Self-assembling, patterning and SPR imaging of a 1,3 alternate bis(dipyridyl)calix[4]arene derivative-Cu2+ complex immobilized on to Au(111) surfaces

Article abstract of DOI:10.1039/b408326c

The electrochemically switchable Cu²⁺ complex of a 1,3 alternate bis(dipyridyl)calix[4]arene derivative forms self-assembled monolayers on Au(111) surfaces. The receptor is patterned on the surface by using microcontact printing procedures and the resulting surface is imaged via SPR.

Full text of DOI:10.1039/b408326c

Self-assembling, patterning and SPR imaging of a 1,3 alternate
bis(dipyridyl)calix[4]arene derivative–Cu2+ complex immobilized on to
Au(111) surfaces†
Giuseppe Arena,*a Annalinda Contino,a Elisa Longo,a Carmelo Sgarlata,a Giuseppe Spoto*a and
Valeria Zitob
a Dipartimento di Scienze Chimiche, Università di Catania, Viale Andrea Doria 6, 95125, Catania, Italy.
E-mail: garena@dipchi.unict.it; gspoto@dipchi.unict.it; Fax: +39 095 337678
b Istituto di Biostrutture e Bioimmagini, Sezione di Catania, C.N.R., Viale Andrea Doria 6, 95125, Catania,
Italy
Received (in Columbia, MO, USA) 16th March 2004, Accepted 21st May 2004
First published as an Advance Article on the web 20th July 2004
The electrochemically switchable Cu2+ complex of a 1,3
alternate bis(dipyridyl)calix[4]arene derivative forms self-as-
sembled monolayers on Au(111) surfaces. The receptor is
patterned on the surface by using microcontact printing
procedures and the resulting surface is imaged via SPR.
The modified surface was studied by using polarization modula-
tion infrared reflection–absorption spectroscopy (PM-IRRAS).11
Fig. 2b and 2c show the CH stretching region (3000–2800 cm21) of
the PM-IRRAS spectra of the CBPS modified Au(111) surface and
of the same surface after a 60 minute immersion into Cu(ClO4)2
0.001 mol dm23 ethanol solution, respectively. The IR transmission
spectrum of the CBPS solution is also shown for comparison (Fig.
2a). All the spectra show peaks attributed to the asymmetric and
symmetric stretching vibration modes of the –CH2– and –CH3
groups of the CBPS receptor. The 2918 cm21 and 2849 cm21 bands
detected in the PM-IRRAS spectrum of the anchored CBPS (Fig.
2b), which are assigned to the –CH2– asymmetric (nas) and
symmetric (ns) stretching mode, respectively, are indicative of a
well-ordered, all-trans conformation of the alkyl chains present in
the SAM formed by the CBPS receptor.12 The changes induced by
Cu2+ interaction with the CBPS monolayer are reflected by the
shifts detected by PM-IRRAS. The bands at nas = 2927 cm21 and
at ns = 2856 cm21, assigned to the –CH2– stretching modes of the
Cu2+ complex of the CBPS monolayer (Fig. 2c) are indicative of a
liquid-like, less-ordered conformation of the alkyl moieties.12 Such
conclusions are also supported by the position of the IR
transmission peaks of the CBPS in CHCl3 solution. The bands
assigned to the –CH2– stretching modes in solution (nas = 2926
cm21, ns = 2855 cm21) are virtually superimposable with those
observed in the PM-IRRAS spectrum of the Cu2+ complex of the
CBPS monolayer and well agree with the expected position for the
–CH2– stretching bands of liquid-like (less-ordered) alkyl
chains.12
The experience so far accumulated in the field of molecular devices
has demonstrated that the ability to switch a molecular property is
