4,246 research outputs found
De-agglomeration of nanoparticles in an impactor-assisted fluidized bed
High surface-to-volume ratio and high activity of nanoparticles cause interesting changes in material properties; however, these features often lead to the formation of undesired agglomerates. When agglomerated, nanoparticles lose their outstanding properties; hence, it is essential to break them up prior to use, and prevent the re-agglomeration.
There are several techniques to de-agglomerate nanoparticles, such as rapid expansion of supercritical suspensions (1) and low pressure single stage impactors (2). Utilizing fluidized beds, Pfeffer et al. applied a downwardly facing micro-jet in order to enhance the quality of nanoparticle fluidization (3). Bremer et al. (4) patented a method to de-agglomerate catalyst particles by applying a high velocity jet upwardly in the fluidized bed. Further efforts by Yi (5), using a vibrated fluidized bed, focused on particle mass concentration rather than de-agglomeration of nanoparticles. However, all these attempts were not able to result in long-lasting nano scale particle dispersions.
The main objective of this project is to break up the large fractal-shaped agglomerates to smaller clusters, preferably to individual nanoparticles, using an impactor-assisted fluidized bed. In our work, a fluidized bed is equipped with a pulsed-jet and an impaction plate. The force required to destroy the agglomerates is controlled by the gas jet velocity in the impaction zone. Calculating the impcation velocity determines the kinetic energy of particles upon impaction and makes it possible to measure the fragmentation degree of nanoparticles. This impactor-assisted bed also includes a surface functionalization post-treatment, based on photo-initiated chemical vapor deposition (6), to ensure particle stability.
REFERENCES
1. To, D., R. Dave, X. Yin, and S. Sundaresan, Deagglomeration of nanoparticle aggregates via rapid expansion of supercritical or high-pressure suspensions. AlChE J., 2009. 55(11): p. 2807-2826.
2. Seipenbusch, M., P. Toneva, W. Peukert, and A.P. Weber, Impact Fragmentation of Metal Nanoparticle Agglomerates. Part. Part. Syst. Char., 2007. 24(3): p. 193-200.
3. Pfeffer, R. and J.A.Q.J. Flesch, Fluidized Bed Systems And Methods Including Micro-Jet Flow. 2008, New Jersey Institute Of Technology Evonik Degussa Gmbh.
4. Bremer, N.J., L.R. Trott, and T.R. McDonel, Method for deagglomerating and re-exposing catalyst in a fluid bed reactor. 1992-06-23 The Standard Oil Company.
5. Nurkiewicz, J.Y.T.R., Nanoparticle aerosol generator, USPTO, Editor. 2014, West Virginia University: US.
6. Dorval Dion, C.A., W. Raphael, E. Tong, and J.R. Tavares, Photo-initiated chemical vapor deposition of thin films using syngas for the functionalization of surfaces at room temperature and near-atmospheric pressure. Surf. Coat. Technol., 2014. 244: p. 98-108
Tight lower bound to the geometric measure of quantum discord
Dakic, Vedral and Brukner [Physical Review Letters \tf{105},190502 (2010)]
gave a geometric measure of quantum discord in a bipartite quantum state as the
distance of the state from the closest classical quantum (or zero discord)
state and derived an explicit formula for a two qubit state. Further, S.Luo and
S.Fu [Physical Review A \tf{82}, 034302 (2010)] obtained a generic form of this
geometric measure for a general bipartite state and established a lower bound.
In this brief report we obtain a rigorous lower bound to the geometric measure
of quantum discord in a general bipartite state which dominates that obtained
by S.Luo and S.Fu.Comment: 10 pages,2 figures. In the previous versions, a constraint was
ignored while optimizing the second term in Eq.(5), in which case, only a
lower bound on the geometric discord can be obtained. The title is also
consequently changed. Accepted in Phys.Rev.
