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Journal articles on the topic 'LaSrCuO'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Mycharoen, P., and P. Udomsamuthirun. "The investigation on anomalous isotope effect coefficient of LaSrCuO superconductor." International Journal of Modern Physics B 33, no. 31 (December 20, 2019): 1950379. http://dx.doi.org/10.1142/s021797921950379x.

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In this research, the anomalous isotope effect coefficient of LaSrCuO superconductor was investigated in the weak-coupling method. The constant and van Hove singularity density of state, pseudogap, and the form of pseudogap temperature dependence on critical temperature are included in our calculation. Finally, the numerical results are shown in comparison with the experimental data of LaSrCuO superconductor. We found that the van Hove singularity density of state and the inversely relation of pseudogap temperature and critical temperature can fit well with the anomalous isotope effect coefficient data of LaSrCuO superconductor.

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2

TAO, Hongjie, Yingfei CHEN, Li LU, Qiansheng YANG, Bairu ZHAO, Yinghuan SHI, Yong LU, et al. "ELECTRON TUNNELING MEASUREMENTS OF ENERGY GAP IN SUPERCONDUCTORS YBaCuO, LaSrCuO AND BPBO." International Journal of Modern Physics B 01, no. 02 (June 1987): 555–59. http://dx.doi.org/10.1142/s0217979287000864.

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We have carried out superconducting energy gap measurements for polycrystalline perovskite-structure superconductors YBaCuO, LaSrCuO and BPBO with point contact tunneling. The tunneling conductance curves for YBaCuO, LaSrCuO and BPBO show the energy gap to transition temperature ratio 2Δ/kTc =4.7, 7.8 and 5.05 respectively, which is consistant with the strong-coupling superconductivity.

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3

Buzea, C., H. Myoren, H. B. Wang, K. Nakajima, and T. Yamashita. "Variation of LaSrCuO film temperature during pulsed laser deposition on LaSrGaO substrate." IEEE Transactions on Appiled Superconductivity 9, no. 2 (June 1999): 2398–401. http://dx.doi.org/10.1109/77.784955.

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4

Janossy, B., L. Fruchter, I. A. Campbell, J. Sanchez, I. Tanaka, and H. Kojima. "High field magnetic fluctuations in LaSrCuO." Solid State Communications 89, no. 5 (February 1994): 433–36. http://dx.doi.org/10.1016/0038-1098(94)90207-0.

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5

Khrebtov, I. A., M. B. Krayuhin, V. N. Leonov, A. D. Tkachenko, A. Yu Klimov, D. G. Pavelyev, and A. A. Ivanov. "Bolometric characteristics of YBaCuO and LaSrCuO films." Cryogenics 32 (January 1992): 533–36. http://dx.doi.org/10.1016/0011-2275(92)90223-w.

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6

Malinowski, A., M. Z. Cieplak, M. Berkowski, W. Plesiewicz, and T. Skośkiewicz. "Metal-Insulator Transition in Zinc-Doped LaSrCuO." Acta Physica Polonica A 109, no. 4-5 (April 2006): 617–21. http://dx.doi.org/10.12693/aphyspola.109.617.

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7

Plakida, N. M., and V. S. Shakhmatov. "Structural phase transitions in superconducting LaSrCuO compounds." Physica C: Superconductivity 153-155 (June 1988): 233–34. http://dx.doi.org/10.1016/0921-4534(88)90568-0.

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8

Cieplak, M. Z., A. Abal'oshev, I. Zaytseva, M. Berkowski, S. Guha, and Q. Wu. "Microstructure of the Pulsed Laser Deposited LaSrCuO Films." Acta Physica Polonica A 109, no. 4-5 (April 2006): 573–76. http://dx.doi.org/10.12693/aphyspola.109.573.

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9

Bugoslavsky, Yu V., A. L. Ivanov, A. A. Minakov, and S. I. Vasyurin. "Fishtails and anisotropy in underdoped LaSrCuO single crystals." Physica C: Superconductivity 233, no. 1-2 (November 1994): 67–76. http://dx.doi.org/10.1016/0921-4534(94)00589-3.

