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At least 235 records · Page 13

Oxygen-atom transfer photochemistry of a molecular copper bromate complex

Here, we report the synthesis and oxygen-atom transfer (OAT) photochemistry of [Cu(tpa)BrO 3 ]ClO 4 . In situ spectroscopy and in crystallo experiments indicate OAT proceeds from a Cu–O fragment generated by sequential Cu–O bond cleavage and OAT from BrO x to [Cu(tpa)] + . Furthermore, these results highlight synthetic opportunities in M–O photochemistry and demonstrate the utility of in crystallo experiments to evaluating photochemical reaction mechanisms.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

The effect of copper on the sub-bandgap density of states of CdTe solar cells

Two optical sub-bandgap transitions in CdTe thin-film solar cells have been identified using detailed transient photocapacitance and transient photocurrent spectroscopy measurements. A broad response centered at E V + 0.9 eV directly correlates with the quantity of Cu present in the absorber layer, while a second response at E V + 1.2 eV does not depend on Cu or Zn and may be an intrinsic defect. Furthermore, these results demonstrate the influence of Cu on the sub-bandgap density of states of CdTe, and they are critical to understanding, modeling, and improving its optoelectronic properties.

14 SOLAR ENERGY↗

Determining whether metals nucleate homogeneously on graphite: A case study with copper

In this study, we observe that Cu clusters grow on surface terraces of graphite as a result of physical vapor deposition in ultrahigh vacuum. We show that the observation is incompatible with a variety of models incorporating homogeneous nucleation and calculations of atomic-scale energetics. An alternative explanation, ion-mediated heterogeneous nucleation, is proposed and validated, both with theory and experiment. This serves as a case study in identifying when and whether the simple, common observation of metal clusters on carbon-rich surfaces can be interpreted in terms of homogeneous nucleation. We describe a general approach for making system-specific and laboratory-specific predictions.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Control of the third dimension in copper-based square-lattice antiferromagnets

Using a mixed-ligand synthetic scheme, we create a family of quasi-two-dimensional antiferromagnets, namely, [Cu(HF 2 )(pyz) 2 ]ClO 4 [pyz = pyrazine], [CuL 2 (pyz) 2 ](ClO 4 ) 2 [L = pyO = pyridine-N-oxide and 4-phpy-O = 4-phenylpyridine-N-oxide. These materials are shown to possess equivalent two-dimensional [Cu(pyz) 2 ] 2+ nearly square layers, but exhibit interlayer spacings that vary from 6.5713 to 16.777 Å, as dictated by the axial ligands. We present the structural and magnetic properties of this family as determined via x-ray diffraction, electron-spin resonance, pulsed- and quasistatic-field magnetometry and muon-spin rotation, and compare them to those of the prototypical two-dimensional magnetic polymer Cu(pyz) 2 (ClO 4 ) 2 . We find that, within the limits of the experimental error, the two-dimensional, intralayer exchange coupling in our family of materials remains largely unaffected by the axial ligand substitution, while the observed magnetic ordering temperature (1.91 K for the material with the HF 2 axial ligand, 1.70 K for the pyO and 1.63 K for the 4-phpy-O) decreases slowly with increasing layer separation. Despite the structural motifs common to this family and Cu(pyz) 2 (ClO 4 ) 2 , the latter has significantly stronger two-dimensional exchange interactions and hence a higher ordering temperature. Here, we discuss these results, as well as the mechanisms that might drive the long-range order in these materials, in terms of departures from the ideal S = 1/2 two-dimensional square-lattice Heisenberg antiferromagnet. In particular, we find that both spin-exchange anisotropy in the intralayer interaction and interlayer couplings (exchange, dipolar, or both) are needed to account for the observed ordering temperatures, with the intralayer anisotropy becoming more important as the layers are pulled further apart.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Neutron and X-ray investigations of the Jahn–Teller switch in partially deuterated ammonium copper Tutton salt, (NH 4 ) 2 [Cu(H 2 O) 6 ](SO 4 ) 2

