Perkins Niu 0162D 13222.Pdf

Total Page:16

File Type:pdf, Size:1020Kb

Perkins Niu 0162D 13222.Pdf ABSTRACT SYNTHESIS AND PROPERTIES OF LANTHANIDE METAL-ORGANIC FRAMEWORKS AND LANTHANIDE-METALLOID COMPLEXES: STRUCTURAL DETERMINATION, PHOTOLUMINESCENCE, AND APPLICATIONS Timothy Perkins, Ph.D. Department of Chemistry and Biochemistry Northern Illinois University, 2018 Chong Zheng, Director Materials synthesis is a field at the intersections of chemistry and physics with wide- ranging applications. There is a rich diversity of techniques to develop novel materials, but very little fundamental understanding of the mechanisms that drive the formation of solids, leading to an inability to predict a synthesis for a material with targeted properties. Solvothermal synthesis has garnered much attention in the field due to its relative predictability by combining solution- phase dynamics with reactive inorganic precursors. By incorporating composition-guided organic chemistry, which often benefits from predictable properties, metal-organic frameworks (MOFs) synthesized solvothermally have emerged among the most rationally designed solids in modern science. MOFs are a class of crystalline materials composed of metal-centers linked by organic ligands, forming large, porous networks. Structures, thus some properties, can be predicted given motifs for previously determined metal-center geometries and ligand-bonding environs. Further, targeted properties can be chemically tuned via optimization of the ligand and/or metal. Early efforts in the field resulted in the intriguing materials that failed to be commercially viable due to stability issue. Metal-organic frameworks using lanthanide metal-centers (Ln-MOFs) are thought to increase thermodynamic stability of the material and present unique electronic properties such as photoluminescence. The projects presented herein focus on investigating the properties and stability of lanthanide metal-organic frameworks with a naphthalene-based ligand. To be a commercially viable material, among other things a MOF must be stable in addition to having practical properties. The increased complexity in both the accessible geometries and electronic properties of lanthanides relative to light transition metals makes this work largely exploratory. Novel, isostructural cerium, neodymium, and europium Ln-MOFs comprised of two-dimensional sheets of metal-carboxylate centers bridged by naphthalene were synthesized and photoluminescence properties analyzed. The series of Ln-MOFs studied show they have robust photoactivity that may be exploited in small molecule or ion sensing. Compound [Ce(NO3)(NDC)]n was found to be stable under basic and acidic aqueous conditions, but not thermally stable to 400°C. Small aromatic molecules were screened against [Nd(NO3)(NDC)]n and fluorescence quenching shown to be correlated to spectral overlap, with significant signal quenching of benzene, but no observed selective change in excitation or emission wavelengths. Further, the compound was found to be stable to 300°C in open air. In particular, compound [Eu(NO3)(NDC)]n was shown to be highly fluorescent in water and is readily quenched by trace concentrations of hazardous industrial by-product chromic acid. These investigations represent a broad effort to characterize Ln-MOFs in hopes of guiding the development of similar materials that exhibit robust chemical and thermal stability and relevant properties. Isoreticular synthesis is generally, but not exactly, an appropriate tool for replicating the synthesis with naphthalene-based ligands but different lanthanide metals. Procedurally altering the reported successful synthetic conditions with lanthanide metals is highly likely to produce isostructural and comparably stable compounds that exhibit unique electronic properties. Solvothermal synthesis using thiourea as a reactive solvent was also shown to produce unique lanthanide-metalloid complex germanium (II) sulfide doped lanthanum (III) hydroxide. The complex was found to photocatalytically degrade dye methylene blue in water under UV irradiation. While, not as efficient as known photocatalyst anatase titania, it represents a new class of lanthanum oxides doped with small band gap semiconductors that may be more easily optimized for