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钌硅颗粒-SI.pdf
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S1
Supporting Information
Dynamically Imaging Collision Electrochemistry of Single
Electrochemiluminescence Nano-Emitters
Cheng Ma, Wanwan Wu, Lingling Li, Shaojun Wu, Jianrong Zhang, Zixuan Chen*
and Jun-Jie Zhu*
State Key Laboratory of Analytical Chemistry for Life Science, School of Chemistry
and Chemical Engineering, Nanjing University, 163 Xianlin Ave, Nanjing 210023,
China
Corresponding Authors: Zixuan Chen and Jun-Jie Zhu
Email: [email protected] and [email protected]
Electronic Supplementary Material (ESI) for Chemical Science.
This journal is © The Royal Society of Chemistry 2018
S2
Table of contents
1. Electrochemiluminescence (ECL) coupled with photoluminescence (PL) microscopy set-up
2. Co-localization analyses of ECL images and SEM images
3. ECL reaction kinetics of individual nanoparticles
ECL reaction mechanisms of individual RuDSNs
Relationship between ECL reaction kinetics and the nature of electrode surface
4. ECL emission on the cell upper surface
5. Stochastic collision nanoelectrochemistry
Random walk of single nanoparticle in the electrode vicinity
Horizontal moving trajectory in the collision process
The different surface modification of nanoparticles and electrodes for studying
sticking collision probability
Spatial distribution of collision intensity and frequency across GC electrode surface
ECL intensity distribution of statistic sticking collision events in the CCD-view
Relay probe based on successive collision events
6. COMSOL simulation for sub-particle ECL pattern analysis
Reactions and parameters for digital simulation
Subdomain setting
Physical fields
Meshes settings
Simulation results
7. Experimental section
Chemicals and general techniques
Preparation and characterization of RuDSNs and RuCSPs
8. Description of the movies
9. References
S3
1. Electrochemiluminescence (ECL) coupled with photoluminescence (PL) microscopy set-up.
Figure S1. (a) Schematic illustration of the ECL microscopy setup. Application of a voltage to the work electrode resulted in the ECL emission
of RuDSNs, which was collected by a water-immersion objective of high numerical aperture. The diverging light was focused by the imaging
lens and then was imaged on the EMCCD. (b) Schematic illustration of the PL microscopy setup, which was established based on the ECL
microscope with a light source and filters. The setup used a white light source (mercury lamp) and an Ex filter for excitation light generation.
A dichroic mirror was used to prevent the excitation light from entering the camera. The PL of RuDNSs penetrated an Em filter and then was
imaged on the EMCCD.
Figure S2. Co-localization of the PL image and the ECL image of a same set of RuDSNs. (a) The PL image of the RuDSNs on the GC
electrode. (b) The corresponding ECL image of the same set of RuDSNs. The potential was cyclically scanned from 0 to 1.4 V (vs. Ag/AgCl
reference electrode) at a scan rate of 100 mV/s. The exposure time of EMCCD was 1 s for ECL and PL imaging. Scale bars (white), 20 µm.
a
b
a
b
S4
2. Co-localization analyses of ECL images and SEM images.
Figure S3. (a,c,e) Typical zoom-in ECL images of the RuDSNs on the GC electrode surface. The potential was cyclically scanned from 0 to
1.4 V (vs. Ag/AgCl reference electrode) at a scan rate of 100 mV/s. The exposure time of EMCCD was 1 s. (b,d,f) The corresponding SEM
images of the same set of particles as in (a,c,e). Insets showed the detailed morphologies of RuDSNs numbered with 1-4.
