V. N. Molchanov's research while affiliated with Russian Academy of Sciences and other places

Publications (72)

Article
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Article
Single crystals of the Ca{sub 1-x}Sc{sub x}F{sub 2+x}(x = 0.106, 0.132, 0.156) solid solutions (CaF{sub 2} structure type, space group Fm3-barm) are investigated using X-ray diffraction. It is revealed that the crystals under investigation contain vacancies in the 8c positions and interstitial fluorine ions in the 48i positions. The coordination nu...
Article
The structure of single crystals of the nonstoichiometric phases Ba1 - x R x F2 + x ( R = Er, Yb, Lu; 0.1 < x < 0.3) grown by the Bridgman method from the flux has been studied using X-ray diffraction and neutron diffraction analyses at a temperature of 293 K. The phases have a defect structure of the fluorite type and crystallize in the cubic syst...
Article
The crystal structure of the ordered phase Sr4Lu3F17 prepared by directed crystallization of the melt has been investigated. The crystals have a trigonally distorted fluorite lattice (space group R $$ \bar 3 $$, Z = 6, a = 10.615(2) Å, c = 19.547(6) Å). The Sr4Lu3F17 phase is isostructural to Ba4R3F17 (R = Y, Yb). The distortions of the fluorite ca...
Article
The displacements of Ba2+ cations in the cationic motif of Ba0.78Tm0.22F2.22 crystals, which are representatives of nonstoichiometric fluorite phases Ba1 − x R x F2 + x , are proved for the first time with the use of precision investigations of the fine atomic structure. It is shown that the cation displacements, like the previously revealed displa...
Article
As-grown Cd0.9R 0.1F2.1 (R = La-Nd) crystals were assigned to the CaF2 structure type and their structure was determined by X-ray diffraction. A new octacubic cluster of structural defects in Cd0.9R 0.1F2.1 phases is proposed. The changes in the anionic motif of the Cd0.9R 0.1F2.1 phase can be explained as a result of the formation of tetrahedral [...
Article
As-grown Cd0.9R0.1F2.1(R= La–Nd) crystals were assigned to the CaF2 structure type and their structure was determined by X-ray diffraction. A new octacubic cluster of structural defects in Cd0.9R0.1F2.1 phases is proposed. The changes in the anionic motif of the Cd0.9R0.1F2.1 phase can be explained as a result of the formation of tetrahedral [Cd4 –...
Article
The absolute crystal structures of two enantiomorphic forms of the Ca3Ga2Ge4O14 crystals (a = 8.075(1) Å, c = 4.9723(6) Å, space group P321) with the positive and negative senses of the optical activity are determined using X-ray diffraction analysis. The final R factors are as follows: R = 1.75% and R w = 2.57% for the crystal with the positive se...
Article
The absolute crystal structure of the Ca3TaGa3Si2O14 piezoelectric compound is refined using X-ray diffraction analysis. The unit cell parameters and final R factors are as follows: a = 8.112(1) Å, c = 4.9862(6) Å, space group P321, Z = 1, R = 0.98%, and R w = 1.42%. It is shown that the configuration of the absolute crystal structure inherited fro...
Article
Full-text available
The crystal structure of the new barium borate Ba5(BO3)2(B2O5) is established (R = 0.0436). Single crystals were grown by spontaneous crystallization in the BaO-B2O3-Na2O system using the flux method. This compound crystallizes in the orthorhombic system, sp. gr. P212121; the unit-cell parameters are a = 9.590(2) Å, b = 16.659(3) Å, c = 22.919(6) Å...
Article
The atomic structure of La3Nb0.5Ga5.5O14 single crystals (space group P321, R = 2.21%, R w = 2.31%) at 20 K was determined using X-ray diffraction. A comparative analysis of the structural characteristics determined at temperatures of 293 and 20 K did not reveal a noticeable redistribution of bond valences that could be considered precursors of a p...
