11 research outputs found
Impact of opioid-free analgesia on pain severity and patient satisfaction after discharge from surgery: multispecialty, prospective cohort study in 25 countries
Background: Balancing opioid stewardship and the need for adequate analgesia following discharge after surgery is challenging. This study aimed to compare the outcomes for patients discharged with opioid versus opioid-free analgesia after common surgical procedures.Methods: This international, multicentre, prospective cohort study collected data from patients undergoing common acute and elective general surgical, urological, gynaecological, and orthopaedic procedures. The primary outcomes were patient-reported time in severe pain measured on a numerical analogue scale from 0 to 100% and patient-reported satisfaction with pain relief during the first week following discharge. Data were collected by in-hospital chart review and patient telephone interview 1 week after discharge.Results: The study recruited 4273 patients from 144 centres in 25 countries; 1311 patients (30.7%) were prescribed opioid analgesia at discharge. Patients reported being in severe pain for 10 (i.q.r. 1-30)% of the first week after discharge and rated satisfaction with analgesia as 90 (i.q.r. 80-100) of 100. After adjustment for confounders, opioid analgesia on discharge was independently associated with increased pain severity (risk ratio 1.52, 95% c.i. 1.31 to 1.76; P < 0.001) and re-presentation to healthcare providers owing to side-effects of medication (OR 2.38, 95% c.i. 1.36 to 4.17; P = 0.004), but not with satisfaction with analgesia (beta coefficient 0.92, 95% c.i. -1.52 to 3.36; P = 0.468) compared with opioid-free analgesia. Although opioid prescribing varied greatly between high-income and low- and middle-income countries, patient-reported outcomes did not.Conclusion: Opioid analgesia prescription on surgical discharge is associated with a higher risk of re-presentation owing to side-effects of medication and increased patient-reported pain, but not with changes in patient-reported satisfaction. Opioid-free discharge analgesia should be adopted routinely
Direct Growth of Flexible and Scalable Photocathodes from α‑Brass Substrates
A facile, low cost method to grow
robust and adherent, single phase
metal oxides from an earth-abundant binary alloy has been outlined
and its effectiveness as a photocathode for solar energy harvesting
demonstrated. Cu<sub>0.7</sub>Zn<sub>0.3</sub> (α-brass) foils
were thermally dezincified (removal of surface Zn) at 450 °C
and subsequently oxidized, by varying the temperature from 300 to
600 °C. The brass foil served as the oxide growth substrate as
well as a conductive electrical contact for subsequent photoelectrochemical
testing. CuO nanowires were seen for the 400 and 500 °C samples.
ZnO phase was detected within the concave pores on the sample surface.
The highest photocurrent of 1.8 mA/cm<sup>2</sup> at −0.5 V
vs Ag/AgCl occurred for the sample oxidized at 500 °C with an
incident-photon-to-current-efficiency (IPCE) of 6.9% at 450 nm. This
sample corresponds to the oxide with the lowest surface zinc content
(10 at. %, measured by X-ray photoelectron spectroscopy), indicating
that the presence of ZnO hinders the performance of the photocathode.
The approach demonstrated in this work opens up possibilities for
making large area, scalable photoelectrodes directly on conductive
alloy substrates, leading to simpler electrode fabrication and opportunities
for alloy recycling for sustainable energy harvesting
Amorphous Cu_(2-δ)O as Passivation Layer for Ultra Long Stability of Copper Oxide Nanowires in Photoelectrochemical Environments
Core-shell CuO-Cu_2O nanowires with a surface amorphous Cu2-δO layer leads to high stability photocathodes for use in photoelectrochemical splitting of water. The nanowires are synthesized via carbothermal reduction of CuO nanowires at 300°C during which a 2–3 nm conformal and amorphous Cu_(2-δ)O layer is formed on the nanowire surface. This Cu_(2-δ)O layer enhances photocurrent and improves photocorrosion stability of the nanowires. While catalyst-free, pristine CuO nanowires show a photocurrent density is 0.50 mA/cm^2 and a stability of 53% after 3.4 hours of testing at −0.50 V under AM1.5 G conditions; the catalyst-free, carbothermally reduced nanowires achieve a photocurrent density of 0.75 mA/cm^2 and an improved stability of 96% under identical test conditions. The mechanism of enhanced photocurrent and its stability is discussed in the context of extensive pre and post test nanowire characterization
Amorphous Cu_(2-δ)O as Passivation Layer for Ultra Long Stability of Copper Oxide Nanowires in Photoelectrochemical Environments
