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RESEARCH PAPER · Inorganic Chemistry Frontiers · 2018

Pb 2 BO 3 Br: a novel nonlinear optical lead borate bromine with a KBBF-type structure exhibiting strong nonlinear optical response

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Pb 2 BO 3 Br: a novel nonlinear optical lead borate bromine with a KBBF-type structure exhibiting strong nonlinear optical responseOriginalBaLiZn 3 (BO 3 ) 3 : a new member of the KBe 2 BO 3 F 2 family possessing dense BO 3 triangles and the smallest interlayer distance16Cation-tuned synthesis of the A 2 SO 4 ·SbF 3 (A = Na + , NH 4 + , K + , Rb + ) family with nonlinear optical properties78Flexible coordination of Pb atoms and variable zinc–borate frameworks to construct three Pb 5 Zn 4 B 6 O 18 polymorphs8Ion-induced structural and optical performance evolution in LBO-like crystals: experimental and theoretical investigation13Li3.366Mg0.317B2O5: The first pyroborate in the Li2O-MgO-B2O3 system1Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation Effects211Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials95Centrosymmetric (NH4)2SbCl(SO4)2 and Non-centrosymmetric (NH4)SbCl2(SO4): Synergistic Effect of Hydrogen-Bonding Interactions and Lone-Pair Cations on the Framework Structures and Macroscopic Centricities89Li2BaSc(BO3)2F and LiBa2Pb(BO3)2F with Layered Structures featuring Special Li−O/F Configurations11Na4Yb(CO3)3F: A New UV Nonlinear Optical Material with a Large Second Harmonic Generation Response8The linear and nonlinear optical response of CsGeX3 (X=Cl, Br, and I): The finite field and first-principles investigation26An energy band engineering design to enlarge the band gap of KTiOPO 4 (KTP)-type sulfates via aliovalent substitution66Ba 3 Ca 4 (BO 3 ) 3 (SiO 4 )Cl: a new non-centrosymmetric complex alkaline-earth metal borosilicate chloride with a deep-ultraviolet cut-off edge19Centrosymmetric K 2 SO 4 ·(SbF 3 ) 2 and noncentrosymmetric Rb 2 SO 4 ·(SbF 3 ) 2 resulting from cooperative effects of lone pair and cation size63Exploration of the deep-ultraviolet nonlinear optical materials in the derivatives of KBe2BO3F27From centrosymmetric to noncentrosymmetric: cation-directed structural evolution in X 3 ZnB 5 O 10 (X = Na, K, Rb) and Cs 12 Zn 4 (B 5 O 10 ) 4 crystals26Sn 2 B 7 O 12 F with a 2∞[B 14 O 24 ] 6− layer constructed from the unprecedented [B 7 O 16 ] 11− fundamental building block18Two alkali calcium borates exhibiting second harmonic generation and deep-UV cutoff edges3Ba4M(CO3)2(BO3)2 (M=Ba, Sr): two borate-carbonates synthesized by open high temperature solution method29Structural and Femtosecond Third-Order Nonlinear Optical Properties of Sodium Borate Oxide Glasses: Effect of Antimony98CsSbF 2 SO 4 : An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO 4 (KTP)‐type Structure87CsSbF2SO4: An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO4 (KTP)‐type Structure432K9[B4O5(OH)4]3(CO3)X·7H2O (X = Cl, Br): Syntheses, Characterizations, and Theoretical Studies of Noncentrosymmetric Halogen Borate–Carbonates with Short UV Cutoff Edges16β‐CsB9O14: A Triple‐Layered Borate with Edge‐Sharing BO4 Tetrahedra Exhibiting a Short Cutoff Edge and a Large Birefringence30Research and Development of Zincoborates: Crystal Growth, Structural Chemistry and Physicochemical Properties20Nontoxic KBBF Family Member Zn2BO3(OH): Balance between Beneficial Layered Structure and Layer Tendency81Pb 3 Ba 3 Zn 6 (BO 3 ) 8 and α-BaZn 2 (BO 3 ) 2 : new members of the zincoborates containing two different dimensional Zn–O units8From BaAl 2 (BO 3 ) 2 O to SnAl 2 (BO 3 ) 2 F 2 : structure transformation based on ion regulation3Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook145Novel ultraviolet (UV) nonlinear optical (NLO) materials discovered by chemical substitution-oriented design302Three non-centrosymmetric bismuth phosphates, Li 2 ABi(PO 4 ) 2 (A = K, Rb, and Cs): effects of cations on the crystal structure and SHG response23Two-stage evolution from phosphate to sulfate of new KTP-type family members as UV nonlinear optical materials through chemical cosubstitution-oriented design51PbB5O7F3: A High-Performing Short-Wavelength Nonlinear Optical