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ESI
Stable high-voltage aqueous pseudocapacitive energy storage device with slow self-discharge
Hemesh Avireddy1, Bryan W. Byles3,4, David Pinto3,4, Jose Miguel Delgado Galindo1, Jordi Jacas Biendicho1, Xuehang Wang3,4, Cristina Flox1, Olivier Crosnier5,6, Thierry Brousse5,6, Ekaterina Pomerantseva3,4, Joan Ramon Morante1,2, Yury Gogotsi3,4
1IREC, Catalonia Institute for Energy Research. Jardins de les Dones de Negre 1, 08930. Sant Adrià de Besòs, Spain.2Faculty of Physics, University of Barcelona, Barcelona, Spain3Department of Materials Science & Engineering, Drexel University, Philadelphia, PA 19104, USA4A.J. Drexel Nanomaterials Institute, Drexel University, Philadelphia, PA 19104, USA5Institut des Matériaux Jean Rouxel (IMN), CNRS UMR 6502-Université de Nantes, 2 rue de la Houssinière BP32229, 44322, Nantes Cedex 3, France6Réseau sur le Stockage Electrochimique de l’Energie, FR CNRS 3459, 80039 Amiens Cedex, France
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10 20 30 40 50 60 70
0010008006004
002
103110
109107
105
004 101
104
Inte
nsity
(a.u
)
2
Ti3C2
Ti3AlC2
002
Fig. S1. XRD pattern of titanium aluminum carbide (Ti3AlC2) MAX and titanium carbide (Ti3C2) MXene.
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7 μm
60 μm
a
b
10 μm
c
Coun
ts (a
.u)
Coun
ts (a
.u)
Coun
ts (a
.u)
Energy (keV)
Energy (keV)
Energy (keV)
Fig. S2. SEM image and corresponding EDS spectra of (a) titanium aluminum carbide (Ti3AlC2)
MAX, (b) titanium carbide (Ti3C2) MXene and (c) α-MnO2
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-1.6 -1.4 -1.2 -1.0 -0.8 -0.6 -0.4 -0.2 0.0-1.0
-0.8
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
1.0
E 1 m = E+ - E- = -0.1 V - (- 1.1 V) = 1.0 V
C.E. % = 93 %C.E. % = 94 %
21.9 mAh g-1 (79 Fg-1)
I (A
g-1)
Ewe vs SCE
1 m Potassium acetate 21 m Potassium acetate
Scan rate: 5 mV s-1
32 mAh g-1
(77 Fg-1)
E 21 m = E+ - E- = -0.1 V - (- 1.6 V) = 1.5 V
1 m potassium acetate 21 m potassium acetate
-1.8 -1.7 -1.6 -1.5 -1.4 -1.3 -1.2-1.0x10-1
-8.0x10-2
-6.0x10-2
-4.0x10-2
-2.0x10-2
0.0
I (m
A)
Ewe vs. SCE (V)
a
b
Fig. S3. (a) Cyclic voltammogram of the Ti3C2 Mxene in 1 m (red curve) and 21 m of potassium
acetate electrolyte solution (scan rate: 5 mVs-1). (b) Cyclic voltammogram of a glassy carbon
electrode in 1 m (red curve) and 21 m of potassium acetate electrolyte solution (scan rate 2 mVs-
1).
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21 m at -0.35 vs SCE 30 m at -0.5 vs SCE
0.4 0.8 1.2 1.6 2.0-1.6
-1.2
-0.8
-0.4
0.0
0.79
log
I (m
A)
log (mV s-1)
0.91
-1.4 -1.2 -1.0 -0.8 -0.6 -0.4 -0.2-8
-6
-4
-2
0
2
4
6
8
I (A
g-1)
Ewe vs SCE
2 mVs-1
5 mVs-1
10 mVs-1
20 mVs-1
50 mVs-1
100 mVs-1
21 m
-1.4 -1.2 -1.0 -0.8 -0.6 -0.4 -0.2-8
-6
-4
-2
0
2
4
6
8
I (A
g-1)
Ewe vs SCE
2 mVs-1
5 mVs-1
10 mVs-1
20 mVs-1
50 mVs-1
100 mVs-1
30 m
a
b
c
Fig. S4. Cyclic voltammogram in various scan rates for the Ti3C2 Mxene in (a) 21 m and (b) 30
m of potassium acetate electrolyte solution (scan rates : 2, 5, 10, 20, 50 and 100 mVs-1). (b) Log
plot of current versus scan rate of cyclic voltammograms measured from the Fig. S4a and b.
