Nano Research Nano Res DOI 10.1007/s12274-015-0757-3 Enhanced Li+ storage properties of few-layered MoS2–carbon composite microspheres embedded with Si nanopowders Seung Ho Choi and Yun Chan Kang () Nano Res., Just Accepted Manuscript • DOI 10.1007/s12274-015-0757-3 http://www.thenanoresearch.com on March 4, 2015 © Tsinghua University Press 2015 Just Accepted This is a “Just Accepted” manuscript, which has been examined by the peer-review process and has been accepted for publication. A “Just Accepted” manuscript is published online shortly after its acceptance, which is prior to technical editing and formatting and author proofing. Tsinghua University Press (TUP) provides “Just Accepted” as an optional and free service which allows authors to make their results available to the research community as soon as possible after acceptance. After a manuscript has been technically edited and formatted, it will be removed from the “Just Accepted” Web site and published as an ASAP article. Please note that technical editing may introduce minor changes to the manuscript text and/or graphics which may affect the content, and all legal disclaimers that apply to the journal pertain. In no event shall TUP be held responsible for errors or consequences arising from the use of any information contained in these “Just Accepted” manuscripts. To cite this manuscript please use its Digital Object Identifier (DOI®), which is identical for all formats of publication. 1 TABLE OF CONTENTS (TOC) Enhanced Li+ Storage Properties of Few-Layered MoS2–Carbon Composite Microspheres Embedded with Si Nanopowders Seung Ho Choi, Yun Chan Kang* Department of Materials Science and Engineering, Korea University, Republic of Korea. Few-layered MoS2-carbon composite with high capacities and good cycling performance is successfully applied as a protective matrix of silicon nanopowders. The MoS2–C composite material accommodates the large volume expansion of the Si nanopowders, but it also prevents the formation and propagation of a SEI layer on the Si surface during repeated cycling. The MoS2-C composite microspheres embedded with 30 wt% Si nanopowders with enhanced Li+ storage properties are evaluated as a novel anode material with superior electrochemical properties for lithium-ion batteries. Address correspondence to First Yun Chan Kang, email; [email protected] Nano Research DOI (automatically inserted by the publisher) Research Article Enhanced Li+ Storage Properties of Few-Layered MoS2–Carbon Composite Microspheres Embedded with Si Nanopowders Seung Ho Choi and Yun Chan Kang () Received: day month year ABSTRACT Revised: day month year Few-layered MoS2–carbon composite material is studied as a supporting material of silicon nanopowders. Microspheres of few-layered MoS2–C composite embedded with 30 wt% Si nanopowders are prepared by one-pot spray pyrolysis. The Si nanopowders with high capacity are perfectly surrounded by the few-layered MoS2–C composite matrix. The discharge capacities of the MoS2–C composite microspheres with and without 30 wt% Si nanopowders after 100 cycles are 1020 and 718 mA h g-1 at a current density of 1000 mA g-1, respectively. The spherical morphology of the MoS2–C composite microspheres embedded with Si nanopowders is preserved even after 100 cycles because of their high structural stability during cycling. The MoS2–C composite layer prevents the formation of unstable solid–electrolyte interface (SEI) layers on the Si nanopowders. Furthermore, as the MoS2–C composite matrix exhibits high capacities and excellent cycling performance, these characteristics are also reflected in the MoS2–C composite microspheres embedded with 30 wt% Si nanopowders. Accepted: day month year (automatically inserted by the publisher) © Tsinghua University Press and Springer-Verlag Berlin Heidelberg 2014 KEYWORDS Molybdenum sulfide • Silicon • Anode material • Lithium batteries • Spray pyrolysis 1. Introduction As the technologies for electric vehicles and However, silicon experiences a large volume portable electronic devices develop, silicon is expansion considered an extremely promising anode material insertion–extraction process, resulting in poor cycle for lithium-ion batteries (LIBs) with high capacity properties because of pulverization of materials and and fast charging–discharging properties [1-11]. loss of electrical contact between the electronic Available in abundance, Si is an outstanding LIB materials and the current collector [1-11]. anode material owing to its low discharge potential (300%) Nanostructured during materials and the Li+ carbon-based (< 0.5 V vs. Li/Li ) and the highest theoretical composite materials have been