Ji-Jing Xu1, Zhi-Wen Chang1, Yan-Bin Yin1, Xin-Bo Zhang1. 1. State Key Laboratory of Rare Earth Resources Utilization, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P. R. China.
Abstract
The successful development of Li-O2 battery technology depends on resolving the issue of cathode corrosion by the discharge product (Li2O2) and/or by the intermediates (LiO2) generated during cell cycling. As an important step toward this goal, we report for the first time the nanoporous Ni with a nanoengineered AuNi alloy surface directly attached to Ni foam as a new all-metal cathode system. Compared with other noncarbonaceous cathodes, the Li-O2 cell with an all-metal cathode is capable of operation with ultrahigh specific capacity (22,551 mAh g-1 at a current density of 1.0 A g-1) and long-term life (286 cycles). Furthermore, compared with the popularly used carbon cathode, the new all-metal cathode is advantageous because it does not show measurable reactivity toward Li2O2 and/or LiO2. As a result, extensive cyclability (40 cycles) with 87.7% Li2O2 formation and decomposition was obtained. These superior properties are explained by the enhanced solvation-mediated formation of the discharge products as well as the tailored properties of the all-metal cathode, including intrinsic chemical stability, high specific surface area, highly porous structure, high conductivity, and superior mechanical stability.
The successful development of Li-O2 battery technology depends on resolving the issue of cathode corrosion by the discharge product (Li2O2) and/or by the intermediates (LiO2) generated during cell cycling. As an important step toward this goal, we report for the first time the nanoporous Ni with a nanoengineered AuNi alloy surface directly attached to Ni foam as a new all-metal cathode system. Compared with other noncarbonaceous cathodes, the Li-O2 cell with an all-metal cathode is capable of operation with ultrahigh specific capacity (22,551 mAh g-1 at a current density of 1.0 A g-1) and long-term life (286 cycles). Furthermore, compared with the popularly used carbon cathode, the new all-metal cathode is advantageous because it does not show measurable reactivity toward Li2O2 and/or LiO2. As a result, extensive cyclability (40 cycles) with 87.7% Li2O2 formation and decomposition was obtained. These superior properties are explained by the enhanced solvation-mediated formation of the discharge products as well as the tailored properties of the all-metal cathode, including intrinsic chemical stability, high specific surface area, highly porous structure, high conductivity, and superior mechanical stability.
Rechargeable lithium–oxygen
(Li–O2) batteries
have received rapidly growing attention because of their high theoretical
energy density (3,600 Wh kg–1), their ability to
significantly outperform state-of-the-art Li-ion batteries, and their
potential as a promising alternative to gasoline.[1−7] Before the potential of Li–O2 technology can be
fully realized, however, a number of important issues must be addressed,
such as low round-trip efficiency, low rate capability, and a poor
cycle life.[8,9] The primary cause of these problems is the
poor electrochemical/chemical stability of the Li–O2 system, i.e., the highly reactive reduced oxygen species (Li2O2 or its intermediate LiO2) attack
the cathode and electrolyte, resulting in the formation and accumulation
of undesirable byproducts (e.g., Li2CO3) upon
cycling that lead to performance degradation and premature battery
death.[10,11]It has been recently recognized that
the chemical instability of
the battery can be partially overcome by employing a sophisticated
cathode, reducing the discharge/charge overpotentials to alleviate
electrolyte decomposition,[12,13] and enhancing the electrochemical
stability of the cathode to avoid its own decomposition as well as
electrolyte decomposition promoted by the cathode.[14−16] Consequently,
the stability of the Li–O2 system depends on the
availability of chemically stable cathodes. To date, carbon material
has been widely used as a cathode in Li–O2 batteries.[17−21] The high conductivity, light weight, and rich porous structure of
carbon cathodes endow the Li–O2 batteries with a
high specific capacity and superior rate capability. However, carbon
