Presentation is loading. Please wait.

Presentation is loading. Please wait.

Molecular Chemistry versus Solid State Physics

Similar presentations


Presentation on theme: "Molecular Chemistry versus Solid State Physics"— Presentation transcript:

1 Molecular Chemistry versus Solid State Physics
vacuum state / undisturbed conjugation neutral solution / free radical positive solition / carbocation ( carbenium ion ; carbonium ion) negative soliton / carbanion positive polaron / radical cation negative polaron / radical anion positive bisolition (bipolaron) / carbodication negative bisolition (bipolaron) / carbodianion Frenkel exciton (bound electron-hole pair) / exited state

2 Pi-conjugated systems. Electron transfer and donor-acceptor compounds
Between two molecules with different electron affinity, charge redistribution can take place, anywhere from zero charge to a full electron transfer from one to the other. Charge transfer of anywear from zero charge to one electron charge. Electron transfer means what it literally says: a hole electron is transferred.

3 Smalley, Kroto and Curl 1985

4 1996 Nobel Prize in Chemistry
Curl Jr Kroto Smalley During an intense working week in the autumn of 1985, Robert Curl, Harold Kroto and Richard Smalley made the completely unexpected discovery that the element carbon can also exist in the form of very stable spheres. They termed these new carbon balls fullerenes. The carbon balls are formed when graphite is evaporated in an inert atmosphere. Usually they contain 60 or 70 carbon atoms. A new carbon chemistry has developed around these spheres. It is possible to enclose metals and noble gases in them, to form new superconducting materials with them and to create new organic compounds and polymeric matter for them. The discovery of the fullerenes shows how unexpected and fascinating results can be created when scientists with different experience and research objectives collaborate. An idea from outer space Kroto's special interest in red giant stars rich in carbon led to the discovery of the fullerenes. For years, he had had the idea that long-chained molecules of carbon could form near such giant stars. To mimic this special environment in a laboratory, Curl suggested contact with Smalley who had built an apparatus which could evaporate and analyze almost any material with a laser beam. During the crucial week in Houston in 1985 the Nobel laureates, together with their younger co-workers J. R. Heath and J. C. O'Brien, starting from graphite, managed to produce clusters of carbon consisting mainly of 60 or 70 carbon atoms. These clusters proved to be stable and more interesting than long-chained molecules of carbon. Two questions immediately arose. How are these clusters built? Does a new form of carbon exist besides the two well-known forms graphite and diamond? Fig 1. Schematic drawing of Smalley's cluster apparatus for the laser evaporation of graphite. The carbon clusters are formed in the helium gas flow and then analysed with mass spectrometry. Fig 2. The read-out from the mass spectrometer shows how the peaks corresponding to C60 and C70 become more distinct when the experimental conditions are optimised. Autumn 1985

5 Buckminster Fullerene
1967 World Exhibition in Montreal Spherical building by R. Buckminster Fuller For the 1967 World Exhibition in Montreal the architect R. Buckminster Fuller designed a spherical building which 18 years later gave the clue to the structure of the carbon clusters. He used hexagons and a small number of pentagons to create "curved" surfaces. This year's Nobel Prize laureates assumed that the cluster of 60 carbon atoms - C60 - consists of 12 pentagons and 20 hexagons with carbon atoms at each corner, the same form as a European football. They called the new carbon ball, C60, buckminsterfullerene. In colloquial English the carbon balls became "buckyballs". In Ancient Greece the regular polyhedra symbolised the different elements, earth, air, fire, water, and the universe. The cube was the symbol of earth and the icosahedron the symbol of water. The form of C60 (and a soccer ball) can be derived from an icosahedron in which the corners have been cut off - a truncated icosahedron. Graphite is soft and black and the stable, common form of carbon. Diamond is hard and transparent and the unusual form of carbon. In diamond each carbon atom is bound to four other carbon atoms in a regular repetitive pattern. The density is 3.51 g/cm3. In graphite the carbon atoms are located at the corners of regular and fused hexagons arranged in parallel layers. Its density is considerably lower, 2.26 g/cm3. icosahedron truncated European football graphite diamond icosahedron

6 Fullerene: Introduction
We know a whole family of fullerenes (ranging from C60 to ~ C100), ‘unions’ (concentric carbon spheres of various shapes and sizes) carbon nanotubes (CNT’s, bucky tubes), long, cigar-shaped all-carbon macromolecules that come in a variety of forms and shapes single wall SWCNT’s multi-wall MWCNT’s chiral and achiral All of these new forms have in common that they are constructed from five and six-membered rings of sp2-hybridized carbon atoms The geometrical structure of a fullerene must have exactly 12 pentagonal faces, but may have any number (except 1) of hexagonal faces. Fullerenes are described by the general chemical formula C20+2H where H is the number of hexagonal faces.

