1,769 research outputs found
Thermal behaviour of siliceous faujasite: further structural interpretation of negative thermal expansion
The high-temperature behaviour of siliceous faujasite (Si-Y) was investigated by in situ synchrotron Xray powder diffraction from room temperature up to 1123 K. This porous phase is remarkably stable
when heated, and no phase transitions or changes in symmetry are observed. A marked negative thermal expansion (NTE), already reported in literature for a heating range from 25 to 573 K, was confirmed up to
about 923 K. Above this temperature a positive thermal expansion was observed. Si-Y’s thermal behaviour was interpreted on the basis of the transverse thermal vibrations of the oxygen atoms involved in
the T–O–T linkages and a series of other structural features characterizing the faujasite structure, namely the T–T distances between adjacent tetrahedral sites, the thickness of the double 6-membered rings, and
the ditrigonal index of the 6-membered rings. Moreover, the thermal behaviour of several other anhydrous porous materials with NTE behaviour is discussed and compared to that of Si-Y
Elastic behavior and high pressure-induced phase transition in chabazite: new data from a sample from Nova Scotia
Recently, the high pressure (HP) behavior of a natural chabazite from Vallerano [1] (VALL), and on the synthetic
phases SAPO-34 [1] and ALPO-34 [2], was investigated in the frame of a wider project aimed at understanding
the role of the framework/extraframework content on the compressibility of CHA-type porous materials.
In this work, further structural information is obtained studying the response to HP of another natural chabazite
sample from Nova Scotia (Canada) (NS) (s.g. R-3mR [3]), characterized by a different chemical composition with
respect to VALL. The study was performed by means of in situ synchrotron X-ray powder diffraction (XRPD) and
silicone oil as non-penetrating P-transmitting medium. XRPD experiments were performed in DAC at the BM01
beamline at ESRF (Grenoble, France) with a fixed =0.7355 Ã…. Powder patterns were collected from Pambup to 8.6
GPa and upon decompression. All the features of the Pamb pattern and the unit cell parameters are well recovered
upon P release. Below 2.1 GPa, a and cell parameters slightly decrease and increase respectively with a resulting
volume reduction of 3.6 %. Above 2.1 GPa, a transition to a triclinic P-1 pseudo-rhombohedral phase is observed.
The rhombohedral to triclinic phase transition is accompanied by an abrupt decrease in the unit cell parameters and
in the unit cell volume ( V=-4.0%). Between 2.5 and 5.9 GPa, the triclinic/pseudo-rhombohedral cell parameters
decrease regularly and the unit cell volume variation ( V=-3.0%) indicates a lower compressibility with respect to
that observed before the transition. In the highest P regime (5.9-7.2 GPa), a further slope change, with an increase
in compressibility, is observed. As a whole, V between Pamb and 7.2 GPa is -12.6%. The elastic parameters,
calculated with a second order BM-EoS, are V0 = 826 (1) Ã…3, K0 = 54(3) GPa and V0 = 784(2) Ã…3, K0 = 91(5)
GPa, for the rhombohedral and triclinic phase, respectively.
Preliminary results from Rietveld refinements up to about 1 GPa, suggest that the deformation mechanism acting
in the low-P regime is a cooperative tilting of the tetrahedra belonging to the double 6-ring – resulting in a decrease
of its thickness – accompanied by a simultaneous di-trigonalization of the two 6-rings. A similar mechanism was
previously observed during compression of levyne [4].
The HP-induced cell volume contraction of NS (12.6 %) is higher than that of VALL (10.3%) in the same P range.