cathodes are unstable in the presence of Li2O2 and/or LiO2 upon charging above 3.5 V, and carbon actively
catalyzes electrolyte decomposition upon discharge and charge, resulting
in poor cycle stability of the Li–O2 batteries and
rendering carbon cathodes unsuitable for these batteries.[22−24] This problem can be solved in principle by replacing carbon with
other noncarbonaceous cathode materials. Very few suitable materials,
including noble metals,[25] metal oxides,[26] metal carbide,[27] MoS2,[28] Ru/TiSi2,[29] CoO/Co,[30] Pt/Co3O4,[31] and RuO2/NiO,[32] have
been used in cathodes to date. Although progress has been achieved
regarding battery stability, the use of these noncarbonaceous cathodes
has some disadvantages. All noble metals are expensive and difficult
to fabricate as a cathode. Most metal oxides suffer from low electrical
conductivity. Especially, the high mass and small surface area of
these noncarbonaceous cathodes destroy the key advantage of high specific
capacity offered by Li–O2 batteries (typically less
than 3000 mAh g–1 even based on the weight of the
catalyst). Designing a porous cathode that simultaneously achieves
a high chemical stability and a superior electrochemical performance
remains a daunting challenge.With the above understanding in
mind, we speculate that a porous
metal material coated with a noble metal in the cathode should offer
many advantages, such as (1) high chemical stability against the harsh
and aggressive environment in Li–O2 batteries, (2)
a combination of the good catalytic activity of noble metals and the
high conductivity of base metal materials, and (3) preservation of
the initial nanoporous structure of the base metal materials with
a high specific surface area to ensure rich catalytic active sites,
fast mass transfer, and abundant void space to house the generated
discharge products. To this end, we first report the design of nanoporous
Ni with a nanoengineered AuNi alloy surface directly attached to Ni
foam (AuNi/NPNi/FNi) as a new all-metal cathode system. Highly porous
NPNi/FNi or FNi acts only as an effective current collector that provides
good electron transport, fast mass transfer, and sufficient void volume
to house the generated discharge product Li2O2. The ultrathin AuNi alloy overlayer attached to the surface acts
as an effective electrocatalyst that promotes the formation and decomposition
of Li2O2. The all-metal cathode design excludes
the side reactions involving carbon. This cathode demonstrates the
reversible formation and decomposition of Li2O2 and has relatively low overpotentials, ultrahigh specific capacity,
and high cycle stability due to its unique design in both structure
and component; the values of these properties are many times higher
than those of the noncarbonaceous cathodes previously reported.[25−32]
Results and Discussion
Structural Analysis of the AuNi/NPNi/FNi
Cathode
Figure S1 schematically
illustrates the synthesis
strategy for the AuNi/NPNi/FNi cathode. First, sheet-like nanoporous
Ni (NPNi) is deposited and the tips are attached to the framework
of Ni foam (FNi) using the rapid decomposition of a metalcomplex
with thermal treatment. Then, an adequate amount of Au is deposited
in situ uniformly onto the surface of the NPNi/FNi (Au/NPNi/FNi) by
redox replacement of AuCl4–, where the
morphology and amount of deposited Au can be effectively controlled
by maintaining a constant temperature, concentration, and/or time
of replacement reaction. Finally, the AuNi alloy with 15 atom % Ni
is formed by rapid atom interdiffusion between the Au overlayer and
the NPNi/FNi surface at elevated temperatures (AuNi/NPNi/FNi). The
morphology and porous structure of the AuNi/NPNi/FNi cathode are investigated
using field emission scanning electron microscopy (SEM) and transmission
electron microscopy (TEM). As shown in Figures a and 1b, without
the help of any additional binder or solvent, the tips of AuNi/NPNi
are attached to the framework of the Ni foam, while the large pores
of the Ni foam are kept intact, which ensures the formation of a free-standing
structure and a favorable low-resistance pathway for electron transfer.
Even after the cathode is subjected to strong ultrasound for 1 h (frequency
of 40 kHz, power of 200 W), no AuNi or AuNi/NPNi is removed from the
FNi, indicating the superior mechanical stability of the AuNi/NPNi/FNi
cathode (Figure c).
