11,119 research outputs found
Optofluidic fabrication for 3D-shaped particles.
Complex three-dimensional (3D)-shaped particles could play unique roles in biotechnology, structural mechanics and self-assembly. Current methods of fabricating 3D-shaped particles such as 3D printing, injection moulding or photolithography are limited because of low-resolution, low-throughput or complicated/expensive procedures. Here, we present a novel method called optofluidic fabrication for the generation of complex 3D-shaped polymer particles based on two coupled processes: inertial flow shaping and ultraviolet (UV) light polymerization. Pillars within fluidic platforms are used to deterministically deform photosensitive precursor fluid streams. The channels are then illuminated with patterned UV light to polymerize the photosensitive fluid, creating particles with multi-scale 3D geometries. The fundamental advantages of optofluidic fabrication include high-resolution, multi-scalability, dynamic tunability, simple operation and great potential for bulk fabrication with full automation. Through different combinations of pillar configurations, flow rates and UV light patterns, an infinite set of 3D-shaped particles is available, and a variety are demonstrated
Sengstaken-Blakemore tube as a rescue treatment for hemorrhagic shock secondary to laparoscopic adjustable gastric banding erosion
Gastrointestinal bleeding is an uncommon but potentially life-threatening complication of laparoscopic adjustable gastric banding (LAGB) erosion. We present the use of a Sengstaken-Blakemore tube as a treatment device for severe gastrointestinal bleeding secondary to persistent LAGB erosion. A 72-year-old woman post-LAGB placement presented with hemorrhagic shock from gastric band erosion that was not responsive to endoscopic and angiographic interventions. A salvage attempt to tamponade with a Sengstaken-Blakemore tube resulted in successful resuscitation of the patient. When used judiciously, balloon tamponade serves as a replicable technique to control severe gastric band erosion refractory to standard management
Guest editorial
Author name used in this publication: Chi K. Tse2003-2004 > Academic research: refereed > Publication in refereed journal201805_a bcwhVersion of RecordPublishe
A Fresh Look into the Neutron EDM and Magnetic Susceptibility
We reexamine the estimate of the neutron Electric Dipole Moment (NEDM) from
chiral and QCD spectral sum rules (QSSR) approaches. In the former, we evaluate
the pion mass corrections which are about 5% of the leading Log. results.
However, the chiral estimate can be affected by the unknown value of the
renormalizaton scale nu. For QSSR, we analyze the effect of the nucleon
interpolating currents on the existing predictions. We conclude that previous
QSSR results are not obtained within the optimal choice of these operators,
which lead to an overestimate of these results by about a factor 4. The weakest
upper bound |theta|< 2 10^-9 for the strong CP-violating angle is obtained from
QSSR, while the strongest upper bound |theta|< 1.3 10^-10 comes from the chiral
approach evaluated at the scale \nu=M_N. We also re-estimate the proton
magnetic susceptibility, which is an important input in the QSSR estimate of
the NEDM.Comment: Version to appear in Phys. Lett.
Proposal for reading out anyon qubits in non-abelian quantum Hall state
To detect non-abelian statistics in the quantum Hall state
through interferometry, we apply an analysis similar to the ones proposed for
the non-abelian quantum Hall state. The result is that the
amplitude of the Aharonov-Bohm oscillation of this interference is dependent on
the internal states of quasiholes, but, in contrast to the quantum
Hall state, independent of the number of quasiholes. However, if the quasiholes
are in a superposition state, it is necessary for the interferometer to have
certain additional features to obtain the coefficients.Comment: 16 pages, 2 figures, Latex. Reference added, some errors corrected,
some content changed, some changes in the abstrac
Magmatic record of India-Asia collision
This work was financially co-supported by Chinese Academy of Sciences (XDB03010301) and other Chinese funding agencies (Project 973: 2011CB403102 and 2015CB452604; NSFC projects: 41225006, 41273044, and 41472061).New geochronological and geochemical data on magmatic activity from the India-Asia collision zone enables recognition of a distinct magmatic flare-up event that we ascribe to slab breakoff. This tie-point in the collisional record can be used to back-date to the time of initial impingement of the Indian continent with the Asian margin. Continental arc magmatism in southern Tibet during 80-40 Ma migrated from south to north and then back to south with significant mantle input at 70-43 Ma. A pronounced flare up in magmatic intensity (including ignimbrite and mafic rock) at ca. 52-51 Ma corresponds to a sudden decrease in the India-Asia convergence rate. Geological and geochemical data are consistent with mantle input controlled by slab rollback from ca. 70 Ma and slab breakoff at ca. 53 Ma. We propose that the slowdown of the Indian plate at ca. 51 Ma is largely the consequence of slab breakoff of the subducting Neo-Tethyan oceanic lithosphere, rather than the onset of the India-Asia collision as traditionally interpreted, implying that the initial India-Asia collision commenced earlier, likely at ca. 55 Ma.Publisher PDFPeer reviewe
A rigorous bound on quark distributions in the nucleon
I deduce an inequality between the helicity and the transversity distribution
of a quark in a nucleon, at small energy scales. Then I establish, thanks to
the positivity constraint, a rigorous bound on longitudinally polarized valence
quark densities, which finds nontrivial applications to d-quarks. This, in
turn, implies a bound for the distributions of the longitudinally polarized
sea, which is probably not SU(3)-symmetric. Some model predictions and
parametrizations of quark distributions are examined in the light of these
results.Comment: Talk given at the QCD03 Conference, Montpellier, 2-9 July 200
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