• Aucun résultat trouvé

Spin dephasing in the excited triplet state of F+ -center pairs in CaO

N/A
N/A
Protected

Academic year: 2021

Partager "Spin dephasing in the excited triplet state of F+ -center pairs in CaO"

Copied!
2
0
0

Texte intégral

(1)

HAL Id: jpa-00220052

https://hal.archives-ouvertes.fr/jpa-00220052

Submitted on 1 Jan 1980

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.

Spin dephasing in the excited triplet state of F+ -center pairs in CaO

R. Hond, M. Glasbeek

To cite this version:

R. Hond, M. Glasbeek. Spin dephasing in the excited triplet state of F+ -center pairs in CaO. Journal

de Physique Colloques, 1980, 41 (C6), pp.C6-540-C6-540. �10.1051/jphyscol:19806142�. �jpa-00220052�

(2)

JOURNAL DE PHYSIQUE Colloque C6, supplkment au no 7 , Tome 41, Juillet 1980, page C6-540

Spin dephasing in the excited triplet state of F+-center pairs in CaO

R.

Hond and

M.

Glasbeek

Laboratory for Physical Chemistry, University of Amsterdam, Nieuwe Achtergracht 127, Amsterdam, The Netherlands

Abstract.

-

Spin coherence decay in the photo-excited 3B, state of exchange-coupled F+-center pairs in CaO is studied utilizing techniques for the optical detection of spin echoes and spin locking. The homogeneous dephasing time is shown to decrease rapidly with increasing (low) magnetic field strengths. The phenomenon arises because H induces a magnetic moment within the triplet spin system and as a result dipolar spin-spin interactions become increasingly important in the dephasing processes. As the temperature is raised from 1.5 K up to 10 K, the spin- echo decay shapes are changed from exponential to Gaussian whereas the dephasing time, TM, is increased from 150 ps up to 300 ps. The results are related to existing spectral diffusion theories.

DISCUSSION

Question. - B.

HENDERSON.

lity you mention : (i) the magnetic field dependence.

Can you be sure that dipolar interactions between of the de~hasing shows that coupling is to S =

3

F:

centres and excited F-centres in triplet states do spins, (ii) optically detected cross relaxation also not contribute to the spin dephasing time. shows that coupling is to

S

=

4

centres, (iii) F+-centres are abundant, whereas compared to this the concen- Reply.

-

M .

GLASBEEK.

tration of photo-excited F-centres is negligible.

For a number of reasons we can neglect the possibi-

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19806142

Références

Documents relatifs

Also shown are the calculated projected phase space factor in solid curves. The difference between this curve and the

•=r- = f (Ln v) for the concentration and frequency dependence of the freezing temperature T f clearly indicates the role of the dipolar anisotropy on the freezing of

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

Sample characterisation of PDA and AXT, details of optical pulse compression, effect of temperature, pump fluence and pump energy on the pump-probe spectra of PDA and AXT,

The authors used triphenylene-2,4,10-tricarboxamide derivatives, whose supramolecular chirality is biased to get either P- or M-helices when using chiral solvents.(Mondal et

distribution of the y-rays emitted by the stopped nuclei, by using a thick F2Ba target to stop the recoil-. ing

interaction and its variation with strain which contri- bute to all the five parameters A, ..., 9 ; (ii) cross terms involving direct effect of T2g strains on the

It is obviously interesting to compare this wealth of theoretical results with the greatest number of available experimental data, in order to see if Harker’s theory