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研究生: 劉采靈
Liu, Tsai-Ling
論文名稱: Mn3V2Ge3O12石榴石氧化物的磁結構
Magnetic structure of Mn3V2Ge3O12 garnet oxide
指導教授: 黃建龍
Huang, Chien-Lung
學位類別: 碩士
Master
系所名稱: 理學院 - 物理學系
Department of Physics
論文出版年: 2026
畢業學年度: 114
語文別: 英文
論文頁數: 92
中文關鍵詞: 石榴石氧化物反鐵磁磁結構
外文關鍵詞: garnet oxide, antiferromagnetism, magnetic structure
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  • 本論文利用固態合成法合成Mn3V2Ge3O12 (MVGO)石榴石氧化物樣品,並透過實驗室內的X光粉末繞射儀(Rigaku, MiniFlex II),初步地確認樣品相組成及純度。接著將小塊樣品,利用Quantum design的MPMS3進行AC磁化率、DC磁化率及等溫磁化強度的量測。DC磁化率結果顯示,在外加磁場H = 100 Oe下,MVGO於低溫區呈現兩個磁相變。為進一步釐清其是否具有自旋玻璃行為,本研究透過 AC 磁化率量測觀察峰值隨頻率的變化。結果顯示MVGO 並未展現明顯的頻率相依性,因此可排除自旋玻璃行為的可能性,並確認兩個磁相變溫度分別為TN1 = 4 K 及TN2 = 2.6 K。此外,本研究進行不同外加磁場下的比熱量測,結果顯示兩個相變溫度皆隨磁場增加而往低溫移動,其中TN2 在外加磁場達20 kOe 時被抑制。同時,零場比熱測量顯示磁熵略有降低,在 25 K 時恢復了理論熵值的約 90 %。
    根據上述磁性與比熱量測結果,本研究進一步進行隨溫度變化的中子粉末繞射實驗。結果顯示,TN1 主要源自 Mn2+ 反鐵磁有序,而 TN2 則與 Mn2+及V3+ 的反鐵磁有序有關。磁結構精修結果顯示,Mn2+及V3+ 的有序磁矩明顯小於 spin-only 所預期的理論值。本研究最後根據實驗結果與相關文獻,探討造成磁矩降低的可能原因。

    This thesis reports the synthesis and investigation of the garnet oxide Mn3V2Ge3O12 (MVGO) prepared by the solid-state reaction method. The phase composition and sample purity were first characterized using a laboratory X-ray powder diffractometer (Rigaku, MiniFlex II). Small pieces of the sample were then measured using a Quantum Design MPMS3 system to perform AC susceptibility, DC susceptibility, and isothermal magnetization measurements.
    The DC susceptibility results reveal that MVGO undergoes two magnetic phase transitions in the low-temperature region under an applied magnetic field of H = 100 Oe. To further clarify whether spin-glass behavior exists in this system, AC susceptibility measurements were carried out by examining the frequency dependence of the susceptibility peaks. The results show no obvious frequency dependence, indicating the absence of spin-glass behavior. The two magnetic transition temperatures were determined to be TN1 = 4 K and TN2 = 2.6 K, respectively.
    In addition, specific heat measurements under various applied magnetic fields were performed. The results show that both transition temperatures shift toward lower temperatures with increasing magnetic field, and TN2 is suppressed under an applied magnetic field of 20 kOe. Meanwhile, the zero-field specific heat measurements indicate a slight reduction in magnetic entropy, recovering approximately 90 % of the theoretical entropy value at 25 K.
    Based on the magnetic and specific heat measurements, temperature-dependent neutron powder diffraction experiments were further conducted. The results indicate that TN1 mainly originates from the antiferromagnetic ordering of Mn2+ ions, whereas TN2 is associated with the antiferromagnetic ordering of both Mn2+ and V3+ ions. Magnetic structure refinements reveal that the ordered magnetic moments of Mn2+ and V3+ are significantly smaller than the theoretical values expected from the spin-only model. Finally, possible origins of the reduced magnetic moments are discussed based on the experimental results and relevant literature.