developed to control reversible capacity of approximately 4200 mA h g-1, the volume expansion of the Si electrode [12-36]. which is ten times more than the value for Various types of Si-based nanostructured materials, commercial graphite anodes (372 mA h g-1) [1-11]. such as hollow nanospheres, cubic nanocrystals, + Address correspondence to First Yun Chan Kang, email; [email protected] Nano Res. nanowires, and nanotubes, have improved Li+ electrochemical properties of a LIB anode. For storage properties beyond those of bulk materials example, Zhu et al. reported that a single-layered [12-21]. Although these Si-based nanostructures can MoS2–carbon fiber composite exhibits high capacity tolerate the large change in volume, the formation and long cycle stability for LIBs [45]. However, the of an unstable layer at the solid–electrolyte interface MoS2-based (SEI) between the Si surface and the organic capacities than those of the Si-based materials. The electrolyte leads to low Coulombic efficiency and a layered MoS2-carbon composite material with high decrease in capacity during cycling [8-10,12,21]. structural stability during repeated Li insertion and Carbon-based silicon composite materials have desertion processes could be efficient as the attracted much attention as promising anode supporting material for the Si materials with high Li materials with stable and excellent Li storage ion storage capacities. To the best of our knowledge, electrical metal sulfide–Si composite materials have not been properties because conductivity carbonaceous and of the materials their high stress-buffer layer of had lower reversible reported as anode materials for LIBs applications. Carbon-based In this study, the few-layered MoS2–C composite silicon composite materials such as Si–graphite, microspheres embedded with Si nanopowders were Si–amorphous prepared carbon, [22-36]. + materials Si–C nanotubes, and by one-pot spray pyrolysis, using Si–graphene have long cycle life when the silicon ammonium content in the composite materials was low [22-35]. polyvinylpyrrolidone (PVP), and Si nanopowders. As the Si content in a Si–C composite was increased, Few-layered MoS2 nanosheets embedded in carbon the Li storage properties deteriorated. However, spheres served as a protective matrix of silicon high content of carbon material resulted in nanopowders. In addition to accommodating the increases in the initial irreversible capacity and large volume expansion of the Si nanopowders, the decreases in the reversible capacity [22-31]. Thus, MoS2–C the search for new replacement carbonaceous formation and propagation of the SEI layer on the Si supporting material for the Si anode remains a great surface challenge. electrochemical properties of the microspheres were + In recent years, transition-metal oxides and metal sulfides have been widely studied as anode tetrathiomolybdate, composite during material repeated prevented cycling. the The compared with those of microspheres without the embedded Si nanopowders. materials for LIBs because they have higher theoretical capacities than commercial 2. Experimental section carbonaceous materials [37-43]. Two-dimensional 2.1 Synthesis of few-layered MoS2–C composite (2D) layered MoS2 is especially attractive because of microspheres embedded with Si nanopowders. its high reversible capacity and good cycling MoS2–C composite microspheres embedded with Si performance. Controlled MoS2 materials consisting nanopowders were directly prepared by ultrasonic of single layer or few layers facilitate a fast Li + spray pyrolysis at 800°C; a schematic of the charging–discharging process, which allows the apparatus is shown in Figure S1. A quartz reactor interlayer distance to relax the strain and lower the measuring 1200 mm in length and 50 mm in barrier for Li intercalation [44-47]. Because the diameter was used; the nitrogen flow rate (carrier graphene-like layered MoS2 can be very uniformly gas) was 10 L min-1. A 500-mL volume of distilled mixed water with carbonaceous materials, the was added to 1.8 g of ammonium combination of the two materials has been regarded tetrathiomolybdate as polyvinylpyrrolidone (PVP) to form the spray a fundamental strategy to enhance the | www.editorialmanager.com/nare/default.asp and 5.0 g of Nano Res. solution. The silicon nanopowders (85 nm) were ethylene carbonate and dimethyl carbonate dispersed in the spray solution with ammonium (EC–DMC) with 5% fluoroethylene carbonate. The tetrathiomolybdate and PVP. charging–discharging characteristics of the samples were determined through cycling in the potential 2.2 Characterization. range of 0.001–3.0 V at various fixed current The crystal