photocatalytic processes than investigations on titanium dioxide have proven to be. Such intercalated lanthanum oxides may even have other relevant photo-driven applications, such as light harvesting or water-splitting. NORTHERN ILLINOIS UNIVERSITY DE KALB, ILLINOIS AUGUST 2018 SYNTHESIS AND PROPERTIES OF LANTHANIDE METAL-ORGANIC FRAMEWORKS AND LANTHANIDE-METALLOID COMPLEXES: STRUCTURAL DETERMINATION, PHOTOLUMINESCENCE, AND APPLICATIONS BY TIMOTHY PERKINS © 2018 Timothy Perkins A DISSERTATION SUBMITTED TO THE GRADUATE SCHOOL IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE DOCTOR OF PHILOSOPHY DEPARTMENT OF CHEMISTRY AND BIOCHEMISTRY Doctoral Director: Chong Zheng ACKNOWLEDGEMENTS I am eternally grateful to my advisor, Dr. Chong Zheng. Under his tutelage, he gave me freedom to make mistakes, to learn, and ultimately to earn my successes. His willingness to put so much trust in me and give me latitude over the lab has provided me a solid foundation in successfully designing and executing relevant research. His support is evidenced in the (several) organizational overhauls of the laboratory he has stoically endured, and the collaborative trips to both Beijing and Shanghai we took. I would like to thank Dr. Fuqiang Huang of Peking University and the Shanghai Institute of Ceramics for extending the invitation to use their excellent facilities, and especially his students Jianqiao He and Xian Zhang who taught me so much and were the senior colleagues I did not have at Northern Illinois University. I would also like to extend my gratitude to the members of my committee: Dr. Victor Ryzhov, Dr. Lee Sunderlin, and Dr. Zhili Xiao. Their support and input have been critical not only in helping me shape my work into a completed dissertation, but for years prior. Dr. Ryzhov often acted as a second advisor and has provided me with guidance without which I could not have succeeded. I would very much like to thank Dr. Sunderlin for letting me stop by his office unannounced for many stimulating conversations, as well as lending me tools from his lab more times than he knows. I would be remiss if I did not acknowledge the faith in me Dr. Zhili Xiao placed by recommending me to a colleague at Argonne National Laboratory, which gave me access to some of the best facilities available and exposed me to a professional safety culture I have strived to implement at NIU. iii My group members James O’Sullivan, Sura Ginting, and Crystal Ferels have always been available to lend a hand and bounce around ideas. My undergrad Noel Amaro was a delight to work with and often enabled me to be in two places at once. Aaron Sturtz, the laboratory mechanic, has helped me repair and modify so much equipment he has surely saved the university more than his salary, and saved me countless hours. The electrical expertise of Mike Figora probably saved me from getting shocked a few times, and I couldn’t have upgraded our ovens and furnaces without him. I am also sincerely grateful for all the support Dr. Taesam Kim, instrumental specialist, has provided our research lab over the years. He is not only the first line of defense when troubleshooting but an excellent teacher. I need to give a special thank you to my parents, Dennis and Cindy Perkins, who have unconditionally supported me at every step. Finally, I thank Katherine Didier, who has been my best friend and companion, and has always been a source of encouragement and love. Our responsibility is to do what we can, learn what we can, improve the solutions, and pass them on. Richard Feynman vi TABLE OF CONTENTS Page LIST OF FIGURES…………………………………………………………………………...…vii LIST OF TABLES………………………………………………………………...……………...xi LIST OF APPENDICES…….……………………………………………………..…………....xii LIST OF ABBREVIATIONS …………….……………………………………………………xiii CHAPTER ONE: PERSPECTIVES OF SOLID-STATE PHYSICS, INORGANIC CHEMISTRY, AND THE MATERIALS SCIENCES ................................... 1 1.1. Epistemological Framework ..................................................................................... 1 1.2. Modern Frameworks for Materials Synthesis ........................................................... 6 1.3. Metal-Organic Frameworks .................................................................................... 