Material120An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses224An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses42Effect of Eu3+ in tuning the ultrafast third-order optical nonlinearity in heavy metal borate glasses56Synthesis and Crystal Structure Determination of a Dimeric Complex of Dimethylammoniumbis(p-tert-butylcatecholato) borate0Different mechanism of response of asymmetric lone pair electrons around ns2 cations to birefringence and second harmonic generation7Cs 3 Pb 2 (CH 3 COO) 2 X 5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups75Cs3Pb2(CH3COO)2X5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups22Ba(MoO2F)2(XO3)2 (X = Se and Te): First Cases of Noncentrosymmetric Fluorinated Molybdenum Oxide Selenite/Tellurite Through Unary Substitution for Enlarging Band Gaps and Second Harmonic Generation34Borates: A Rich Source for Optical Materials1089Sn2B5O9Br as an Outstanding Bifunctional Material with Strong Second‐Harmonic Generation Effect and Large Birefringence84Sn3B8O15: A Ternary Tin(II) Borate with Flexible [B8O18]12– Fundamental Building Block Formed by [B7O16]11– and [BO3]3– Groups10An antimony( iii ) borate with large birefringence exhibiting unwonted [B 5 O 11 ] fundamental building blocks and dimeric [Sb 2 O 6 ] clusters26Barium fluoroiodate crystals with a large band gap and birefringence22Pb 2 TiFO(SeO 3 ) 2 Br: a new polar compound with the strongest second harmonic generation in the selenite bromide family29Pb 2.28 Ba 1.72 B 10 O 19 featuring a three-dimensional B–O anionic network with edge-sharing [BO 4 ] obtained under ambient pressure6Different mechanism of stereochemical activity and birefringence in post-transition metal halides: A first-principles investigation1RETRACTED: Influence of gamma irradiation on photoluminescence and nonlinear optical properties of Eu3+ activated heavy metal borate glasses28KCs2[Pb2Br5(HCOO)2]: A Polar 3D Lead‐Bromide Framework Exhibiting Strong Second‐Harmonic Generation Response10Two Tellurium(IV)-Based Sulfates Exhibiting Strong Second Harmonic Generation and Moderate Birefringence as Promising Ultraviolet Nonlinear Optical Materials28Unprecedented Formation of Potassium Borate Based Carbonate from Chloral Hydrate, Potassium Carbonate and Boric Acid1Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate212Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate22Noncentrosymmetric Rb3(COOH)3(H3BO3)2 vs Centrosymmetric Cs3(COOH)3(H3BO3)214M4O(IO3)3(I3O7F3)BF4 (M = Pb, Sr): Promising Nonlinear Optical Materials Featuring the Unprecedented Windmill-Shaped [I3O7F3]2– Polyfluoroiodate Anion12[C(NH 2 ) 3 ]BiCl 2 SO 4 : an excellent birefringent material obtained by multifunctional group synergy40KF·B(OH) 3 : a KBBF-type material with large birefringence and remarkable deep-ultraviolet transparency33KLi 2 CO 3 F: a beryllium-free KBBF-type deep-UV carbonate with an enhanced interlayer interaction and large birefringence20Metal oxyhalides: an emerging family of nonlinear optical materials124α-LiMB 9 O 15 (M = Sr, Pb): flexible [B 3 O 7 ] units leading to the low temperature phase of β-LiMB 9 O 15 (M = Sr, Pb)11Layered Perovskite-like Nitrate Cs2Pb(NO3)2Br2 as a Multifunctional Optical Material40Inorganic nonlinear optical materials7The strong alternating built-in electric field sourced by ball milling on Pb2BO3X (X Cl, Br, I) piezoelectric materials contributes to high catalytic activity50Shedding Light on the Structure and Characterization of K2ZnGe2O6: A Phase-Matchable Nonlinear Optical Crystal19Crystal Growth of K2HCO3F·H2O with a Very Short Cutoff Edge and Large Birefringence17Design of a new ultraviolet nonlinear optical material KNO3SO3NH3 exhibiting an unexpected strong second harmonic generation response44Cs2B4O5(OH)4: A new hydrated borate with a short UV cutoff edge2SbHPO3F: 2D van der Waals Layered Phosphite Exhibiting Large Birefringence32Cd(NH 2 SO 3 ) 2 · x H 2 O ( x = 0, 2): new sulfamates with a unique coordination environment and reversible phase transitions20A Cation-Driven Approach toward Deep-Ultraviolet Nonlinear Optical Materials17A new stable polymorph of Li 2 TeMo 3 O 12 with wide mid-infrared transparency and a large Raman response17KMB 4 O 6 F 3 (M = Co, Fe): two-dimensional magnetic fluorooxoborates with triangular lattices directed by triangular BO 3 units16New