A high-magnification observation (Figure d) of the AuNi/NPNi/FNi cathode reveals that
AuNi/NPNiconsists of fully developed and well-connected 3D macropores
with a wide size range (500 nm to 3.0 μm). The low-magnification
TEM image (Figure e) further illustrates the highly porous nature of AuNi/NPNi. From
the pore-size distribution (inset in Figure f), two types of pores are clearly observed,
micropores (∼3–4 nm) and mesopores, with a wide size
range (∼5–100 nm), which is in agreement with the TEM
results (Figure e).
The highly porous structure of AuNi/NPNi offers a high specific area
of 20.29 m2 g–1AuNi/NPNi,
which is confirmed by the nitrogen absorption–desorption isotherms
(Figure f). Based
on the inductively coupled plasma optical emission spectrometry (ICP-OES)
result (the weight ratio of AuNi to AuNi/NPNi is 0.53 atom %, Table S1), the calculated specific area of the
AuNi overlayer is 3828.3 m2 g–1AuNi, which offers a large cathode–electrolyte contact area to
ensure high availability of the catalytic active sites in the Li–O2 cell. Furthermore, the highly porous nature of metallicAuNi/NPNi
results in an ultralow density (ρ = 3.8 mg cm–3), which is comparable to that of carbon aerogels (ρ ≥
2.0 mg cm–3)[33,34] and lower than that
of other ultralight materials (ρ ≥ 8.0 mg cm–3)[35−37] (Figure g). The
powder X-ray diffraction (PXRD) analysis of AuNi/NPNi/FNi (Figure h) reveals that the
diffraction peaks can be indexed to well-crystallized Au (PDF No.
65-8601) and Au85Ni15 alloy. The high-magnification
TEM image reveals that the NPNi surface is well-covered by the AuNi
overlayer with a thickness of ∼2.1 nm (Figure i and Figure S2). This thickness and constitution of the AuNi alloy were determined
by continuously optimized experimental results (Figures S3, S4, and S5). This unique all-metalAuNi/NPNi/FNi
cathode with a nanoengineered AuNi surface simultaneously fulfills
five key requirements for use as a Li–O2 battery
cathode: good catalytic activity endowed by the AuNi alloy surface,
highly porous structure endowed by NPNi/FNi, high mechanical stability
endowed by the free-standing structure, good conductivity, and, especially,
high chemical stability. All of these advantages are beneficial for
the electrochemical performance of the Li–O2 batteries.
Figure 1
Structure
of the cathode. (a) Field emission scanning electron
microscopic (FESEM) image and photograph (inset) of the pristine FNi.
(b) FESEM image and photograph (inset) of the as-prepared AuNi/NPNi/FNi
cathode. (c) Morphology of the AuNi/NPNi/FNi cathode after ultrasonic
processing. (d) Enlarged image of b. (e) TEM image of the AuNi/NPNi.
(f) Nitrogen adsorption–desorption isotherms and pore-size
distribution (inset) of AuNi/NPNi. (g) Black AuNi/NPNi on stamen.
(h) X-ray diffraction patterns of the AuNi/NPNi/FNi cathode and the
patterns of the as-prepared Au85Ni15 alloy.
The patterns for standard Au and Ni are also shown for reference.
(i) Enlarged image of e. NPNi is covered with a AuNi alloy overlayer
with a thickness of 2.1 nm.
Structure
of the cathode. (a) Field emission scanning electron
microscopic (FESEM) image and photograph (inset) of the pristine FNi.
(b) FESEM image and photograph (inset) of the as-prepared AuNi/NPNi/FNi
cathode. (c) Morphology of the AuNi/NPNi/FNi cathode after ultrasonic
processing. (d) Enlarged image of b. (e) TEM image of the AuNi/NPNi.
(f) Nitrogen adsorption–desorption isotherms and pore-size
distribution (inset) of AuNi/NPNi. (g) Black AuNi/NPNi on stamen.
(h) X-ray diffraction patterns of the AuNi/NPNi/FNi cathode and the
patterns of the as-prepared Au85Ni15 alloy.
The patterns for standard Au and Ni are also shown for reference.
(i) Enlarged image of e. NPNi is covered with a AuNi alloy overlayer
with a thickness of 2.1 nm.