18 1.4. Lanthanide-Metal-Organic Frameworks ................................................................. 40 CHAPTER TWO: THE SYNTHESIS AND PHOTOLUMINESCENCE PROPERTIES OF [CE(NO3)(NDC)•2DMA]n............................................................................. 45 2.1. Synthesis of [Ce(NO3)(NDC)•2DMA]n ................................................................. 45 2.2. Structural Characterization of [Ce(NO3)(NDC)•2DMA]n ...................................... 46 2.3. Stability of [Ce(NO3)(NDC)•2DMA]n .................................................................... 53 2.4. Photoluminescence Properties of [Ce(NO3)(NDC)]n.............................................. 55 CHAPTER THREE: THE SYNTHESIS AND PHOTOLUMINESCENCE PROPERTIES OF [ND(NO3)(NDC)•2DMA]n ............................................................................ 61 3.1. Structural Characterization of [Nd(NO3)(NDC)•2DMA]n ..................................... 61 3.2. Stability of [Nd(NO3)(NDC)•2DMA]n ................................................................... 66 3.3. Photoluminescence Properties
Recommended publications
  • Additional Teacher Background Chapter 4 Lesson 3, P. 295
    Additional Teacher Background Chapter 4 Lesson 3, p. 295 What determines the shape of the standard periodic table? One common question about the periodic table is why it has its distinctive shape. There are actu- ally many different ways to represent the periodic table including circular, spiral, and 3-D. But in most cases, it is shown as a basically horizontal chart with the elements making up a certain num- ber of rows and columns. In this view, the table is not a symmetrical rectangular chart but seems to have steps or pieces missing. The key to understanding the shape of the periodic table is to recognize that the characteristics of the atoms themselves and their relationships to one another determine the shape and patterns of the table. ©2011 American Chemical Society Middle School Chemistry Unit 303 A helpful starting point for explaining the shape of the periodic table is to look closely at the structure of the atoms themselves. You can see some important characteristics of atoms by look- ing at the chart of energy level diagrams. Remember that an energy level is a region around an atom’s nucleus that can hold a certain number of electrons. The chart shows the number of energy levels for each element as concentric shaded rings. It also shows the number of protons (atomic number) for each element under the element’s name. The electrons, which equal the number of protons, are shown as dots within the energy levels. The relationship between atomic number, energy levels, and the way electrons fill these levels determines the shape of the standard periodic table.
    [Show full text]
  • ELECTRONEGATIVITY D Qkq F=
    ELECTRONEGATIVITY The electronegativity of an atom is the attracting power that the nucleus has for it’s own outer electrons and those of it’s neighbours i.e. how badly it wants electrons. An atom’s electronegativity is determined by Coulomb’s Law, which states, “ the size of the force is proportional to the size of the charges and inversely proportional to the square of the distance between them”. In symbols it is represented as: kq q F = 1 2 d 2 where: F = force (N) k = constant (dependent on the medium through which the force is acting) e.g. air q1 = charge on an electron (C) q2 = core charge (C) = no. of protons an outer electron sees = no. of protons – no. of inner shell electrons = main Group Number d = distance of electron from the nucleus (m) Examples of how to calculate the core charge: Sodium – Atomic number 11 Electron configuration 2.8.1 Core charge = 11 (no. of p+s) – 10 (no. of inner e-s) +1 (Group i) Chlorine – Atomic number 17 Electron configuration 2.8.7 Core charge = 17 (no. of p+s) – 10 (no. of inner e-s) +7 (Group vii) J:\Sciclunm\Resources\Year 11 Chemistry\Semester1\Notes\Atoms & The Periodic Table\Electronegativity.doc Neon holds onto its own electrons with a core charge of +8, but it can’t hold any more electrons in that shell. If it was to form bonds, the electron must go into the next shell where the core charge is zero. Group viii elements do not form any compounds under normal conditions and are therefore given no electronegativity values.