Multipartite entanglement in fermionic systems via a geometric measure
We study multipartite entanglement in a system consisting of
indistinguishable fermions. Specifically, we have proposed a geometric
entanglement measure for N spin-1/2 fermions distributed over 2L modes (single
particle states). The measure is defined on the 2L qubit space isomorphic to
the Fock space for 2L single particle states. This entanglement measure is
defined for a given partition of 2L modes containing m >= 2 subsets. Thus this
measure applies to m <= 2L partite fermionic system where L is any finite
number, giving the number of sites. The Hilbert spaces associated with these
subsets may have different dimensions. Further, we have defined the local
quantum operations with respect to a given partition of modes. This definition
is generic and unifies different ways of dividing a fermionic system into
subsystems. We have shown, using a representative case, that the geometric
measure is invariant under local unitaries corresponding to a given partition.
We explicitly demonstrate the use of the measure to calculate multipartite
entanglement in some correlated electron systems. To the best of our knowledge,
there is no usable entanglement measure of m > 3 partite fermionic systems in
the literature, so that this is the first measure of multipartite entanglement
for fermionic systems going beyond the bipartite and tripartite cases.Comment: 25 pages, 8 figure
The obscured X-ray source population in the HELLAS2XMM survey: the Spitzer view
Recent X-ray surveys have provided a large number of high-luminosity,
obscured Active Galactic Nuclei (AGN), the so-called Type 2 quasars. Despite
the large amount of multi-wavelength supporting data, the main parameters
related to the black holes harbored in such AGN are still poorly known. Here we
present the results obtained for a sample of eight Type 2 quasars in the
redshift range 0.9-2.1 selected from the HELLAS2XMM survey, for which we used
Ks-band, Spitzer IRAC and MIPS data at 24 micron to estimate bolometric
corrections, black hole masses, and Eddington ratios.Comment: 6 pages, to appear in "The Multicoloured Landscape of Compact Objects
and their Explosive Progenitors: Theory vs Observations" (Cefalu, Sicily,
June 2006). Eds. L. Burderi et al. (New York: AIP
Fractal-like hierarchical organization of bone begins at the nanoscale
INTRODUCTION: The components of bone assemble hierarchically to provide stiffness and toughness. Deciphering the specific organization and relationship between bone’s principal components—mineral and collagen—requires answers to three main questions: whether the association of the mineral phase with collagen follows an intrafibrillar or extrafibrillar pattern, whether the morphology of the mineral building blocks is needle- or platelet-shaped, and how the mineral phase maintains continuity across an extensive network of cross-linked collagen fibrils. To address these questions, a nanoscale level of three-dimensional (3D) structural characterization is essential and has now been performed. RATIONALE: Because bone has multiple levels of 3D structural hierarchy, 2D imaging methods that do not detail the structural context of a sample are prone to interpretation bias. Site-specific focused ion beam preparation of lamellar bone with known orientation of the analyzed sample regions allowed us to obtain imaging data by 2D high-resolution transmission electron microscopy (HRTEM) and to identify individual crystal orientations. We studied higher-level bone mineral organization within the extracellular matrix by means of scanning TEM (STEM) tomography imaging and 3D reconstruction, as well as electron diffraction to determine crystal morphology and orientation patterns. Tomographic data allowed 3D visualization of the mineral phase as individual crystallites and/or aggregates that were correlated with atomic-resolution TEM images and corresponding diffraction patterns. Integration of STEM tomography with HRTEM and crystallographic data resulted in a model of 3D mineral morphology and its association with the organic matrix. RESULTS: To visualize and characterize the crystallites within the extracellular matrix, we recorded imaging data of the bone mineral in two orthogonal projections with respect to the arrays of mineralized collagen fibrils. Three motifs of mineral organization were observed: “filamentous” (longitudinal or in-plane) and “lacy” (out-of-plane) motifs, which have been reported previously, and a third “rosette” motif comprising hexagonal crystals. Tomographic reconstructions showed that these three motifs were projections of the same 3D assembly. Our