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Supporting information for
MoS2 Nanosheets Decorated Ni3S2@MoS2 Coaxial Nanofibers: Constructing an Ideal
Heterostructure for Enhanced Na-Ion Storage
Jin Wanga,b
, Jilei Liu
b, Hao Yang
c,d,*,
Dongliang Chao
b, Jiaxu Yan
b, Serguei V. Savilov
e,
Jianyi Linf and Zexiang Shen
a,b,*
a Energy Research Institute (ERI@N), Interdisciplinary Graduate School, Nanyang
Technological University, Research Techno Plaza, 50 Nanyang Drive, 637553, Singapore
b Division of Physics and Applied Physics, School of Physical and Mathematical Sciences,
Nanyang Technological University, 21 Nanyang Link, 637371, Singapore
c School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou, 221116
Jiangsu, P.R. China
d Jiangsu Key Laboratory of Advanced Laser Materials and Devices, Jiangsu Normal
University, Xuzhou, 221116 Jiangsu, P.R. China
e Department of Chemistry, M. V. Lomonosov Moscow State University, Moscow 119991,
Russia
f Energy Research Institute (ERI@N), Nanyang Technological University, 50 Nanyang Drive,
637553, Singapore
E-mail: [email protected] (Z.X. Shen)
E-mail: [email protected] (H. Yang)
Keywords: molybdenum sulfide, Ni3S2, graphene, core/shell, sodium ion batteries
2
Materials and Methods
Growth of Ni/Graphene foams: The growth of Ni/graphene foams (Ni/GF) was achieved by chemical
vapor deposition (CVD) using First Nano's EasyTube 3000 System with a modified recipe as our
previous reported method.[1]
In a typical process, nickel foams with a size of 8×8 cm were directly
used as the scaffold templates and were loaded into a 5 in. quartz tube inside a horizaontal tube
furnace. Then, the furnace was heated to 1000 oC under Ar (500 sccm) plus H2 (200 sccm) atmosphere
and stayed at the peak temperature for 5 min in order to clean the nickel foam surfaces and eliminate
the thin surface oxide layer. After the annealing procedure, a small amount of CH4 was introduced into
the reaction tube at ambient pressure. The flow rates of CH4, H2, and Ar were 50, 100, and 800 sccm,
respectively. After two min, Ni/GF can be obtained after being rapidly cooled to room temperature at a
rate of ~100 oC min
-1 under a constant flow of Ar (500 sccm) and H2 (200 sccm).
Synthesis of few-layer MoS2 nanosheets decorated elongated core/shell Ni3S2@MoS2 coaxial
nanofibers on Ni/graphene foam: MoS2/Ni3S2@MoS2 nanofibers were prepared using a facile one-step
hydrothermal process. In a typical experiment, the mixed solution was prepared by dissolving 150 mg
of thiourea (NH2CSNH2), 75 mg of sodium molybdate and 0.2 g of Polyvinylpyrrolidone (PVP) in 30
mL of distilled water. Then, this resulting solution was transferred into Teflon-lined stainless steel
autoclave. A piece of Ni/GF with an area of 8 cm2 was immersed into the reaction solution. The
autoclave was then sealed and the hydrothermal reaction was conducted at 200 oC for 12 h. After the
autoclave was cooled down to room temperature, the samples were rinsed with DI water for several
times and then dried in an electric oven at 60 oC for 12 h. The achieved samples were thermally
decomposed in a tube furnace at 400 oC for 2 h under H2/Ar (5:95 v/v) atmosphere with a heating rate
of 10 oC min
−1. For the comparison, the samples were prepared with the same reactant concentration at
200 oC for different reaction time.