    [Show full text]
  • Periodic Table of the Elements Notes
    Periodic Table of the Elements Notes Arrangement of the known elements based on atomic number and chemical and physical properties. Divided into three basic categories: Metals (left side of the table) Nonmetals (right side of the table) Metalloids (touching the zig zag line) Basic Organization by: Atomic structure Atomic number Chemical and Physical Properties Uses of the Periodic Table Useful in predicting: chemical behavior of the elements trends properties of the elements Atomic Structure Review: Atoms are made of protons, electrons, and neutrons. Elements are atoms of only one type. Elements are identified by the atomic number (# of protons in nucleus). Energy Levels Review: Electrons are arranged in a region around the nucleus called an electron cloud. Energy levels are located within the cloud. At least 1 energy level and as many as 7 energy levels exist in atoms Energy Levels & Valence Electrons Energy levels hold a specific amount of electrons: 1st level = up to 2 2nd level = up to 8 3rd level = up to 8 (first 18 elements only) The electrons in the outermost level are called valence electrons. Determine reactivity - how elements will react with others to form compounds Outermost level does not usually fill completely with electrons Using the Table to Identify Valence Electrons Elements are grouped into vertical columns because they have similar properties. These are called groups or families. Groups are numbered 1-18. Group numbers can help you determine the number of valence electrons: Group 1 has 1 valence electron. Group 2 has 2 valence electrons. Groups 3–12 are transition metals and have 1 or 2 valence electrons.
    [Show full text]
  • Periodic Table 1 Periodic Table
    Periodic table 1 Periodic table This article is about the table used in chemistry. For other uses, see Periodic table (disambiguation). The periodic table is a tabular arrangement of the chemical elements, organized on the basis of their atomic numbers (numbers of protons in the nucleus), electron configurations , and recurring chemical properties. Elements are presented in order of increasing atomic number, which is typically listed with the chemical symbol in each box. The standard form of the table consists of a grid of elements laid out in 18 columns and 7 Standard 18-column form of the periodic table. For the color legend, see section Layout, rows, with a double row of elements under the larger table. below that. The table can also be deconstructed into four rectangular blocks: the s-block to the left, the p-block to the right, the d-block in the middle, and the f-block below that. The rows of the table are called periods; the columns are called groups, with some of these having names such as halogens or noble gases. Since, by definition, a periodic table incorporates recurring trends, any such table can be used to derive relationships between the properties of the elements and predict the properties of new, yet to be discovered or synthesized, elements. As a result, a periodic table—whether in the standard form or some other variant—provides a useful framework for analyzing chemical behavior, and such tables are widely used in chemistry and other sciences. Although precursors exist, Dmitri Mendeleev is generally credited with the publication, in 1869, of the first widely recognized periodic table.
    [Show full text]
  • • What I Hope to Convey to You Is That Rare Earths Are Uniquely Required for High Performance Magnets
    • What I hope to convey to you is that rare earths are uniquely required for high performance magnets. • First a quick introduction to Arnold – the company I’ve worked for since 1992. • Arnold’s history in magnetics and magnetic materials extends back to 1895 and has included almost every commercially supplied permanent and soft magnetic product. • Today Arnold is focused on: SmCo, Alnico and bonded permanent magnets; precision thin metals – both magnetic and non-magnetic; magnetic assemblies for motors, magnetic levitation, sensing and separation technologies; and most recently we have responded to customer requests to develop and supply ultra-high performance permanent magnet motors for select applications. • Let’s start by answering this question: What makes rare earth elements so special? • The rare earth elements consist of the 15 lanthanide elements (lanthanum to lutetium) plus yttrium and scandium. • Yttrium and scandium are directly above lanthanum in the periodic table and have chemical properties that are very similar to the lanthanides – that is why they are usually included with them. • Note cesium and barium precede lanthanum in row 6 of the periodic table and that hafnium, element number 72, continues row 6 right after lutetium, the lanthanide with the highest atomic number, 71. • Note too, row 4 of the table which contains the transition elements including iron, cobalt and nickel. We’ll be making some comparison between the two groups of elements in later slides. • Rare earth elements (REEs) have considerable chemical similarities thus making them difficult to separate from each other. • That is one reason they were late in being discovered, isolated and incorporated in alloys and compounds.