Ultraviolet Nonlinear Optical Crystal Rb3Hg2(SO4)3Cl3Two UV optical crystals with strong optical anisotropy, large band gaps and an α-BBO type structure7Unveiling the Superior Optical Properties of Novel Melamine‐Based Nonlinear Optical Material with Strong Second‐Harmonic Generation and Giant Optical Anisotropy74Nonlinear optical crystals KPb3(3-C5H4NCOO)2Br5 and KPb3(3-C5H4NCOO)2Cl3Br2 with new Pb-centered nitrogen-halide polyhedrons obtained by the halide anionic substitution4Cd2Nb2Te4O15: A Novel Pseudo‐Aurivillius‐Type Tellurite with Unprecedented Nonlinear Optical Properties and Excellent Stability40Pb(OH)I: A lead(II)-based oxyhalide with a large birefringence5Centrosymmetric Rb2Sb(C2O4)2.5(H2O)3 and Noncentrosymmetric RbSb2(C2O4)F5: Two Antimony (III) Oxalates as UV Optical Materials20Heteroanionic LaBrVIO4 (VI = Mo, W): Excellence in Both Nonlinear Optical Properties and Photoluminescent Properties11ASn(C10H12N2O8)Cl·H2O (A = K, Rb): Nonlinear optical crystals with new distorted Sn(IV)-centered nitrogen-oxygen-chloride polyhedron and wide band gaps6Two van der Waals Layered Antimony(III) Phosphites as UV Optical Materials11Deep‐Ultraviolet Transparent Mixed Metal Sulfamates with Enhanced Nonlinear Optical Properties and Birefringence11Deep‐Ultraviolet Transparent Mixed Metal Sulfamates with Enhanced Nonlinear Optical Properties and Birefringence75K(NH4)Zn2(PO4)2: a Beryllium-Free Sr2Be2B2O7 Derivative with Enhanced Interlayer Connectivity7Design of alkali lead oxybromides with a strong second-harmonic generation response and large birefringence1Exploration of antimony( iii ) oxyhalides via single-site substitution in quest of large birefringence10Hydrogen bonding bolstered head-to-tail ligation of functional chromophores in a 0D SbF 3 ·glycine adduct for a short-wave ultraviolet nonlinear optical material32Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates153Exceptional Optical Anisotropy Enhancement Achieved Through Dual‐Ions Cosubstitution Strategy in Novel Hybrid Bismuth Halides23An Unprecedented [BO2]‐Based Deep‐Ultraviolet Transparent Nonlinear Optical Crystal by Superhalogen Substitution33An Unprecedented [BO2]‐Based Deep‐Ultraviolet Transparent Nonlinear Optical Crystal by Superhalogen Substitution1Enhanced UV Nonlinear Optical Properties in Layered Germanous Phosphites through Functional Group Sequential Construction11Enhanced UV Nonlinear Optical Properties in Layered Germanous Phosphites through Functional Group Sequential Construction116LiNa2Ca8B12O24F6Cl and Li1.2Na2.8B6O11: A Case of Cation-Induced Birefringence Enhancement via Dimensional Changes of Highly Polymerized [B12O24] Motifs10Breaking Performance Barriers in KBe 2 BO 3 F 2 (KBBF) Analogs by Functional Group Self‐Polymerization5Breaking Performance Barriers in KBe 2 BO 3 F 2 (KBBF) Analogs by Functional Group Self‐Polymerization48Insight into the Origin of Second Harmonic Generation and Rational Design in the Metal Halide Borates7Pb 4 O 3 I 2 : A Lead Oxyhalide IR Optical Crystal with an Unprecedented 1 ∞ [O 3 Pb 4 ] Chain Featuring a Wide Transmittance Range and Large Birefringence3The spin–orbit coupling induced stereochemical activity and nonlinear optical response in Pb2BO3X (X = Cl, Br, I)2Review of KBe2BO3F2-like second-order nonlinear optical materials and their structure-performance relationships13Halide Ion-Directed Symmetry Control in π-Conjugated Molecular Crystals6Recent Progress in the Design and Synthesis of Nonlinear Optical Crystals with Stereochemically Active Lone Pairs8[Pb(ptz)(OH)(H2O)]: A Hybrid Nonlinear Optical Crystal with Large Birefringence0Oxygen Vacancy Engineering toward Enhanced Dielectric and Ionic Conductivity Properties in Single Crystal LiNbMoO 61A universal synthetic strategy for noncentrosymmetric lead oxyhalide frameworks with strong second-harmonic generation0Ba 5 Zn 4 (B 3 O 6 ) 2 (B 12 O 24 ): A Borate with Edge-Sharing [BO 4 ] Tetrahedral Connection by Introducing Zn into β-BaB 2 O 42The First Silver Lead Borate, AgPb[B5O9]0The Parallel Coplanar Alignment of Planar Non‐π‐Conjugated [Pb 3 Br 3 ] Rings for a Stable Ultraviolet Nonlinear Optical Crystal0Unlocking Hidden Potential via Reprogrammed Mineral Structures: How Anionic Transformation Achieves Ultraviolet Nonlinear Optical Performance0