Article
Abstract—The structures of as-grown Cd0.90R0.10F2.10 (R = Sm–Lu and Y) crystals are determined and related to the CaF2 structure type. It is assumed that in all the crystals R3+ and Cd 2+ ions form clusters with the tetrahedral configuration of the [Cd2R2F26] and [CdR3F26] cations. The concentration of [Cd2R2F26] cations in crystals with R = Er–Lu...
Article
The absolute structure of La3Ga5SiO14 piezoelectric crystals (a = 8.1746(6) Å, c = 5.1022(4) Å, space group P321, Z = 1) with the positive sense of rotation of the plane of polarization is refined using X-ray diffraction analysis (R = 1.37%, R w = 1.71%, 2413 unique reflections, max sinθ/λ = 1.15 Å−1). The contributions from the anharmonicity of t...
Article
The structures of as-grown Cd0.90 R 0.10F2.10 (R = Sm-Lu and Y) crystals are determined and related to the CaF2 structure type. It is assumed that in all the crystals R 3+ and Cd2+ ions form clusters with the tetrahedral configuration of the [Cd2 R 2F26] and [CdR 3F26] cations. The concentration of [Cd2 R 2F26] cations in crystals with R = Er-Lu an...
Article
Full-text available
The structure of a K0.93Ti0.93Nb0.07OPO4 single crystal is studied at the temperature 30 K. The measurements are performed on a four-circle HUBER-5042 diffractometer with a DISPLEX DE-202 cryostat. Processing of the diffraction data and the preliminary refinement of the model are performed using the ASTRA program package. The final refinement of th...
Article
Abstract—The structures of the CdF2 and Cd0.90Tb0.10F2.10 crystals, the first representatives of the family of nonstoichiometric CdF2-based Cd1 – xRxF2 + x phases (R = La–Lu, Y), are determined by X-ray diffraction analysis. The structures belong to the CdF2 structure type. The nonstoichiometric CaF2 phases have structural defects—interstitial fluo...
Article
The crystal structure of monoclinic La3SbZn3Ge2O14 crystals from the langasite family is determined by X-ray diffraction analysis [a = 5.202(1) Å, b = 8.312(1) Å, c = 14.394(2) Å, β = 90.02(1), sp. gr. A2, Z = 2, and R/R w = (5.2/4.6)%]. The structure is a derivative of the Ca3Ga2Ge4O14-type structure (a = 8.069 Å, c = 4.967 Å, sp. gr. P321, Z = 1...
Article
The complete X-ray structure determination of Czochralski grown La3Zr0.5Ga5Si0.5O14 single crystals with the Ca3Ga2Ge4O14 structure is performed (sp. gr. P321, a = 8.226(1) Å, c = 5.1374(6) Å, Z = 1, Mo K α1 radiation, 1920 crystallographically independent reflections, R = 0.0166, R w = 0.0192). The absolute structure is determined. It is shown tha...
Article
Full-text available
Crystals of NaBaBO3 were grown by spontaneous crystallization on a platinum loop from the BaO-B2O3-Na2O system using the flux technique. The crystals have a highly disordered block structure. X-ray diffraction study λMoKα, 518 independent reflections, R = 0.0272) demonstrated that the structure of these crystals is identical with that established p...
Article
Abstract—The structure of Ba 0.75Lu 0.25F 2.25 crystals grown from melt has been studied by X-ray diffraction analysis (4729 measured reflections, 269 independent reflections with I > 3 s (I ), R = 1.1%, Rw = 0.7%). The crystals are crystallized in the cubic system, sp. gr. Pm m, with the lattice parameter a = 5.9870(9) Å. A new complex of defects...
Article
The crystal structure of bismutocolumbite, Bi(Nb0.79Ta0.21)O-4 with orthorhombic (sp. gr. Pnna) stibio-tantalite structure type at ambient conditions has been determined at 2.59 and 9.56 GPa, and 23 degreesC. Crystal data and results of structure refinement using powder X-ray diffraction and Rietveld analysis for Bi-rich stibiocolumbite, (Sb0.52Bi0...