    [Show full text]
  • Ionic Interactions in Lanthanide Halides
    Ionic Interactions in Lanthanide Halides Z. Akdeniz, Z. Çiçek, and M. P. Tosia Department of Physics, University of Istanbul, Istanbul, Turkey and Abdus Salam International Centre for Theoretical Physics, 1-34014 Trieste, Italy a INFM and Classe di Scienze, Scuola Normale Superiore, 1-56126 Pisa, Italy Reprint requests to Prof. M. P. T.; Fax: +39-050-563513; E-mail: [email protected] Z. Naturforsch. 55 a, 861-866 (2000); received September 27, 2000 We determine a model of the ionic interactions in RX3 compounds (where R is a metal in the rare-earth series from La to Lu and X = CI, Br or I) by an analysis of data on the static and dynamic structure of their molecular monomers. The potential energy function that we adopt is patterned after earlier work on Aluminium trichloride [Z. Akdeniz and M. P. Tosi, Z. Naturforsch. 54a, 180 (1999)], but includes as an essential element the electric polarizability of the trivalent metal ion to account for a pyramidal shape of RX3 molecules. From data referring mostly to trihalides of elements at the ends and in the middle of the rare-earth series (/. e. LaX3, GdX3 and LuX3), we propose systematic variations for the effective valence, ionic radius and electric polarizability of the metal ions across the series. As a first application of our results we predict the structure of the Dy2Cl6 and Dy2Br6 molecular dimers and demonstrate by comparison with electron diffraction data that lanthanide-ion polarizability plays a quantitative role also in this state of tetrahedral-like coordination. Key words: Ionic Clusters; Molten Salts.
    [Show full text]
  • 24. SOLUTION CHEMISTRY of the LANTHANIDE ELEMENTS Gregory
    .24. SOLUTION CHEMISTRY OF THE LANTHANIDE ELEMENTS Gregory R. Choppin Department of Chemistry Florida State University Tallahassee, Florida 32306,U.S.A. ABSTRACT Complexes of the lanthanide elements provide insight into the factors which are important in ionically bonded systems. The enthalpy and entropy terms of complexation are a measure of the role of hydration effects while the free energy measures the metal-ligand interaction. The role of ligand basicity in the nature of the complex as an inner sphere or a solvent- separated outer sphere species is reviewed. An equation which has been used successfully to calculate stability constants which agree with experimental values is described and shown to be useful in establishing models for lanthanide complexing. The stability of complexes as a function of canonical structure of organic ligands and of ligand ring size is discussed. A study of charge polarization in conjugated organic ligands complexed by lanthanide cations is described. .25. SOLUTION CHEMISTRY OF THE LANTHANIDE ELEMENTS I. INTRODUCTION The development of separation methods using ion exchange resins has provided chemists with large quantities of very pure individual lanthanide elements. As a result, in the last 30 years research in lanthanide chemistry has been relatively intensive and has led to a rather satisfactory understanding of the chemical behavior of these elements as well as to the growing utilization of them in a variety of technological applications. A central feature of lanthanide chemistry is the strongly ionic character of the bonding between lanthanide cations and other atoms. As a result of this ionicity, they can be classified as "hard" (strongly acidic) cations.