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10

Марченко, А. В., Ф. С. Насрединов, В. С. Киселев, П. П. Серегин, and К. Б. Шахович. "ЭФФЕКТИВНЫЕ ЗАРЯДЫ АТОМОВ ВТСП КЕРАМИК LaSrCuO, ОПРЕДЕЛЕННЫЕ В РЕЗУЛЬТАТЕ АНАЛИЗА ПАРАМЕТРОВ ЯДЕРНОГО КВАДРУПОЛЬНОГО ВЗАИМОДЕЙСТВИЯ, "Физика и химия стекла"." �� , no. 5 (2018): 504–12. http://dx.doi.org/10.7868/s0132665118050074.

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Методом сравнения рассчитанных (модель точечных зарядов) и экспериментальных (мессбауэровская спектроскопия и ядерный магнитный резонанс) параметров ядерного квадрупольного взаимодействия показано, что эффективные заряды всех атомов решеток сверхпроводящих керамик LaSrCuO соответствуют стандартным степеням их окисления за исключением атомов плоскостного кислорода, пониженный заряд которых интерпретируется как результат локализации на них дырки, возникающей при замещении ионов Laна Sr.

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11

Remmel, J., J. Geerk, G. Linker, O. Meyer, R. Smithey, B. Strehlau, and G. C. Xiong. "Superconductivity and structure of ion irradiated LaSrCuO thin films." Physica C: Superconductivity 165, no. 2 (January 1990): 212–20. http://dx.doi.org/10.1016/0921-4534(90)90170-j.

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12

Sutton, R. A., M. E. McHenry, and K. E. Sickafus. "Annealing of irradiation induced defects in a LaSrCuO crystal." IEEE Transactions on Appiled Superconductivity 7, no. 2 (June 1997): 2001–4. http://dx.doi.org/10.1109/77.620982.

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13

Ariosa, D., C. Cancellieri, P. H. Lin, and D. Pavuna. "Fermi surface determination from wavevector quantization in LaSrCuO films." Applied Physics Letters 92, no. 9 (March 3, 2008): 092506. http://dx.doi.org/10.1063/1.2891813.

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14

ANGILELLA, G. G. N., G. BALESTRINO, P. CERMELLI, P. PODIO-GUIDUGLI, and A. A. VARLAMOV. "STRAIN-INDUCED ELECTRONIC TOPOLOGICAL TRANSITIONS IN LaSrCuO THIN FILMS." International Journal of Modern Physics B 17, no. 04n06 (March 10, 2003): 542–47. http://dx.doi.org/10.1142/s0217979203016200.

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We review a Ginzburg-Landau phenomenological model for the dependence of the critical temperature on microscopic strain in tetragonal high-T c cuprates. Such a model is in agreement with the experimental results for LSCO under epitaxial strain, as well as with the hydrostatic pressure dependence of T c in most cuprates. In particular, a nonmonotonic dependence of T c on hydrostatic pressure, as well as on in-plane or apical microstrain, is derived. From a microscopic point of view, such results can be understood as due to the proximity to an electronic topological transition (ETT). In the case of LSCO, we argue that such an ETT can be driven by a strain-induced modification of the band structure, at constant hole content, at variance with a doping-induced ETT, as is usually assumed.

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15

Fruchter, L., C. Giovannella, and I. A. Campbell. "The breaking torque concept in a sintered LaSrCuO sample." Journal of the Less Common Metals 151 (May 1989): 1–11. http://dx.doi.org/10.1016/0022-5088(89)90290-7.

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16

Nishiyama, K., K. Nagamine, H. Kitazawa, E. Torikai, H. Kojima, and I. Tanaka. "Probing oxygen in high Tc superconductor LaSrCuO by negative muons." Hyperfine Interactions 65, no. 1-4 (February 1991): 1015–26. http://dx.doi.org/10.1007/bf02397757.

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17

Senoussi, S., F. Mosbah, O. Sarrhini, and S. Hammond. "The anisotropy of the irreversible magnetizations of YBCO and LaSrCuO." Physica C: Superconductivity 211, no. 3-4 (June 1993): 288–98. http://dx.doi.org/10.1016/0921-4534(93)90135-d.

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18

Zhang, Ling-Yun, Jia-Tih Lin, Bo-Zang Li, and Fu-Cho Pu. "Thermal Properties of High Temperature Superconductors: Soliton Statistics Approach." Modern Physics Letters B 11, no. 04 (February 10, 1997): 149–54. http://dx.doi.org/10.1142/s0217984997000207.

