博碩士論文 103222603 詳細資訊

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姓名 林仲杰(Lim Chong Chiat)  查詢紙本館藏   畢業系所 物理學系
(Studying Neutral Gold Clusters by the Brownian-type and Metadynamics Molecular Dynamics Simulations)
★ 金屬叢集的融化現象★ 帶電膠體系統之液態-液態/固態相變研究
★ 低濃度電解質在奈米管內異常的擴散和導電性★ 一價和多價叢集原子的熱穩定現象
★ 金屬與合金分子叢集的結構★ 物理系統之能量與焓分佈之統計力學研究
★ 膠體系統平衡相域與動態凝聚之研究★ 合金金屬叢集的溫度效應
★ 介面膠體叢聚現象的理論研究★ 帶電膠體懸浮液的相圖與液態-玻璃相變研究
★ 膠體相圖之理論計算★ 膠體、棒狀粒子混合系統之相圖的理論分析
★ 利用時間序列的統計方法研究金屬叢集的動力學★ 由分子動力學模擬探討層狀石墨烯的成長與碳化矽基板上多層石墨烯的熱穩定性
★ 金銅合金金屬叢集(N=38)的磁性性質研究★ 膠體、盤狀粒子混合系統的兩階段動態相變區域
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摘要(中) 本研究採用參數化之泛密度函數緊密捆綁(Density Functional Tight Binding, DFTB)理論,計算電中性金叢集之力場,并結合了布朗式(Brownian-type)分子動力學演算法[S. K. Lai, W. D. Lin, K. L. Wu, W. H. Li, and K. C. Lee, J. Chem. Phys. 121, 1487 (2004)],針對該系統在Nose-Hoover恆溫系統下之情況,進行模擬與研究。首先,我們在溫度於300K對所預備之四組金叢集進行模擬數據分析,從其熱力動力效應中推斷出它們的(a)結構流動性(b)鏡像對稱,與(c)二維到三維的變相現象。在所有分子動力學實驗模擬中,其所使用之叢集的離子各初始坐標位置是透過一套個別的優化演算法[T.W. Yen, T.L. Lim, T.L. Yoon and S.K. Lai, Comput. Phys. Commun. 220, 143 (2017)]取得。該優化演算法可在各別的叢集能量函數中使用DFTB理論獲取最低能量之結構。而應用同樣的初始結構模式,本文也在300K溫度中獨立地進行亞穩動力之分子動力學(MMD)模擬,與此同時在三組叢集裏使用集體變量(collective variable, CV) 空間,而不是以離子的位置坐標表示的傳統配置空間,來產生偏能軌跡。這MMD模擬旨在探索金叢集在CV 空間裏之時間性變化。
我們透過DFTB理論架構下所計算之能量函數的叢集分析結果,與應用一經驗勢(empirical potential)理論所得之MMD模擬結果作?比較。這經驗勢是透過塊材固態數據來決定能勢參數。我們期待這樣的對照能揭示s-d 混成軌域在金叢集的電子與結構特徵所扮演的微妙和重要角色。
總結來?,本文深入探討所選之叢集的若共價行?,同時也檢驗以上所描述在布朗式分子動力學與 MMD 模擬裏的(a)至(c)現象。
摘要(英) The parametrized density functional tight-binding (DFTB) theory is used to calculate the force field of a neutral gold cluster and it is then combined with the Brownian-type molecular dynamics (MD) algorithm [S. K. Lai, W. D. Lin, K. L. Wu, W. H. Li, and K. C. Lee, J. Chem. Phys. 121, 1487 (2004)] to perform simulation studies for this system within the Nose-Hoover thermostat scheme. We analyze the simulation data for four selected Au clusters which were prepared at T=300 K, and deduce from their thermally evolved behaviors the (a) fluxional character, (b) chiral behavior, and (c) traits of the bi- to tridimensional transition. In all of these MD simulations studies, the initial input position coordinates of ions in these clusters were the lowest energy configurations which we obtained separately from an optimization algorithm [T.W. Yen, T.L. Lim, T.L. Yoon and S.K. Lai, Comput. Phys. Commun. 220, 143 (2017)] where the individual cluster’s energy function employed is within the same DFTB theory. Using these same initial structures, we carried out also independent metadynamics MD (MMD) simulations at 300 K and generated biased trajectories for two of these selected clusters in a collective-variable space instead of the conventional configurational space in terms of the position coordinates of ions. The MMD simulations serve to explore the temporal change of Au clusters in the collective-variable space. It is hoped that an analysis of clusters whose energy functions are calculated in the DFTB theory in the latter and the comparison of simulation results with similar MMD simulations conducted with an empirical potential whose potential parameters are determined from bulk solid-state data would shed light on the subtlety and importance of s-d hybridization which is known to play an important role in both the electronic and structural properties of Au clusters. In this work, we delve into the effects of this covalent-like behavior of these selected clusters, examining them in parallel the features (a)-(c) mentioned above in Brownian-type MD and MMD simulations.