The calculation of active materials: For MoS2/Ni3S2@MoS2 nanofibers, the total mass of the active
materials includes the mass of MoS2 and Ni3S2. The mass of Ni3S2 and MoS2 can be exactly calculated
by a FeCl3 etching method. In a typical experiment, the obtained MoS2/Ni3S2@MoS2 electrode was
immersed in a mixed solution of FeCl3 (1M) and HCl (0.5M) for 48 h. Then, the Ni foam can be
removed according to the reaction: Ni + 2FeCl3 → NiCl2+ 2FeCl2. Meanwhile, the Ni3S2 can be
oxidized to NiS2 according to the reaction: Ni3S2 + 4FeCl3 → NiS2+ 4FeCl2 + 2NiCl2, which can also
be demonstrated by the XRD patterns and TEM images of the electrode after etched in a solution of
FeCl3 (Figure S1). Therefore, the calculation of Ni3S2 and MoS2 is described as following: A circular
electrode (MoS2/Ni3S2@MoS2 nanofibers supported on Ni/GF) with a diameter of 12 mm was
immersed in a solution of 1M FeCl3 and 0.5 M HCl for 48 h. The weight decrement (x mg) can be
directly calculated by weighting the electrode before and after etched, which includes the residual Ni
foam and the loss of the element Ni from Ni3S2 to NiS2 (0.488*m(Ni3S2)). Another circular Ni/GF disk
with the same size was immersed in a mixed solution of 1M FeCl3 and 0.5M HCl for 48 h. The weight
of Ni foam (y mg) can be directly calculated by weighting the obtained sample before and after
3
reaction etched in a solution of FeCl3, which is equal to the element Ni in the electrode
(MoS2/Ni3S2@MoS2 nanofibers supported on Ni/GF), including the residual Ni foam and the element
Ni in Ni3S2 (0.732*m(Ni3S2)). Then, the mass of Ni3S2, m=(y-x) mg ×MNi3S2/MNi =(y-x) mg ×
(240/58.8) = 4.08*(y-x) mg, where M is the molecular weight or atomic weight. The mass of MoS2
can be calculated by divided the mass of Ni/GF and Ni3S2 from the mass of MoS2/Ni3S2@MoS2
nanofibers. In order to get an accurate data, we always calculated the weight of MoS2 and Ni3S2 based
on at least five sets of data.
Characterization: The X-ray powder diffraction (XRD) pattern of each sample was recorded on a
Bruke D8 Advance powder X-ray diffractometer using Cu Kα radiation (λ=0.15406 nm). Field
emission scanning electron microscopy (FESEM, Model JSM-7600F, JEOL Ltd., Tokyo, Japan) was
used to characterize the morphologies of the synthesized samples. Transmission electron microscopy
(TEM) images were taken using a JOEL JEM 2100F microscope. Raman spectroscopy was recorded
by Renishaw Raman Microscopy with 2.33 eV (532 nm) excitation laser. The Si peak at 520 cm−1
was
used as a reference to calibrate the wavenumber. The XPS measurements were performed with a VG
ESCALAB 220i-XL system using a monochromatic Al Kα1 source (1486.6 eV). All XPS spectra
were obtained in the constant pass energy (CPA) mode. The pass energy of analyser was set to be 10
eV to have high measurement accuracy. The binding energy scale was calibrated with pure Au, Ag
and Cu by setting the Au 4f7/2, Ag 3d5/2 and Cu 2p3/2 at binding energy of 84.0, 368.3 and 932.7 eV,
respectively. The surface area analysis was conducted using Brunauer-Emmett-Teller (BET) theory
(Micromeritics, ASAP 2020).