Electrochemical Properties of the AuNi/NPNi/FNi Cathode
The electrochemical properties of the AuNi/NPNi/FNi cathode were
then examined in a Li–O2 cell. The FNi, NPNi/FNi,
AuNi/FNi, and AuNi/NPNi cathodes (prepared using a similar process
to that used for AuNi/NPNi/FNi in the absence of FNi) adhered onto
FNi by the binder Nafion (AuNi/NPNi@FNi) and the Au/NPNi/FNi cathode
were employed for comparison (Figures S6 and S7). Figure a shows
the first discharge–charge voltage profiles of the Li–O2 cells with the FNi, NPNi/FNi, AuNi/FNi, AuNi/NPNi@FNi, Au/NPNi/FNi,
and AuNi/NPNi/FNi cathodes at a current density of 1.0 A g–1. There is almost no discharge/charge voltage platform of the Li–O2 cells using the FNi and NPNi/FNi cathodes, indicating that
FNi and NPNi/FNi do not have catalytic activity in the cell. Therefore,
porous NPNi/FNi or FNi acts only as an effective current collector
that provides good electron transport, fast mass transfer, and sufficient
void volume to house the generated discharge products Li2O2. The ultrathin Au or AuNi alloy overlayer attached
to the surface acts as an effective electrocatalyst that promotes
the formation and decomposition of Li2O2. Note
that the discharge and charge voltage of the Li–O2 cell can be significantly improved with the help of the AuNi/NPNi/FNi
cathode, which enhances the round-trip efficiency that is vital for
electrochemical energy storage devices. In detail, the discharge voltage
of the Li–O2 cell with a AuNi/NPNi/FNi cathode is
higher than that with AuNi/NPNi@FNi and Au/NPNi/FNi cathodes by ∼30
mV; its charge voltage is much lower than that with the AuNi/NPNi@FNi
cathode by 140 mV and that with the Au/NPNi/FNi by 200 mV. This result
is further supported by the oxidation of the artificially Li2O2-loaded cathodes in Li–O2 cells, indicating
that a similar reduction in the oxidation potential is obtained (Figure S8 and details). The electrochemical processes
of oxygen in the Li–O2 cell were also investigated
using cyclic voltammetry (CV). Figure b presents the CV response of the cells at a constant
scan rate of 0.05 mV s–1. The cycle curve reveals
that the AuNi/NPNi/FNi cathode exhibits a higher oxygen reduction
(ORR) onset potential, a lower evolution reaction (OER) onset potential,
and a higher ORR/OER peak current compared with those of the other
cathodes. These results indicate that AuNi/NPNi/FNi exhibits a superior
electrochemical performance toward both the formation and decomposition
of the discharge product (Li2O2), which might
be derived from the synergy of the following advantageous factors:
the higher catalytic activity of the AuNi alloy overlayer than that
of Au, which is derived from lattice contraction; the large surface
area that provides more reaction sites for the ORR and OER; the highly
porous nature, which facilitates the continuous oxygen and lithium
ion flow into and out of the inner cathode via larger tunnels (Figure S9); and the cathode surface-induced solvation-mediated
formation/decomposition mechanism of Li2O2 that
benefits the ORR and OER reactions (vide infra).
Figure 2
Electrochemical performance.
(a) First charge–discharge
curves of lithium–oxygen (Li–O2) cells with
the six types of cathodes at a current density of 1.0 A g–1 and a specific capacity limit of 3,000 mAh g–1. (b) CV of the six types of cathodes in Li–O2 cells
at a constant scan rate of 0.05 mV s–1. (c) The
rate capability of the Li–O2 cells at the current
density of 1.0 A g–1. Inset in c is the enlarged
discharge profile of the Li–O2 cells with FNi and
NPNi/FNi cathodes. (d) Comparison of the specific capacities of some
noncarbonaceous cathodes previously reported. (e) FESEM images of
the discharged Au/NPNi/FNi cathode when the discharge capacity is
limited to 3,000 mAh g–1. (f) FESEM images of the
discharged AuNi/NPNi/FNi cathode. Insets of e and f show the corresponding
enlarged FESEM images. (g) A mechanism of electrochemical growth of
the film-like and nanosheet-like Li2O2.
