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HAL Id: jpa-00231231

https://hal.archives-ouvertes.fr/jpa-00231231

Submitted on 1 Jan 1976

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Fine structure in a smectic stepped drop

J. van der Veen, H.B. Haanstra

To cite this version:

J. van der Veen, H.B. Haanstra. Fine structure in a smectic stepped drop. Journal de Physique

Lettres, Edp sciences, 1976, 37 (3), pp.43-44. �10.1051/jphyslet:0197600370304300�. �jpa-00231231�

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L-43

FINE STRUCTURE IN A SMECTIC STEPPED DROP

J. VAN DER VEEN and H. B. HAANSTRA

Philips

Research Laboratories

Eindhoven,

The Netherlands

(Re~u

le 1 er decembre 1975,

accepte

le

8 janvier 1976)

Résumé. - Dans une goutte à gradins de p, p’-di-n-nonyl azoxybenzène, la présence des petits gradins est visible grâce à la

microscopie

électronique. La hauteur de ces gradins

correspond

à la

distance réticulaire trouvée par diffraction des rayons X.

Abstract. - In a

stepped

drop of p, p’-di-n-nonyl azoxybenzene in the smectic A phase, the

presence of small steps can be made visible, using electron

microscopy.

The height of these steps

corresponds

to the

interplanar spacing

as found by X-ray diffraction.

LE JOURNAL DE PHYSIQUE - LETTRES TOME 37, MARS 1976,

Classification

Physics Abstracts

0.691 - 0.692 - 7.130 - 7.180

In

liquid crystals

there is a

long-range

orientational

ordering.

The molecules are, on average,

aligned

with their

long

axes

parallel

to a

preferred

direction.

In the nematic

phase

the centers of mass of the mole- cules are distributed at random. In the smectic A

phase

the centers of mass are

arranged

in

layers.

These

layers

have a thickness of the order of the molecular

length

and are

perpendicular

to the pre- ferred direction. The distribution of the centers of

mass is

again

random within the

layers.

A small amount of a substance in the smectic A

phase

on a substrate can

give

a so-called

stepped

FIG. 1. - Scanning electron micrograph of a stepped drop of

p, p’-di-n-nonylazoxybenzene. Magnification 100 x.

drop.

The

drop

does not have a smooth surface but consists of a series of terraces that terminate in a

sharp step

or

edge.

These

steps

are not of

equal height

and

comprise

many smectic

layers,

as was

FIG. 2. - Transmission electron micrograph of a carbon replica

of the stepped drop. Magnification 195.000 x.

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyslet:0197600370304300

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L-44 JOURNAL DE PHYSIQUE - LETTRES

found

by Grandjean [1].

In this letter we report on the fine structure of these steps.

Stepped drops

of p,

p’-di-n-nonylazoxybenzene (K

45o

SA

76.5~ I

[2])

can be undercooled to room

temperature quite easily.

A

photograph

of such a

stepped drop

is shown in

figure

1. The

edges

are

distinctly

visible and we wondered whether a fine structure could be made visible with the aid of elec- tron

microscopy.

In order to have sufficient resolu-

tion,

the thickness of the

sample

should not exceed

about 0.1 pm. For such a thin

sample

the intensive electron

bombardment,

necessary for a

high magni- fication,

causes too

high

a

temperature.

Therefore a

replica

was made. First a

shadowing material,

for

which carbon was

chosen,

was

evaporated

onto the

stepped drop,

at an

angle

of 30° with the substrate.

Then the

replica material, again carbon,

was

applied

on the

rotating specimen

at an

angle

of 45~. After

dissolving

the azoxy

compound

in acetone a

replica

of very low

graininess

was obtained. The

study

of

this

replica

revealed very small

steps

as shown in

figure

2. The

height

of these

steps

is of the order of 30

A, corresponding

to an estimated molecular

length

of 32.8

A (from

a

Dreiding stereomodel).

We

also

investigated

the smectic

phase by X-ray

diffrac-

tion with Cu Ka radiation and found an

interplanar spacing

of 33.7

A.

We conclude that with the aid of electron

microscopy

a fine structure,

consisting

of very small

steps,

can be made visible in a smectic A

stepped drop.

The

height

of these small

steps corresponds approximately

to the molecular

length.

We wish to thank Mr. H. C. Donkersloot for

recording

the

X-ray

diffraction

pattern.

References

[1] GRANDJEAN, F., C. R. Hebd. Séan. Acad. Sci. 166 (1917) 165.

[2] VAN DER VEEN, J., DE JEU, W. H., WANNINKHOF, M. W. M.

and TIENHOVEN, C. A. M., J. Phys. Chem. 77 (1973) 2153.

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