data revealed that needle-shaped, curved nanocrystals merge laterally to form platelets, which further organize into stacks of roughly parallel platelets separated by gaps of approximately 2 nanometers. These stacks of platelets, single platelets, and single acicular crystals coalesce into larger polycrystalline aggregates exceeding the lateral dimensions of the collagen fibrils, and the aggregates span adjacent fibrils as continuous, cross-fibrillar mineralization. CONCLUSION: Our findings can be described by a model of mineral and collagen assembly in which the mineral organization is hierarchical at the nanoscale. First, the data reveal that mineral particles are neither exclusively needle- nor platelet-shaped, but indeed are a combination of both, because curved acicular elements merge laterally to form slightly twisted plates. This can only be detected when the organic extracellular matrix is preserved in the sample. Second, the mineral particles are neither exclusively intrafibrillar nor extrafibrillar, but rather form a continuous cross-fibrillar phase where curved and merging crystals splay beyond the typical dimensions of a single collagen fibril. Third, in the organization of the mineral phase of bone, a helical pattern can be identified. This 3D observation, integrated with previous studies of bone hierarchy and structure, illustrates that bone (as a material, as a tissue, and as an organ) follows a fractal-like organization that is self-affine. The assembly of bone components into nested, helix-like patterns helps to explain the paradoxical combination of enhanced stiffness and toughness of bone and results in an expansion of the previously known hierarchical structure of bone to at least 12 levels
Genomic comparison of diverse Salmonella serovars isolated from swine.
Food animals act as a reservoir for many foodborne pathogens. Salmonella enterica is one of the leading pathogens that cause food borne illness in a broad host range including animals and humans. They can also be associated with a single host species or a subset of hosts, due to genetic factors associated with colonization and infection. Adult swine are often asymptomatic carriers of a broad range of Salmonella servoars and can act as an important reservoir of infections for humans. In order to understand the genetic variations among different Salmonella serovars, Whole Genome Sequences (WGS) of fourteen Salmonella serovars from swine products were analyzed. More than 75% of the genes were part of the core genome in each isolate and the higher fraction of gene assign to different functional categories in dispensable genes indicated that these genes acquired for better adaptability and diversity. High concordance (97%) was detected between phenotypically confirmed antibiotic resistances and identified antibiotic resistance genes from WGS. The resistance determinants were mainly located on mobile genetic elements (MGE) on plasmids or integrated into the chromosome. Most of known and putative virulence genes were part of the core genome, but a small fraction were detected on MGE. Predicted integrated phage were highly diverse and many harbored virulence, metal resistance, or antibiotic resistance genes. CRISPR (Clustered regularly interspaced short palindromic repeats) patterns revealed the common ancestry or infection history among Salmonella serovars. Overall genomic analysis revealed a great deal of diversity among Salmonella serovars due to acquired genes that enable them to thrive and survive during infection
Energy Deposition Studies for Possible Innovative Phase II Collimator Designs
Due to the known limitations of Phase I LHC collimators in stable physics conditions, the LHC collimation system will be complemented by additional 30 Phase II collimators. The Phase II collimation system is designed to improve cleaning efficiency and to minimize the collimator-induced impedance with the main function of protecting the Super Conducting (SC) magnets from quenching due to beam particle losses. To fulfil these requirements, different possible innovative collimation designs were taken in consideration. Advanced jaw materials, including new composite materials (e.g. Cu–Diamond), jaw SiC insertions, coating foil, in-jaw instrumentation (e.g. BPM) and improved mechanical robustness of the jaw are the main features of these new promising Phase II collimator designs developed at CERN. The FLUKA Monte Carlo code is extensively used to evaluate the behavior of these collimators in the most radioactive areas of LHC, supporting the mechanical integration. These studies aim to identify the possible critical points along the IR7 line
- …