In order to understand the effects of density fluctuations in composite systems, we have studied the effects of compression rate on the final density and density variations in a system of hard spheres. Systems of 900 and 1800 mono-sized spheres are placed in a box with periodic boundary conditions in the x and y directions and walls at z=0 and z=w(t). Using hard-sphere interactions between the particles, the cell is compressed at a constant rate κ∝−dw/dt under isothermal conditions until the pressure diverges and an overlap occurs between the particles or with the walls. The final particle volume is then subdivided into smaller cells, each containing about 15 particles with a local density p(x). Macroscopic fluctuations in the density are measured by the coarseness parameter Cp=σp/p¯, where σp is the standard deviation of the local densities and p¯ is the average density. Surprisingly, the coarseness reaches a maximum at intermediate compression rates and, within the range of compression rates studied, the most homogeneous particle packings are generated by fast compressions. For compression rates above 1, the distribution function of the local densities is a Gaussian with a mean close to the random dense packing value p(x)≈0.64. For compression rates below 1, local regions vary from randomly dense-packed [p(x)≈0.64] to close-packed [ p(x)≈0.74] with a correspondingly high coarseness. So for κ〈1, the distribution function is bimodal with peaks near the random-dense packing and the close-packing values. At the highest compression rates, the pressure exhibits no anomalies and the radial distribution function shows no signs of crystallization. Consequently, the densities and coarseness are very reproducible. At slower compression rates with κ〈1, large variations in the final densities and coarsenesses coincide with the formation of local crystallites in portions of the volume. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Industrial & engineering chemistry 40 (1948), S. 2054-2059 
    ISSN: 1520-5045
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Industrial & engineering chemistry 41 (1949), S. 112-119 
    ISSN: 1520-5045
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Industrial & engineering chemistry 46 (1954), S. 1917-1921 
    ISSN: 1520-5045
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 6365-6367 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Double layer thin films of permalloy (layer thickness 200–1300 A(ring)) with tantalum (50 A(ring)) as a nonmagnetic spacer have been prepared by e-beam evaporation. The effect of deposition parameters, especially the substrate temperature on the magnetic properties of these films has been examined. The coercivity(Hc) of the double layer films was found to be very sensitive to the substrate temperature in the permalloy layer thickness range of 200–600 A(ring). The coercivity of the films deposited at 40 °C is lower than at 300 °C and is almost independent of the Permalloy layer thickness. The XRD patterns and STM images of these two films exhibit large differences in permalloy grain size and grain orientation. However, the Hc of the single layer films deposited under the same conditions as the double layer films shows no significant change in this thickness region. The results indicate that the change of interface condition is primarily responsible for the Hc variation in the coupled films deposited at different substrate temperatures and strongly suggest that interface roughness plays a dominant role in the coupling between the permalloy layers.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5978-5980 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This work considers the role of magnetic dipole coupling in multilayers typically comprising a ferromagnetic material separated by a nonmagnetic metal spacer, e.g., NiFe/Ta. It has been suggested previously that dipolar fields may play an important role in the coupling of magnetic layers through a nonmagnetic spacer, in particular where surface roughness at the interface is significant. This work considers a first-order calculation of the dipole coupling energy and magnetic field between two adjacent layers. It is shown that dipole coupling energies originating from surface corrugations can behave in the same manner as a coercive field in terms of dependence on nonmagnetic spacer thickness and the degree of roughness. Interestingly, calculations also show that both ferromagnetic- and antiferromagnetic-like coupling can be explained in terms of this model. The role of the spacer thickness, magnetic layer thickness, and the form of the roughness is discussed.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 6997-6999 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The low coercivity of uniaxial thin nickel-iron multilayer films, prepared according to E. W. Hill, J. P. Li, and J. K. Birtwistle [J. Appl. Phys. 69, 4526 (1991)], makes them attractive for magnetic sensor applications. Barkhausen jumps, causing noise, limit the performance of such sensors. It has been reported [R. F. Soohoo, J. Appl. Phys. 69, 5871 (1991)] that, for any given sample under identical initial conditions, these Barkhausen jumps are deterministic rather than noisy in nature. This is consistent with the fact that the defect structure of a given sample is deterministic. This study compares power spectra and coercivity distributions from Barkhausen pulses obtained by applying varying alternating fields to thin permalloy films. The effect of an orthogonal bias field is also examined. The samples under examination consist of both single layer and bilayer films, produced as continuous layers by vacuum evaporation and ion milled into 40 mm diameter discs. The permalloy is of 80/20 composition and has a total thickness of 100 nm. The bilayer films have a nonmagnetic tantalum interlayer of thickness 5 nm. The rate of change of the applied field was varied between 2918.4 and 11.4 Oe/s, at an initial amplitude of 90 Oe. The results show that the Barkhausen pulses have a strong deterministic trend, but also contain a smaller nondeterministic component. As the frequency and amplitude are decreased, this random effect becomes larger. As might be expected when an orthogonal bias field is applied to the samples, the amplitudes of the pulses are decreased. The films also exhibit a corresponding reduction in coercivity.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 5862-5864 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Thin film Permalloy strips are used extensively for magnetoresistive sensors both in magnetometry and magnetic recording. A determination of magnetization distributions is vital to allow optimization of sensor performance. Results from a previously described scanning laser microscope (SLM) unambiguously determine magnetization distributions to submicron resolution. Operating the SLM in a mode sensitive to magnetization angles about the long axis of the strip shows typical closure domains. If the mode is sensitive to fluctuations about the strip short axis then light and dark bands are observed. These results indicate that the magnetization is not parallel with the strip edges within the domains as normally considered for closure domains. The SLM images are compared with results from a previously described numerical micromagnetic model. Results from the model compare well with those from the SLM, confirming the ability of the model to reliably predict domain activity in Permalloy strips. Results are shown for Permalloy strips of approximately 15 μm×50 μm and 250 A(ring) thick in the presence of dc and ac magnetic fields.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 6519-6521 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This work considers the use of geometric alterations to the edges of a strip of thin magnetoresistive material used to make a magnetometer device. The geometric features in the form of narrow fins are intended to improve the performance of the device by pinning the magnetization at the strip edges at an angle corresponding to the high sensitivity region of the magnetoresistance curve, thus including this region in the contribution to total resistance change. Both theoretical calculations using a micromagnetic model and experimental work on a prototype device are described. Results show that the device behaves closely to the modeling predictions, exhibiting a large sensitivity of 17 μV/V/μT, 70% greater than a more conventional device, with the additional capability of a trimmable orthogonal field rejection. Differences between the predicted and measured devices are described in terms of the shortcomings of the model and to domain activity in the device.
    Type of Medium: Electronic Resource
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