Article
Langasite (La3Ga5SiO14) crystallizes in the polar space group P321. Here we report the pressure dependence of the lattice parameters at high hydrostatic pressures up to 10.2 GPa. The results presented in terms of compressibility agree well with results from measurements of the elastic constants. According to a Birch-Mumaghan equation of state, the...
Article
Two fluorite-type phases (P and F) possessing different defect structures were isolated from products of double recrystallization of a melt of the nominal composition (with respect to the charge)Ba0.8Yb0.2F2.2. The P phase crystallized in the space group Pm3m with a = 6.096(1) Å. The structure was refined to R = 2.19% and R w = 2.14% (142 independ...
Article
The analysis of the structural variations in cuprates with different types of conductivity has shown that cooling from room temperature prior to the transition into the superconducting state results in transfer of a small part of the charge (approximately several hundredths of an electron charge per unit cell) from the reservoir to the conducting l...
Article
Precision X-ray structural studies of the La3Nb0.5Ga5.5O14 and Sr3Ga2Ge4O14 single crystals were carried out. The space group P321 was confirmed. The anomalous X-ray scattering was taken into account to establish the absolute structures (chirality) of the crystals; they proved to be of different sign. The structural features responsible for the opt...
Article
The structure of a K0.96Ti0.96Nb0.04OPO4 single crystal was established by the methods of the X-ray diffraction analysis. Additional positions of K atoms were established. In the superionic state, these atoms provide ionic transport in the crystals.
Article
The structure of a K0.96Ti0.96Nb0.04OPO4 single crystal was established by the methods of the X-ray diffraction analysis. Additional positions of K atoms were established. In the superionic state, these atoms provide ionic transport in the crystals.
Article
The structure of NaCs5Mo7O24.5H(2)O was established by X-ray diffraction analysis (lambda Mo, 7279 reflections, R-aniso = 5.3%). The parameters of the triclinic unit-cell are as follows: a = 10.517 Angstrom, b = 10.824 Angstrom, c = 16.916 Angstrom, a = 66.930, beta = 67.14 degrees, gamma = 72.40 degrees; Z = 2; P (1) over bar. The compact groups c...
Article
The structure of samarium disulfide SmS1.9, space group P42/n; lattice constants a= 19.717(2)Å; c = 15.928(1) Å has been determined and refined by LS method to R = 0.0345; R(w) = 0.0419. The structure is a tenfold superstructure from the structure type ZrSSi. [S2]2- dumbbells with interatomic distances 2.146(1) Å between S atoms were observed in th...
Article
The structure of the presodyme disulfide PrS2 has been determined and refined by the LS method in space group P2(1)/b11 (14) with a = 4.054(1) Angstrom b = 8.058(1) Angstrom; c = 8.079(1) Angstrom and alpha = 90.08(2)degrees to the final values of discrepancy factors R = 0.0188; R-w = 0.0204. The structure is a derivative structure of the ZrSSi (or...
Article
The atomic structure of high-temperature superconductor YBa2Cu4O8 single crystals with Tc ≈ 70 K has been refined from the X-ray diffraction data (sp. gr. Ammm, a - 3.8400(7), b = 3.8704(7), c = 27.225(3) Å, Rw = 0.83%, R = 0.60%). The deviation of thermal vibrations of heavy atoms from the harmonic law has been established. The analysis of the pro...
Article
The structures of superconducting Tl2Ba2CaCu2O8 (T-c similar to 110 K) and YBa2Cu4O8 (T-c similar to 70 K) were investigated by single-crystal X-ray diffraction techniques in a wide temperature range. Some of the structure parameters show anomalous behaviour in the vicinity of the critical temperature. The most pronounced structural change is the s...
Article
The structures of superconducting Tl 2Ba 2CaCu 2O 8 (T c ∼ 110 K) and YBa 2Cu 4O 8 (T c ∼ 70 K) were investigated by single-crystal X-ray diffraction techniques in a wide temperature range. Some of the structure parameters show anomalous behaviour in the vicinity of the critical temperature. The most pronounced structural change is the shift of the...