    [Show full text]
  • Alternative Periodic Tables Have Been Proposed That Address Mn Fe 25 28 Cr P S Co Some of the Shortcomings of Mendeleev’S Table (See Pp
    GROUP 4: CHEMISTRY H He Li Be B C N O F Ne Na Mg Al Si P S Cl Ar K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe Cs Ba La Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn Fr Ra Ac Rf Db Sg Bh Hs Mt Ds Rg Cn Nh Fl Mc Lv Ts Og Ce Pr Nd Pm Sm Eu Gd Td Dy Ho Er Tm Yb Lu Alternative Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No Lr n=1 Simplified periodic table H He* 1 2 N O n=2 7 8 C Li Be F• periodic tables 6 3 4 9 B Ne* 5 10 Several alternative periodic tables have been proposed that address Mn Fe 25 28 Cr P S Co some of the shortcomings of Mendeleev’s table (see pp. 2–6). Do you n=3 24 15 16 27 V Si Na Mg Cl• Ni PERIODICPERIODIC 23 14 11 12 17 28 DIVIDE think they work better than the version on your classroom wall? Ti Al Ar* Cu 22 2 2 29 ALKALI Sc Zn 21 30 METALS NOBLE 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 Gd Tb GASES Uue 2 65 Og Ubn Cm 1 H He Eu Tc Ru Dy Fr SUPERACTINIDES Am Bk 63 43 44 66 Rn Pu Sm Mo As Se Rh Ho Np Gd Tb 2 Li Be B C N O F Ne Ra U Eu 62 42 33 34 45 67 Xe Cs n=4 Pa Sm Dy Cf Pm Nb Ge K Ca Br• Pb Er Th Pm 3 Na Mg Al Si P S Cl Ar 61 41 32 19 20 35 46 68 Ts Kr Rb Ba Ac Nd Ho Pr Er Es Nd Zr Ga Kr* Ag Tm At K Sr Tm 4 K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr 60 40 31 36 47 69 I Ar Ce Fm La Yb Md Pr Y Cd Yb Br Na Ca Lu 59 39 48 70 Cl Ne No 5 Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe He Li LANTHANIDES & ACTINIDESLr F Mg Y Ce Lu Be Hf Rf 58 71 O H Sc Zr 6 Cs Ba La Ce Pr Nd Pm Sm Eu Gd Td Dy Ho Er Tm Yb Lu Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn S Ta Db Se
    [Show full text]
  • I Anomalous Properties of Elements I That MOW "Long Periods" of Elements
    James E. Huheey and Caroline L. Huheey I Anomalous Properties of Elements University of Maryland College Park, 20742 I that MOW"Long Periods" of Elements The phenomenon known as the lantha- difficulties in their separation are well-documented (3). nide contraction has long been appreciated as an impor- Less well-explored are the cases in which the lanthanide tant factor in determining the properties of the lan- contraction results in different properties for the post- thanide and post-lanthanide elements. Appreciation lanthanide elements (4). In general, these may be re- of this phenomenon is of obvious heuristic value with lated to greater effective nuclear charge and attraction regard to research efforts directed towards these ele- for electrons in the heavier elements. ments. In addition there is an implicit pedagogical Table I lists the ground state ionization energies (6) value that has been discussed at some length (1) and for the elements rubidium-xenon (Period Five) and which is included in most descriptive discussions of these cesium-radon (Period Six). The pre-lanthanide ele- elements. It is the purpose of this paper to examine ments cesium, barium, and lanthanum have ionization the physical nature of this phenomenon and extend the energies less than their lighter congeners as expected for concept to other parts of the periodic table. the main group elements. The effect of the addition of fourteen protons to the nucleus and fourteen poorly shielding 4f electrons is a higher ionization energy for hafnium than for zirconium. 811 of the following sixth period transition elements have higher ionization ener- gies than their lighter congeners and the trend persists as far as lead.