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Fig. S5. Cyclic voltammogram of a glassy carbon electrode (CHI instruments) in 21 m potassium acetate electrolyte at a scan rate of 2 mV s-1
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0 20
25
50
75
2.4 V
0 20
25
50
75
2.3 V
0 20
25
50
75
1.5 V
0 20
25
50
75
2.5 V
0 20
25
50
75
1.6 V
0 20
25
50
75
1.7 V
0 20
25
50
75
1.8 V
0 20
25
50
75
1.9 V
0 20
25
50
75
2.0 V
0 20
25
50
75
2.1 V
0 20
25
50
75
2.2 V
Curr
ent d
ensit
y (m
A g-1
)
Time (h)
Fig. S6. Voltage-hold tests in asymmetric Ti3C2 // α-MnO2 cell. Voltage-hold tests indicate a slight evolution of parasitic current at 2.3 V. Beyond that, leakage current start to decrease, which implies the breakdown of the cell.
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-1.6 -1.2 -0.8 -0.4 0.0 0.4 0.8 1.2-200
-100
0
100
200
Cur
rent
den
sity
(mA
g-1)
Ewe vs SCE (V)
Ti3C2 MXene MnO2
0.0 0.5 1.0 1.5 2.0
-100
0
100
200
Cur
rent
den
sity
(m
A g
-1)
Ecell (V)
before hold test after hold tests
After 2.5 V hold tests
-1.6 -1.2 -0.8 -0.4 0.0 0.4 0.8 1.2-200
-100
0
100
200
Cur
rent
den
sity
(mA
g-1)
Ewe vs SCE (V)
Ti3C2 MXene MnO2
a
b
c
Fig. S7. Cyclic voltammogram of (a) Ti3C2 // α-MnO2 cell before and after hold tests at 2.5 V for 2 h. Cyclic voltammogram of both individual electrodes at 5 mV s-1 (b) before and (c) after hold tests. Extension of the cell voltage to 2.5 V widens the MnO2 electrochemical potential window.
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0.0 0.5 1.0 1.5 2.0
0.8
1.0
E v
s S
CE
(V)
Time (h)
at 2.2 V hold test at 2.5 V hold test
0.0 0.5 1.0 1.5 2.0-1.6
-1.5
-1.4
E v
s S
CE
(V)
Time (h)
at 2.2 V hold test at 2.5 V hold test
alpha-MnO2
Ti3C2
a
b
Fig. S8. Evolution of potential during hold tests for (a) α-MnO2 and (b) Ti3C2 electrode.
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0 20 40 60 80 100 120 140 160 1800.0
0.5
1.0
1.5
2.0
E c
ell (
V)
t (s)
0.25 Ag-1
0.5 Ag-1
0.75 Ag-1
1 Ag-1
2 Ag-1
Fig. S9. Charge and discharge curve of Ti3C2 // α-MnO2 asymmetric supercapacitor in 21 m
potassium acetate at different current densities (weight of both electrodes).
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R1 CPE1
R2 W1
Element Freedom Value Error Error %R1 Free(±) 9.836 0.23387 2.3777CPE1-T Free(±) 4.3668E-06 1.7072E-06 39.095CPE1-P Free(±) 0.84903 0.034084 4.0145R2 Free(±) 15.56 0.90682 5.8279W1-R Free(±) 1670 49.217 2.9471W1-T Free(±) 9.599 0.39952 4.1621W1-P Free(±) 0.46661 0.003206 0.68708
Chi-Squared: 0.0020853Weighted Sum of Squares: 0.16891
Data File: c:\users\jjacas\desktop\coses pendents\hemesh\respond to reviewers\transform\total_1.z
Circuit Model File: C:\Users\JJacas\Desktop\coses pendents\hemesh\respond to reviewers\transform\MODEL.mdl
Mode: Run Fitting / Selected Points (0 - 43)Maximum Iterations: 100Optimization Iterations: 0Type of Fitting: ComplexType of Weighting: Calc-Modulus
a b
c
1.4 V 1.5 V 1.6 V 1.7 V 1.8 V 1.9 V 2.0 V 2.1 V 2.2 V
0 1000 2000 3000 40000
1000
2000
3000
4000
Ti3C2Tx // MnO2
-Img.