Article
X-ray diffraction study of YBa2Cu3O7-δ single crystals with intermediate oxygen content showed an ordered arrangement of oxygen atoms in the cuprate planes. Depending on the oxygen content, the blocks of the compositions YBa2Cu3O7 and YBa2Cu3O6.5 or YBa2Cu3O6.5 are formed in the crystals. It is shown that the so-called superconducting tetragonal Y-...
Article
High-precision x-ray crystallographic studies of YBa2Cu4O8 single crystals (T c =70 K) are performed at eight temperatures in the interval 20–295 K. It is found that a number of structural parameters exhibit anomalous behavior near the superconducting transition of the crystal. A characteristic effect near the phase transition is the displacement o...
Article
The atomic structure of a single-domain Tm0.962Ba2Cu3O6.97 single crystal in a zirconia crucible has been performed by the methods of X-ray structure analysis. The results obtained are compared with the structural data on a TmBa2Cu2.972O6.89 crystal grown in an alumina crucible with partial incorporation of aluminum into the growing crystal.
Article
Mass transfer and phase formation processes accompanying interdiffusion in the Dy2O3-BaO-CuO system are studied at 930°C in air. Several phases formed by reaction diffusion are identified, and their cation stoichiometry ranges determined. Mass transfer in this system occurs primarily through diffusion of Cu and Ba cations via vacancies of single-cr...
Article
The structural parameters determined by the precision X-ray structure analysis are compared for isostructural single crystals of the nonsuperconducting TlBa2LaCu2O7 phase and the superconducting TlBa2(Ca0.87Tl0.13)Cu2O7 (Tc = 80 K), (Tl1.90Cu0.10)Ba2CuO6.18 (Tc = 30 K), (Tl1.85Cu0.15)Ba2CuO6 (Tc = 110 K), and (Tl1.85Cu0.15)Ba2(Ca0.875Tl 0.125)Cu2O8...
Article
Nearly twin-free TmBa2Cu3O7−x single crystals of high crystalline perfection were grown from nonstoichiometric melts in the system Tm2O3BaO(BaO2CuO(Cu2O) in air atmosphere. The superconducting transition temperatures and widths depend on crystallization conditions and are Tc = 89–91 K and ΔTc = 0.2 K for the best samples. Morphology of the crysta...
Article
The crystal structure of a tetragonal single crystal of Tl-2201 with Tc = 30 K has been determined by the X-ray diffraction technique (a = 3.8717(3), c = 23.224(3) Å, space group I4/mmm, Z = 2). The chemical composition is found to be Tl1.90(1)Cu.0.10(1)Ba2CuO6.18(4). Displacements of Tl and O3 atoms from their symmetric sites have been observed. S...
Article
Crystal structure of tetragonal single crystals of TI-2201 have been determined by X-ray diffraction technique. Structural parameters of TI-2201 crystals with various Tc have been compared. It was shown that Tc variation is accompanied by changes in Cu-O bonds and the distance between Ba and the CuO2 plane.
Article
Accurate X-ray structural studies of Tl-2212 single crystal, T-c=110K, have been performed at 296, 160, 130, 90 and 60K. Some atomic displacements which occur during the superconducting phase transition are related with Ba, O3 and O1 atoms. Significant anomalies during the phase transition have been found in the behavior of parameters of atomic the...
Article
The structure of superconducting Tl2Ba2CaCu2O8 (Tc = 110 K) was refined from single-crystal X-ray diffraction data measured at temperatures 296, 160, 130, 90 and 60 K. The refinements indicate a positional disorder of the thallium and oxygen atoms in the Tl-O layers, resulting in locally orthorhombic symmetry. The macroscopic symmetry of the specim...
Article
Single crystals of 2201 phase with various superconducting transition temperatures ranging from nonsuperconducting to 110K have been obtained. An X-ray structural study of tetragonal single crystals with Tc = 110 K, space group 14/mmm, a = 3.8686(3), c = 23.259(3) Å, has been carreid out. We have found that thallium atoms are partially replaced by...
