ALBERT

All Library Books, journals and Electronic Records Telegrafenberg

Language
Number of Hits per Page
Default Sort Criterion
Default Sort Ordering
Size of Search History
Default Email Address
Default Export Format
Default Export Encoding
Facet list arrangement
Maximum number of values per filter
Auto Completion
Topics (search only within journals and journal articles that belong to one or more of the selected topics)
Feed Format
Maximum Number of Items per Feed
feed icon rss

Your email was sent successfully. Check your inbox.

An error occurred while sending the email. Please try again.

Proceed reservation?

Export
Filter
Collection
  • 1
    facet.materialart.
    Unknown
    PANGAEA
    In:  Supplement to: Watts, Keith F; Varga, L L; Feary, David A (1993): Origins, timing, and implications of Miocene to Pleistocene turbidites, debris flows, and slump deposits of the Queensland Trough, northeastern Australia (Site 823). In: McKenzie, JA; Davies, PJ; Palmer-Julson, A; et al. (eds.), Proceedings of the Ocean Drilling Program, Scientific Results, College Station, TX (Ocean Drilling Program), 133, 379-445, https://doi.org/10.2973/odp.proc.sr.133.248.1993
    Publication Date: 2024-01-09
    Description: More than 2000 turbidite, debris-flow, and slump deposits recovered at Site 823 record the history of the Queensland Trough since the middle Miocene and provide new insights about turbidites, debris flow, and slump deposits (herein termed gravity deposits). Changes in the composition and nature of gravity deposits through time can be related to tectonic movements, fluctuations in eustatic sea level, and sedimentological factors. The Queensland Trough is a long, relatively narrow, structural depression that formed as a result of Cretaceous to Tertiary rifting of the northeastern Australia continental margin. Thus, tectonics established the geometry of this marginal basin, and its steep slopes set the stage for repeated slope failures. Seismic data indicate that renewed faulting, subsidence, and associated tectonic tilting occurred during the early late Miocene (continuing into the early Pliocene), resulting in unstable slopes that were prone to slope failures and to generation of gravity deposits. Tectonic subsidence, together with a second-order eustatic highstand, resulted in platform drowning during the late Miocene. The composition of turbidites reflects their origin and provides insights about the nature of sedimentation on adjacent shelf areas. During relative highstands and times of platform drowning, planktonic foraminifers were reworked from slopes and/or drowned shelves and were redeposited in turbidites. During relative lowstands, quartz and other terrigenous sediment was shed into the basin. Quartzose turbidites and clay-rich hemipelagic muds also can record increased supply of terrigenous sediment from mainland Australia. Limestone fragments were eroded from carbonate platforms until the drowned platforms were buried under hemipelagic sediments following the late Miocene drowning event. Bioclastic grains and neritic foraminifers were reworked from neritic shelves during relative lowstands. During the late Pliocene (2.6 Ma), the increased abundance of bioclasts and quartz in turbidites signaled the shallowing and rejuvenation of the northeastern Australia continental shelf. However, a one-for-one relationship cannot be recognized between eustatic sea-level fluctuations and any single sedimentologic parameter. Perhaps, tectonism and sedimentological factors along the Queensland Trough played an equally important role in generating gravity deposits. Turbidites and other gravity deposits (such as those at Site 823) do not necessarily represent submarine fan deposits, particularly if they are composed of hemipelagic sediments reworked from drowned platforms and slopes. When shelves are drowned and terrigenous sediment is not directly supplied by nearby rivers/point sources, muddy terrigenous sediments blanket the entire slope and basin, rather than forming localized fans. Slope failures affect the entire slope, rather than localized submarine canyons. Slopes may become destabilized as a result of tectonic activity, inherent sediment weaknesses, and/or during relative sea-level lowstands. For this reason, sediment deposits in this setting reflect tectonic and eustatic events that caused slope instabilities, rather than migration of different submarine fan facies.
    Keywords: Ocean Drilling Program; ODP
    Type: Dataset
    Format: application/zip, 4 datasets
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 2