This is congruent with the lower content in large extraframework potassium cations of NS, which contribute to
sustain the porous structure in VALL
The cryogenic RWELL: a stable charge multiplier for dual-phase liquid-argon detectors
The operation of a cryogenic Resistive WELL (RWELL) in liquid argon vapor is
reported for the first time. It comprises a Thick Gas Electron Multiplier
(THGEM) structure coupled to a resistive Diamond-Like Carbon (DLC) anode
deposited on an insulating substrate. The multiplier was operated at cryogenic
temperature (90~K, 1.2~bar) in saturated argon vapor and characterized in terms
of charge gain and electrical stability. A comparative study with standard,
non-resistive THGEM (a.k.a LEM) and WELL multipliers, confirmed the RWELL
advantages in terms of discharge quenching - thus superior gain and stability
Gut microbiome in pediatric acute leukemia: From predisposition to cure
The gut microbiome (GM) has emerged as a key factor in the genesis and progression of many diseases. The intestinal bacterial composition also influences treatment-related side effects and even the efficacy of oncological therapies. Acute leukemia (AL) is the most common cancer among children and the most frequent cause of cancer-related death during childhood. Outcomes have improved considerably over the past 4 decades, with the current long-term survival for acute lymphoblastic leukemia being ∼90%. However, several acute toxicities and long-term sequelae are associated with the multimodal therapy protocols applied in these patients. Specific GM configurations could contribute to the multistep developmental hypothesis for leukemogenesis. Moreover, GM alterations occur during the AL therapeutic course and are associated with treatment-related complications, especially during hematopoietic stem cell transplantation. The GM perturbation could last even after the removal of microbiome-modifying factors, like antibiotics, chemotherapeutic drugs, or alloimmune reactions, contributing to several health-related issues in AL survivors. The purpose of this article is to provide a comprehensive review of the chronological changes of GM in children with AL, from predisposition to cure. The underpinning biological processes and the potential interventions to modulate the GM toward a potentially health-promoting configuration are also highlighted
Cryogenic RPWELL: a novel charge-readout element for dual-phase argon TPCs
The first operation of a cryogenic Resistive Plate WELL (RPWELL) detector in
the saturated vapor of liquid argon is reported. The RPWELL detector was
composed of a Thick Gas Electron Multiplier (THGEM) electrode coupled to a
metallic anode via FeO/YSZ ceramics (FeO in weight equal to
75), with tunable bulk resistivity in the range 10 - 10
cm. The detector was operated at liquid argon temperature in
saturated argon vapor (90~K, 1.2~bar) and characterized in terms of its
effective charge gain and stability against discharges. Maximum stable gain of
G17 was obtained, without discharges. In addition, preliminary results
from novel 3D-printed thermoplastic plates doped with carbon nanotubes are
presented
The Glasgow-Maastricht foot model, evaluation of a 26 segment kinematic model of the foot
BACKGROUND: Accurately measuring of intrinsic foot kinematics using skin mounted markers is difficult, limited in part by the physical dimensions of the foot. Existing kinematic foot models solve this problem by combining multiple bones into idealized rigid segments. This study presents a novel foot model that allows the motion of the 26 bones to be individually estimated via a combination of partial joint constraints and coupling the motion of separate joints using kinematic rhythms. METHODS: Segmented CT data from one healthy subject was used to create a template Glasgow-Maastricht foot model (GM-model). Following this, the template was scaled to produce subject-specific models for five additional healthy participants using a surface scan of the foot and ankle. Forty-three skin mounted markers, mainly positioned around the foot and ankle, were used to capture the stance phase of the right foot of the six healthy participants during walking. The GM-model was then applied to calculate the intrinsic foot kinematics. RESULTS: Distinct motion patterns where found for all joints. The variability in outcome depended on the location of the joint, with reasonable results for sagittal plane motions and poor results for transverse plane motions. CONCLUSIONS: The results of the GM-model were comparable with existing literature, including bone pin studies, with respect to the range of motion, motion pattern and timing of the motion in the studied joints. This novel model is the most complete kinematic model to date. Further evaluation of the model is warranted
Novel resistive charge-multipliers for dual-phase LAr-TPCs: towards stable operation at higher gains
Cryogenic versions of Resistive WELL (RWELL) and Resistive Plate WELL
(RPWELL) detectors have been developed, aimed at stable avalanche
multiplication of ionization electrons in dual-phase TPCs. In the RWELL, a thin
resistive layer deposited on top of an insulator is inserted in between the
electron multiplier (THGEM) and the readout anode; in the RPWELL, a resistive
plate is directly coupled to the THGEM. Radiation-induced ionization electrons
in the liquid are extracted into the gaseous phase. They drift into the THGEM's
holes where they undergo charge multiplication. Embedding resistive materials
into the multiplier proved to enhance operation stability due to the mitigation
of electrical discharges - thus allowing operation at higher charge gain
compared to standard THGEM (a.k.a. LEM) multipliers. We present the detector
concepts and report on the main preliminary results
Scintillation of Ar/CF mixtures: glass-THGEM characterization with 1% CF at 1-1.5 bar
Argon gas doped with 1% wavelength-shifter (CF) has been employed in an
optical time projection chamber (OTPC) to image cosmic radiation. We present
results obtained during the system commissioning, performed with two stacked
glass-THGEMs and an EMCCD camera at 1 bar. Preliminary estimates indicate that
the combined optical gain was of the order of 10 (ph/e), producing sharp
and high-contrast raw images without resorting to any filtering or
post-processing. A first assessment of the impact of pressurization showed no
change in the attainable gains when operating at 1.5 barComment: Added reference with DOI, fixed error with axis label in plo
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