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At least 73 records · Page 4

Materials Data on Er(CuGe)2 by Materials Project

ErCu2Ge2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent Cu and eight equivalent Ge atoms. All Er–Cu bond lengths are 3.28 Å. All Er–Ge bond lengths are 3.10 Å. Cu is bonded to four equivalent Er and four equivalent Ge atoms to form a mixture of distorted corner, edge, and face-sharing CuEr4Ge4 tetrahedra. All Cu–Ge bond lengths are 2.43 Å. Ge is bonded in a 9-coordinate geometry to four equivalent Er, four equivalent Cu, and one Ge atom. The Ge–Ge bond length is 2.45 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(SiRh)2 by Materials Project

ErRh2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent Rh and eight equivalent Si atoms. All Er–Rh bond lengths are 3.21 Å. All Er–Si bond lengths are 3.11 Å. Rh is bonded to four equivalent Er and four equivalent Si atoms to form a mixture of distorted corner, edge, and face-sharing RhEr4Si4 tetrahedra. All Rh–Si bond lengths are 2.40 Å. Si is bonded in a 9-coordinate geometry to four equivalent Er, four equivalent Rh, and one Si atom. The Si–Si bond length is 2.41 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(FeGe)2 by Materials Project

ErFe2Ge2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent Fe and eight equivalent Ge atoms. All Er–Fe bond lengths are 3.23 Å. All Er–Ge bond lengths are 3.08 Å. Fe is bonded to four equivalent Er and four equivalent Ge atoms to form a mixture of distorted edge, face, and corner-sharing FeEr4Ge4 tetrahedra. All Fe–Ge bond lengths are 2.35 Å. Ge is bonded in a 9-coordinate geometry to four equivalent Er, four equivalent Fe, and one Ge atom. The Ge–Ge bond length is 2.57 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(CoGe)2 by Materials Project

ErCo2Ge2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent Co and eight equivalent Ge atoms. All Er–Co bond lengths are 3.20 Å. All Er–Ge bond lengths are 3.07 Å. Co is bonded to four equivalent Er and four equivalent Ge atoms to form a mixture of distorted edge, corner, and face-sharing CoEr4Ge4 tetrahedra. All Co–Ge bond lengths are 2.33 Å. Ge is bonded in a 9-coordinate geometry to four equivalent Er, four equivalent Co, and one Ge atom. The Ge–Ge bond length is 2.56 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(GeRu)2 by Materials Project

ErRu2Ge2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent Ru and eight equivalent Ge atoms. All Er–Ru bond lengths are 3.25 Å. All Er–Ge bond lengths are 3.27 Å. Ru is bonded in a 4-coordinate geometry to four equivalent Er and four equivalent Ge atoms. All Ru–Ge bond lengths are 2.44 Å. Ge is bonded in a 9-coordinate geometry to four equivalent Er, four equivalent Ru, and one Ge atom. The Ge–Ge bond length is 2.54 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(Al10Cr)2 by Materials Project

Er(CrAl10)2 crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Er is bonded in a 4-coordinate geometry to sixteen Al atoms. There are four shorter (3.13 Å) and twelve longer (3.20 Å) Er–Al bond lengths. Cr is bonded to twelve Al atoms to form CrAl12 cuboctahedra that share corners with six equivalent CrAl12 cuboctahedra, edges with eighteen equivalent AlErAl10Cr cuboctahedra, and faces with six equivalent AlErAl10Cr cuboctahedra. There are six shorter (2.56 Å) and six longer (2.80 Å) Cr–Al bond lengths. There are three inequivalent Al sites. In the first Al site, Al is bonded in a distorted linear geometry to two equivalent Er and twelve equivalent Al atoms. All Al–Al bond lengths are 3.09 Å. In the second Al site, Al is bonded to one Er, one Cr, and ten Al atoms to form distorted AlErAl10Cr cuboctahedra that share corners with fifteen equivalent AlErAl10Cr cuboctahedra, edges with two equivalent AlErAl10Cr cuboctahedra, edges with three equivalent CrAl12 cuboctahedra, a faceface with one CrAl12 cuboctahedra, and faces with fifteen equivalent AlErAl10Cr cuboctahedra. There are a spread of Al–Al bond distances ranging from 2.70–2.92 Å. In the third Al site, Al is bonded in a 12-coordinate geometry to two equivalent Cr and ten Al atoms. All Al–Al bond lengths are 2.82 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(BO2)3 by Materials Project

