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SUPPORTING INFORMATION PERYLENE-DIIMIDE-CYSTEINE DERIVATIVES SELF-ASSEMBLED ONTO (111) GOLD SURFACE: EVIDENCE OF ORDERED AGGREGATION. E.Kozma 1 , F.Galeotti 1 , G.Grisci 1 , L.Barba 2 , G. Arrighetti 2 , M. Catellani 1 , G.Scavia 1 , W.Porzio 1 (*) 1 Istituto per lo studio delle Macromolecole del CNR via E. Bassini 15 20133 Milano Italy 2 Istituto di Cristallografia-Sincrotrone Elettra, Strada Statale 14-Km 163,5 Area Science Park, 34149 Basovizza, Trieste, Italy

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SUPPORTING INFORMATION

PERYLENE-DIIMIDE-CYSTEINE DERIVATIVES SELF-ASSEMBLED ONTO (111) GOLD SURFACE: EVIDENCE OF ORDERED AGGREGATION.

E.Kozma1, F.Galeotti1, G.Grisci1, L.Barba2, G. Arrighetti2 , M. Catellani1, G.Scavia1, W.Porzio1(*)

1Istituto per lo studio delle Macromolecole del CNR via E. Bassini 15 20133 Milano Italy2Istituto di Cristallografia-Sincrotrone Elettra, Strada Statale 14-Km 163,5 Area Science Park, 34149

Basovizza, Trieste, Italy

Figure S1. a) 2D GIXD pattern of PDI-Cys/AUEV film immersed in 0.1 mM solution for 48 h.

The red arrows indicate Au-crystal spacings. Intensity is represented as a function of the

transferred momentum components Qxy and Qz. b) Preferential orientations and relative intensity

of [111] and [002] Au rings are evidenced in this screenshot of Fit2d graphic window. This was the

software employed to extract profiles from the patterns and the integration limits are evidenced in

the two images.

Figure S2. Height images of AUEV after 48h PDI-Cys deposition

Figure S3. PDI-Cys/AUAN height images at different deposition times at 6 h (a, b,c) , 24 h (d,e,f)

and 48 h (g,h,i).

Figure S4. OP profiles of Au films onto silicon substrate: annealed (thick line), as deposited by

thermal evaporation (dotted line).

Figure S5. XRD OP profiles extracted from 2D images taken from a PMI-Cys/Au film

immersed in 0.1 mM solution for 48h, at different incidence angles (°) as indicated in different

curves.

A) B)

Figure S6. GIWAXS profiles of A) PDI/Au and B) PMI/Au cast films extracted from 2D

patterns: OP profiles (thick line), and IP profile (thin line). Vertical bars indicate typical d-spacing

denoting molecular packing (see text). High angle peaks (25°-27° 2-theta) are attributed to the

substrate impurities.

Figure S7. GIWAXS profiles extracted from 2D patterns of PDI-Cys on annealed Au cast film,

very thin (~20 nm), OP (red line), IP (blue line). Vertical bars indicate orders of main spacing

related to molecular -stacking. Higher angles peaks have been attributed to Silicon substrate

impurities.

Figure S8. Sketch of possible model of PDI-Cys molecular stacking onto annealed Au surface,

as derived from molecular modeling using MATSTUDIO [3]. Note the shift of adjacent molecules to

allow acceptable intermolecular contacts.

Table 1s. D-spacings and crystallite size, derived from OP and IP profile extracted by 2D images of

both PMI-Cys/Au and PDI-Cys/Au measured films.

PDI-Cys

Sample Profile

OP

IP

Immersion time 6h 24h 48h 6h 24h 48h

Au untreated - 0.98/25 a 1.0/20; 1.1/18

0.73/16; 0.685/13

0.457/30 0.465/10 0.476- 0.457b

Au annealed 0.71/20 0.71/22 0.71/24 - - -

0.71 nm

PMI-Cysc

Sample Profile OP IP

Immersion time 24h 48h 24h 48h

Au untreated - 1.06/9 - -

Au annealed 0.71/10 0.71/24 - -

a The values are expressed in nm. The former indicated d-spacing and the latter corresponding

crystallite size (L) along with the crystallographic direction estimated according to [1,2]. bAt least three peaks are detected which widths yield, after deconvolution, L<10 nm. cDue to molecule poor solubility only larger immersion times were reported, as the smaller one

gave barely detectable effects.

Line profile analysis can be applied only if more orders of same crystallographic direction are

detected. Presently the Hosemann approximation was adopted, 1,2 namely the parameters

considered were the lattice fluctuation factor defined as g(hkl) = (d2 (hkl)/d(hkl)

2- 1) 1/2, indicating the

standard deviation of d(hkl) evaluated over more orders of the considered crystallographic direction

(CD), and non uniform strain indicated by rms = (e2)1/2 , where e = δd(hkl)/d(hkl), defined as root

mean square of the lattice variations in the sample.

Only in case of out-of-plane profiles of for both PMI-Cys/Au and PDI-Cys/Au annealed films,

immersed for long time (48 h), the analysis could supply values of g(100/200) and rms parameters: i.e.

0.026 and 0.007 for PMI , and 0.0075 and 0.002 for PDI respectively.

REFERENCES

[1] A. M. Hindeleh, R. Hosemann, Microparacrystals – the intermediate stage between crystalline

and amorphous. J. Mater. Sci. 1991, 19 , 5127–36 and ref. therein.

[2] S. Enzo, G. Fagherazzi, A. Benedetti, S. Polizzi , A profile-fitting procedure for analysis of

broadened X-ray-diffraction peaks. 1. Methodology, J. Appl. Cryst. 1988, 21, 536–540.

[3] MATSTUDIO modeling release 4.0, Accelrys Inc. 9685 Scranton Rd. San Diego CA (USA) 2003

(www.accelrys.com).