Z (O
hm)
Real Z (Ohm)
0 500 10000
500
1000
d
datafit
datafit
Fig. S10. (a) Impedance data show a high frequency semicircle with an inclined spike
of ~45° at intermediate frequencies, (b) Open circuit or capacitive behavior at even
lower frequencies, (c) Equivalent circuit used for the fitting and (d) Nyquist plot at different
voltages for the Ti3C2 // α-MnO2 cell. Inset shows the impedance behavior at the knee frequency.
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Fig. S11. Capacitance over scan rate performance of YP-50 // YP-50 and Ti3C2 // α-MnO2 cell in
21 m potassium acetate electrolyte.
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Figure 8: Different tunnels structures used in the present study
0.0 0.5 1.0 1.5 2.0-100
-50
0
50
100C
urre
nt d
ensi
ty (m
A g
-1)
Ecell (V)
Before hold tests
After 25 hr hold test
Scan rate: 5 mVs-1
0 5 10 15 20 250
5
10
Cur
rent
den
sity
(mA
g-1)
Time (hr)
0 5 10 15 20 250.80
0.75
Ew
e (
MnO
2) v
s S
CE
Time (hr)
0 5 10 15 20 25-1.45
-1.40
Ece
(Ti 3C
2Tx)
vs S
CE
Time (hr)
a b c
dFig. S12. Cyclic voltammogram of the Ti3C2 // α-MnO2, before and after 25 h hold tests at 2.2 V
in 21 m potassium acetate electrolyte. Current is normalised to the mass of both the electrodes.
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0 5 10 15 20 250.80
0.79
0.78
0.77
0.76
0.75
Ew
e (
MnO
2) vs
SC
E (V
)
Time (h)
0 5 10 15 20 25-1.45
-1.44
-1.43
-1.42
-1.41
-1.40
Ece
(Ti 3C
2) vs
SC
E (V
)
Time (h)
a
b
Fig. S13. Evolution of potential during long term hold tests for (a) α-MnO2 and (b) Ti3C2
electrode at 2.2 V for 25 h in 21 m water-in-salt potassium acetate electrolyte.
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10 100 1000
1
10E
nerg
y (m
Wh
cm-3)
Power (Wh cm-3)
AC // MnO2 in 21 m LiTFSI AC // AC in 31 m LiTFSI AC // AC in 7 m LiTFSI AC // AC in 21 m KoAC Ti3C2 // MnO2 in 21 m KoAC
Fig. S.14. Ragone plot showing the correlation between the volummetric energy and power
density between the asymmetric cell of Ti3C2 // α-MnO2 and YP-50 // YP-50. The observed
volumetric energy density of Ti3C2 // α-MnO2 cell (16.80 mWh cm-3 at 137 mW cm-3) is higher
than the existing supercapacitors based on water-in-salt electrolytes, such as and AC // MnO2 in
21 m Li-TFSI [1] (10 mWh cm-3 at 44 mW cm-3 mWh cm-3), AC // AC in 7 m Li-TFSI [2] (6
mWh cm-3 at 49 mW cm-3) and AC // AC cell in 31 m Li-TFSI (8 mWh cm-3 at 57 mW cm-3
mWh cm-3 at 137 mW cm-3).AC : Activated carbon; LiTFSI: lithium bis(trifluromethane)-
sulfonimide; KoAc: potassium acetate
References:
[1] A. Gambou-Bosca, D. Bélanger, Electrochemical characterization of MnO2-based composite in the presence of salt-in-water and water-in-salt electrolytes as electrode for electrochemical capacitors, J. Power Sources. 326 (2016) 595–603. doi:10.1016/j.jpowsour.2016.04.088.
[2] P. Lannelongue, R. Bouchal, E. Mourad, C. Bodin, M. Olarte, S. le Vot, F. Favier, O.
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Fontaine, “Water-in-Salt” for Supercapacitors: A Compromise between Voltage, Power Density, Energy Density and Stability, J. Electrochem. Soc. 165 (2018) A657–A663. doi:10.1149/2.0951803jes.
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