    中文摘要 i Abstract ii Acknowledgements iv Contents v List of Tables vii List of Figures viii 1 Introduction 1 1.1 Garnet structure 1 2 Motivation 3 3 Experimental methods 5 3.1 Sample preparation 5 3.2 X-ray powder diffraction 7 3.3 Magnetic properties measurement system 3 11 3.3.1 Vibrating sample magnetometer, VSM 12 3.3.2 Josephson junction 12 3.4 Physical properties measurement system, PPMS 14 3.4.1 Dilution Refrigerator (DR) 15 3.4.2 Specific heat 18 3.5 Neutron powder diffraction 21 4 Theory 25 4.1 Specific heat 25 4.1.1 Phonon contribution: Debye and Einstein models 26 4.1.2 Magnetic contribution and magnetic entropy 28 4.2 Magnetic symmetry and representational analysis 30 4.2.1 Landau theory of phase transitions 30 4.2.2 Magnetic order parameters and representational analysis 32 4.2.3 Rietveld refinement 35 5 Data analysis 42 5.1 Crystal structure of MVGO 42 5.2 Magnetic properties of MVGO 46 5.3 Specific heat of MVGO 54 5.4 Neutron powder diffraction of MVGO 58 5.5 Phase diagram 69 6 Conclusion 71 References 73

    [1] Vladimir Cherepanov, Igor Kolokolov, and Victor L’vov. The saga of YIG: Spectra, thermodynamics, interaction and relaxation of magnons in a complex magnet. Physics Reports, 229(3):81–144, 1993.
    [2] O. A. Petrenko, C. Ritter, M. Yethiraj, and D. McK Paul. Investigation of the low-temperature spin-liquid behavior of the frustrated magnet gadolinium gallium garnet. Phys. Rev. Lett., 80:4570–4573, May 1998.
    [3] Haruo Sawada. Electron density study of garnets: Z3Ga5O12; Z = Nd, Sm, Gd,Tb. Journal of Solid State Chemistry, 132(2):300–307, 1997.
    [4] Q. Cui, Q. Huang, Jose A. Alonso, Denis Sheptyakov, C. R. De la Cruz, M. T. Fern´andez-D´ıaz, N. N. Wang, Y. Q. Cai, D. Li, X. L. Dong, H. D. Zhou, and J.-G. Cheng. Complex antiferromagnetic order in the garnet Co3Al2Si3o12. Phys. Rev.B, 101:144424, Apr 2020.
    [5] Jiahua Min, Shuhan Zheng, Jingwen Gong, Xiyu Chen, Fei Liu, Yunlong Xie, Yongjun Zhang, Zhen Ma, Meifeng Liu, Xiuzhang Wang, Hong Li, and Jun-Ming Liu. Magnetoelectric effect in garnet Mn3Al2Ge3O12. Inorganic Chemistry, 61(1):86–91, 2022.
    [6] S. Mohanty, A. Magar, Vikram Singh, S. S. Islam, S. Guchhait, A. Jain, S. M. Yusuf, A. A. Tsirlin, and R. Nath. Double magnetic transitions, complex field-induced phases, and large magnetocaloric effect in the frustrated garnet compound Mn3Cr2Ge3O12. Phys. Rev. B, 109:134401, Apr 2024.
    [7] MyScope Training. Xrd practical.
    [8] Charles Kittel. Introduction to Solid State Physics. Wiley, New York, 8 edition, 2005.
    [9] Physical Society of Taiwan. Introduction to neutron powder diffraction and its applications.
    [10] FIZ Karlsruhe - Leibniz Institute for Information Infrastructure. Inorganic crystal structure database (ICSD).
    [11] K. Momma and F. Izumi. Vesta 3 for three-dimensional visualization of crystal, volumetric and morphology data. J. Appl. Crystallogr., 44:1272–1276, 2011.
    [12] Quantum Design. MPMS3 - magnetic property measurement system.
    [13] ResearchGate. Schematic diagram of a vibrating sample magnetometer.
    [14] ResearchGate. Illustration of a superconducting quantum interference device (SQUID).
    [15] A. Koz low. Principles of dilution refrigeration.
    [16] H. Cao. Refrigeration below 1 Kelvin. Journal of Low Temperature Physics, 204:175–205, 2021.
    [17] R. Bachmann, Jr. DiSalvo, F. J., T. H. Geballe, R. L. Greene, R. E. Howard, C. N. King, H. C. Kirsch, K. N. Lee, R. E. Schwall, H.U. Thomas, and R. B. Zubeck. Heat capacity measurements on small samples at low temperatures. Review of Scientific Instruments, 43(2):205–214, 02 1972.
    [18] J.C. Lashley, M.F. Hundley, A. Migliori, J.L. Sarrao, P.G. Pagliuso, T.W. Darling, M. Jaime, J.C. Cooley, W.L. Hults, L. Morales, D.J. Thoma, J.L. Smith, J. Boerio-Goates, B.F. Woodfield, G.R. Stewart, R.A. Fisher, and N.E. Phillips. Critical examination of heat capacity measurements made on a quantum design physical property measurement system. Cryogenics, 43(6):369–378, 2003.
    [19] Wen-Hsien Li. Romance of slow neutrons. Science Education Monthly, (53-11), 2014.