Er(BO2)3 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are four inequivalent Er3+ sites. In the first Er3+ site, Er3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Er–O bond distances ranging from 2.25–2.83 Å. In the second Er3+ site, Er3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Er–O bond distances ranging from 2.26–2.58 Å. In the third Er3+ site, Er3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Er–O bond distances ranging from 2.27–2.52 Å. In the fourth Er3+ site, Er3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Er–O bond distances ranging from 2.31–2.65 Å. There are six inequivalent B3+ sites. In the first B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.46–1.53 Å. In the second B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.45–1.53 Å. In the third B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There is three shorter (1.47 Å) and one longer (1.48 Å) B–O bond length. In the fourth B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There is two shorter (1.45 Å) and two longer (1.53 Å) B–O bond length. In the fifth B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.46–1.52 Å. In the sixth B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.45–1.54 Å. There are fifteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Er3+ and two B3+ atoms. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Er3+ and two B3+ atoms. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Er3+ and two equivalent B3+ atoms. In the fourth O2- site, O2- is bonded in a trigonal planar geometry to three B3+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Er3+ and two B3+ atoms. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Er3+ and two B3+ atoms. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to three Er3+ and one B3+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Er3+ and two B3+ atoms. In the ninth O2- site, O2- is bonded in a 3-coordinate geometry to one Er3+ and two B3+ atoms. In the tenth O2- site, O2- is bonded in a 2-coordinate geometry to two Er3+ and two B3+ atoms. In the eleventh O2- site, O2- is bonded in a distorted trigonal planar geometry to one Er3+ and two equivalent B3+ atoms. In the twelfth O2- site, O2- is bonded in a 3-coordinate geometry to one Er3+ and two equivalent B3+ atoms. In the thirteenth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Er3+ and two equivalent B3+ atoms. In the fourteenth O2- site, O2- is bonded in a 2-coordinate geometry to two Er3+ and two equivalent B3+ atoms. In the fifteenth O2- site, O2- is bonded in a bent 120 degrees geometry to one Er3+ and two equivalent B3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Er(SiPt)2 by Materials Project

ErPt2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent Pt and eight equivalent Si atoms. All Er–Pt bond lengths are 3.23 Å. All Er–Si bond lengths are 3.18 Å. Pt is bonded to four equivalent Er and four equivalent Si atoms to form a mixture of distorted edge, corner, and face-sharing PtEr4Si4 tetrahedra. All Pt–Si bond lengths are 2.47 Å. Si is bonded in a 9-coordinate geometry to four equivalent Er, four equivalent Pt, and one Si atom. The Si–Si bond length is 2.31 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(BRh)4 by Materials Project

ErRh4B4 crystallizes in the tetragonal P4_2/nmc space group. The structure is three-dimensional. Er is bonded in a 12-coordinate geometry to twelve equivalent Rh and twelve equivalent B atoms. There are four shorter (2.95 Å) and eight longer (3.18 Å) Er–Rh bond lengths. There are eight shorter (3.03 Å) and four longer (3.16 Å) Er–B bond lengths. Rh is bonded in a 5-coordinate geometry to three equivalent Er and five equivalent B atoms. There are a spread of Rh–B bond distances ranging from 2.21–2.24 Å. B is bonded in a 6-coordinate geometry to three equivalent Er, five equivalent Rh, and one B atom. The B–B bond length is 1.80 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(BC)2 by Materials Project

ErB2C2 crystallizes in the tetragonal P4_2/mmc space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent B and eight equivalent C atoms. All Er–B bond lengths are 2.72 Å. All Er–C bond lengths are 2.69 Å. B is bonded in a 2-coordinate geometry to four equivalent Er and two equivalent C atoms. Both B–C bond lengths are 1.60 Å. C is bonded in a 2-coordinate geometry to four equivalent Er, two equivalent B, and one C atom. The C–C bond length is 1.42 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er(PO3)3 by Materials Project