Electrochemical performance.
(a) First charge–discharge
curves of lithium–oxygen (Li–O2) cells with
the six types of cathodes at a current density of 1.0 A g–1 and a specific capacity limit of 3,000 mAh g–1. (b) CV of the six types of cathodes in Li–O2 cells
at a constant scan rate of 0.05 mV s–1. (c) The
rate capability of the Li–O2 cells at the current
density of 1.0 A g–1. Inset in c is the enlarged
discharge profile of the Li–O2 cells with FNi and
NPNi/FNi cathodes. (d) Comparison of the specific capacities of some
noncarbonaceous cathodes previously reported. (e) FESEM images of
the discharged Au/NPNi/FNi cathode when the discharge capacity is
limited to 3,000 mAh g–1. (f) FESEM images of the
discharged AuNi/NPNi/FNi cathode. Insets of e and f show the corresponding
enlarged FESEM images. (g) A mechanism of electrochemical growth of
the film-like and nanosheet-like Li2O2.Figure c shows
the first discharge curves of the Li–O2 cells with
the six types of cathodes at current densities of 1.0 A g–1. The Li–O2 cell with the AuNi/NPNi/FNi cathode
exhibits an ultrahigh discharge capacity of 22,551 mAh g–1AuNi, which is more than 15 times higher than that with
the reported noncarbonaceous cathodes (with discharge capacities typically
less than 3,000 mAh g–1) (Figure d); this is the best capacity reported to
date in this field.[25−32] Note that the discharge capacity of the Li–O2 cell
with the FNi and NPNi/FNi cathodes is negligible within the voltage
range, which suggests that the discharge capacities of Li–O2 cells are derived from ORR on Au or on the AuNi alloy overlayer.
Similarly, the discharge capacity of the Li–O2 cell
with the AuNi/FNi cathodes is very low (2,468 mAh g–1AuNi), indicating that the highly porous structure and
the large specific surface area of NPNi result in the high discharge/charge
capacity. This highly porous nature provides sufficient available
void volume to house the generated discharge products, resulting in
a substantially enhanced discharge capacity. The Li–O2 cell with the AuNi/NPNi@FNi cathode exhibits a much lower discharge
capacity (13,110) than that with the Au/NPNi/FNi cathode (17,944)
(Figure c), indicating
that the free-standing structure promotes the key advantage of the
NPNi porous structure, which is consistent with Figure S6. Unexpectedly, even with the same porous structure,
the discharge capacity of the Li–O2 cell with the
AuNi/NPNi/FNi cathode is much higher than that with the Au/NPNi/FNi
cathode by ∼4,607 mAh g–1. The difference
in the specific capacities of the two cathodes is considered to arise
from the different deposition behaviors and morphologies of the discharge
product. To this end, the morphologies of the two cathodes after discharge
were examined. Figures e and 2f show the SEM images of the discharged
Au/NPNi/FNi and AuNi/NPNi/FNi cathodes at a fixed capacity of 3,000
mAh g–1. After discharge of the cell, the surface
of the Au/NPNi/FNi cathode was almost fully covered by film-like discharge
products (Figure e),
which inevitably impedes oxygen, lithium-ion, and charge transfer
within the cathode during subsequent discharge, resulting in severe
polarization and premature finishing of the discharge process, causing
low capacities and high overpotential. In sharp contrast, the nanosheet-like
discharge products are uniformly and loosely dispersed onto the surface
of the AuNi/NPNi/FNi cathode (Figure f); this arrangement helps maintain active sites for
the ORR on the cathode, supporting the electrochemical reaction during
subsequent discharge and leading to high capacities of the Li–O2 cell. PXRD analysis of the discharged cathodes confirmed
that Li2O2 is the only crystalline product in
the two cases, regardless of the difference in morphology (Figure S10). We argue that the difference in
morphology of the two discharge processes arises from an elevated
solution-mediated mechanism for Li2O2 formation
that overcomes the charge transport limitations inherent in the surface
growth of Li2O2.[38]Figure g schematically
shows the feasible mechanisms of electrochemical growth of the film-like
and nanosheet-like Li2O2. First, O2 undergoes a one-electron reduction to O2– on the ORR site of two cathodes. On the Au/NPNi/FNi cathode, the
superoxide species (O2–* and/or LiO2*, where * indicates surface-adsorbed O2– and LiO2) adsorb onto the cathode surface and undergo
a second reduction on the neighboring ORR site of Au, immediately
forming Li2O2 thin films on the cathode surface.