    [20] Maxim Avdeev and James R. Hester. Echidna: a decade of high-resolution neutron powder diffraction at OPAL. Journal of Applied Crystallography, 51(6):1597–1604, 2018.
    [21] Andrew J Studer, Mark E. Hagen, and Terrence J. Noakes. Wombat: The high-intensity powder diffractometer at the OPAL reactor. Physica B: Condensed Matter, 385-386:1013–1015, 2006.
    [22] J. Rodr´ıguez-Carvajal. Recent advances in magnetic structure determination by neutron powder diffraction. Physica B, 192:55–69, 1993.
    [23] A. S. Wills. A new protocol for the determination of magnetic structures using simulated annealing and representational analysis (SARAh). Physica B: Condensed Matter, 276–278:680–681, 2000.
    [24] LibreTexts Engineering. Debye model for specific heat, 2024.
    [25] Daniel Arovas. 5.6: The ideal bose gas. LibreTexts Physics, 2024.
    [26] Charles Kittel. Introduction to Solid State Physics. Wiley, New York, 8th edition, 2005.
    [27] Stephen Blundell. Magnetism in Condensed Matter. Oxford University Press, 10 2001.
    [28] Nigel Goldenfeld. Lectures on Phase Transitions and the Renormalization Group. Addison-Wesley, 1992.
    [29] Jan Friedrich. Overview of Closure Methods for the Closure Problem of Turbulence, pages 59–103. Springer International Publishing, Cham, 2021.
    [30] E. F. Bertaut. Representation analysis of magnetic structures. Acta Crystallographica Section A, 24:217, 1968.
    [31] Wikipedia contributors. Maschke’s theorem — wikipedia, The Free Encyclopedia, 2026.
    [32] Yu. A. Izyumov and V. E. Naish. Symmetry analysis in neutron diffraction studies of magnetic structures. Journal of Magnetism and Magnetic Materials, 12:239–248, 1979.
    [33] H. M. Rietveld. The crystal structure of some alkaline earth metal uranates of the type M3UO6. Acta Crystallographica, 20:508–513, 1966.
    [34] H. M. Rietveld. A profile refinement method for nuclear and magnetic structures. Journal of Applied Crystallography, 2:65–71, 1969.
    [35] H. P. Klug and L. E. Alexander. X-ray Diffraction Procedures. John Wiley, New York, 2nd edition, 1959.
    [36] G. K. Wertheim, M. A. Butler, K. W. West, and D. N. E. Buchanan. Determination of the gaussian and lorentzian content of experimental line shapes. Review of Scientific Instruments, 45(11):1369–1371, 1974.
    [37] P. Thompson, D. E. Cox, and J. B. Hastings. Rietveld refinement of debye–Scherrer synchrotron x-ray data from Al2O3. Journal of Applied Crystallography, 20:79–83, 1987.
    [38] Juan Rodr´ıguez-Carvajal. An Introduction to the Program FullProf 2000. Laboratoire L´eon Brillouin (CEA-CNRS), CEA/Saclay, Gif sur Yvette Cedex, France, 2001. Version July 2001.
    [39] Christian Lipp, Sabine Strobel, Falk Lissner, and Rainer Niewa. Garnet-type Mn3Cr2(GeO4)3. Acta Crystallographica Section E: Structure Reports Online, 68:i35, 2012.
    [40] V. O. Garlea, R. Jin, D. Mandrus, B. Roessli, Q. Huang, M. Miller, A. J. Schultz, and S. E. Nagler. Magnetic and orbital ordering in the spinel MnV2O4. Phys. Rev. Lett., 100:066404, Feb 2008.
    [41] Sam Mugiraneza and Alannah M. Hallas. Tutorial: A beginner’s guide to interpreting magnetic susceptibility data with the curie–weiss law. Communications Physics, 5:95, 2022.
    [42] Claudine Lacroix, Philippe Mendels, and Fr´ed´eric Mila, editors. Introduction to Frustrated Magnetism: Materials, Experiments, Theory, volume 164 of Springer Series in Solid-State Sciences. Springer, Berlin, Heidelberg, 2011.
    [43] Kim Myung-Whun, J. S. Kim, T. Katsufuji, and R. K. Kremer. Magnetic susceptibility and specific heat of a spinel mnv2o4 single crystal. Phys. Rev. B, 83:024403, Jan 2011.
    [44] Oak Ridge National Laboratory Neutron Scattering Division. Introduction to magnetic structures, 2014.
    [45] B.C. Tofield and B.E.F. Fender. Covalency parameters for Cr3+, Fe3+ and Mn4+ in an oxide environment. Journal of Physics and Chemistry of Solids, 31(12):2741–2749, 1970.

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