Elsevier

Organic Electronics

Volume 1, Issue 1, December 2000, Pages 49-56
Organic Electronics

Influence of deposition temperature on the structure of 3,4,9,10-perylene tetracarboxylic dianhydride thin films on H-passivated silicon probed by Raman spectroscopy

https://doi.org/10.1016/S1566-1199(00)00008-2Get rights and content

Abstract

Raman spectroscopy was used to characterize the structural order in thin organic films of 3,4,9,10-perylene tetracarboxylic dianhydride (PTCDA). Films of the same average thickness were grown by organic molecular beam deposition on hydrogen-passivated p-type silicon (1 0 0) substrates at different growth temperatures between 230 and 470 K. The Raman spectra of all samples exhibit four external vibrational modes, that occur as a consequence of the arrangement of the PTCDA molecules in a crystalline environment. The full width at half maximum of these phonon lines decreases with increasing temperature of the substrate during deposition. A similar tendency is also observed for the Raman-active internal molecular modes. In addition, with increasing deposition temperature the diffusely scattered light background in the Raman spectra increases, as well as the photoluminescence background in the high frequency range. We relate the observed spectral changes to an increase in the size of the crystalline domains within the films with increasing deposition temperature, an effect that is macroscopically reflected by an enhanced degree of surface roughness. The different quality of the crystalline PTCDA domains was also complementary revealed by X-ray diffraction measurements.

Introduction

Thin films of organic semiconductors have already proved a great potential for optoelectronic devices [1]. Progress has greatly benefited from controlled film deposition under clean ultra-high vacuum (UHV) conditions: organic molecular beam deposition (OMBD). Additional potential for future applications lies in combining organic and inorganic semiconductors for electronic devices. Device performance will markedly be influenced by the degree of structural order in the organic films which to a large extent controls the electronic properties (such as carrier mobilities) as well as the optical ones. The structural order itself is expected to depend critically on the growth parameters, in particular on the substrate temperature.

The film formation properties of the archetype organic molecule 3,4,9,10-perylene tetracarboxylic dianhydride (PTCDA) on a variety of inorganic substrates have already been studied by a number of experimental and theoretical methods [1], [2], [3], [4]. The most commonly used substrate materials have been weakly interacting ones, such as metals (e.g. Ag and Au), highly oriented pyrolytic graphite, and insulators (NaCl, SiO2, Al2O3) [1], while investigations using the more reactive surfaces of more common inorganic semiconductors such as silicon and gallium arsenide have been scarce.

On clean GaAs(1 0 0) [5] or Si(1 0 0) [6] surfaces a strong chemical interaction occurs between the anhydride groups of the molecules at the interface and the substrate, predominantly with the dangling bonds and defects. This usually results in the formation of small crystalline domains, in nearly random azimuthal orientation. Improved structural order is observed when reactive semiconductor substrate surfaces are passivated, e.g. by reaction with chalcogen or hydrogen atoms in the case of GaAs and Si substrates, respectively. The passivation induces a reduction of chemically active sites mainly by saturating dangling bonds [7]. Hence the work to be presented here concentrates on the deposition of PTCDA on hydrogen terminated Si(1 0 0), for the latter see [8]. Substrate temperature is a further important parameter that can control structural order. It was indeed already observed by X-ray diffraction (XRD) that the crystallite size drastically increased as temperature was raised from 320 to 370 K [9] when PTCDA was deposited on Si(1 0 0) wafers with natural oxide.

We have previously demonstrated that Raman spectroscopy is a versatile tool to characterize PTCDA films [10], [11]. Raman spectra provide information on the internal vibrational modes of PTCDA molecules as well as on external vibrational modes (phonons). The latter were detected for all films deposited on passivated semiconductor substrates at frequencies between 40 and 125 cm−1. These Raman active modes are of rotational–vibrational (libronic) origin in the PTCDA molecular crystal which has monoclinic symmetry (space group C2h5) with two molecules per unit cell (for a detailed discussion see [12]).

The first Raman study of the influence of substrate temperature on the growth process of PTCDA films on hydrogen-passivated (H-passivated) (1 0 0) oriented silicon surfaces to be reported here, reveals marked changes in the PTCDA phonon spectra. These changes can be correlated with the degree of structural order using additional XRD data.

Section snippets

Experimental

PTCDA films were grown on p-type (1 0 0) oriented silicon substrates by OMBD. The organic source material purchased from Lancaster was purified twice by sublimation at 575 K under high vacuum (10−6 Pa). To clean and passivate the surface, substrates were wet-chemically treated under atmospheric conditions. The first step of the chemical treatment consists of a 2 min etching in hydrofluoric acid (HF, 40%) to remove the silicon oxide and the organic contaminants, and thereafter H-passivate the

Results

The PTCDA evaporation rate used in our experiments leads to film deposition only when the substrate temperature is below 470 K. The film colour varied from bluish green for the sample grown at 230 K to reddish brown for that at 410 K. The film topography observed with an Olympus Microscope (objective magnification 100) was mirror-like for the films grown on substrates at RT and below, but for elevated temperatures a granular structure occurred. A similar observation was already reported by

Raman spectroscopy

In Section 3 we have described the differences observed in the Raman spectra for PTCDA films deposited at various substrate temperatures. These results will be related in this section to a structural model.

Using LEED, AES and total current spectroscopy we have recently observed that PTCDA forms islands on H-passivated Si(1 1 1) substrates [18] when deposited at RT. Assuming the same growth mode for PTCDA on Si(1 0 0), the presence of the PTCDA phonon bands in the Raman spectra reveal the

Summary

PTCDA films with an average thickness of 40 nm were grown on H-passivated Si(1 0 0) by OMBD at four different substrate temperatures: 235, 295, 360, 410 K. At higher temperatures no PTCDA deposition was observed for the evaporation rate of 3 Å min−1 used.

Raman spectra of the films were recorded in situ after the growth was completed. In the spectra of all samples we observe the presence of four external vibrational modes characteristic of the PTCDA molecular crystal. The FWHM of these phonon lines

Acknowledgements

This research was supported by the Graduiertenkolleg “Dünne Schichten und nichtkristalline Materialien” at Technische Universität Chemnitz, and by the EU funded Human Potential Research Training Network DIODE (contract no.: HPRN-CT-1999-00164).

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