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We develop a soliton statistics approach to discuss the lattice effect of high temperature superconductor in the Davydov model on the basis of the bisoliton idea. We prove that lattice displacement in the Davydov model satisfies ϕ4 field form. Critical temperature of high temperature superconductor is studied from statistics of lattice kink. We have shown that the lattice effect is pronounced for thermal properties of high temperature superconductors. Comparision between theoretical and experimental results are good agreement for LaSrCuO and YBaCuO superconductor materials.

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19

Civale, L., H. Safar, F. de la Cruz, D. A. Esparza, and C. A. D'Ovidio. "The nature of the magnetic flux behavior of the superconductor LaSrCuO." Solid State Communications 65, no. 2 (January 1988): 129–33. http://dx.doi.org/10.1016/0038-1098(88)90672-2.

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20

SI, QIMIAO. "SPIN DYNAMICS IN THE NORMAL STATE OF HIGH-Tc SUPERCONDUCTORS." International Journal of Modern Physics B 08, no. 01n02 (January 20, 1994): 47–72. http://dx.doi.org/10.1142/s0217979294000038.

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We summarize our recent theoretical studies on the spin dynamics in the normal state of the metallic cuprates. The contrasting wave vector dependence of the dynamical spin structure factor S (q, ω) in LaSrCuO and YBaCuO systems are attributed to the differences in the fermiology, in conjunction with strong Coulomb correlations. These effects are found to account also for the anomalous temperature and frequency dependence of S (q, ω). We conclude that the low energy spin dynamics of the metallic cuprates are described in terms of correlated quasiparticles with a Luttinger Fermi surface and a non-zero antiferromagnetic exchange interaction.

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21

Berg, H., R. Müller, R. Borowski, B. Freitag, I. Müller, and B. Roden. "Improvement of the cation-distribution in the polycrystalline high-temperature superconductor LaSrCuO." Journal of Alloys and Compounds 267, no. 1-2 (March 1998): 279–82. http://dx.doi.org/10.1016/s0925-8388(97)00525-2.

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22

Li, Rukang, Xiao Wu, Zhuyao Chen, Yitai Qian, Changfei Zhu, Hongbing Wei, Shunxi Wang, Jian Sha, and Jiansheng Xia. "The superconductivity and metal-insulator transition in the Mg doped LaSrCuO system." Physics Letters A 144, no. 1 (February 1990): 35–38. http://dx.doi.org/10.1016/0375-9601(90)90044-o.

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23

SUGAWARA, K., N. ARAI, A. KOUZUKI, S. ICHIMURA, H. NAOI, K. HOTTA, and H. HIROSE. "ANOMALOUS BEHAVIORS OF NON-RESONANT MICROWAVE ABSORPTIONS OF SUPERCONDUCTORS." International Journal of Modern Physics B 14, no. 16 (June 30, 2000): 1633–50. http://dx.doi.org/10.1142/s0217979200001631.

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The non-resonant microwave absorption (NRMA) measurements have been intensively performed for superconducting thin films of YBa 2 Cu 3 O y fabricated on MgO (100) substrates and powder samples of LaSrCuO systems. In order to complement the study, we also review the NRMA of BiSrCaCuO system. A particular attention has been paid to the following phenomena: (i) phases, (ii) effect of current, (iii) directional effect of applied magnetic field, (iv) hysteresis, (v) microwave power absorbed as a function of magnetic field, (vi) linewidth in the vicinity of T c , and (vii) modulation amplitude effect. A preliminary study on ( La 0.98 Dy 0.02)1.85 Sr 0.15 CuO 4 was also reported.

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24

Kao, Ying-Jer, Qimiao Si, and K. Levin. "Commensurate and incommensurate structure of the neutron cross section in LaSrCuO and YBaCuO." Physica C: Superconductivity 341-348 (November 2000): 2165–66. http://dx.doi.org/10.1016/s0921-4534(00)01234-x.

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25

SUGAHARA, MASANORI, JUN ASAI, and MASASI FUKUTOMI. "EXPERIMENT OF DIELECTRIC QUANTUM INTERFERENCE IN LOW-DOPED c-ORIENTED LaSrCuO FILM CRYSTAL." Modern Physics Letters B 16, no. 10n11 (May 10, 2002): 375–82. http://dx.doi.org/10.1142/s0217984902003828.

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An experiment is made on the dielectric property of c-oriented low-doped La 2 - x Sr x CuO 4 thin film crystal. The film-thickness dependence of the electric polarization of the low-doped films shows a logarithmically cyclic positive and negative polarization change at "anomalous thicknesses" of the film. Interference patterns are observed around the anomalous thicknesses in the polarization-charge dependence of the ‖ c film "capacitance" by the measurement of the stored charge in equilibrium under step voltage application. These results are well explained based on the model of the quantum- Hall-effect-like state in the accumulated 2D planes.