of relevance to the design and development of new nanodevices.1,2
Metal complexes have been shown to act as switches, which can be
operated through external inputs.3 The anchoring of new metal
complexes showing switchable properties on to solid supports is
thus a fundamental step toward incorporating a molecular switch
into a solid-state device.
Here we report on the characterization of a Au(111) surface
modified with an electrochemically switchable Cu2+ complex of
25,27-bis(1-propyloxy)-26,28-bis(2,2A-dipyridyl-6-methoxy)calix-
[4]arene in the 1,3 alternate conformation (CBP).4,5 The
[Cu(CBP)]2+ complex has been already shown to undergo a quasi-
reversible one-electron redox process in CH3CN solution.5 This
process is characterized by a difference between the cathodic and
anodic peak potential (DEp = 110 mV; sweep rate: 100 mV s21
;
reference electrode: silver/silver nitrate; background electrolyte:
0.1 mol dm23 tetrabutylammonium perchlorate)5 that, although
larger than the theoretical value, is well below the value (180 mV)
that is considered a limit value for a reversible process;6 both the
anodic over cathodic peak current ratio (ipa/ipc = 0.9), close to
unity, and the linearity of ip vs. the square root of the sweep rate (R
=
0.998)5 further indicate that [Cu(CBP)]2+ may be quasi-
The above reported results confirm that CBPS forms well
ordered SAMs on Au(111) surfaces. SAMs anchored on to solid
surfaces are still able to complex Cu2+ ions even though the
complexation increases the disorder of the SAMs.
In view of the fact that electrochemically switchable metal ion
complexes anchored on to solid surfaces can find practical
reversibly reduced.
Two dialkyl sulfide moieties were introduced into CBP to yield
a receptor (25,27-bis[12-(thiododecyl)undecyloxy]-26,28-bis(2,2A-
dipyridyl-6-methoxy)calix[4]arene 1,3 alternate, CBPS) (see ESI†)
that would easily self-assemble on to Au(111) surfaces.7 Fourier
transform–surface plasmon resonance (FT-SPR) was employed to
check whether the immobilized receptor was still able to complex
Cu2+.8 Fig. 1 shows two representative sensorgrams obtained when
pumping a Cu(ClO4)2 1 3 1024 mol dm23 ethanol solution over the
bare gold surface and the CBPS self-assembled monolayer,
respectively. In the experiments pure ethanol was pumped before
and after the Cu(ClO4)2 solution. Whilst the baseline goes back
virtually to its initial position when the experiment is carried out
with a bare gold surface (Fig. 1a), it shifts by some 60 cm21
,
corresponding to a change in the refractive index of Dn = 3.6 3
1024,9 when pumping pure ethanol over the CBPS monolayer after
the Cu(ClO4)2 solution (Fig. 1b). This results from the interaction
of Cu2+ ions with the anchored CBPS receptor. It is noteworthy that
non-specific interactions between the Cu(ClO4)2 and the bare gold
surface do not cause significant changes in the FT-SPR response
(Fig. 1a).
† Electronic supplementary information (ESI) available: procedures for the
synthesis of CBPS, 1H NMR data. See http://www.rsc.org/suppdata/cc/b4/
b408326c/
Fig. 1 FT-SPR sensorgrams obtained by pumping a Cu(ClO4)2 1 3 1024
mol dm23 ethanol solution over a bare gold surface (A) and the CBPS
monolayer (B).
1812
C h e m . C o m m u n . , 2 0 0 4 , 1 8 1 2 – 1 8 1 3
T h i s j o u r n a l i s © T h e R o y a l S o c i e t y o f C h e m i s t r y 2 0 0 4