In contrast, on the AuNi/NPNi/FNi cathode, the continuous ORR site
of Au is severed by the presence of the Ni atom, which prevents the
second reduction of the superoxide species and promotes their diffusion
into the electrolyte, forming dissolved solvates of superoxide species
(LiO2(sol) and/or O2–(sol)).
The dissolved species undergo disproportionation, ultimately forming
large Li2O2 nanosheet-like crystals. However,
in a real system, Li2O2 growth is more complicated,
and further studies using a combination of electrochemical and theoretical
approaches are in progress to elucidate the exact functions of the
AuNi/NPNi/FNi cathode.Another considerable improvement of the
Li–O2 cell with the AuNi/NPNi/FNi cathode is the
cycling stability. These
cells were tested with the recently widely used capacity limited cycle
method. Figure a presents
the typical voltage profiles for Li–O2 cells with
AuNi/NPNi@FNi, Au/NPNi/FNi, and AuNi/NPNi/FNi cathodes cycled at a
rate of 1.0 A g–1 and with a fixed capacity of 3,000
mAh g–1. The voltage obtained at the discharge terminal
of the AuNi/NPNi@FNi cathode in the Li–O2 cell is
>2.0 V for 286 cycles. In contrast, the discharge voltages of the
Au/NPNi/FNi and AuNi/NPNi@FNi cathodes degrade to 2.0 V after only
65 and 95 cycles, respectively. This finding confirms that the AuNi/NPNi/FNi
cathode has superior rechargeability and cycling stability. To further
understand this superior cycling stability, the evolution of the morphology
of the three discharged cathodes after the first and 50th cycles was
examined. In the AuNi/NPNi/FNi cathode, the platelet-like Li2O2 structure disappeared, and the initial nanoporous structure
of the whole cathode was almost fully recovered after the first recharge,
indicating good reversibility and structural stability of the AuNi/NPNi/FNi
cathode (Figure d).
Even after 50 cycles, the AuNi/NPNi/FNi cathode was only covered by
a few small particles (Figure g), which can be ascribed to Li2CO3,
HCO2Li, or CH3CO2Li from the side
reactions of the Li2O2 and/or intermediates,
such as LiO2*, and electrolyte upon cycling (Figure S13). In contrast, in the Au/NPNi/FNi
and AuNi/NPNi@FNi cathodes, massive Li2CO3 and
lithium carboxylates were packed densely onto the cathode surface
(Figures e, 3f, and S13). This continuous
accumulation of byproducts upon cycling hinders the transport of the
superoxide species, electrons, and lithium ions within the cathode
during subsequent cycling, consequently leading to the failure of
the Li–O2 cell with these cathodes. We speculate
that the superior rechargeability of the AuNi/NPNi/FNi cathode might
be derived from the synergy of the following advantageous factors:
the structural stability of AuNi/NPNi/FNi helps to maintain stable
cathode integrity upon cycling, the free-standing structure of the
AuNi/NPNi/FNi cathode can provide a fast electron conduction to the
cathode–Li2O2 interface, the uniformly
and loosely distributed Li2O2 nanosheets provide
sufficient Li2O2–electrolyte interfaces
that support the electrochemical reaction during the charge process,
and the AuNi/NPNi/FNi cathode significantly alleviates the high-potential-induced
electrolyte decomposition during charging by lowering the charge voltage.[12,13]
Figure 3
Cathode
rechargeability. (a) Variation of the terminal voltage
upon the discharge of the Li–O2 cells with the three
types of cathodes at current densities of 1.0 A g–1 and a specific capacity limit of 3000 mAh g–1.
