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MODULAR ASPECTS IN INORGANIC STRUCTURES Giovanni FERRARIS [email protected]

tools to model inorganic crystal structures

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Page 1: tools to model inorganic crystal structures

MODULAR ASPECTS IN INORGANIC STRUCTURES

Giovanni FERRARIS

[email protected]

Page 2: tools to model inorganic crystal structures

CRYSTAL STRUCTURES

Ti

Ti

Ti

Ti

Ca

Ti

Ti

Ti

Ti

Atoms

Coordinationpolyhedra Cages of zeolites

Page 3: tools to model inorganic crystal structures

TETRAHEDRAL / OCTAHEDRAL MODULES

T O TO

+ =

TOT beams

biopyriboles

Page 4: tools to model inorganic crystal structures

BIOPYRIBOLES

amphibole

chesterite

jimthompsonite

Page 5: tools to model inorganic crystal structures

Cubic and Hexagonalperovskites

Cubic ABCPolytype 3C

Hexagonal ACPolytype 2H

Page 6: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGY

Ti

Ti

Ti

Ti

Ca

Ti

Ti

Ti

Ti

Modules of perovskite-type structure alternated with other modules occur in

materials of interest for science and technology → hybrid or intergrowth

perovskites

Three-dimensional (sharing of corners along three directions)

Two-dimensional (sharing of corners along two directions)

Mono-dimensional (sharing of corners along one direction)

Zero-dimensional (isolated octahedra)

Page 7: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGY

Projection in the planes (100), (1-10) and (001), in the order, of the octahedral sheets stacked along [001], [111], and [110]. Different periodicities in the stacked planes are selective of the interlayer.

[001] [111] [110]

(100) (1-10) (001)

Page 8: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGY

TlBa2Can-1CunO2n+3 tallium cuprate series of superconductors

n = 31223

n = 4 1234

n = 51245

n = 1121

n = 21212

Page 9: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGYTl2Ba2Can-1CunO2n+4 tallium cuprate series of

superconductors

n = 1221 n = 2

2212

n = 32223 n = 4

2234

Page 10: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGY

SUPERCONDUCTING OXYCARBONATES

Polysomatic series (Sr2CuO2CO3)m(XpSr2CuO5)n (m > n) based on (001) perovskite layers connected by CO3 groups

A

B

CuO2

Sr2CO3

CuO2

SrO

XO

SrO

A

B

CuO2

Sr2CO3

CuO2

SrO

XO

SrO

m = 1 n = 1m = 1 n = 0 m = 2 n = 1

Page 11: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGYORGANIC-INORGANIC HYBRID PEROVSKITES

(RNH3)2An-1BnX3n+1 series based on (001) layersEngineering in the (C4H9NH3)2(CH3NH3)n-1SnnI3n+1 polysomatic series1. n =1 → large band gap semiconductor2. The resistivity decreases by increasing n3. Metallic behaviour for n ≥ 34. The n = ∞ material (CH3NH3)SnI is a p-type metalNon-linear optical properties and electroluminescence

Page 12: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGYORGANIC-INORGANIC HYBRID PEROVSKITES

A'2AmBmX3m+2 (n = 1, 2, 3) series based on (110) layers

Page 13: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGYORGANIC-INORGANIC HYBRID PEROVSKITES

A'2Aq-1BqX3q+3 (n = 1, 2, 3) series based on (111) layers

Page 14: tools to model inorganic crystal structures

Perovskite modules (anion)intercalated with organic molecules (cation).

Combining properties of the organic part (e.g., luminescence andplastic) with those of the inorganic part (e.g., electrical and

mechanical). Tailoring can play on:

Nature of the A (dodecahedral) and B (octahedral) cations.Nature of the X anion (usually a halide).Orientation and thickness of the perovskite layer.

Series of organic-inorganic layered perovskites can be built by:1. Keeping fix the perovskite layer and changing organic interlayer;2. Keeping fix the interlayer and changing the thickness of perovskite;3. Varying the thickness of both layers.

PEROVSKITE MODULES AND TECHNOLOGYORGANIC-INORGANIC HYBRID PEROVSKITES

Page 15: tools to model inorganic crystal structures

PEROVSKITE MODULES AND TECHNOLOGY

An+1BnX3n+1 polysomatic series (Ruddlesden-Popper series) n (001) perovskite layers alternate with one sodium-chloride-like layer

On (La,Ba)2CuO4 (n = 1) Bednorz and Müller (1986) discovered high-Tc superconductivity with Tc ~ 30 K.

Sr1.8La1.2Mn2O7 (n = 2) shows colossal magnetoresistance.

Page 16: tools to model inorganic crystal structures

LEFT - Palmierite-type structure = 9Rperovskite with partial filling oftetrahedral and octahedral sites.

RIGHT – Alternation of palmierite-typeand 2H-perovskite modules

PALMIERITE TYPE

Page 17: tools to model inorganic crystal structures

MAGNETOPLUMBITE-TYPE

(111) spinel layers

Page 18: tools to model inorganic crystal structures

T+O+T

TETRAHEDRAL / OCTAHEDRAL MODULESLAYER SILICATES

chloritetalc

mica

+ empty interlayer+ cations

+ O layer

Page 19: tools to model inorganic crystal structures

TOT MODULES AND TECHNOLOGY

PILLARED CLAYS

Page 20: tools to model inorganic crystal structures

MODULES IN REAL STRUCTURES

talc

ph

phengite

Page 21: tools to model inorganic crystal structures

MICA (module M) BAFERTISITE (module B)

ASTROPHYLLITE (B1M1)NAFERTISITE (B1M2)

HETEROPHYLLOSILICATESA row of Ti polyhedra periodically substitutes a row of Sitetrahedra in a TOT layer. Three types of HOH layers are

known. BmMn polysomatic series.

+ Ti octahedra (pyramids) =

Page 22: tools to model inorganic crystal structures

MEMBERS OF THE BmMn SERIES

B1M0 bafertisite

Ba2{(Fe,Mn)4[Ti2O2(O,OH)2Si4O14](O,OH)2}

B1M1 astrophyllite

(K,Na)3(Fe,Mn)7[Ti2O3Si8O24](O,OH)4

I2+nY4+3n[Ti2(O)2+pSi4+4nO14+10n](O)2+2n

B1M2 nafertisite

(Na,K,�)4(Fe2+,Fe3+,�)10[Ti2O3Si12O34](O,OH)6

Page 23: tools to model inorganic crystal structures

HOH MODULES AND TECHNOLOGYPILLARED HETEROPHYLLOSILICATES?

Page 24: tools to model inorganic crystal structures

PALYSEPIOLES

sepiolite palygorskite kalifersite

Indigofera suffruticosa

+

Page 25: tools to model inorganic crystal structures