關鍵字(中) ★ 亞穩動力之分子動力學模擬
★ 泛密度函數緊密捆綁理論
★ 金屬叢集
關鍵字(英) ★ metadynamics MD simulation
★ density functional tight-binding theory
★ metallic clusters
論文目次 中文摘要 i
Abstract ii
Acknowledgements iii
Table of Contents iv
List of Figures vi
List of Tables ix
Explanation of Symbols xi
I. Introduction 1
II. Theory and Computational Methods 6
2.1 DFTB theory 6
2.1.1 DFTB parameters 7
2.2 MD simulation in collective variable space 8
2.2.1 Theoretical background: statistical mechanics and collective variables 8
2.2.2 Simulation background: Brownian-type MD simulation and collective
variables 9
2.2.3 Simulation background: selected collective variables 11
2.3 MMD simulation in CV-space: theory 11
2.4 MMD simulation in CV-space: well-tempered simulation technique 13
III. Results and Discussion 17
3.1 Brownian-type MD simulations: energy functions calculated by
Gupta-potential and DFTB-A theory 18
3.1.1 Gupta potential for Au9 and Au10 22
3.1.2 DFTB-A theory for Au9 and Au10 23
3.2 Brownian-type MD simulations: energy function calculated by
DFTB-B theory 24
3.3 Brownian-type MD simulations for Au15: enantiomeric structures 26
3.4 MMD simulations: energy functions by Gupta-potential and DFTB-A 29
3.4.1 Gupta potential: Au9 29
3.4.2 DFTB-A theory: Au9 33
3.4.3 DFTB-B theory: Au8 38
IV. Conclusion 42
Bibliographies 44
Appendix A: Well-tempered technique 48
Appendix B: Reaction coordinate for Au15 52
參考文獻 [1] A. Laio and M. Parrinello, Proc. Natl. Acad. Sci. U.S.A. 99, 12562 (2002). See also the three comprehensive reviews, A. Laio and F. L. Gervasio, Rep. Prog. Phys. 71, 126601 (2008); A. Barducci, M. Bonomi and M. Parrinello, Wiley Interdiscip. Rev. Comput. Mat. Sci. 1, 826 (2011); O. Valsson, P. Tiwary, and M. Parrinello, Annu. Rev. Phys. Chem. 67, 159 (2016).
[2] A. F. Voter, Phys. Rev. Lett. 78, 3908 (1997).
[3] M. M. Steiner, P. A. Genilloud, and J. W. Wilkins, Phys. Rev. B 57, 10236 (1998).
[4] J. A. Rahman and J. C. Tully, J. Chem. Phys. 116, 8750 (2002).
[5] D. Hamelberg, J. Mongan, and J. A. McCammon, ibid. 120, 11919 (2004).