FESEM images of the recharged (b) Au/NPNi/FNi, (c) AuNi/NPNi@FNi,
and (d) AuNi/NPNi/FNi cathodes after the first cycle. FESEM images
of the recharged (e) Au/NPNi/FNi, (f) AuNi/NPNi@FNi, and (g) AuNi/NPNi/FNi
cathodes after the 50th cycle. Insets of b–g show the corresponding
enlarged FESEM images.
Cathode
rechargeability. (a) Variation of the terminal voltage
upon the discharge of the Li–O2 cells with the three
types of cathodes at current densities of 1.0 A g–1 and a specific capacity limit of 3000 mAh g–1.
FESEM images of the recharged (b) Au/NPNi/FNi, (c) AuNi/NPNi@FNi,
and (d) AuNi/NPNi/FNi cathodes after the first cycle. FESEM images
of the recharged (e) Au/NPNi/FNi, (f) AuNi/NPNi@FNi, and (g) AuNi/NPNi/FNi
cathodes after the 50th cycle. Insets of b–g show the corresponding
enlarged FESEM images.
Electrochemical Stability of the AuNi/NPNi/FNi Cathode
To
verify the electrochemical stability of the cathode, undischarged
FNi, NPNi/FNi, Au/NPNi/FNi, and AuNi/NPNi/FNi cathodes were also directly
subjected to electrochemical oxidation in Li–O2 cells
at a current density of 1.0 A g–1 (Figure S14). The Li–O2 cell with the four
all-metal cathodes demonstrated a continuous charge capacity upon
charging above 4.2 V, which may be due to the oxidation of the electrolyte
and cathode (Figure S14a). PXRD analysis
of the four charged cathodes confirmed that there were no peaks for
Ni oxides and/or Au oxides, suggesting that the cathodes were not
oxidized upon charging (Figures S14b–S14e). Unexpectedly, oxidation of the all-metal cathodes was not observed,
even after 50 discharge/recharge cycles (Figure S15). These results confirmed that the four all-metal cathodes
have superior electrochemical stability in Li–O2 cells, which encouraged a further investigation into the electrochemical
stability of the Li–O2 system with the all-metal
cathodes. To this end, the parasitic electrochemistry/chemistry in
the Li–O2 cells was examined using quantitative
Fourier transform infrared (FTIR) and 1H nuclear magnetic
resonance (NMR) spectroscopy (Figure ). The conventional SP carbon cathode was also employed
for comparison (Figure S16). The FTIR spectra
indicate that the discharge products in Li–O2 cells
withboth AuNi/NPNi/FNi and SP carbon cathodes after the first discharge
are overwhelmingly dominated by Li2O2 (Figure a). However, after
the 40th cycle, FTIR provides clear evidence of significant side reactions
on the pristine SP carbon cathode. In addition to Li2O2, the peaks at ∼864, 1441, and 1500 cm–1 can be assigned to Li2CO3, that at ∼1371
cm–1 to HCO2Li, and that at ∼1615
cm–1 to CH3CO2Li (Figure b). In contrast,
significantly weaker peaks are ascribed to side products on the AuNi/NPNi/FNi
cathode after the 40th cycle and may have resulted from the partial
decomposition of the ether-based electrolyte. Based on the FTIR calibration
curves obtained in our recent work[12,38,39] the molar ratio of the Li2O2 to the side products (Li2CO3, CH3CO2Li, and HCO2Li) was determined using the
obtained FTIR spectra (Figures a and 4b). In sharp contrast, the Li2O2/side product ratio at the end of 40 cycles for
the Li–O2 cell with the SP carbon cathode was only
41.3/58.7, which is much lower than that obtained with the AuNi/NPNi/FNi
cathode (87.7/12.3). In addition, 1H NMR spectroscopy (Figures c and 4d) indicates that the amount of electrolyte decomposition
products (CH3CO2Li and HCO2Li) on
the AuNi/NPNi/FNi cathode is much less than that on the SP carbon
cathode during cycling, which is consistent with the above FTIR results.