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26

Hammond, S., M. Mosbah, S. Senoussi, P. Manuel, and H. Kojima. "Collapse of the vortex pinning force in LaSrCuO for H//a-b planes." Journal of Physics: Condensed Matter 5, no. 13 (March 29, 1993): L183—L188. http://dx.doi.org/10.1088/0953-8984/5/13/006.

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27

Kudriavtsev, Eugene M., and Sergey D. Zotov. "Experimental research of reflection variation sign change at T∼300 K in LaSrCuO ceramic." Physica C: Superconductivity 408-410 (August 2004): 736–38. http://dx.doi.org/10.1016/j.physc.2004.03.059.

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28

BERG, H., R. MUELLER, R. BOROWSKI, B. FREITAG, I. MUELLER, and B. RODEN. "ChemInform Abstract: Improvement of the Cation-Distribution in the Polycrystalline High-Temperature Superconductor LaSrCuO." ChemInform 29, no. 24 (June 22, 2010): no. http://dx.doi.org/10.1002/chin.199824219.

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29

Nishiyama, K., K. Kojima, K. Nagamine, E. Torikai, I. Tanaka, H. Kojima, and H. Kitazawa. "Anisotropic paramagnetic shift of ??O in the highT c related materials LaSrCuO and LaCuO." Hyperfine Interactions 79, no. 1-4 (1993): 873–78. http://dx.doi.org/10.1007/bf00567620.

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30

Cuadra-Solís, P. de-J., J. M. Hernandez, A. García-Santiago, J. Tejada, J. Vanacken, and V. V. Moshchalkov. "Avalanche-like vortex penetration driven by pulsed microwave fields in an epitaxial LaSrCuO thin film." Journal of Applied Physics 114, no. 23 (December 21, 2013): 233902. http://dx.doi.org/10.1063/1.4848997.

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31

Cuadra-Solís, P. J., J. M. Hernández, A. García-Santiago, J. Tejada, J. Vanacken, and V. V. Moshchalkov. "Magnetic moment relaxation studies by swept and pulsed microwave technique in LaSrCuO epitaxial thin film." Physica C: Superconductivity and its Applications 468, no. 7-10 (April 2008): 805–8. http://dx.doi.org/10.1016/j.physc.2006.11.016.

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32

Cieplak, Marta Z., M. Berkowski, A. Abal’oshev, S. Guha, and Q. Wu. "The effect of strain on the microstructure and superconductivity of pulsed laser deposited LaSrCuO films." Superconductor Science and Technology 19, no. 6 (April 26, 2006): 564–72. http://dx.doi.org/10.1088/0953-2048/19/6/025.

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33

Levin, K., Qimiao Si, and Yuyao Zha. "Theory of the spin dynamics in the cuprates: Comparison of the LaSrCuO and YBaCuO families." Physica C: Superconductivity 235-240 (December 1994): 71–74. http://dx.doi.org/10.1016/0921-4534(94)91317-x.

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34

Torikai, E., K. Nagamine, K. Nishiyama, E. Hirose, P. Birrer, I. Tanaka, H. Kojima, S. Srinivas, T. P. Das, and S. Maekawa. "Interaction of paramagnetic electron with highT c supercurrent in LaSrCuO studied by (μ−O) probe." Hyperfine Interactions 97-98, no. 1 (December 1996): 387–94. http://dx.doi.org/10.1007/bf02150187.

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35

Zhong, H., and R. Zeng. "Structure of LaSrMO4(M = Mn, Fe, Co, Ni, Cu) and their catalytic properties in the total oxidation of hexane." Journal of the Serbian Chemical Society 71, no. 10 (2006): 1049–59. http://dx.doi.org/10.2298/jsc0610049z.

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Perovskite-type LaSrMO4 (M = Mn, Fe, Co, Ni, Cu) mixed oxides were prepared by the decomposition of amorphous citric and ethylenediaminetetraacetic acid complexes and investigated by the XRD, FTIR, BET, TPR, TPD and XPSmethods. Their catalytic behavior in the total oxidation of hexane was examined. The following activity order was found LaSrCoO4 > LaSrNiO4 > LaSrCuO4 > LaSrFeO4 > LaSrMnO4. This is explained in terms of oxygen vacancies and mobile lattice oxygen, particle size and BET surface area. .