Er(PO3)3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are four inequivalent Er3+ sites. In the first Er3+ site, Er3+ is bonded to six O2- atoms to form ErO6 octahedra that share corners with six PO4 tetrahedra. There are a spread of Er–O bond distances ranging from 2.22–2.28 Å. In the second Er3+ site, Er3+ is bonded to six O2- atoms to form ErO6 octahedra that share corners with six PO4 tetrahedra. There are a spread of Er–O bond distances ranging from 2.21–2.25 Å. In the third Er3+ site, Er3+ is bonded to six O2- atoms to form ErO6 octahedra that share corners with six PO4 tetrahedra. There are a spread of Er–O bond distances ranging from 2.24–2.26 Å. In the fourth Er3+ site, Er3+ is bonded to six O2- atoms to form ErO6 octahedra that share corners with six PO4 tetrahedra. There are a spread of Er–O bond distances ranging from 2.20–2.25 Å. There are nine inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 12–26°. There is two shorter (1.50 Å) and two longer (1.61 Å) P–O bond length. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 12–26°. There are a spread of P–O bond distances ranging from 1.49–1.61 Å. In the third P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 24–45°. There are a spread of P–O bond distances ranging from 1.50–1.62 Å. In the fourth P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 27–34°. There is two shorter (1.50 Å) and two longer (1.61 Å) P–O bond length. In the fifth P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 29–30°. There is two shorter (1.50 Å) and two longer (1.60 Å) P–O bond length. In the sixth P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 26–36°. There are a spread of P–O bond distances ranging from 1.50–1.62 Å. In the seventh P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 11–26°. There is two shorter (1.50 Å) and two longer (1.60 Å) P–O bond length. In the eighth P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 28–38°. There are a spread of P–O bond distances ranging from 1.50–1.62 Å. In the ninth P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two ErO6 octahedra and corners with two PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 25–29°. There is two shorter (1.50 Å) and two longer (1.61 Å) P–O bond length. There are twenty-seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Er3+ and one P5+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the sixth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the seventh O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the ninth O2- site, O2- is bonded in a linear geometry to one Er3+ and one P5+ atom. In the tenth O2- site, O2- is bonded in a linear geometry to one Er3+ and one P5+ atom. In the eleventh O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the twelfth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the thirteenth O2- site, O2- is bonded in a 2-coordinate geometry to one Er3+ and one P5+ atom. In the fourteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the fifteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the sixteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the seventeenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the eighteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the nineteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom. In the twentieth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two P5+ atoms. In the twenty-first O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the twenty-second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two P5+ atoms. In the twenty-third O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the twenty-fourth O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the twenty-fifth O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the twenty-sixth O2- site, O2- is bonded in a linear geometry to one Er3+ and one P5+ atom. In the twenty-seventh O2- site, O2- is bonded in a bent 150 degrees geometry to one Er3+ and one P5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Er(SiPt)2 by Materials Project

ErPt2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded in a 8-coordinate geometry to eight equivalent Pt and eight equivalent Si atoms. All Er–Pt bond lengths are 3.25 Å. All Er–Si bond lengths are 3.28 Å. Pt is bonded in a 9-coordinate geometry to four equivalent Er and four equivalent Si atoms. All Pt–Si bond lengths are 2.41 Å. Si is bonded to four equivalent Er and four equivalent Pt atoms to form a mixture of distorted edge, face, and corner-sharing SiEr4Pt4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Er by Materials Project

Er is Copper structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Er is bonded to twelve equivalent Er atoms to form a mixture of corner, edge, and face-sharing ErEr12 cuboctahedra. All Er–Er bond lengths are 3.51 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er by Materials Project

Er is Tungsten structured and crystallizes in the cubic Im-3m space group. The structure is three-dimensional. Er is bonded in a distorted body-centered cubic geometry to eight equivalent Er atoms. All Er–Er bond lengths are 3.43 Å.

36 MATERIALS SCIENCE↗

Materials Data on Er by Materials Project

Er is Magnesium structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Er is bonded to twelve equivalent Er atoms to form a mixture of face, edge, and corner-sharing ErEr12 cuboctahedra. There are six shorter (3.46 Å) and six longer (3.59 Å) Er–Er bond lengths.