Cell Assembly and Electrochemical Measurements: To test the anode performance of all synthesised
materials, CR 2032 coin cells were assembled in an Argon-filled glovebox (Mbraun, Unilab, Germany)
with the as-fabricated MoS2/Ni3S2 hybrid electrode as the working electrode (with diameter of 12 mm,
without any binder or additives). For the fabrication of lithium ion battery, the metallic lithium foil as
the counter-electrode, 1 M LiPF6 in ethylene carbonate (EC)−dimethyl carbonate (DME) (1:1 in
volume) as the electrolyte, and a polypropylene (PP) film (Cellgard 2400) as the separator. For the
fabrication of sodium ion battery, the metallic sodium foil as the counter-electrode, 1M NaPF6 in
ethylene carbonate (EC)−diethyl carbonate (DEC)−fluoroethylene carbonate (FEC) (1:1:0.03 in
volume) as the electrolyte, and glass fiber as the separator. Galvanostatic charging and discharging
tests were conducted using a battery tester (NEWARE) at different current rates. In the measurements,
both theoretical capacities of the composites for LIBs and SIBs were regarded as 1000 mAh g-1
. Cyclic
voltammetry (CV) was performed using an electrochemical workstation (CHI 760D, Chenhua,
Shanghai) from 10 mV to 3 V at a scanning rate of 0.5 mV s-1
. Electrochemical impedance
spectroscopy (EIS) were also carried out with an electrochemical workstation over a frequency range
from 106
Hz to 100 mHz at open circuit potential after two galvanostatic charging and discharging
cycles at 100 mA g-1
.
4
Table S1 A survey of electrochemical properties of MoS2 and Ni3S2 for NIBs.
Electrode
description
1st Specific
capacity
(mAhg-1
)
1st Coulombic
efficiency
Cycling stability Rate performance
MoS2/Ni3S2@Mo
S2 coaxial
nanofiber
(This work)
1045.1 mAh g-1
at 100 mA g-1
77%
462 and 330.8 mA
g−1
after 400
cycles at current
densities of 2 and
5 A g-1
856.8, 778.4, 722.1,
647.1, 578.2, 507.4
and 429.5 mAh g−1
at 100, 200, 500,
1000, 2000, 3000
and 5000 mA g−1
.
MoS2/graphene
paper [1]
520 mAh g-1
at 25 mA g-1
46.2%
218 mAh g-1
after
20 cycles at 25
mA g-1
240 and 214 mAh
g-1
at 25 and 100
mA g-1
MoS2
nanoflowers [2]
243 mAh g-1
at 200 mA g-1
88%
350 mAh g-1
at 50
mA g-1
, 300 mAh
g-1
at 1 A g-1
and
195 mAh g-1
at 10
A g-1
after 20
cycles
200 and 175 mAh
g-1
at 1 and 10 A g-1
MoS2 nanosheets [3]
998 mAh g-1
at 200 mA g-1
41%
386 mA h g-1
at 50
mA g-1
after 100
cycles
350 mA h g-1
at 80
mA g-1
, 305 mA h
g-1
at 160 mA g-1
,
and 251 mA h g-1
at
320 mA g-1
MoS2-graphene
microspheres [4]
797 mAh g-1
at 200 mA g-1
72%
480 mA h g-1
at
200 mA g-1
after
50 cycles
427, 355, 306, 273,
and 234 mA h g-1
at
1, 3, 5, 7 and 10 A
g-1
TiO2@MoS2
nanofibers [5]
985 mAh g-1
at 100 mA g-1
73%
474 mA h g-1
at
100 mA g-1
after
30 cycles
600 mA h g-1
even
at 5 C
MoS2/C
nanospheres [6]
1500 mAh g-1
at
100 mA g-1
44.7%
520 mA h g-1
at
100 mA g-1
after
50 cycles
390 mA h g-1
even
at 2 C
MoS2 embedded
in carbon
nanfibers [7]
854 mAh g-1
at 100 mA g-1
52%
484 and 253 mA h
g-1
at 1 and 10 A
g-1
after 100 cycles
854, 700, 623, 436,
331, 224, 155, and
75 mAh g-1
for
current densities of
0.1, 0.5, 1, 5, 10, 20,
30, and
50 A g-1
MoS2/C
nanofibers [8]
471.2 mAh g
-1
at 100 mA g-1
81.2%
283.9 mA h g-1
at
100 mA g-1
after
600 cycles
283.3, 246.5 and
186.3 mA h g-1
at
0.5, 1 and 2 A g-1
MoS2/graphene
composite [9]
1680 mAh g
-1
at 20 mA g-1
47.6%
340 mA h g-1
at 20
mA g-1
after 100
cycles
MoS2/graphene
microspheres [10]
640 mAh g
-1
at 100 mA g-1
62.5%
340 mAh g-1
at 100 mA g-1
after
50 cycles
230 mA h g-1
at 5 A
g-1
Ni3S2-PEDOT [11]
458 mAh g-1
at 100 mA g-1
83.6%
400 mAh g−1
after
50 cycles at
600mAg−1
600, 503, 408 and
310 mAh g-1
at 150,
300, 600 and 1200
5
mA g-1
Ball-milling of
Ni3S2 powders [12]
420 mAh g-1
at
100 mA g-1
89.5%
342 mAh g−1
after
150 cycles at
100mAg−1
6
Figure S1 (a) XRD patterns, (b) and (c) SEM images, and (d)-(f) TEM images of
Ni3S2@MoS2 electrode after etched in a FeCl3 solution.