[6] D. Perez, B. P. Uberuaga, Y. Shim, J. G. Amar, A. F. Voter, Annu. Rep. Comput. Chem. 5, 79 (2009).
[7] U. Doshi, D. Hamelberg, Biochim. Biophys. Acta 1850, 878 (2015).
[8] Reference 1 above has listed several program packages which can be used for metadynamics MD simulations.
[9] M. Elstner, D. Porezag, G. Jungnickel, M. Haugk, T. Frauenheim, S. Suhai, and G. Seifert, Phys. Rev. B 58, 7260 (1998).
[10] P. Koskinen, P., H. Hakkinen, G. Seifert, S. Sanna, T. Frauenheim and M. Moseler, New J. Phys. 8, 9 (2006).
[11] N. W. Ashcroft and D. Stroud, in Solid State Physics, edited by F. Seitz, D. Turnbull, and H. Ehrenreich (Academic, New York, 1978), Vol. 33, p.1.
[12] Y. Zeiri, Phys. Rev. E 51, R2769 (1995).
[13] J. A. Niesse and H. R. Mayne, J. Chem. Phys. 105, 4700 (1996).
[14] D. J. Wales and J. P. Doye, J. Phys. Chem. A 101, 5111 (1997).
[15] Z. Li and H. A. Scheraga, Proc. Natl. Acad. Sci. U. S. A. 84, 6611 (1987).
[16] R. N. Barnett and U. Landman, Phys. Rev. B 48, 2081 (1993).
[17] P. Calaminici, J. M. Vasquez-Perez, and D. A. Espindola Velasco, Can. J. Chem. 91, 591 (2013).
[18] T.D. Kuhne, WIREs Comput. Mol. Sci. 4, 391 (2014).
[19] R. P. Gupta, Phys. Rev. B 23, 6265 (1981).
[20] M. W. Finnis and J. E. Sinclair, Phil Mag A 50, 45 (1984); Erratum Philos Mag A 53, 161 (1986).
[21] A. P. Sutton and J. Chen, Philos. Mag. Lett. 61, 139 (1990).
[22] T.W. Yen, T.L. Lim, T.L. Yoon and S.K. Lai, Comput. Phys. Commun. 220, 143 (2017).
[23] We checked that a replacement of the empirical potential by a DFT-based semi-empirical potential such as the parametrized DFTB theory of Fihey et al. (Ref 32 below), at only this step did not lead to the anticipated prediction of the transition size.
[24] J. L. Wang, G. H. Wang and J. J. Zhao, Phys. Rev. B 66, 035418 (2002).
[25] Y. Dong and M. Springborg, Eur. Phys. J. D 43, 15 (2007).
[26] B. Kiran, S. Balusu, H. J. Zhai, S. Yoo, X. C. Zeng, and L. S. Wang, Proc. Natl. Acad. Sci. U. S. A. 102, 961 (2005).
[27] S. Yoo and X. C. Zeng, Angew. Chem., Int. Ed. 44, 1491 (2005).
[28] J. Bai, Li. F. Cui, J. Wang, S. Yoo, X. Li, J. Jellinek, C. Koehler, T. Frauenheim, L. S. Wang, and X. C. Zeng, J. Phys. Chem. A 110, 908 (2006).
[29] Th. Frauenheim, G. Seifert, M. Elstner, Z. Hajnal, G. Jungnickel, D. Porezag, S. Suhai, and R. Scholz, Phys. Stat. Sol. (b) 217, 41 (2000).
[30] Th. Frauenheim, G. Seifert, M. Elstner, Th. Niehaus, C. Kohler, M. Amkreutz, M. Sternberg, Z. Hajnal, Aldo Di Carlo and S. Suhai, J. Phys.: Condens. Matter 14, 3015 (2002).
[31] T. W. Yen and S. K. Lai, J. Chem. Phys. 142, 084313 (2015).