Article
X-ray analysis is used to study the atomic structure of Tl-phase 2212 single crystals at 296, 160, and 60 K. The transition to the superconducting state is accompanied by significant shifts of TlO-layer atoms and anomalous changes in the CuO5 pyramids. Local rhombic distortions of the structure associated with shifts of Tl atoms occur before and af...
Article
X-ray diffraction, acoustic, and thermal studies of La2CuO4 single crystals have been used to determine the tetra-orthorhombic transition and anomalies in the temperature dependence of longitudinal sound absorption and velocity associated with the interaction of the acoustic and optical branches of the phonon spectrum of La2CuO4. The different temp...
Article
A method has been developed for preparing monodomain crystals of TmBa2Cu(3-x)O(7-y) superconductors with Tc = 90-92 for a transition width of less than 1 deg. The atomic structure of a mondomain specimen of TmBa2Cu(2.972)O(6.89) is analyzed, and its structure is compared with that of Y-superconductors.
Article
Investigations of single crystals of (La1-xSrx)2CuO4-† (x=0.12, 0.10 and 0.03) showed that statistical Sr distribution over La sites varies from equaly probable in (La0.97Sr0.03)2CuO4, sp.gr. Abma, Tc= 15 K to La replacement by Sr only in one of two nonequivalent positions of sp.gr. Pbma in La(La0.76Sr0.24)CuO3.92, Tc=5 K. The ordering in Sr distri...
Article
The atomic structures and oxygen contents of YBa2Cu3O(6.24), YBa2Cu3O(6.59), and YBa2Cu3O(6.97) crystals are determined. Based on the profiles of X-ray diffraction reflections in YBa2Cu3O(6.24) single crystals, the coexistence of structural blocks with tetragonal and rhombic symmetries is established. The compositions of these blocks are YBa2Cu3O6...
Article
Structure data on superconducting tetragonal-phase superconducting crystals in the Y-Ba-Cu-O system at a critical temperature of about 50 K are presented. It is shown that the tetragonal phases, as well as the rhombic ones, possess superconducting properties. The presence or the absence of these properties is connected with the content of oxygen, w...
Article
X-ray structural analysis of YBa2Cu3O(7-x) single crystals was performed before and after annealing in oxygen. An atomic mechanism for the transition from the tetragonal to the rhombic phase is established on the basis of the analysis, and atomic-structure elements connected with superconductivity are indicated.
Article
Tetragonal single crystals of YBaâCu{sub 2.910}O{sub 6.58} with {Tc} â¼ 45-60 K are grown in ZrOâ crucibles. In the framework of the P4/mmm symmetry, a = 3.867(1), and c = 11.734(1) â«, the atomic structure of the crystals is refined. An analysis of the structural data led the authors to conclude about the random nature of the tetragonal symmetry o...

Citations

... It is the most common structural unit found in BaF 2 -REF 3 fluorite and fluorite related phases [16]. Nevertheless, in fluorite type BaF 2 -REF 3 (RE=Yb-Lu) phases new type of structural unit RE 8 Ba 6 F 71 (octahedral alkali earth supercluster) was recently discovered [40]. Indeed, two distinct Er 3+ sites were also found in the rhombohedral Ba 4 Yb 3 F 17 [27]. ...
... A range of the intersite CDW potential that reaches out in real space is within two lattice constants of 6~10 Å when the lattice constant in a metal is considered 4 ± 1 Å. Experimental evidence of the CDW in oxide superconductors is a distortion of octahedral structure observed just below T c 45,46 and discontinuity 27 of the bulk modulus at T c . For superconductivity, when the CDW potential is introduced, the on-site critical Coulomb energy U c in the BR picture should be present at the bipolaron, then, as a nonlocal potential, V e-ph = V CDW + U c < 0 is considered a constant, because V CDW and U c are determined as fixed values in a crystal. ...