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36

Nettel, Stephen. "HTSC Isotope Effect with Soft Lattice Modes." International Journal of Modern Physics B 17, no. 13 (May 20, 2003): 2527–38. http://dx.doi.org/10.1142/s0217979203018429.

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An attempt is made to understand the isotope effects measured by Zhao et al. in LaSrCuO in terms of a previous theory for high Tc superconductors, a theory based on pair coupling by soft lattice modes. In the theory, the lattice elastic energy originating with the ion-electron correlation limits the gap. Here we note that this elastic energy does not depend directly on the ionic masses. However, the mechanical lattice parameters in the neighborhood of a structural phase transition are so sensitive that the free energy of oscillation and, hence, the masses are able to have an influence. Minimization of the free energy of the solid with respect to the lattice deformation leads to an equation of state, as basis for finding the effects of the ionic mass changes. With the measured isotope effects at several values of doping as input to the calculation, we obtain, as output, very plausible results for the Fermi energy, the lattice softening, and the electron-phonon coupling constant.

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37

Fenton, E. W. "Possible evidence for an incommensurate spin density wave in the stanford electron tunneling studies into LaSrCuO." Solid State Communications 64, no. 1 (October 1987): 27–29. http://dx.doi.org/10.1016/0038-1098(87)90513-8.

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38

Kudriavtsev, E. M., S. D. Zotov, V. V. Krivov, and M. Autric. "Temperature dependence of the velocity of the wave of reflection and conduction in NdCeCuO, YBaCuO and LaSrCuO." Physica C: Superconductivity 282-287 (August 1997): 1145–46. http://dx.doi.org/10.1016/s0921-4534(97)00701-6.

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39

Varshney, Dinesh, G. S. Patel, and R. K. Singh. "An intralayer pairing mechanism for the coexistence of charge- and spin-density waves induced superconductivity in LaSrCuO." Superconductor Science and Technology 15, no. 11 (October 18, 2002): 1617–27. http://dx.doi.org/10.1088/0953-2048/15/11/323.

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40

FRIEDEL, JACQUES, and MAHITO KOHMOTO. "MAGNETISM, PHONONS AND ANISOTROPY OF HIGH TEMPERATURE CUPRATES SUPERCONDUCTORS." International Journal of Modern Physics B 15, no. 05 (February 20, 2001): 511–26. http://dx.doi.org/10.1142/s0217979201004678.

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Phonon or electron mediated weak BCS attraction is enough to have high critical temperature if a van Hove anomaly is at work. This could apply to electron doped compounds and also to compounds with CuO 2 planes overdoped in holes, where T c decreases with increasing doping. If phonons dominate, it should lead to an anisotropic but mainly s superconductive gap, as observed recently in overdoped LaSrCuO, and probably also in electron doped compounds. If electrons dominate, a d-gap should develop as observed in a number of cases. In the underdoped range, the observed decrease of T c with hole doping can be related in all cases to the development of antiferromagnetic fluctuations which produces a magnetic pseudogap, thus lowering the density of states at the Fermi level. The observed mainly d-superconductive gap then can be due to a prevalent superconductive coupling through antiferromagnetic fluctuations; it could also possibly be attributed to the same phonon coupling as in the overdoped range, now acting on Bloch functions scattered in the magnetic pseudogap. More systematic studies of superconductive gap anisotropy and of magnetic fluctuations would be in order.

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41

Bugoslavsky, Yu V., A. L. Ivanov, V. A. Kovalsky, and A. A. Minakov. "Magnetic flux rotation and two types of additional maxima in magnetization curves of LaSrCuO single crystals in tilted magnetic field." Physica C: Superconductivity and its Applications 257, no. 3-4 (February 1996): 284–90. http://dx.doi.org/10.1016/0921-4534(95)00720-2.

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42

Pashitskii, E. A. "The critical temperature as a function of the number of Cooper pairs, and the superconductivity mechanism in a layered LaSrCuO crystal." Low Temperature Physics 42, no. 12 (December 2016): 1184–86. http://dx.doi.org/10.1063/1.4973010.

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43

Osofsky, M. S., R. J. Soulen, Weidong Si, Xianghui Zeng, A. Soukiassian, and Xiaoxing Xi. "Equivalence of the strain and doping dependence of the superconductive T/sub c/ in LaSrCuO: influence of the metal-insulator transition." IEEE Transactions on Appiled Superconductivity 13, no. 2 (June 2003): 2799–802. http://dx.doi.org/10.1109/tasc.2003.812019.