These observations clearly demonstrate the superiority of the Li–O2 cells with the all-metal cathode in terms of the electrochemical/chemical
stability, which can be ascribed to the ability of AuNi/NPNi/FNi to
effectively avoid the possible side reactions between the conventional
carbon defect sites and the Li2O2 or between
the defect sites and the electrolyte.[22−24] In addition, the low
charge potential observed with the all-metal cathode alleviates the
high-potential-induced decomposition of the electrolyte during charging,
which also contributes to the high electrochemical/chemical stability.[12,13]
Figure 4
Parasitic
electrochemistry/chemistry. FTIR spectra of the conventional
SP carbon and AuNi/NPNi/FNi cathodes after (a) the first discharge
and (b) the 40th discharge. The spectra for Li2O2, Li2CO3, HCO2Li, and CH3CO2Li are also shown for reference. 1H NMR
spectra of the conventional SP carbon and AuNi/NPNi/FNi cathodes after
(c) the first discharge and (d) the 40th discharge. The spectra for
TEGDME, HCO2Li, and CH3CO2Li are
also shown for reference.
Parasitic
electrochemistry/chemistry. FTIR spectra of the conventional
SP carbon and AuNi/NPNi/FNi cathodes after (a) the first discharge
and (b) the 40th discharge. The spectra for Li2O2, Li2CO3, HCO2Li, and CH3CO2Li are also shown for reference. 1H NMR
spectra of the conventional SP carbon and AuNi/NPNi/FNi cathodes after
(c) the first discharge and (d) the 40th discharge. The spectra for
TEGDME, HCO2Li, and CH3CO2Li are
also shown for reference.
Conclusions
In conclusion, the design of a porous cathode
that simultaneously
achieves a high chemical stability and a superior electrochemical
performance remains a daunting challenge. In this work, we first developed
nanoporous Ni with a nanoengineered AuNi alloy surface directly attached
to Ni foam (AuNi/NPNi/FNi) as a new all-metal cathode system. Compared
with the popularly used carbon cathode, the AuNi/NPNi/FNi cathode
is advantageous in that it does not show measurable reactivity toward
the discharge product (Li2O2) and/or the reaction
intermediates (LiO2). The Li–O2 cell
with an all-metal cathode demonstrates the reversible formation and
decomposition of Li2O2 and relatively low overpotentials,
ultrahigh specific capacity, and cycle stability. These superior properties
are explained by the enhanced solvation-mediated formation of the
discharge products as well as the tailored properties of the all-metal
cathode, including intrinsic chemical stability endowed by the metal
nature, high specific surface area and the highly porous structure
that provide sufficient void volume to house the generated discharge
products and fast mass transfer, the high conductivity that enables
fast electron transfer from the reaction sites, and superior mechanical
stability that helps to maintain stable cathode integrity upon cycling.
The results also suggest that both the material and structure of the
cathode should be optimized to simultaneously achieve a high chemical
stability and a superior electrochemical performance of Li–O2 batteries.
Authors: Muhammed M Ottakam Thotiyl; Stefan A Freunberger; Zhangquan Peng; Yuhui Chen; Zheng Liu; Peter G Bruce Journal: Nat Mater Date: 2013-09-01 Impact factor: 43.841
Authors: B D McCloskey; A Speidel; R Scheffler; D C Miller; V Viswanathan; J S Hummelshøj; J K Nørskov; A C Luntz Journal: J Phys Chem Lett Date: 2012-03-30 Impact factor: 6.475
Authors: Jun Lu; Yu Lei; Kah Chun Lau; Xiangyi Luo; Peng Du; Jianguo Wen; Rajeev S Assary; Ujjal Das; Dean J Miller; Jeffrey W Elam; Hassan M Albishri; D Abd El-Hady; Yang-Kook Sun; Larry A Curtiss; Khalil Amine Journal: Nat Commun Date: 2013 Impact factor: 14.919
Authors: Bryan D McCloskey; Alexia Valery; Alan C Luntz; Sanketh R Gowda; Gregory M Wallraff; Jeannette M Garcia; Takashi Mori; Leslie E Krupp Journal: J Phys Chem Lett Date: 2013-08-23 Impact factor: 6.475