Core-shell CuO-Cu_2O nanowires with a surface amorphous Cu2-δO layer leads to high stability photocathodes for use in photoelectrochemical splitting of water. The nanowires are synthesized via carbothermal reduction of CuO nanowires at 300°C during which a 2–3 nm conformal and amorphous Cu_(2-δ)O layer is formed on the nanowire surface. This Cu_(2-δ)O layer enhances photocurrent and improves photocorrosion stability of the nanowires. While catalyst-free, pristine CuO nanowires show a photocurrent density is 0.50 mA/cm^2 and a stability of 53% after 3.4 hours of testing at −0.50 V under AM1.5 G conditions; the catalyst-free, carbothermally reduced nanowires achieve a photocurrent density of 0.75 mA/cm^2 and an improved stability of 96% under identical test conditions. The mechanism of enhanced photocurrent and its stability is discussed in the context of extensive pre and post test nanowire characterization
Indirect Phase Transformation of CuO to Cu<sub>2</sub>O on a Nanowire Surface
The
reduction of CuO nanowires (NWs) to Cu<sub>2</sub>O NWs undergoes
an indirect phase transformation on the surface: from single crystalline
CuO, to a disordered Cu<sub>2−δ</sub>O phase, and then
to crystalline Cu<sub>2</sub>O. A 9–12 nm disordered Cu<sub>2−δ</sub>O is formed on the NW surface by exposing CuO
NWs to CO at 1 Torr, 300 °C for 30 min. After 60 min, this layer
decreases to 2–3 nm and is eliminated after 180 min. Energy
dispersive X-ray spectroscopy using a scanning tunneling electron
microscope and across a single NW reveals the disordered layer to
be O-rich with respect to Cu<sub>2</sub>O with a maximum at. % Cu:O
= 1.8. X-ray photoelectron spectroscopy shows adsorbed CO on the surface
as evidence of the reduction reaction. Micro-Raman spectroscopy tracks
the transformation in NWs as a function of reduction time. A CO enabled
surface reduction reaction coupled to diffusion-limited transport
of “nonlattice” O to the surface is proposed as a mechanism
for Cu<sub>2−δ</sub>O formation. The initial buildup
of out-diffusing O to the surface appears to aid the formation of
the disordered surface layer. The transformation follows Ostwald–Lussac’s
law which predicts formation of unstable phases over stable phases,
when phase transformation rates are limited by kinetic or diffusional
processes. The study provides a generalized approach for facile growth
of few nanometer transient layers on multivalent, metal oxide NW surfaces
Highly Conducting, <i>n</i>‑Type Bi<sub>12</sub>O<sub>15</sub>Cl<sub>6</sub> Nanosheets with Superlattice-like Structure
Modulating the type
and magnitude of electrical conductivity remains
a basic requirement for a semiconductor’s widespread acceptability
and use. Here, we convert nanosheets of BiOCl, a V–VI–VII
ternary semiconductor, to an oxygen-rich Bi<sub>12</sub>O<sub>15</sub>Cl<sub>6</sub> phase. In the process, the intrinsic conductivity
switches from <i>p</i>-type to <i>n</i>-type.
The phase change is achieved using a vacuum annealing step at 500
°C for 1 h. BiOCl nanosheets convert to the Bi<sub>12</sub>O<sub>15</sub>Cl<sub>6</sub> phase via volatilization of BiCl<sub>3</sub> resulting in a unique superlattice like structure with a periodicity
of 1.48 nm. Correspondingly, the band gap decreases from 3.41 to 2.48
eV from the raising of the valence band edge. Activation energy for
electrical conductivity reduces from 862 meV for BiOCl to 778 meV
for Bi<sub>12</sub>O<sub>15</sub>Cl<sub>6</sub>, and a corresponding
photoconductivity increase of 80× is observed. Density functional
theory calculations predict changes to the valence band and increase
in the Fermi level toward the conduction band edge for the Bi<sub>12</sub>O<sub>15</sub>Cl<sub>6</sub> nanosheetsin accordance
with experimental data. The availability of both <i>p</i>- and <i>n</i>-type ternary semiconducting systems widen
the application base for Bi–O–Cl based materials
Cationically Substituted Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl Nanosheets as Li Ion Battery Anodes
Cation substitution
of Bi<sup>3+</sup> with Fe<sup>3+</sup> in
BiOCl leads to the formation of ionically layered Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl nanosheets. The synthesis follows a hydrolysis
route using bismuth(III) nitrate and iron(III) chloride, followed
by postannealing at 500 °C. Room temperature electrical conductivity
improves from 6.11 × 10<sup>–8</sup> S/m for BiOCl to
6.80 × 10<sup>–7</sup> S/m for Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl. Correspondingly, the activation energy for electrical
conduction reduces from 862 meV for pure BiOCl to 310 meV for Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl. These data suggest improved charge
mobility in Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl nanosheets. Density
functional theory calculations confirm this behavior by predicting
a high density of states near the Fermi level for Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl. The improvement in electrical conductivity is
exploited in the electrochemical performance of Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl nanosheets. The insertion capacity of Li<sup>+</sup> ions shows an increase of 2.5×, from 215 mAh·.g<sup>–1</sup> for undoped BiOCl to 542 mAh·g<sup>–1</sup> for Bi<sub>0.7</sub>Fe<sub>0.3</sub>OCl after 50 cycles at a current density
of 50 mA·g<sup>–1</sup>. Thus, the direct substitution
of Bi<sup>3+</sup> sites with Fe<sup>3+</sup> in BiOCl results in
nanosheets of an ionically layered ternary semiconductor compound
which is attractive for Li ion battery anode applications