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  1. BaLiZn 3 (BO 3 ) 3 : a new member of the KBe 2 BO 3 F 2 family possessing dense BO 3 triangles and the smallest interlayer distance

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  2. Cation-tuned synthesis of the A 2 SO 4 ·SbF 3 (A = Na + , NH 4 + , K + , Rb + ) family with nonlinear optical properties

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  3. Flexible coordination of Pb atoms and variable zinc–borate frameworks to construct three Pb 5 Zn 4 B 6 O 18 polymorphs

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  4. Ion-induced structural and optical performance evolution in LBO-like crystals: experimental and theoretical investigation

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  5. Li3.366Mg0.317B2O5: The first pyroborate in the Li2O-MgO-B2O3 system

    Inorganic Chemistry Communications · 2018-05-17

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  6. Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation Effects

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  7. Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials

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  8. Centrosymmetric (NH4)2SbCl(SO4)2 and Non-centrosymmetric (NH4)SbCl2(SO4): Synergistic Effect of Hydrogen-Bonding Interactions and Lone-Pair Cations on the Framework Structures and Macroscopic Centricities

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  9. Li2BaSc(BO3)2F and LiBa2Pb(BO3)2F with Layered Structures featuring Special Li−O/F Configurations

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  10. Na4Yb(CO3)3F: A New UV Nonlinear Optical Material with a Large Second Harmonic Generation Response