    Publication Date: 2024-01-09
    Keywords: 133-823A; 133-823B; 133-823C; AGE; Comment; Comment 2 (continued); Coral Sea; DEPTH, sediment/rock; Description; DRILL; Drilling/drill rig; DSDP/ODP/IODP sample designation; Event label; Joides Resolution; Layer thickness; Leg133; Ocean Drilling Program; ODP; Sample code/label; Structure; Texture
    Type: Dataset
    Format: text/tab-separated-values, 8280 data points
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 3
    Publication Date: 2024-01-09
    Keywords: 133-823; AGE; COMPCORE; Composite Core; Coral Sea; DEPTH, sediment/rock; Description; Description 2 (continued); Joides Resolution; Leg133; Ocean Drilling Program; ODP; Rock type; Sample code/label; Texture
    Type: Dataset
    Format: text/tab-separated-values, 2807 data points
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 4
    Publication Date: 2024-01-09
    Keywords: 133-823; Age model; COMPCORE; Composite Core; Coral Sea; DEPTH, sediment/rock; Description; Duration; Joides Resolution; Layer thickness; Leg133; Lithologic unit/sequence; Ocean Drilling Program; ODP; Sedimentation rate; Two-way traveltime
    Type: Dataset
    Format: text/tab-separated-values, 115 data points
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 5
    Publication Date: 2024-01-09
    Keywords: 133-823A; 133-823B; 133-823C; Abbreviation; Age model; Ageprofile Datum Description; Calculated; Coral Sea; DEPTH, sediment/rock; Description; DRILL; Drilling/drill rig; DSDP/ODP/IODP sample designation; Event label; Joides Resolution; Leg133; Ocean Drilling Program; ODP; Sample code/label; Sample code/label 2; Sedimentation rate; Type
    Type: Dataset
    Format: text/tab-separated-values, 239 data points
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5547-5549 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Measurement of P, the percentage reduction in remanence after the application of 1≤n≤104 reverse field pulses of width 0.6 ns ≤ τ ≤9 ns, are reported for five particulate tape samples including γ-Fe2O3, Co-γFe2O3, Fe, and two different barium ferrites. For τ(approximately-greater-than)τc, P depended only on nτ. It increases quite rapidly at small values of nτ depending on the media and then at higher values of nτ approximately linearly with log(nτ). In the linear regime, the decrements δ (% change/decade) agree within experimental error with the quasistatic values obtained from viscosity measurements between 10 and 100 s. Considering the arbitrariness of the logarithmic assumption, it is remarkable that the decrement is the same over eleven orders of magnitude. The reduction in P at τ〈τc is evidence for time-limited switching as reported previously. However, the dependence of P on nτ for small nτ cannot be explained by the usual viscosity model but is consistent with reptation, a phenomenon suggested by Néel.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 4995-4997 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: FeTaN single-crystal thin films were grown in order to investigate the dependence of the crystalline anisotropy constant, K1, on the Ta and nitrogen content. Films with 5 and 10 wt % Ta and different nitrogen contents were prepared by dc sputtering on MgO(100) substrates at elevated temperatures. The film/substrate orientation was (100)(parallel)(100) and [100](parallel)[110]. The values of K1 were determined by measuring the in-plane angular dependence of the ferromagnetic resonance spectra and agreed very well with the values obtained from torque measurements, indicating that the total volume was biaxial cubic material. The hysteresis loops were characteristic of biaxial anisotropy and the anisotropy fields estimated from magnetization curves were consistent with the resonance and torque data. In Fe, K1 was (4.8±0.1)×105 ergs/cc in good agreement with the bulk value. In FeTa, K1 decreased to (4.4±0.1)×105 and (3.5±0.1)×105 ergs/cc for 5 and 10 wt % Ta content, respectively, and further to (2.7±0.1)×105 and (2.1±0.1)×105 ergs/cc in (Fe95Ta5)N depending on the nitrogen content. The nitrogen addition to Fe90Ta10 resulted in the formation of epitaxial (FeTa)4N which is an fcc structure with a negative K1 of (−1.5±0.2)×105 ergs/cc. