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Glazer, Matthew P.B.,Wang, Junjie,Cho, Jiung,Almer, Jonathan D.,Okasinski, John S.,Braun, Paul V.,Dunand, David C. Elsevier 2017 Journal of Power Sources Vol.367 No.-
<P><B>Abstract</B></P> <P>Volume changes associated with the (de)lithiation of a nanostructured Ni<SUB>3</SUB>Sn<SUB>2</SUB> coated nickel inverse opal scaffold anode create mismatch stresses and strains between the Ni<SUB>3</SUB>Sn<SUB>2</SUB> anode material and its mechanically supporting Ni scaffold. Using <I>in operando</I> synchrotron x-ray diffraction measurements, elastic strains in the Ni scaffold are determined during cyclic (dis)charging of the Ni<SUB>3</SUB>Sn<SUB>2</SUB> anode. These strains are characterized using both the center position of the Ni diffraction peaks, to quantify the average strain, and the peak breadth, which describes the distribution of strain in the measured volume. Upon lithiation (half-cell discharging) or delithiation (half-cell charging), compressive strains and peak breadth linearly increase or decrease, respectively, with charge. The evolution of the average strains and peak breadths suggests that some irreversible plastic deformation and/or delamination occurs during cycling, which can result in capacity fade in the anode. The strain behavior associated with cycling of the Ni<SUB>3</SUB>Sn<SUB>2</SUB> anode is similar to that observed in recent studies on a Ni inverse-opal supported amorphous Si anode and demonstrates that the (de)lithiation-induced deformation and damage mechanisms are likely equivalent in both anodes, even though the magnitude of mismatch strain in the Ni<SUB>3</SUB>Sn<SUB>2</SUB> is lower due to the lower (de)lithiation-induced contraction/expansion.</P> <P><B>Highlights</B></P> <P> <UL> <LI> Lithiation-induced strains quantified in a Ni<SUB>3</SUB>Sn<SUB>2</SUB> inverse opal anode <I>in operando</I>. </LI> <LI> Lithiation induces compressive average strains in Ni inverse opal scaffold. </LI> <LI> Ni inverse opal scaffold strain distribution reversibly broadens upon lithiation. </LI> <LI> Three measured volumes show similar cyclic strain averages and distributions. </LI> <LI> Ni<SUB>3</SUB>Sn<SUB>2</SUB> measured cyclic strains are similar to prior Si inverse opal anode studies. </LI> </UL> </P> <P><B>Graphical abstract</B></P> <P>[DISPLAY OMISSION]</P>
Nguyen, Quoc Hai,Hung, Nguyen Thanh,Park, Sang Joon,Kim, Il Tae,Hur, Jaehyun Elsevier 2019 ELECTROCHIMICA ACTA Vol.301 No.-
<P><B>Abstract</B></P> <P>A carbon-free intermetallic zinc titanium alloy (carbon-free Zn/Ti) anode, comprising active Zn nanoparticles finely dispersed in Zn<SUB>x</SUB>Ti<SUB>y</SUB> (Zn<SUB>0.6</SUB>Ti<SUB>0.4</SUB> and Zn<SUB>3</SUB>Ti) intermetallic buffer, is prepared via a thermal-treatment followed by a high-energy mechanical milling process for a lithium-ion battery (LIB) anode. As a counter-intuitive phenomenon, without the need of a carbon matrix, the carbon-free Zn/Ti alloy exhibits superior cyclic performance (∼1064 mAh cm<SUP>−3</SUP> of volumetric capacity after 350 cycles), a good rate capability (85% capacity retention at 3 A g<SUP>−1</SUP> compared to its capacity at 0.1 A g<SUP>−1</SUP>), and a high initial coulombic efficiency (88%). Although the use of hybrid TiC-C matrix as a control sample still affords highly stable cyclic performance and good rate capability, it exhibits a relatively lower capacity than a carbon-free alloy electrode. The enhanced performance of carbon-free Zn/Ti anodes for LIBs is owing to the presence of stable and cohesive Zn<SUB>x</SUB>Ti<SUB>y</SUB> intermetallic phases that provide high conductivity and mechanical stability, thereby mitigating the large volume changes of Zn particles during the lithiation/delithiation processes. High-performance Zn-Zn<SUB>x</SUB>Ti<SUB>y</SUB> can be seen as a new promising anode for the next-generation energy storage technology.</P> <P><B>Highlights</B></P> <P> <UL> <LI> Carbon-free Zn-Zn<SUB>x</SUB>Ti<SUB>y</SUB> alloy was developed as a new promising anode in LIBs. </LI> <LI> Zn-Zn<SUB>x</SUB>Ti<SUB>y</SUB> alloy was synthesized by heat-treatment followed by HEMM. </LI> <LI> Zn<SUB>x</SUB>Ti<SUB>y</SUB> acted as effective buffers with high conductivity and mechanical stability. </LI> <LI> Zn-Zn<SUB>x</SUB>Ti<SUB>y</SUB> anode outperformed its counterpart with added carbon (Zn-TiC-C). </LI> <LI> Zn-Zn<SUB>x</SUB>Ti<SUB>y</SUB> anodes demonstrate the extremely high volumetric capacity. </LI> </UL> </P> <P><B>Graphical abstract</B></P> <P>[DISPLAY OMISSION]</P>