structure of the MoS2–C composite densities. The cyclic voltammetry (CV) microspheres embedded with Si nanopowders was measurements were carried out at a scan rate of 0.1 investigated by X-ray diffractometry (XRD; X’pert mV s-1. Dimensions of the negative electrode were 1 PRO MPD, PANalytical, The Netherlands), using cm × 1 cm and mass loading was approximately 1.2 Cu Kradiation (= 1.5418 Å ). The morphological mg cm-2. features were investigated using field-emission scanning electron microscopy (FE-SEM; S-4800, Hitachi, Japan) and high-resolution transmission 3. Results and discussion Scheme 1 shows the formation mechanism of the electron microscopy (HR-TEM; JEM-2100F, JEOL, few-layered Japan) at a working voltage of 200 kV. The specific embedded with Si nanopowders via the one-step surface areas of the composite microspheres were and continuous spray-pyrolysis process. Droplets calculated from a Brunauer–Emmett–Teller (BET) were formed from the colloidal spray solution analysis of nitrogen adsorption isotherms (TriStar consisting of Si nanopowders dispersed in an 3000 gas adsorption MoS2–C composite microspheres analyzer, Micromeritics, USA). The composite microspheres were also investigated using X-ray photoelectron spectroscopy (XPS;ESCALAB 210, VG Scientific, now Thermo Scientific, USA) with Al K radiation (1486.6 eV). 2.3 Electrochemical measurements. The capacities properties of and the cycling composite microspheres were determined using a 2032-type coin cell. The electrode was prepared from a mixture containing 70 wt% of the active material, 15 wt% of Super P (conductive carbon black), and 15 wt% of sodium carboxymethyl Scheme 1. Formation mechanism of the few-layered MoS2–C composite microsphere cellulose (CMC) as the binder. embedded with Si nanopowders via the one-step and continuous spray-pyrolysis Lithium metal and a microporous process. polypropylene film were used as the aqueous solution of ammonium tetrathiomolybdate counter electrode and separator, respectively. The and PVP. In this study, PVP acted as a stabilizer for electrolyte was 1 M LiPF6 in a 1:1 (v/v) mixture of www.theNanoResearch.com∣www.Springer.com/journal/12274 | Nano Research Nano Res. the Si nanopowders and the source material for amorphous carbon, thus preventing the stacking of MoS2 layers [45,48]. In the precursor solution, the surface of the Si nanopowder was functionalized with water-soluble PVP. The drying of each droplet produced a composite microsphere of Si–ammonium-tetrathiomolybdate–PVP in the front part of the reactor that was maintained at 800°C. Thermal decomposition of ammonium tetrathiomolybdate into MoS2 and carbonization of PVP under the nitrogen atmosphere resulted in a Si–MoS2–C composite microsphere at the rear part of the reactor. In other words, one MoS2–C composite microsphere Si Figure. 1 Morphologies of the the MoS2-C composite and microspheres embedded with 30 wt% Si nanopowders. a,b) decomposition of one droplet, and few-layered FE-SEM images, c-f) TEM images, g) elemental mapping ultra-small nanoplates of MoS2 were embedded images of Mo, S, Si, and C components. nanopowders was embedded formed by with drying within the MoS2–C composite microsphere. The MoS2–C elastic enclosed within the composite microsphere. The two-dimensional structure completely covered the TEM images (Figures 1d and e) show the Si individual Si nanopowders. The content of Si nanopowders dispersed within the MoS2–C matrix. nanopowders in the composite microsphere could Figures 1e and 1f show the amorphous-fluid-like be controlled by changing the amount of Si structure nanopowders dispersed in the spray solution. few-layered MoS2 nanosheets were uniformly The composite layers morphologies of the microspheres MoS2–C composite MoS2–C matrix, in which distributed within the amorphous carbon matrix; structure, was fully covered by MoS2–C layers, as The composite shown by the arrows. The enlarged TEM image in microspheres shown in Figure 1 was 30 wt% based the inset of Figure 1f reveals clear lattice fringes on MoS2. The morphology of the commercial Si separated nanopowders used in this study is shown in Figure corresponds to the interplanar distance between the S2; the nanopowder had a mean size of 85 nm and a (111) planes of a Si nanoparticle [19]. The elemental slightly aggregated structure. The FE-SEM and low mapping resolution TEM images revealed that the composite distributions of MoS2, C, and Si nanopowders. The microspheres had a spherical shape and did not necking between the Si nanopowders resulted in show any tendency to aggregate. The surface of the some segregation of Si component in the low composite powder, as shown in