COMMUNICATIONS
tion.[6] In these experiments, the electrochemical sensorÐ
usually a microdisk electrode with a tip diameter of a few
micrometersÐhas to be positioned in close proximity to the
object. The approach of the microelectrode to the biological
object is, in general, performed under control of an optical
microscope using manual- or piezo-actuated micromanipula-
tors for positioning of the sensor tip. The electrode is slowly
moved towards the cell until it slightly touches the cell
membrane, which is visualized by its bending. The tip is then
retracted for a defined distance allowing, in principal, adjust-
ment of the membrane-to-electrode distance within a range of
several hundred nanometers to two micrometers. Although
this approach has been successfully used in recent years,[3]
there are significant drawbacks, such as a) possible contam-
ination of the electrode surface due to its contact with the cell
membrane, b) insufficient reproducibility of the tip-to-cell
distance, which becomes even more difficult using smaller
microelectrodes, that are hardly visible in the optical micro-
scope, c) eventual deterioration of the cell at the contact point
or mechanical depolarization of the cell, and d) the impossi-
bility to investigate sequentially different spots on the same
cell.
After initial investigations of biological samples by means
of scanning electrochemical microscopy (SECM),[7] attempts
have been recently undertaken to visualize the metabolism
and the redox activity of individual cells.[8] However, one of
the major problems in conventional SECM experiments is the
constant z-height of the microelectrode, which does not allow
differentiation between variations in the tip-to-sample dis-
tance and changes of the local electrochemical activity. In
order to overcome these limitations, we have introduced a
shear-force based constant-distance control into the SECM.[9]
The benefits and limitations had been described in detail
recently.[10] In short, the microelectrode vibrates at its
resonance frequency with typical amplitudes of only a few
nanometers with use of a piezo-pusher. Simultaneously, a
laser beam is focused onto the very end of the vibrating
electrode and the resulting Fresnel diffraction pattern is
projected onto a split photodiode. Amplitude and phase
information about the vibrating tip is obtained by the
amplification of the difference signal from the split photo-
diode with respect to the agitation signal using a lock-in
amplifier. With decreasing tip-to-sample distance, increasing
shear forces between tip and sample surface lead to a damping
of the vibration amplitude and to a phase shift, which can be
used to continuously keep a predefined damping value related
to a constant distance of about 50 ± 100 nm by means of a
software-controlled feedback loop.
[5] a) R. C. D. Brown, J. Chem. Soc. Perkin Trans. 1 1998, 3293 ± 3320;
b) A. R. Brown, P. H. H. Hermkens, H. C. J. Ottenheijm, D. C. Rees,
Synlett 1998, 817 ± 827; c) P. H. H. Hermkens, H. C. J. Ottenheijm,
D. C. Rees, Tetrahedron 1997, 53, 5643 ± 5678; d) J. S. Früchtel, G.
Jung, Angew. Chem. 1996, 108, 19 ± 43; Angew. Chem. Int. Ed. Engl.
1996, 35, 17 ± 40; e) F. Balkenhohl, C. von dem Bussche-Hünnefeld,
A. Lansky, C. Zechel, Angew. Chem. 1996, 108, 2436 ± 2502; Angew.
Chem. Int. Ed. Engl. 1996, 35, 2288 ± 2354.
[6] a) D. J. Gravert, K. D. Janda, Chem. Rev. 1997, 97, 489 ± 509; b) U.
Grether, H. Waldmann, Angew. Chem. 2000, 112, 1688 ± 1691; Angew.
Chem. Int. Ed. 2000, 39, 1629 ± 1632.
[7] a) A. Studer, S. Hadida, R. Ferritto, S. Y. Kim, P. Jeger, P. Wipf, D. P.
Curran, Science 1997, 275, 823 ± 826; b) A. Studer, P. Jeger, P. Wipf,
D. P. Curran, J. Org. Chem. 1997, 62, 2917 ± 2924; d) A. Studer, D. P.
Curran, Tetrahedron 1997, 53, 6681 ± 6696; e) J. J. J. Juliette, D.