applications only if a spatial control of their distribution on to the
surface is achieved, we patterned gold surfaces by depositing our
systems. Microcontact printing (mCP) of SAMs has been proposed
as a method for patterning organic molecules on to solid supports at
scales > 1 mm.13 This procedure was used to pattern the CBPS
receptor on to Au(111) surfaces.14 The patterned surfaces were
imaged by using SPR imaging.15 A representative SPR image of the
CBPS patterned Au(111) surface is shown in Fig. 3. SPR results
show that CBPS may be patterned on to the surface in an ordered
manner with relative ease and speed.
In conclusion we have shown that the CBPS receptor, whose
parent (CBP) compound can be reversibly reduced in solution,
forms well-ordered SAMs on Au(111) surfaces. CBPS is still able
to complex Cu2+ ions, thus providing a system that can be
electrically operated; to this end, studies are under way to check
whether the Cu2+ complex of the CBPS still works within a real
microelectronic device. In addition, we have shown that the CBPS
system may be patterned on to a gold surface by mCP procedures
and that the patterned surface may be imaged by SPR much faster
than it is usually accomplished via other surface-sensitive imaging
techniques.
MIUR is acknowledged for partial financial support.
Notes and references
1 V. Balzani, A. Credi and M. Venturi, Molecular Devices and Machines,
Wiley-VCH, Weinheim, 2003.
2 Molecular Switches, ed. B. L. Feringa, Wiley-VCH, Weinheim, 2001.
3 (a) V. Amendola, L. Fabbrizzi, M. Licchelli, C. Mangano, P.
Pallavicini, L. Parodi and A. Poggi, Coord. Chem. Rev., 1999, 190–192,
649; (b) S. Sortino, S. Petralia, S. Conoci and S. Di Bella, J. Am. Chem.
Soc., 125, 2003, 1122.
4 G. Arena, A. Contino, E. Longo, D. Sciotto, C. Sgarlata and G. Spoto,
Tetrahedron Lett., 2003, 44, 5415.
5 R. P. Bonomo, personal communication.
6 A. M. Bond, Modern Polarographic Methods in Analytical Chemistry,
Marcel Dekker, New York, 1980.
7 CBPS monolayers were prepared by immersing the gold substrates in a
1022 mol dm23 ethanol–chloroform (3 : 1, v/v) solution of the receptor
for at least 48 h at 60 °C. The samples were then removed from the
solution and rinsed with large amounts of ethanol and chloroform. All
glassware used in monolayer preparation was cleaned in piranha
solutions (concentrated H2SO4 and 33% H2O2 in a 3 : 1 v/v ratio) and
rinsed with copious amounts of high-purity water (Milli-Q Element
Ultrapure Water) before use. Warning: piranha solutions should be
handled with caution as they can detonate unexpectedly.
8 FT-SPR experiments were carried out by using an FT-SPR 100 (GWC
Instruments, WI) apparatus. The light beam from an external port of a
Nexus 870 FT-IR spectrometer (Nicolet, WI), equipped with a Quartz-
Halogen source and a XT-KBr beam splitter, was used as the near-IR
source of the FT-SPR. Gold substrates (GWC Instruments, WI) were
obtained by thermally evaporating a gold layer (450 Å) on to SF-10
glass slides. Chromium (50 Å) was used as the adhesion layer. Gold
substrates were brought into optical contact with the SF-10 equilateral
prism present in the FT-SPR by using a refractive index matching fluid
(Cargille Laboratories).
9 The FT-SPR sensor response was converted into refractive index
changes by using 10 independent sucrose aqueous calibrating solutions
whose concentration ranged from 0 to 17%. The refractive indexes of
the sucrose solutions were obtained from the literature (ref. 10).
10 Handbook of Chemistry and Physics, 71st edn., ed. D. R. Lide, CRC
Press, Boston, 1990.
Fig. 2 PM-IRRAS spectra of the monolayer formed from CBPS on gold (B)
and of the same monolayer after Cu2+ ion complexation (C) in the
3000–2800 cm21 spectral region. The IR transmission spectrum of the
CBPS in solution (A) is shown for comparison.
11 PM-IRRAS experiments were conducted on a Nicolet Nexus 870,
equipped with a PM-IRRAS external unit. The polarization was
achieved by using a wire-grid polarizer and modulated by using a 50
kHz ZnSe photoelastic modulator (PEM-90, Hinds Instruments, OR).
The IR beam was collected by a BaF2 lens and focused on to an MCT
detector, after reflection at grazing angle (83°) from the gold surface.
The signal was demodulated by a Synchronous Sampling Demodulator
(GWC Instruments, WI) to measure the differential intensity of p- and
s-polarized IR radiations. The reported normalized differential re-
flectance spectra results from the average of 1000 spectra collected with
a resolution of 2 cm21
.
12 M. D. Porter, T. B. Bright, D. L. Allara and C. E. D. Chidsey, J. Am.
Chem. Soc., 1987, 109, 3559.
13 (a) Y. Xia and G. M. Whitesides, Angew. Chem., Int. Ed., 1998, 37, 550;
(b) Y. Xia, J. A. Rogers, K. E. Paul and G. M. Whitesides, Chem. Rev.,
1999, 99, 1823.
14 Polydimethylsiloxane (PDMS, Sylgard 184, Dow Corning, MI) stamps
were created from patterns (masters) having 200 mm 3 200 mm squares.
The stamp was “inked” with a 0.01 mol dm23 3 : 1 (v/v) ethanol–
chloroform solution of CBPS. Organic microstructures were generated
by bringing the stamp into contact with a clean Au substrate.
15 SPR imaging experiments were carried out by using a SPRimager
(GWC Instruments, WI) apparatus. SPR images were acquired using the
V++ software (Digital Optic, New Zealand) and analyzed by using the
Scion Image Beta 4.02 (Scion Corp., MD) software package.
Fig. 3 Representative SPR image of the CBPS patterned gold surface.
C h e m . C o m m u n . , 2 0 0 4 , 1 8 1 2 – 1 8 1 3
1813