Figure 1, had an resolution elemental mapping images as shown in embossed structure owing to the Si nanopowders Figure S3. MoS2 and the carbon material were in the amount the enclosed Si nanopowders are shown in Figure 1. content small of the Si nanopowder, which formed an embossed Si a an of designed containing with by distance images in of Figure 0.31 1g nm, which show the uniformly distributed all over the composite microspheres. The Si nanopowders were also well dispersed within the MoS2–C composite matrix. The dozens of the Si nanopowders were dispersed in | www.editorialmanager.com/nare/default.asp Nano Res. one composite microsphere as shown in Figure 1g. microspheres are shown in Figure S5. The Considering that MoS2 was converted into MoO3 composite microspheres had completely spherical when heated in air, the carbon content in the shape and showed no tendency to aggregate. The composite microspheres was estimated as 23 wt%, HR-TEM image in Figure S4d shows the uniform as measured by thermogravimetric analysis (see distribution of MoS2 nanosheets over the entire Figure S4). carbon matrix formed from the carbonization process that restricted the of MoS2 layers. Figure 2. Morphologies of the MoS2-C composite microspheres embedded with 60 wt% Si nanopowders: a,b) Figure 3. Properties of the MoS2-C composite FE-SEM images, c-f) TEM images, and g) elemental mapping microspheres embedded with 30 wt% and 60 wt% Si images of Mo, S, Si, and C components. nanopowders. a) XRD patterns, b) XPS C1s spectrum of the MoS2-C composite microspheres embedded with 30 The morphologies of the MoS2–C composite wt%, c) XPS Mo3d spectrum, d) XPS S2p spectrum. microspheres embedded with a high amount of Si nanopowders are shown in Figure 2. The designed The structural characteristics of the MoS2–C Si content in the composite microspheres was 60 composite wt% based on MoS2. The composite microsphere nanopowders are shown in Figure 3. The XRD shown in Figure 2 had a more embossed structure patterns of the composite microspheres with low than that of the microspheres shown in Figure 1 and high amounts of Si nanopowders had broad because of the high Si nanopowder content. The Si peaks corresponding to a hexagonal MoS 2 structure nanopowders were well dispersed within the and sharp peaks of the Si phase. Broad peaks of composite microspheres, as shown by arrows in MoS2 layers were observed at 2θ of approximately Figures 2d and 2e. The Si nanopowders located near 33° and 59°. However, the (002) reflections of the the surface of the composite microsphere, as shown stacked MoS2 layers at 2θ ~ 16° were not observed, in Figure 2f, had a uniform MoS2–C composite indicating the presence of only few-layered MoS2 coating. The elemental mapping images in Figure [45-47]. Therefore, the results of the XRD patterns 2g also show uniform distributions of MoS 2, C, and confirm Si nanopowders within the composite microsphere. nanosheets in the MoS2–C composite microspheres The embedded with Si nanopowders. Figures 3b-d morphologies of the MoS2–C composite microspheres the formation embedded of with few-layered www.theNanoResearch.com∣www.Springer.com/journal/12274 | Nano Si MoS2 Research Nano Res. shows the XPS peaks of the MoS2–C composite octahedral LixMoS2 [44-47,52-56]. The peak at microspheres Si around 0.6 V corresponds to the conversion nanopowders. The C1s XPS peak centered at 284.6 reaction, in which LixMoS2 was decomposed into eV in Figure 3b, which corresponds to the binding metallic Mo nanocrystals embedded in a Li2S energy of the sp C–C bond, confirms the formation matrix, and formation of a SEI layer on the MoS 2–C of amorphous carbon by the carbonization process surface, which resulted from electrochemically of PVP [49]. Two strong Mo3d XPS peaks at around driven electrolyte degradation [44-47,52-54]. The 229.4 and 232.5 eV in Figure 3c, which can be third reduction peak located at 0.05 V is attributed attributed to Mo3d5/2 and Mo3d3/2 binding energies to the reaction to form Li–Si alloys [12-21]. In the of MoS2, respectively, confirm the formation of first anodic scan, three oxidation peaks attributed to MoS2 ammonium metallic Mo nanocrystals and Li–Si alloys were tetrathiomolybdate [50,51]. The peaks at 162.0 and observed. The first two anodic peaks observed at 163.1 eV, also shown in Figure 2d, can be indexed as voltages of 0.3 and 0.55 V are attributed to the S2p [50,51]. The negligible peak intensities of Si2p in de-alloying reactions of Li–Si alloys [12-21]. The Figure S6 confirm that the Si nanopowder particles third anodic peak was observed at a voltage of 2.3 were completed covered by MoS2–C composite V, which corresponds to the