Â
Rutherford, I. T. Horvath, J. A. Gladysz, J. Am. Chem. Soc. 1999,
121, 2696 ± 2704.
[8] A. G. M. Barret, M. L. Smith, F. J. Zecri, Chem. Commun. 1998,
2317 ± 2318.
[9] Reviews: a) L. F. Tietze, F. Haunert in Stimulating Concepts in
Chemistry (Eds.: F. Vögtle, J. F. Stoddart, M. Shibasaki), Wiley-
VCH, Weinheim, 2000, pp. 39 ± 64; b) L. F. Tietze, U. Beifuû, Angew.
Chem. 1993, 105, 137 ± 170; Angew. Chem. Int. Ed. Engl. 1993, 32,
131 ± 164; c) L. F. Tietze, Chem. Rev. 1996, 96, 115 ± 136; d) L. F.
Tietze, A. Modi, Med. Res. Rev. 2000, 20, 304 ± 322. Further
publications: e) L. F. Tietze, Y. Zhou, Angew. Chem. 1999, 111,
2076 ± 2078, Angew. Chem. Int. Ed. 1999, 38, 2045 ± 2047; f) L. F.
Tietze, Y. Zhou, E. Töpken, Eur. J. Org. Chem. 2000, 2247 ± 2252;
g) L. F. Tietze, J. Bachmann, J. Wichmann, Y. Zhou, T. Raschke,
Liebigs Ann. 1997, 881 ± 886.
[10] a) NaOH (1n), CbzCl, RT, 15 h; b) ROH, camphor sulfonic acid,
reflux, 15 h, quantitative over both stages; c) DIBAL-H (1n in
hexane), CH2Cl2, 788C, 2 h, 60 ± 84%: Y. Tajeuchi, A. Yamada, T.
Suzuki, T. Koizumi, Tetrahedron, 1996, 52, 225 ± 232.
[11] G. Hesse, Methoden Org. Chem. (Houben-Weyl) 4th ed. 1952-, Vol. 6/
1d, 1978, pp. 136 ± 139.
Spatially Resolved Detection of
Neurotransmitter Secretion from Individual
Cells by Means of Scanning Electrochemical
Microscopy
Andreas Hengstenberg, Andrea Blöchl,
Irmgard D. Dietzel, and Wolfgang Schuhmann*
Microelectrochemical methods, especially constant-poten-
tial amperometry and fast-scan cyclic voltammetry,[1] provide
possibilities to investigate biological systems with cellular or
subcellular spatial resolution determined mainly by the size of
the available microelectrodes.[2] Among the biological phe-
nomena studied so far at single cells or substructures of single
cells are individual exocytosis events,[3] oxygen consump-
tion,[4] photosynthetic activity,[5] and ion channel distribu-
Thus, adaptation of the shear-force based constant-distance
control of the tip-to-sample gap to biological preparations at
the single-cell level should, on the one hand, allow the
problems occurring with manual microelectrode positioning
to be overcome and, on the other hand, enable detectable
variations of chemical species at different sites of a biological
preparation.
Using platinum microelectrodes sealed in glass capillaries,
which can be easily positioned over hard sample surfaces
using the shear-force positioning mode, no satisfying results
could be obtained. In preliminary experiments using adher-
[*] Prof. Dr. W. Schuhmann, Dr. A. Hengstenberg[]
Analytische ChemieÐElektroanalytik & Sensorik
Ruhr-Universität Bochum, 44780 Bochum (Germany)
Fax : (49)234-321-4683
Priv.-Doz. Dr. A. Blöchl, Priv.-Doz. Dr. I. D. Dietzel
Lehrstuhl für Molekulare Neurobiochemie
Ruhr-Universität Bochum, 44780 Bochum (Germany)
[ ] Present address:
BioCurrents Research Center (NIH:NCRR)
Marine Biological Laboratory
7 MBL Street, Woods Hole, MA 02543 (USA)
Angew. Chem. Int. Ed. 2001, 40, No. 5
ꢀ WILEY-VCH Verlag GmbH, D-69451 Weinheim, 2001
1433-7851/01/4005-0905 $ 17.50+.50/0
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