3. ECL reaction kinetics of individual nanoparticles
ECL reaction mechanisms of individual RuDSNs: As shown in Figure 2, when the electrode potential was
scanned beyond 0.7 V, the enhancement of the oxidation current suggested that the direct oxidation of coreactant
TPA occurred,
[1]
which was confirmed by the controlled trials (Figure S4). Then, the initial ECL signal started following
the oxidation of TPA and reached a maximum at 0.87 V. It should be pointed out that the potential of this ECL peak
was too negative to directly oxidize RuDSN@Ru(bpy)
3
2+
to RuDSN@Ru(bpy)
3
3+
, which can be further reduced by
TPA free radicals to form emitter RuDSN@Ru(bpy)
3
2+
*. The ECL signal that was observed herein was attributed to
the “revisited” route involving both TPA cation radicals (TPA
•+
) and TPA free radicals (TPA
•
):
[2]
TPAH
+
⇌ TPA + H
+
(1)
TPA – e → TPA
•+
(2)
TPA
•+
→ TPA
•
+ H
+
(3)
TPA
•
+ RuDSN@Ru(bpy)
3
2+
→ P
1
+ RuDSN@Ru(bpy)
3
+
(4)
TPA
•+
+ RuDSN@Ru(bpy)
3
+
→ TPA + RuDSN@Ru(bpy)
3
2+
* (5)
RuDSN@Ru(bpy)
3
2+
* → RuDSN@Ru(bpy)
3
2+
+ hv (6)
Where TPAH
+
is Pr
3
NH
+
, TPA
•+
is Pr
3
N
•+
, TPA
•
is Pr
2
NC
•
HCH
2
CH
3
, P
1
is Pr
2
N
+
=CHCH
2
CH
3
.
a
b
c
d
e
f
S5
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
0
50
100
150
200
250
300
Current (A)
E (V vs Ag/AgCl)
Bare GC electrode
SiO
2
particles
RuDSNs
TPA
RuDSNs+TPA
Figure S4. CV curves of bare GC electrode (black line), GC electrode immobilized by either silica nanoparticles (red line) or RuDSNs (blue
line) in PBS buffer, and bare GC electrode (green line) and GC electrode immobilized by RuDSNs (purple line) in PBS buffer containing 100
mM TPA coreactant. The potential was cyclically scanned from 0 to 1.4 V at a scan rate of 20 mV/s.
As the potential continues to scan beyond 0.87 V, the ECL intensity of the nanoparticles starts to decrease,
although the oxidation current increases and then reaches a peak at 1.05 V. The contravention between the ECL
emission intensity and the oxidation current is attributed to direct anodic oxidation of TPA
•
at the electrode interface.
[1,
3]
It is noteworthy that we observe a small ECL peak at 1.19 V. It derives from the direct oxidation of Ru(bpy)
3
2+
inside
the nanoparticle based on the electron tunnelling/hopping mechanism,
[4]
which is consistent with the oxidation
current of Ru(bpy)
3
2+
(Figure S5). This phenomenon is supported by the numerical simulated result reported by
Paolucci and co-workers.
[2a]
RuDSN@Ru(bpy)
3
2+
– e → RuDSN@Ru(bpy)
3
3+
(7)
TPA
•
+ RuDSN@Ru(bpy)
3
3+
→ P
1
+ RuDSN@Ru(bpy)
3
2+
* (8)
RuDSN@Ru(bpy)
3
3+
+ RuDSN@Ru(bpy)
3
+
→ RuDSN@Ru(bpy)
3
2+
* + RuDSN@Ru(bpy)
3
2+
(9)
This is the first time that the ECL emission by the electron tunnelling and hopping mechanism at single-
nanoparticle level is observed, although the “revisited” route is verified by imaging the ECL profile in single
microbeads as well as SECM-ECL experiments.
[2b, 2c]
It is noteworthy that the ECL-potential curve can accurately
reveal specific electrochemical reaction without the interference from the charge-discharge current, side reactions
and water decomposition reaction, which are inevitable in traditional CV measurements. In addition, as illustrated in
Figure 2m, the ECL-potential curve shows a zero background signal from the blank electrode substrate during the
entire ECL process, which demonstrates the high accuracy and sensitivity for imaging local electrochemical reactions
by our ECL microscopy.
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
-50
0
50
100
150
200
Current (A)
E (V vs. Ag/AgCl)
Ru(bpy)
3
2+
in PBS buffer
1.12 V
Figure S5. CV curve of 400 µM Ru(bpy)
3
2+
in 100 mM PBS buffer. Work electrode: GC electrode. The potential is cyclically scanned from 0
to 1.4 V at a scan rate of 100 mV/s.
Relationship between ECL reaction kinetics and the nature of electrode surface: A crucial point in the efficiency
of the ECL generation is the chemical and physical state of the electrode surface where the ECL process is initiated.
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