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44

Sugahara, M., H. Kaneda, M. Fukutomi, J. Asai, M. Wada, H. Hasegawa, and N. N. Bogolubov. "Macroscopic Quantum Effect Based on No-Field Quantum Hall Effect Found in Electric Properties of Low-Doped c-Oriented LaSrCuO Film Crystal." Modern Physics Letters B 17, no. 19 (August 20, 2003): 1021–44. http://dx.doi.org/10.1142/s0217984903005962.

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We study the film-thickness dependence of ||c dielectric polarization of La 1.95 Sr 0.05 CuO 4 thin film crystal, and find the existence of special film thicknesses where the polarization reveals a large amplitude alternate change with sign change. At the special thicknesses, we find interference patterns in the polarization-charge dependence of the film capacitance. With the use of small area device, we observe in the film the quantum resonance between the current-induced oscillation and coherent electromagnetic wave of microwaves (10 GHz), the CO 2 laser (10.6 μm), and the He–Ne laser (3.39 μm). A theoretical study based on the no-field quantum Hall effect is made to explicate these effects.

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45

Sugahara, Masanori, Tomonori Urata, Takeshi Kawabata, Jun Asai, Masashi Fukutomi, Mihoko Wada, and Sergei Kruchinin. "Proposal of controlled NOT gate using FQHE system and observation of large life time of laser triggered conductance change in LaSrCuO film with localization." Physica C: Superconductivity 367, no. 1-4 (February 2002): 234–36. http://dx.doi.org/10.1016/s0921-4534(01)01041-3.

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46

VANDOORN, R., I. FULLARTON, R. DESOUZA, J. KILNER, H. BOUWMEESTER, and A. BURGGRAAF. "Surface oxygen exchange of LaSrCoO." Solid State Ionics 96, no. 1-2 (March 2, 1997): 1–7. http://dx.doi.org/10.1016/s0167-2738(97)00011-8.

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47

Sun, Yifei, Jianhui Li, Yimin Zeng, Babak Shalchi Amirkhiz, Mengni Wang, Yashar Behnamian, and Jingli Luo. "A-site deficient perovskite: the parent for in situ exsolution of highly active, regenerable nano-particles as SOFC anodes." Journal of Materials Chemistry A 3, no. 20 (2015): 11048–56. http://dx.doi.org/10.1039/c5ta01733e.

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Introduction of A-site deficiency on Ni-doped LaSrCrO₃ anodes helps form highly mobile oxygen vacancies and remarkably enhances Ni nanoparticle reducibility, and significantly increases electronic conductivity and catalytic activity.

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48

Sun, Yi-Fei, Jian-Hui Li, Lin Cui, Bin Hua, Shao-Hua Cui, Jian Li, and Jing-Li Luo. "A-site-deficiency facilitated in situ growth of bimetallic Ni–Fe nano-alloys: a novel coking-tolerant fuel cell anode catalyst." Nanoscale 7, no. 25 (2015): 11173–81. http://dx.doi.org/10.1039/c5nr02518d.

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Ni, Fe-doped A-site-deficient LaSrCrO₃ were fabricated with an in situ exsolution of uniformly dispersed nano Ni, Fe and Ni–Fe alloy, which enhance the electrical conductivity greatly and promote the electrochemical performance with better coking resistance.

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49

Kao, Ting-Hui, Hiroya Sakurai, Taras Kolodiazhnyi, Yutaro Suzuki, Momoko Okabe, Toru Asaka, Koichiro Fukuda, et al. "Crystal structure and physical properties of Cr and Mn oxides with 3d3 electronic configuration and a K2NiF4-type structure." Journal of Materials Chemistry C 3, no. 14 (2015): 3452–59. http://dx.doi.org/10.1039/c4tc02458c.

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YSrCrO₄ is first synthesized. The magnetic and dielectric properties of YCaCrO₄, LaSrCrO₄ and A₂MnO₄ (A = Sr and Ca) are investigated together with YSrCrO₄.

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50

Mazo, G. N., O. A. Shlyakhtin, and S. N. Savvin. "Synthesis of LaSrCuO4−δ at reduced temperatures." International Journal of Inorganic Materials 3, no. 1 (January 2001): 31–35. http://dx.doi.org/10.1016/s1466-6049(00)00098-2.

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