[32] A. Fihey, C. Hettich, J. Touzeau, F. Maurel, A. Perrier, C. Kohler, B. Aradi and T. Frauenheim, J. Comput. Chem. 36, 2075 (2015).
[33] V. Makinen, P. Koskinen, and H. Hakkinen, Eur. Phys. J. D 67, 1 (2013).
[34] P. Koskinen, and V. Makinen, Comput. Mat. Sci. 47, 237 (2009).
[35] P. Gruene, B. Butschke, J. T. Lyon, M. Rayner and A. Fiekicke, Z. Phys. Chem. 228, 337 (2014).
[36] P. Koskinen, H. Hakkinen, B. Huber, B. von Issendorff, and M. Moseler, Phys. Rev. Lett. 98, 015701 (2007).
[37] W. M. C. Foulkes and R. Haydock, Phys. Rev. B 39, 12520 (1989).
[38] P. Hohenberg and W. Kohn, Phys. Rev. 136, B864 (1964).
[39] W. Kohn and L. J. Sham, Phys. Rev. 140, A1133 (1965).
[40] A very recent work by Gaus et al. [M. Gaus, A. Goez, and M. Elstner, J. Chem. Theory Comput. 9, 338 (2013)] has expanded δn(r) up to third order.
[41] P. Koskinen, H. Hakkinen, G. Seifert, S. Sanna, T. Frauenheim and M. Moseler, New J. Phys. 8, 9 (2006).
[42] L. F. L. Oliveira, N. Tarrat, J. Cuny, J. Morillo, D. Lemoine, F. Spiegelman, and M. Rapacioli, J. Phys. Chem. A 120, 8469 (2016).
[43] S. K. Lai, W. D. Lin, K. L. Wu, W. H. Li, and K. C. Lee, J. Chem. Phys. 121, 1487 (2004).
[44] S. K. Lai, P. J. Hsu, K. L. Wu, W. K. Liu and M. Iwamatsu, J. Chem. Phys. 117, 10715 (2002).
[45] A. Barducci, G. Bussi, M. Parrinello, Phys. Rev. Lett. 100, 02063 (2008).
[46] M. Bonomi, D. Branduardi, G. Bussi, C. Camilloni, D. Provasi, P. Raiteri, D. Donadio, F. Marinelli, F. Pietrucci, R.A. Broglia and M. Parrinello, Comput. Phys. Commun. 180, 1961 (2009).
[47] M. Bonomi, A. Barducci and M. Parrinello, J Comput Chem 30, 1615 (2009).
[48] S.K. Lai and Wafa Maftuhin, National Central University M.Sc. thesis, unpublished (2018).
[49] S.K. Lai and Nurulia Sinta Rahmani, National Central University M.Sc. thesis, unpublished (2018).
[50] D. Liu and J. Nocedal, Math. Program. 45, 503 (1989)
[51] A. Vargas, G. Santarossa, M. Iannuzzi, and A. Baiker, Phys. Rev. B 80, 195421 (2009).
[52] G. Rossi, A. Rapallo, C. Mottet, A. Fortunelli, F. Baletto, and R. Ferrando, Phys. Rev. Lett. 93, 105503 (2004).
[53] E.M. Fernandez, J.M. Soler, I.L. Garzon, L.C. Balbas, Phys. Rev. B 70, 165403 (2004).
[54] B. Assadollahzadeh and P. Schwerdtfeger, J. Chem. Phys. 131, 064306 (2009).
[55] A. V. Walker, J. Chem. Phys. 122, 094310 (2005).
[56] X. B. Li, H.Y. Wang, X. D. Yang and Z. H. Zhu, J. Chem. Phys. 126, 084505 (2007).
[57] G. Zanti and D. Peeters, Theor. Chem. Acc. 132, 1300 (2013).
[58] P. J. Hsu, S. A. Cheong, and S. K. Lai, J Chem. Phys. 140, 204905 (2014).
指導教授 賴山強(San-Kiong Lai) 審核日期 2018-8-13
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