10 20 30 40 50 602(deg)
Inte
nsit
y (
a.u
.)
MoS2
CNiS2(a)
(d)
(b) (c)
(e) (f)
1 μm 100 nm
0.69 nm
20 nm 10 nm 1 nm
MoS2 belt
0.27 nm(100)MoS2
7
Figure S2 (a) XRD patterns and (b) Raman spectra of MoS2/Ni3S2 and Ni3S2@MoS2. FESEM
images of (c) MoS2/Ni3S2 and (d) Ni3S2@MoS2
500 1000 1500 2000 2500 3000 3500
Ni3S2Ni3S2
2DG
D
MoS2
Raman Shift (cm-1)
In
ten
sit
y (
a.u
.)
MoS2@Ni3S2
MoS2/Ni3S2
10 20 30 40 50 60 70 802(deg)
Inte
nsit
y (
a.u
.)
MoS2
C
MoS2/Ni3S2
MoS2@Ni3S2
Ni3S2Ni
10 20 30 40 502(deg)
Inte
ns
ity
(a
.u.)
(a) (b)
200 nm
(d)
100 nm
(c)
8
Figure S3 (a) Charge and discharge curves and (b) cycling behavior of pure GF as anode of
SIBs at a current density of 200 mAh g–1
.
0 5 10 15 20 25 30 35
0.5
1.0
1.5
2.0
2.5
3.0 1st
2nd
3rd
(a)
Specific Capacity (mAh g-1
)
Po
ten
tia
l (V
vs.
Na )
0 50 100 150 200
0
5
10
15
20
25
30
35
Cap
acit
y (
mA
h g
-1)
Cycle number
(b)
9
Figure S4 Nyquist plots of MoS2/Ni3S2@MoS2 electrode during 400 charge/discharge cycle
at different cycles. The resistance is simulated using the inset of equivalent circuit model.
0 100 200 300 400
0
100
200
300
400
500
Z' (ohm)
-Z''
(oh
m)
Fresh cell
50 cycle
100 cycle
200 cycle
300 cycle
400 cycle
Rsf
CPE2
WRct
CPE1Ri
10
Figure S5 (a), (b) Representative photograph showing the dimension and flexibility of the
MoS2/Ni3S2@MoS2 electrode. (c) Optical images of the flexible poach SIB. (d) The voltmeter
of the flexible SIB when flat, after flexing once and after flexing for 30 cycles.
Flat After 1 flex cycle After 30 flex cycle Flat after 30 flex cycle
(a) (b) (c)
(d)
Flat After 1 flex cycle After 30 flex cycle Flat after 30 flex cycleFlat After 1 flex cycle After 30 flex cycle Flat after 30 flex cycle
11
Figure S6 SEM images of MoS2/Ni3S2 electrode as anode of SIBs after long-term cycles.
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(a) (b)
10 μm 1 μm