7 Fullerene: Production
Total Synthesis Approaches Fullerene generation by vaporization of graphite or by combustion of hydrocarbons is very effective and certainly unbeatable what facile production in large quantities is concerned. However, total synthesis approaches are attractive because (a) specific fullerenes could be made selectively and exclusively (b) new endohedral fullerenes could be formed (c) heterofullerenes (d) other cluster modified fullerenes could be generated using relate synthesis protocols Conversion og cyclophane into C60 in the gas phase in laser desorption mass spectrometry Synthesis of circumtrindene, representig 60% of C60 Generation of C60 by cyclodehydrogenation of polyarene

8 Larger quantities Fullerenes in quantities Five years after the discovery of the fullerenes, the astrophysicists D. R. Huffmann and W. Krätschmer and their co-workers managed to produce fullerenes in larger quantities. When two rods of graphite are heated to a high temperature by an electric arc discharge in an atmosphere of helium at a pressure of 13 kPa the graphite rods are slowly consumed and soot is formed. Approximately 10% of the soot is made of C60 and C70. The soot is collected and treated with benzene to dissolve the fullerenes, which can then be separated using chromatographic methods. Hoffmann in Arizona and Kratchmer in Heidelberg in 1990 Resistive heating of graphite Arc Heating of Graphite Inductive heating of graphite and other carbon sources (acetylene) Pyrolyses of hydrocarbons ( naphtalene)

9

10 C60 is a strong electron acceptor.
Fullerene: Chemistry One can draw resonance structures for fullerene C60 . Nevertheless only one structure really represents it most appropriately: the one which all c=c double bonds are in the hexagons. The hexagons are much better be considered as cyclohexatrienes than as benzene rings. C60 is a strong electron acceptor.

11 face centered cubic arrangement
Structure C60 2 types of bonds 180 Å3 1.38 Å 20 hexagons = 12 pentagons 1.45 Å Deviation from planarity Crystal lattice face centered cubic arrangement M. Prato J. Mater. Chem. 1997, 7, 1097.

12 Properities of Bucky Balls
Bandgap of 1.68ev C60 (purple) Bandgap of 1.76ev C70 (red) Strong absorptions between 190 and 410 Unique optical properties C60 decay very easily to low lying triplet state No reorganization energy….accelarates charge separation and hence long lived states (optical limiter and lubricant, MRI contrast reagent)

13 Functionalisation exohedral endohedral ‘outside’ ‘inside’
Ce, Gd,Eu,Nd,Sm,Tb,Ho

14 Fullerene: Chemistry 1,2 additions
DBU

15 Fullerene: Chemistry 1,3 additions

16 Fullerene: Chemistry 1,3 additions (Prato addition)
There are almost no limitations for R2 For the α-amino acid derivative, R1=H is not possible

17 Fullerene: Chemistry 1,3 additions (diazomethane addition)
In-situ formation of diazo compounds from tosylhydrazones

18 Fullerene: Chemistry 1,3 additions (diazomethane addition)

19 Fullerene: Chemistry 1,3 additions (addition of azides)
Azides react in the same way as the diazo compounds, however, the reaction stops at the [5,6]-adduct. Theoretical investigations indicate stepwise mechanism in which the cleavage of the N-N single bond precedes the breaking of the C-N bond During extrusion of N2 the steric effect of the leaving N2 molecule prevents the addition of the nitrene substituent to the [6,6] bond and forces the addition to an adjacent [5,6] ring junction.

20 Fullerene: Chemistry Grignard addition

21 Fullerene: Chemistry Diels Alder additions
C60 is the dienophile, a reactive one since it is electrophilic. At elevated temperatures, the reaction is reversible. This seriously limits its applications The monoadducts can be isolated at low temperature The monoadduct cannot be isolated

22 Fullerene: Formation of bis-adducts
After the first addition, there are still 29 double bonds left in the C60 fragment, these bonds are still reactive. The reaction is usually stopped before it goes to completion, to get a maximum yield of the mono-adduct. The second addition to one of the other C=C bonds give rise to various isomeric adducts.

23

24 Photovoltaics Bandgap of 1.68ev C60 Bandgap of 1.76ev C70

25

26

27

28

29

30

31

32

33

34

35

36

37

38

39

40

41

42

43 Nanotube Biosensor

44

45

46

47

48

49

50

51

52

53 Pi-conjugated systems. Color and Charge transport
In -conjugated molecules, the frontier orbitals (HOMO and LUMO) are related to the -electron system. Therefore the color of the molecules is primarily determined by the HOMO-LUMO gap. Especially when it comes to the design of -conjugated polymers, a set of parameters influencing the band-gap can be defined. The intrinsic band-gap of an isolated conjugated polymer chain can be described as a combination of contributions of energies, related to 1 bond length variation 2 resonance stabilization energy 3 inter-ring torsion angle 4 inductive or resonance effect from substituents Eg=Er+RE+E+ER

54 Pi-conjugated systems. Color and Charge transport
Hopping of the charge from one molecule to another. ( the electronic overlap between a charged molecule and a neutral neighbor) The way the charge is delocalized inside a molecule is of importance. Speaking physics, charge transport means transport of either an electron or a hole. For chemists it is essential to realize this is very different from moving the charges or electrons involved in cations, anions, or free radicals. Example: if a charge is to hop from a (carbo) cationic molecule to a neighboring neutral analogue, this would have to happen through proton transfer instead of an electron hopping from one to the other.


Download ppt "Molecular Chemistry versus Solid State Physics"

Similar presentations


Ads by Google