The structural phase transition accompanied by a Jahn–Teller switch has been studied over a range of H/D ratios in (NH 4 ) 2 [Cu(H 2 O) 6 ](SO 4 ) 2 (ACTS). In particular, single-crystal neutron diffraction investigations of crystals with deuteration in the range 50 to 82% are shown to be consistent with previous electron paramagnetic resonance (EPR) experiments exhibiting a phase boundary at 50% deuteration under ambient pressure. Polycrystalline samples show that the two phases can co-exist. In addition, single-crystal neutron and polycrystalline X-ray diffraction pressure experiments show a shift to lower pressure at 60% deuteration versus previous measurements at 100% deuteration.

deuterium isotope phase transition↗

Thermodynamics of copper‐manganese and copper‐iron spinel solid solutions

Abstract High‐temperature oxide melt solution calorimetry has been performed to investigate the energetics of spinel solid solutions in the Mn 3 O 4 ‐CuMn 2 O 4 and Fe 3 O 4 ‐CuFe 2 O 4 systems. The spinel solid solutions were synthesized by a ceramic route and calcined at appropriate temperatures to obtain single phase samples. The drop solution enthalpies of the solid solutions in the Mn 3 O 4 ‐CuMn 2 O 4 system are the same within experimental error as the enthalpies of drop solution of mechanical mixtures of the end‐members, indicating a zero heat of mixing, i.e., ideal mixing in terms of enthalpy. In Fe 3 O 4 ‐CuFe 2 O 4 , the drop solution enthalpy of the solid solutions shows a positive deviation from those of the mechanical mixture of the end‐members, suggesting negative mixing enthalpy. The formation enthalpies of the spinel solid solutions from their constituent oxides plus oxygen and from the elements were also determined.

Sahu, Sulata K.↗

Electrical and Thermal Properties of Cold-Sprayed Bulk Copper and Copper-Tungsten Samples at Cryogenic Temperatures

The de­vel­op­ment of high ther­mal con­duc­tiv­ity coat­ings with pure cop­per or cop­per-tung­sten alloy could be ben­e­fi­cial to im­prove the heat trans­fer of bulk Nb cav­i­ties for con­duc­tion cool­ing ap­pli­ca­tions and to in­crease the stiff­ness of bulk Nb cav­i­ties cooled by liq­uid he­lium. Cold-spray is an ad­di­tive man­u­fac­tur­ing tech­nique suit­able to grow thick coat­ings of ei­ther Cu or CuW on a Nb sub­strate. Bulk (~5 mm thick) coat­ings of Cu and CuW were de­posited on stan­dard 3 mm thick, high-pu­rity Nb sam­ples and smaller sam­ples with 2 mm x 2 mm cross sec­tion were cut for mea­sur­ing the ther­mal con­duc­tiv­ity and the resid­ual re­sis­tiv­ity ratio. The sam­ples were sub­jected to an­neal­ing at dif­fer­ent tem­per­a­tures and a max­i­mum RRR of ~130 and ~40 were mea­sured for the Cu sam­ples and CuW sam­ples, re­spec­tively.

Pokhrel, H.↗

Electrical and Thermal Properties of Cold-Sprayed Bulk Copper and Copper-Tungsten Samples at Cryogenic Temperatures

The de­vel­op­ment of high ther­mal con­duc­tiv­ity coat­ings with pure cop­per or cop­per-tung­sten alloy could be ben­e­fi­cial to im­prove the heat trans­fer of bulk Nb cav­i­ties for con­duc­tion cool­ing ap­pli­ca­tions and to in­crease the stiff­ness of bulk Nb cav­i­ties cooled by liq­uid he­lium. Cold-spray is an ad­di­tive man­u­fac­tur­ing tech­nique suit­able to grow thick coat­ings of ei­ther Cu or CuW on a Nb sub­strate. Bulk (~5 mm thick) coat­ings of Cu and CuW were de­posited on stan­dard 3 mm thick, high-pu­rity Nb sam­ples and smaller sam­ples with 2 mm x 2 mm cross sec­tion were cut for mea­sur­ing the ther­mal con­duc­tiv­ity and the resid­ual re­sis­tiv­ity ratio. The sam­ples were sub­jected to an­neal­ing at dif­fer­ent tem­per­a­tures and a max­i­mum RRR of ~130 and ~40 were mea­sured for the Cu sam­ples and CuW sam­ples, re­spec­tively.

Pokhrel, H.↗