... The thermal conductivity of a fused and, even more so, ceramic sample, can differ from the thermal conductivity of a single crystal by dozens and hundreds of times. So, the thermal conductivity can be decreased due to the thermal resistance of the boundaries between grains in an alloy and also due to a porous ceramic structure [7,8]. Thus, a very topical problem is the development of a reliable method of estimating the thermal conductivity of a material from the experimental data on their characteristics, the values of which are independent of whether a single-crystal or polycrystalline sample is used in the experiment. ...
... The reason for this behavior remains unclear a is apparently related to the thermodynamic instability of BaF2-based solid solutions at l temperatures. Many studies have been devoted to the investigations of the defect structure in c centrated solid solutions formed upon the incorporation of rare-earth fluorides of the rium group into barium fluoride [44][45][46][47]. There is no unambiguous interpretation of th from the point of view of the cluster structure of defects. ...
... LGS and its isomorphs exhibit quality and electromechanical coupling factors which are, respectively, four [2] and two times [3] greater than those of quartz. One of the most important features of LGX is its phase transition, which occurs under high temperature at its melting temperature of 1473°C and under high pressure at 10 GPa [4]. These excellent properties of LGS and its isomorphs provide promising applications for sensors and timing applications in the oil and gas industry for high-temperature and high-pressure (HTHP) applications. ...
... Stibiotantalite is isostructural with other ABO 4 typestructure series minerals (Keller 1962, Zubkova et al. 2002. Their crystal structures typically consist of chains of edge-sharing AO 6 octahedra parallel to the a axis, and BO 6 octahedral sheets are combined with AO 6 along with the c axis (Kazantsev et al. 2002, Zubkova et al. 2002. They are also characterized by the presence of cations with lone-pair electrons (Sb 3þ , Bi 3þ ) (Thornton 1977, Amador et al. 1988, which cause distortion in B 3þ O 6 octahedra. ...
... The anion core of the clusters consists of interstitial anions. According to the principle of local charge compensation, the impurity cations R 3+ are located around the anion core to form cation-anion clusters [2][3][4][5]. The presence of vacancies in the main anionic motif and interstitial anions in one or more positions is considered to be evidence of cluster formation in the disordered M 1−x R x F 2+x phases. ...
... Due to the fact that the electroneutrality condition for the refined composition is not satisfied, we assumed that a certain number of Ca 2+ ions in the structure are interstitial ones, as for the (La 2.964 ◻ 0.036 )La i(0.036) Zr 0.5 Ga 5 Si 0.5 O 14 [26]. The analysis of the residual nuclear density does not exclude such possibility. ...
... However, the use of these compounds depends on the composition (in other words, on the type and concentration of point defects), which does not coincide with the composition of the initial charge. There are quite a few works devoted to the structural investigation of CNGS [6,8,11] and LGN [6,17,18] crystals. All of them were performed using X-ray, and the occupancies were refined only in some cases. ...
... In both compounds, the absence of X-ray scattering contrast between Ga 3+ /Ge 4+ and Zn 2+ /Ge 4+ means that the distribution of these cations over the three framework sites (B, C, and D) cannot be obtained directly by conventional (non-anomalous) X-ray diffraction methods, and instead indirect routes (e.g., analysis based on refined bond distances) have been used to deduce the nature and extent of cation ordering. 17 Such isoelectronic pairs can be distinguished directly by neutron d i ff r a c t i o n ( N P D ) , a s d e m o n s t r a t e d f o r La 3 Ga 5−x Ge 1+x O 14+x/2 , 13 but NPD alone cannot be used for direct analysis of more complex systems with three or more isoelectronic cations distributed over the framework sites B, C, and D. Atomic-resolution STEM-EDS mapping offers a solution to this problem by detecting each element type directly with a spatial resolution of around 2−3 Å. While this technique is most often used qualitatively, intensities of atomic columns can be extracted by Gaussian curve fitting which is most often applied to 1D line profiles to provide quantitative information about atomic site occupancies. ...