    [Show full text]
  • Excited State Properties of Lanthanide Complexes: Beyond Ff States
    Inorganica Chimica Acta 359 (2006) 4130–4138 www.elsevier.com/locate/ica Excited state properties of lanthanide complexes: Beyond ff states Arnd Vogler *, Horst Kunkely Institut fu¨r Anorganische Chemie, Universita¨t Regensburg, D-93040 Regensburg, Germany Received 3 May 2006; accepted 27 May 2006 Available online 7 June 2006 Abstract Generally, metal-centered ff states dominate the discussion of the excited state properties of lanthanide complexes. In particular, the luminescence properties of Eu(III) and Tb(III) compounds have been studied in great detail for many decades. However, other types of excited states such as MC fd, MLCT, LMCT, MMCT and IL are also of interest. In this context, we have recently examined the excited state behavior of selected Ce(III), Ce(IV), Eu(II) and Gd(III) complexes which are luminescent and/or photoreactive. Ó 2006 Elsevier B.V. All rights reserved. Keywords: Electronic spectra; Luminescence; Photochemistry; Lanthanides; Cerium; Europium; Gadolinium 1. Introduction coefficients and the radiative lifetimes of ff states are rather large (10À3 s). Owing to the small absorption coefficients Lanthanide (Ln) compounds play an important role in of Ln3+, the excitation can be facilitated by suitable ligands the field of luminescence spectroscopy. In the ground which absorb the light and subsequently transfer the exci- states, the electron configuration of lanthanide cations tation energy to the emissive Ln3+ ion. In addition, appro- extends from f0 to f14. All lanthanides form stable com- priate ligands may prevent radiationless deactivations. This pounds in the oxidation state III, representing the ground behavior is illustrated by various Eu3+ and Tb3+ com- state configuration f1 (Ce3+)tof14 (Lu3+).
    [Show full text]
  • (A) Lanthanide (Ln) Zinc Telluride by Means of Experimental and Quantum-Chemical Techniques
    crystals Article Revealing the Bonding Nature in an ALnZnTe3-Type Alkaline-Metal (A) Lanthanide (Ln) Zinc Telluride by Means of Experimental and Quantum-Chemical Techniques Katharina Eickmeier and Simon Steinberg * Institute of Inorganic Chemistry, RWTH Aachen University, Landoltweg 1, D-52074 Aachen, Germany; [email protected] * Correspondence: [email protected]; Tel.: +49-241-80-92075 Received: 17 September 2020; Accepted: 8 October 2020; Published: 10 October 2020 Abstract: Tellurides have attracted an enormous interest in the quest for materials addressing future challenges, because many of them are at the cutting edge of basic research and technologies due to their remarkable chemical and physical properties. The key to the tailored design of tellurides and their properties is a thorough understanding of their electronic structures including the bonding nature. While a unique type of bonding has been recently identified for post-transition-metal tellurides, the electronic structures of tellurides containing early and late-transition-metals have been typically understood by applying the Zintl Klemm concept; yet, does the aforementioned formalism actually − help us in understanding the electronic structures and bonding nature in such tellurides? To answer this question, we prototypically examined the electronic structure for an alkaline metal lanthanide zinc telluride, i.e., RbDyZnTe3, by means of first-principles-based techniques. In this context, the crystal structures of RbLnZnTe3 (Ln = Gd, Tb, Dy),
    [Show full text]
  • Lanthanide Chalcogenolate Complexes: Syntheses, Structures
    中国科技论文在线 http://www.paper.edu.cn Coordination Chemistry Reviews 250 (2006) 2059–2092 Review Lanthanide chalcogenolate complexes: Syntheses, structures and applications in organic chemistry Hong-Xi Li a, Yan-Jun Zhu a, Mei-Ling Cheng a, Zhi-Gang Ren a, Jian-Ping Lang a,b,∗, Qi Shen a a Key Laboratory of Organic Synthesis of Jiangsu Province, School of Chemistry and Engineering, Suzhou University, Suzhou 215123, Jiangsu, PR China b State Key Laboratory of Coordination Chemistry, Nanjing University, Nanjing 210093, Jiangsu, PR China Received 18 October 2005; accepted 9 February 2006 Available online 23 February 2006 Contents 1. Introduction ........................................................................................................... 2060 2. Methods of preparation ................................................................................................. 2060 2.1. Protonolysis reaction ............................................................................................. 2060 2.2. Salt metathesis reaction........................................................................................... 2062 2.3. Oxidation–reduction reaction ..................................................................................... 2063 2.3.1. Oxidation reaction of divalent lanthanocene complexes ...................................................... 2063 2.3.2. Reaction of elemental lanthanide and REER ................................................................ 2065 2.3.3. Reaction of Ln/M amalgam with REER and trans-metallation
    [Show full text]