conversion reaction of layers. The BET surface areas of the MoS2–C metallic Mo and Li2S to MoS2 [52-56]. From the composite microspheres with 0 and 30 wt% Si second cycle onward, the reduction and oxidation nanopowders g-1, peaks overlapped considerably, indicating the respectively. The addition of Si nanopowders superior reversible cycling performance of the increased the porosity of the MoS2–C composite MoS2–C composite microspheres with 30 wt% Si. microspheres as shown in Figure S7. Figure 4b shows the initial discharge and charge embedded with 30 wt% 2 by decomposition were 17.0 of and 64.3 m2 The electrochemical properties of the MoS2–C composite microspheres with and without embedded Si nanopowders are presented in Figure 4. Figure 4a shows the cyclic voltammogram (CV) curves microspheres of the composite with 30 wt% Si during the first four cycles at a scan rate of 0.1 mV s-1 in the voltage range of 0.001–3 V. Three reduction peaks resulting from lithium insertion into MoS2 and Si were observed in the first cathodic scan. The first reduction peak located at 1.4 V is attributed to the intercalation of Li ions into the hexagonal MoS2 lattice, followed by phase transformation to | www.editorialmanager.com/nare/default.asp Nano Res. curves of the MoS2–C composite microspheres with nanopowders decreased steadily to 1129 mA h g-1 and without embedded Si nanopowders at a for the 100th cycle. However, the composite current density of 1000 mA g-1. The initial discharge microspheres with 30 wt% Si nanopowders showed curves with stable discharge capacities during further cycling embedded Si nanopowders had clear plateaus at after achieving the maximum capacity at the 20 th around 0.1 V owing to the reaction of Li with Si to cycle, and had a value of 1020 mA h g-1 at the 100th form Li–Si alloys. However, the obvious plateaus cycle. The embedded Si nanopowders increased the corresponding to the formation of LixMoS2 and Mo capacities of the MoS2–C composite microspheres. nanocrystals embedded in a Li 2S matrix were not The Coulombic efficiencies of the composite observed in the initial discharge curves of the three microspheres samples amorphous-fluid-like nanopowders (Figure 4c) had high values above structure of the MoS2–C composite. The initial 99.5% from the 2nd cycle. The Li ion storage discharge capacities of the MoS2–C composite properties of the MoS2–C composite microspheres microspheres Si were compared with those of the MoS2 powders nanopowders were 1100, 1448, and 1746 mA h g , prepared by the spray pyrolysis process reported in respectively, and their initial Coulombic efficiencies the previous literature [52]. The bare MoS2 powders were 69.5, 65.3, and 67.8%, respectively. with filled and yolk-shell structures had discharge of the composite because of with microspheres the 0, 30, and 60 wt% -1 embedded with 30 wt% Si The cycling performances of the three samples at capacities of 362 and 687 mA h g-1 for 100th cycle at a a current density of 1000 mA g-1 are shown in current density of 1 A g-1, respectively. Embedding Figure 4c. The MoS2–C composite microspheres of Si nanopowders with high capacities improved without Si nanopowders had discharge capacities of the Li ion storage properties of the MoS2 material. 740 and 718 mA h g for the 2 -1 nd and 100 cycles, th Electrochemical impedance spectroscopy (EIS) respectively. The capacity retention of the MoS2–C was composite microspheres without Si nanopowders electrochemical properties of the MoS2–C composite measured from the 2 microspheres that the nd cycle was 97%, indicating few-layered to confirm embedded with the 30 superior wt% Si composite nanopowders. The impedance measurements were microspheres had excellent cycling performance carried out at room temperature before and after 10, even at a high current density of 1000 mA g-1. The 30, 50, and 100 cycles at a current density of 1000 discharge capacities of the MoS2–C composite mA g-1. The resulting Nyquist plots, shown in microspheres with embedded Si nanopowders Figure increased during cycling for the first 20 cycles. The medium-frequency range, which is assigned to the gradual Si charge-transfer resistance of the electrodes, and a nanopowders with a mean size of 85 nm during the line inclined at ~45° to the real axis at low first 20 cycles increased the capacities of the frequencies, which corresponds to lithium diffusion composite microspheres with increasing cycle within the electrode [58,59]. The charge-transfer number [28,57]. The increase in the oxidation peak resistance of the electrode decreased after the first intensity in the CV curves in Figure 3a, related to cycle owing to the transformation