36 MATERIALS SCIENCE↗

Optical and microstructural characterization of Er 3+ doped epitaxial cerium oxide on silicon

Rare-earth ion dopants in solid-state hosts are ideal candidates for quantum communication technologies, such as quantum memories, due to the intrinsic spin–photon interface of the rare-earth ion combined with the integration methods available in the solid state. Erbium-doped cerium oxide (Er:CeO 2 ) is a particularly promising host material platform for such a quantum memory, as it combines the telecom-wavelength (~ 1.5 μm) 4f–4f transition of erbium, a predicted long electron spin coherence time when embedded in CeO 2 , and a small lattice mismatch with silicon. In this work, we report on the epitaxial growth of Er:CeO 2 thin films on silicon using molecular beam epitaxy, with controlled erbium concentration between 2 and 130 parts per million (ppm). We carry out a detailed microstructural study to verify the CeO 2 host structure and characterize the spin and optical properties of the embedded Er 3+ ions as a function of doping density. In as-grown Er:CeO 2 in the 2–3 ppm regime, we identify an EPR linewidth of 245(1) MHz, an optical inhomogeneous linewidth of 9.5(2) GHz, an optical excited state lifetime of 3.5(1) ms, and a spectral diffusion-limited homogeneous linewidth as narrow as 4.8(3) MHz. We test the annealing of Er:CeO 2 films up to 900 °C, which yields narrowing of the inhomogeneous linewidth by 20% and extension of the excited state lifetime by 40%.

36 MATERIALS SCIENCE↗

Lifetime measurements of 0 + states in Er 168 with the Doppler-shift attenuation method

Here, the lowest-lying shape oscillations of deformed nuclei have been described as quadrupole in nature (λ = 2), resulting in two types of vibrations or oscillations: β vibrations with oscillations along the symmetry axis (K π = 0 + ) and γ vibrations breaking axial symmetry with a projection of K π = 2 + on the symmetry axis. The γ vibration seems to be well characterized as the first K π = $2^+_1$ (or $2^+_γ$) band in deformed nuclei and exhibits a systematic behavior across the region. The nature of the K π = 0 + excitations, however, has remained poorly understood and has been open to debate for some decades. The goal of this work is to understand the nature of 0 + states observed in 168 Er through measurements of the lifetimes of these states and to determine if they are consistent with oscillations built on a deformed ground state, the minima of other coexisting shapes, single-particle states, or a mixture of effects. Lifetimes of excited states in the 168 Er nucleus were measured with the Doppler Shift Attenuation Method (DSAM) and the inelastic neutron scattering reaction, (n, n'γ), at the University of Kentucky Accelerator Laboratory. Numerous 0 + states had been observed by the (p, t) reaction. We confirm the 0 + states at 1217.2, 1421.5, 1833.6, 2364.9, 2392.1, and 2643.0 keV in 168 Er. We could not, however, support the previous assignments of 0 + levels at 2114.1, 2200.6, 2572.5, and 2617.4 keV. We report measured lifetimes for six confirmed 0 + excitations and additional members of 0 + bands. The results for 168 Er show that it is the third excited K π = 0 + ($0^+_4$) excitation that carries the collective strength and, therefore, the potential to be an oscillation on the ground state. This result is similar to the case in 166 Er, where it was also the $0^+_4$ state that exhibited greater collectivity than the first excited K π = 0 + band. The Delaroche et al. prediction for a collective K π = 0 + band is at E T =1.818 MeV which corresponds the third excited K π = 0 + band.

73 NUCLEAR PHYSICS AND RADIATION PHYSICS↗

Materials Data on ErS by Materials Project

ErS is Halite, Rock Salt structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Er is bonded to six equivalent S atoms to form a mixture of edge and corner-sharing ErS6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Er–S bond lengths are 2.73 Å. S is bonded to six equivalent Er atoms to form a mixture of edge and corner-sharing SEr6 octahedra. The corner-sharing octahedral tilt angles are 0°.

36 MATERIALS SCIENCE↗