• Aucun résultat trouvé

THE PAIR Π-ELECTRON CORRELATION OF THE SUPERCONDUCTING TYPE IN THE COMPLEX MOLECULES

N/A
N/A
Protected

Academic year: 2021

Partager "THE PAIR Π-ELECTRON CORRELATION OF THE SUPERCONDUCTING TYPE IN THE COMPLEX MOLECULES"

Copied!
3
0
0

Texte intégral

(1)

HAL Id: jpa-00217634

https://hal.archives-ouvertes.fr/jpa-00217634

Submitted on 1 Jan 1978

HAL is a multi-disciplinary open access

archive for the deposit and dissemination of

sci-entific research documents, whether they are

pub-lished or not. The documents may come from

teaching and research institutions in France or

abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est

destinée au dépôt et à la diffusion de documents

scientifiques de niveau recherche, publiés ou non,

émanant des établissements d’enseignement et de

recherche français ou étrangers, des laboratoires

publics ou privés.

THE PAIR Π-ELECTRON CORRELATION OF THE

SUPERCONDUCTING TYPE IN THE COMPLEX

MOLECULES

V. Kresin

To cite this version:

(2)

JOURNAL DE PHYSIQUE Colloque C6, suppliment au no 8, Tome 39, aozit 1978, page ~ 6 - 4 7 9

THE P A I R II-ELECTRON CORRELATION OF THE SUPERCONDUCTING TYPE I N THE COMPLEX MOLECULES

V.Z. Kresin

Moscow Correspondance PedagogicaZ Institute, U.S.S.R.

RQsum6.- Nous considBrons les corr6lations de paires des Qlectrons n et le mdcanisme de cette corrl- lation. On peut expliquer les propridtds optiques et magndtiques de moldcules complexes par cette cor- rdlation. Nous discutons les transitions tunnel S-N dans les processus Blectrochimiques et le trans- port des Blectrons dans les membranes biologiques.

Abstract.- We consider the pair correlation of a-electrons. The mechanisms of pair correlation is dis- cussed. Optical and magnetic properties of complex molecules can be explained by this correlation. S-N tunnel transitions in the electrochemical processes and electron transfer in the biological men-

brains are discussed.

Some large molecules are characterized by the the number of a-electrons is odd.

presence of a large number of T-electrons. For exam- The pair correlation has also an important ple the aromatic compounds, the biological active effect on the magnetic properties of the large mole- molecules always contain a-electrons/l/. These col- cules since it gives rise to the observed anomalous

lectivized a-electrons move in the field of the diamagnetism of the n-electron systems. We found a-core, which is formed by the ions and by noncollec- the paramagnetic susceptibility in the direction

tivized a-electrons. perpendicular to the plane of the molecules :

a-electrons form the finite Fermi-system and their properties can be described by the methods of theory of finite ~ermi-s~stems/2/.

The present report deals with the pair correla- tion in the a-electron system. We have discussed this problem in/3/ and we are going report here some new results.

It's worth noting that the pair correlation ta- kes place in a number of Fermi systems (superconduc- tivity in the metals, pair correlation of nucleons in atomic nuclei). a-electrons and nucleons both form the finite Fermi-systems.

The pair correlation mechanisms in n-electron systems are analogous to superconducting mechanisms. This effect is due to the interaction of a-electrons with a-core. The main role play the virtual

n-u

-

electrons transitions.

What properties are due to the effect's of pair correlation ? At first, there is energy gap in the molecules, which contain even number of n-electrons. It's clear enough that a large n-electron-system should have approximately equidistant energy levels (it's a quasiclassical system). However the spectrum of the even-number a-electron-system displays a big disproportion. Namely, the energy difference between the ground state and the first excited state is much greater than this one between the first and se- cond states. The levels are equidistant only when

One can conclude that X ip'<xlp, A=O A=O

'

Van- Vleck's paramagnetism). The effects of pair corre- lation depress the paramagnetism. It leads to the anomalous diamagnetism.

There following simple relation :

X I D

= yap ; y

"

cF/4mc2 ,a

-

the component of the

-

P

electric susceptibility in the direction lying in the plane of molecule. This relation can be verified experimentally.

Energy gap decreases in the strong magnetic field. In this case 6A % .'H Such dependence was

observed in /4/. It is worth noting that this effect should have an opposite sign in the absence of pair correlation.

Let's consider now the tunnel effects. S-N- transitions are observed in the electrochemical reactions. The oxidation of aromatic molecules re- presents the tunnel transition of n-electrons from molecule to the electrode. Thanks to the correlation effect it is possible to observe by definite volta- ge simultaneous transition of two electrons. This effect was really observed in the experiments.

The charge transfer in the biological mem- brains represents another example of tunnel effects.

(3)

We consider the movement of two T-electrons through the row of aromatic molecules, The distance between

References

molecules is definite. The pair correlation is the / l / Pullman,B., Pullman,A., Quantum Biochemistry cause of the ~ h a s e coherence in a-electron system. (Interscience, N.Y.) 1963

Such a coherence leads to the Josephson tunnel ef- /2/ Migdal,A., Theory of Finite Fermi System and Application to Atomic Nuclei (Interscience,N.Y)

fect in the biological membrains. ( 1 967)

/3/ Kresin,V., Litovchenko,V., Panasenko,A., J. Chem. Phys.,

63

(1975) 3613

141 Canters,W., U a. Mol. Phys.

E

(1972) 1203

Références

Documents relatifs

sufficient to consider the pair formation process in a uniform transversal field in the presence of incohe- rent multiple scattering described by formulae (4).. and

sufficient to consider the pair formation process in a uniform transversal field in the presence of incohe- rent multiple scattering described by formulae (4).. and

Only for some of those rare earth iron compounds, in which the rare earth atoms have their total moment coupled antiparallel to the iron moment, a compensation

There is one feature of al1 the studies cited above that involve geometries in which (low frequency) surface modes are present. When on writes down the magnon

All aspects of the structure of a molecule can be changed by pressure, but the largest changes will often occur to the internal rotation angles because the forces preventing

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

- It is shown how the free energy can be constructed as functional of the one-body distribution function and the exact statistical-mechanical stability condition is

Additionally single excitations were allowed in the rest of the vlrtual space by combining 3h-2v in the valence plus the complete 2h-lp space (referred as 3h-2v+2h-lp), or