of the crystalline the de-alloying reaction of Li–Si alloys during structure into an amorphous-fluid-like structure cycling, also indicates gradual activation of the Si during nanopowders. After achieving the maximum value charge-transfer resistance then remained constant of 1390 mA h g , the discharge capacity of the through the 100th cycle. The line inclined at ~45° to composite the real axis at low frequencies was also well activation of MoS2–C conducted highly crystalline -1 microspheres with 60 wt% Si S8, the indicate first a semicircle discharge in process. www.theNanoResearch.com∣www.Springer.com/journal/12274 | Nano the The Research Nano Res. maintained during the first 100 cycles, indicating the good lithium-diffusion properties of the electrode. The morphology of the composite microsphere embedded with 30 wt% Si nanopowders after 100 cycles are shown in Figure S9. The spherical shape of the composite microsphere remained even after 100 cycles because of their high structural stability during cycling as Figure 5. Long-term cycling properties of the MoS2-C the Si nanopowders with high capacities were composite microspheres embedded with 30 wt% Si at a current completely surrounded by the few-layered MoS2–C density of 5.0 A g-1. composite matrix. The elemental mapping images revealed the uniform distributions of MoS2, C, and microspheres Si nanopowders within the composite microsphere nanopowders at an extremely high current density even after cycling. The elastic MoS2–C composite of 5 A g-1. The gradual activation during cycling for matrix accommodated the large volume change of the the Si nanopowders during the repeated process of capacities of the composite microspheres. The Li+ ion insertion–extraction. As a result, the composite microspheres attained the maximum formation of a stable SEI layer outside the surface discharge capacity of 728 mA g h-1 after the first 100 during electrochemical cycles and then steadily maintained this capacity properties of the composite microspheres, while the for another 400 cycles. The discharge capacity of the MoS2–C composite layer prevented the formation of composite microspheres for the 500th cycle was 695 unstable SEI layers on the Si nanopowders. mA h g-1, and their capacity retention measured Furthermore, from the 100th cycle was 95.4%. cycling improved the MoS2–C the composite matrix embedded with 30 first 100 cycles increased the wt% Si discharge exhibited high capacities and excellent cycling performances, which were then shown by the MoS2–C composite microspheres embedded with 30 4. Conclusions In summary, a few-layered MoS2-carbon wt% Si nanopowders. The rate performance of the composite with high capacities and good cycling MoS2–C composite microspheres embedded with 30 performance wt% Si nanopowders is shown in Figure 4d. The protective matrix of silicon nanopowders. Each current densities increased stepwise from 0.5 to 7 A MoS2–C composite microsphere embedded with Si g-1; for each step, 10 cycles were measured to nanopowders evaluate the rate performance. The stable reversible decomposing one droplet containing ammonium discharge capacities of the composite microspheres tetrathiomolybdate, PVP, and Si nanopowders. The decreased from 1175 to 677 mA h g-1 as the current MoS2–C composite material accommodated the density increased from 0.5 to 7 A g-1. The discharge large volume expansion of the Si nanopowders, but capacity of the composite microspheres recovered it also prevented the formation and propagation of to 1190 mA h g-1 as the current density was restored a SEI layer on the Si surface during repeated to 0.5 A g-1. cycling. The embedded Si nanopowders increased Figure 5 shows the long-term performance of the MoS2–C composite cycling was was successfully formed by applied drying as a and the capacity of the MoS2–C composite microspheres, and its volume fraction in the composite microspheres could be controlled by changing the amount of Si nanopowders dispersed in the spray | www.editorialmanager.com/nare/default.asp Nano Res. solution. The amount of MoS2 and carbon in the [4] Szczech, J. R.; Jin, S. Nanostructured Silicon for High composite microspheres could also be controlled by Capacity Lithium Battery Anodes. Energy Environ. Sci. 2011, 4, changing 56–72. the concentrations of ammonium tetrathiomolybdate and PVP that were dissolved in [5] Magasinki, A.; Dixon, P.; Hertzberg, B.; Kvit, A.; Ayala, J.; the spray solution. The composite microspheres of Yushin, G. High-Performance Lithium-Ion Anodes Using a MoS2, carbon, and silicon with enhanced Li + storage Hierarchical Bottom-Up Approach. Nat. 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