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 87 (2000), S. 6433-6435 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have studied the differences in the temperature dependence of exchange anisotropy of PdPtMn/CoFeB, NiFe, and NiFeTa bilayers to understand the role of ordering temperatures. The three different ferromagnetic layers [Curie temperatures: TCNiFeTa(400 °C)〈TCNiFe(570 °C)〈TCCoFeB(1040 °C)] exchange biased by the same antiferromagnet [Néel temperature: TNPdPtMn(600 °C)] showed significantly different behavior: the exchange bias field was monotonically decreasing with temperature for the CoFeB and showed distinct, broad peak for NiFe and NiFeTa at a lower temperature before it decreased above 200 °C. The temperature dependence of exchange anisotropy, calculated from the measured exchange bias field and saturation magnetization, was also different for the three bilayers as a result of the differences in Hua and MFM. The results could be understood by the modified thermal fluctuation aftereffect model, which includes the temperature dependence of the ferromagnetic magnetization and the assumption that the ordering temperature of the ferromagnetic film is different at the interface with antiferromagnet from the rest of the ferromagnetic film due to the exchange coupling with a material with high Néel temperature. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 6943-6945 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Conventional and specular spin valve films in a current perpendicular to plane (CPP) structure have been investigated. The specular spin valve film with bottom type structure had two oxidized layers: one in the pinned layer, which was oxidized during an in situ deposition process, and the other in the free layer, which was a naturally oxidized Cu/Ta cap. Both films had increasing resistance, R, and resistance change, ΔR, with decreasing element size. The conventional spin valve film showed a resistance times area product, RA, of 144 mΩ μm2 and a resistance change area product, ΔRA, of 0.7 mΩ μm2 while the specular spin valve film showed RA of 1120 mΩ μm2 and ΔRA of 23 mΩ μm2. The ΔRA of the specular spin valve film was about 33 times larger than that of the conventional spin valve film. The calculated magnetoresistance (MR) ratios, MRSV, of each spin valve film were 1.9% and 2.3%, respectively. We think oxidized layers in the spin valve film caused the specular electron scattering and this lengthened the path of the conduction electrons, enhancing the interfacial and bulk spin dependent scattering. We estimated the output voltage change of the 0.01 μm2 element, the size required for 150 Gb/in.2 recording density, of the specular spin valve film in CPP mode to be 5.3 mV. It was almost six times larger than that of the conventional spin valve film at constant power consumption. Specular spin valve film are advantageous for the CPP structure element for future giant MR sensors. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 83 (1998), S. 5955-5966 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Epitaxial FeTaN films (∼1500 Å) were grown as a function of nitrogen flow rate on epitaxial Cu(001) buffer layers (∼2000 Å) on Si(001) single crystal substrates to investigate the effect of Ta and nitrogen on the magnetocrystalline anisotropy and magnetostriction. Detailed structural investigation by transmission electron microscopy and x-ray diffraction showed that the FeTaN films were epitaxial with the Pitsch orientation relationship of FeTaN(110)(parallel)Cu(001) and FeTaN〈111〉(parallel)Cu〈110〉, which allows four different in-plane variants to coexist in the film. It was found that the saturation magnetization did not change with nitrogen addition (∼1600 emu/cc) up to 2% lattice dilation. The values of K1 and λ100 of Fe decreased slightly (20% and 10%, respectively), while λ111 increased with increasing nitrogen content and eventually changed sign at ∼2% normalized lattice dilation. These results qualitatively agree with our earlier findings on (001) oriented FeTaN epitaxial films on MgO single crystal substrates. Also, our calculated saturation magnetostriction for nanocrystalline samples agrees very well with published data on the same FeTaN composition. Based on Hoffmann's ripple theory the ripple constant is calculated for nanocrystalline films using the Doyle–Finnegan model for the local average anisotropy and our measured single crystal constants. It was found that the effect of nitrogen on reducing the average anisotropy through the fundamental constants is not significant, and therefore the major factor in achieving a low ripple constant (i.e., soft magnetic properties) is the grain size, the number of grains across the thickness and the thin film stress. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
Close ⊗
This website uses cookies and the analysis tool Matomo. More information can be found here...