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  11. The linear and nonlinear optical response of CsGeX3 (X=Cl, Br, and I): The finite field and first-principles investigation

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  12. An energy band engineering design to enlarge the band gap of KTiOPO 4 (KTP)-type sulfates via aliovalent substitution

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  13. Ba 3 Ca 4 (BO 3 ) 3 (SiO 4 )Cl: a new non-centrosymmetric complex alkaline-earth metal borosilicate chloride with a deep-ultraviolet cut-off edge

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  15. Exploration of the deep-ultraviolet nonlinear optical materials in the derivatives of KBe2BO3F2

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  16. From centrosymmetric to noncentrosymmetric: cation-directed structural evolution in X 3 ZnB 5 O 10 (X = Na, K, Rb) and Cs 12 Zn 4 (B 5 O 10 ) 4 crystals

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  20. Structural and Femtosecond Third-Order Nonlinear Optical Properties of Sodium Borate Oxide Glasses: Effect of Antimony

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  21. CsSbF 2 SO 4 : An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO 4 (KTP)‐type Structure

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  23. K9[B4O5(OH)4]3(CO3)X·7H2O (X = Cl, Br): Syntheses, Characterizations, and Theoretical Studies of Noncentrosymmetric Halogen Borate–Carbonates with Short UV Cutoff Edges

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  24. β‐CsB9O14: A Triple‐Layered Borate with Edge‐Sharing BO4 Tetrahedra Exhibiting a Short Cutoff Edge and a Large Birefringence

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  27. Pb 3 Ba 3 Zn 6 (BO 3 ) 8 and α-BaZn 2 (BO 3 ) 2 : new members of the zincoborates containing two different dimensional Zn–O units

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  28. From BaAl 2 (BO 3 ) 2 O to SnAl 2 (BO 3 ) 2 F 2 : structure transformation based on ion regulation

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  29. Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook

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  30. Novel ultraviolet (UV) nonlinear optical (NLO) materials discovered by chemical substitution-oriented design

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  31. Three non-centrosymmetric bismuth phosphates, Li 2 ABi(PO 4 ) 2 (A = K, Rb, and Cs): effects of cations on the crystal structure and SHG response

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  32. Two-stage evolution from phosphate to sulfate of new KTP-type family members as UV nonlinear optical materials through chemical cosubstitution-oriented design

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  33. PbB5O7F3: A High-Performing Short-Wavelength Nonlinear Optical Material

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  34. An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses

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  36. Effect of Eu3+ in tuning the ultrafast third-order optical nonlinearity in heavy metal borate glasses

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  37. Synthesis and Crystal Structure Determination of a Dimeric Complex of Dimethylammoniumbis(p-tert-butylcatecholato) borate

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  38. Different mechanism of response of asymmetric lone pair electrons around ns2 cations to birefringence and second harmonic generation

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  39. Cs 3 Pb 2 (CH 3 COO) 2 X 5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups

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  40. Cs3Pb2(CH3COO)2X5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups

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  41. Ba(MoO2F)2(XO3)2 (X = Se and Te): First Cases of Noncentrosymmetric Fluorinated Molybdenum Oxide Selenite/Tellurite Through Unary Substitution for Enlarging Band Gaps and Second Harmonic Generation

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  42. Borates: A Rich Source for Optical Materials

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  43. Sn2B5O9Br as an Outstanding Bifunctional Material with Strong Second‐Harmonic Generation Effect and Large Birefringence

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  44. Sn3B8O15: A Ternary Tin(II) Borate with Flexible [B8O18]12– Fundamental Building Block Formed by [B7O16]11– and [BO3]3– Groups

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  45. An antimony( iii ) borate with large birefringence exhibiting unwonted [B 5 O 11 ] fundamental building blocks and dimeric [Sb 2 O 6 ] clusters

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  46. Barium fluoroiodate crystals with a large band gap and birefringence

    Inorganic Chemistry Frontiers · 2021-01-01

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