Search for: All records

Quaternary metal‐chalcogenides combining rare‐earth cations with late transition metal cations are attracting growing attention for their optical properties, such as for solar energy conversion or second harmonic generation. Synthetic explorations of theII₃‐I₂‐IV₂‐Ch₈family (II = Eu;I = Cu or Ag;IV = Si, Ch = S or Se) have yielded Eu₃Ag₂Si₂S₈(1) and Eu₃Cu_1.08(1)Si_2.42(1)Se₈(2). Their structures have been characterized by X‐ray diffraction to form in the noncentrosymmetric space groupI3dand to exhibit two distinct types of mixed‐site occupancies, for the Ag(I) cations in1and mixed Cu(I)/Si(IV) cations in2. In both, the cation disorder occurs to achieve charge balancing with the chalcogenide anions. A high yield of1can be achievedwith optical measurements showing indirect and direct band transitions of ≈2.2(1) and ≈2.4(1) eV, respectively. Its second harmonic generation response is found to be relatively strong, approximately 0.9 × AgGaS₂, confirming its noncentrosymmetric structure. Band structure calculations reveal the valence and conduction band edges stem predominantly from the filled Ag(I)/Cu(I)‐based states and empty Si(IV)‐based states, respectively, with additional contributions from the chalcogenide anions. Calculation results also show that cation disorder facilitates a reduction in the antibonding interactions between the Ag(I)/Cu(I)d‐based and chalcogenidep‐based states. 

Pb₂Ga₃F₆(SeO₃)₂X₃·2H₂O achieve a better balance between the large SHG effect and wide band gap in the current HTO family. 

Planar MO 3 (M = B, C, N) units have frequently been considered important structural components of novel birefringent crystal materials. An efficient approach for constructing new functional crystals is to simultaneously assemble multiple structural motifs together. Two compounds, Na 3 Rb 6 (CO 3 ) 3 (NO 3 ) 2 X·6H 2 O (X = Br and Cl), were synthesized by the integration of three kinds of anionic groups. More interestingly, the [CO 3 ] 2− and [NO 3 ] − groups in Na 3 Rb 6 (CO 3 ) 3 (NO 3 ) 2 X·6H 2 O are all coplanar with the aid of [NaO 7 ] 13− polyhedra, which can enhance the anisotropic polarizability. Na 3 Rb 6 (CO 3 ) 3 (NO 3 ) 2 X·6H 2 O have a large theoretical birefringence of ∼0.165 at 1064 nm and possess a short UV cut-off edge of ∼230 nm. Additionally, the two compounds exhibit good crystal growth habits. These properties illustrate that Na 3 Rb 6 (CO 3 ) 3 (NO 3 ) 2 X·6H 2 O are promising UV birefringent crystals.