Antiferromagnetic Ordering in TmCu2

Intermetallic compound TmCu₂ crystalizes in the orthorhombic structure, orders antiferromagnetically (AF) and exhibits four different AF phases below T _N = 6.5 K. In all these phases the Tm magnetic moment is parallel to the b-axis. The ground-state AF1 (T < 3.4 K) corresponds to the squared-up AF structure with propagation vector ₀₁ = (5/8, 0, 0) and magnetic unit cell 8a × b × c. Narrow phases AF2 and AF3 (3.3 K < T < 3.7 K and 3.6 K < T < 4.6 K) are 'spin-slip'-derivatives from the AF1 structure, yielding propagation vectors ₀₂ = (0.633, 0, 0.02) and ₀₃ = (0.618, 0, 0), respectively. The phase AF4 (4.4 K < T < T _N) is then incommensurate transversal spin-wave with the propagation ₀₄ = (0.64, 0, 0). The co-existence of AF phases indicates the first-order transitions between them.     

Design of a functional protein for molecular recognition: specificity of ligand binding in a metal-assembled protein cavity probed by 19f NMR

A metal-assembled homotrimeric coiled coil based on the GCN4-p1 sequence has been designed that noncovalently binds hexafluorobenzene and other similar ligands in a hydrophobic cavity, created by making the core substitution Asn16Ala ([Fe(bpyGCN4-N16A)3]2+). The KD of binding of hexafluorobenzene with [Fe(bpyGCN4-N16A)3]2+ was observed to be 1.1(9) x 10(-4) M by diffusion NMR experiments. A control coiled coil with the core substitution Asn16Val ([Fe(bpyGCN4-N16V)3]2+) exhibited a significantly weaker association with hexafluorobenzene, providing evidence that even in the absence of structural data, benzene-like ligands bind in the cavity created by the Asn16Ala substitution. 19F NMR was employed to observe hexafluorobenzene binding and to monitor titrations with competing hydrophobic and polar ligands similar in size and shape to hexafluorobenzene. All hydrophobic ligands bound with greater affinity than the polar ligands in the hydrophobic core, although the cavity seems to be somewhat flexible in terms of the sizes of molecules it can accommodate. Thus 19F NMR has proved to be a useful spectral tool to probe molecular recognition in a hydrophobic cavity of a metal-assembled coiled coil.     

Optical isolator using two tandem phase modulators

We propose and demonstrate an integrated optical isolator in InP using two phase modulators in series. The phase modulators are driven with a single-frequency signal in quadrature. Theoretically there is no effect on the forward signal, and the carrier of the backward signal can be eliminated, the energy distributed to other frequencies. We achieve a carrier isolation of 11?dB and an excess insertion loss of 2.3?dB. Such an isolator can be monolithically integrated with a laser without extra materials or magnetic fields.     

All-channel tunable optical dispersion compensator based on linear translation of a waveguide grating router

We propose and demonstrate a compact tunable optical dispersion compensation (TODC) device with a 100 GHz free spectral range capable of mitigating chromatic dispersion impairments. The TODC is based on longitudinal movement of a waveguide grating router, resulting in chromatic dispersion compensation of ±1000 ps/nm. We employed our TODC device for compensating 42.8 Gbit/sec differential phase-shifting keying signal, transmitted over 50 km fiber with a -2 dB power penalty at 10??.     

The 15N chemical shifts in mixed NB2Si and NBSi2 environments of Si3B3N7--a theoretical investigation

Nuclear magnetic resonance (NMR) chemical shifts in solids may be calculated by ab initio methods approximating the solid state by molecular clusters. We employed this technique to obtain estimates of (15)N chemical shifts in NB(2)Si and NBSi(2) environments in the solid state. Such nitrogen environments are found in amorphous (Si/B/N-)ceramics which exhibit very interesting features such as high thermal and mechanical stability. We based our calculations on cutouts of hypothetical Si(3)B(3)N(7) crystals suggested by Kroll and Hoffmann [Silicon boron nitrides: hypothetical polymorphs of Si(3)B(3)N(7), Angew. Chem. Int. Ed. 37 (1998) 2527]. Taking the systematic errors of our calculations into account we expect the chemical shifts in NBSi(2) environments around -293+/-5ppm. Chemical shifts in NB(2)Si environments are expected at -272+/-6ppm. The range of the calculated chemical shifts in NBSi(2) environments coincides with experimental chemical shifts in molecular compounds. Experimental chemical shifts of NB(2)Si nitrogen in molecules appear at lower field than our calculated chemical shifts in the solid state.