2021
DOI: 10.1016/j.xcrp.2021.100569
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Low-sintering-temperature garnet oxides by conformal sintering-aid coating

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Cited by 36 publications
(18 citation statements)
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“…However, the lithium dendrite growth inside pure LLZTO persists due to the Li deposition along grain boundaries, although the desirable Li-ion conductivity is obtained via the Ta doping strategy. The homogeneity of Ta distribution in pure LLZTO is usually neglected. Ta-rich and Ta-poor zones are found to coexist within the matrix of LLZTO grains, while the Ta-rich zone appears along the grain boundaries around the void defects. , Critical current density (CCD) of symmetric cells with SSEs is normally less than 2 mA cm –2 at room temperature. , Long-term cycling performance is severely hampered owing to the lithium dendrite growth. , The lithium dendrite formation is attributed to the high electronic conductivity and low ionic conductivity around the void defects at the grain boundaries. The electrons reduce Li ions to form metallic Li (Li + to Li 0 ), resulting in local short-circuit phenomena. , The mechanism of short-circuit in garnet SSEs is different from that in liquid electrolytes, where lithium dendrites first nucleate at the Li/electrolyte interface, further propagate along the grain boundaries or through the voids. , Therefore, achieving the homogeneous Ta distribution and eliminating the void defects are promising strategies to suppress lithium dendrite growth. Wen and co-workers introduced Li 6 Zr 2 O 7 particles to regulate the Li 2 O atmosphere and fill the voids along the grain boundaries during the sintering of LLZTO. The CCD was improved to 1.4 mA cm –2 at room temperature.…”
Section: Introductionmentioning
confidence: 99%
“…However, the lithium dendrite growth inside pure LLZTO persists due to the Li deposition along grain boundaries, although the desirable Li-ion conductivity is obtained via the Ta doping strategy. The homogeneity of Ta distribution in pure LLZTO is usually neglected. Ta-rich and Ta-poor zones are found to coexist within the matrix of LLZTO grains, while the Ta-rich zone appears along the grain boundaries around the void defects. , Critical current density (CCD) of symmetric cells with SSEs is normally less than 2 mA cm –2 at room temperature. , Long-term cycling performance is severely hampered owing to the lithium dendrite growth. , The lithium dendrite formation is attributed to the high electronic conductivity and low ionic conductivity around the void defects at the grain boundaries. The electrons reduce Li ions to form metallic Li (Li + to Li 0 ), resulting in local short-circuit phenomena. , The mechanism of short-circuit in garnet SSEs is different from that in liquid electrolytes, where lithium dendrites first nucleate at the Li/electrolyte interface, further propagate along the grain boundaries or through the voids. , Therefore, achieving the homogeneous Ta distribution and eliminating the void defects are promising strategies to suppress lithium dendrite growth. Wen and co-workers introduced Li 6 Zr 2 O 7 particles to regulate the Li 2 O atmosphere and fill the voids along the grain boundaries during the sintering of LLZTO. The CCD was improved to 1.4 mA cm –2 at room temperature.…”
Section: Introductionmentioning
confidence: 99%
“…68,69 Such benefits of an amorphous phase (with a different chemistry compared to our work) in the grain boundaries on mechanical and electrochemical properties have been reported before, but often only relatively low CCD values of about 0.5 mA cm −2 were achieved. [38][39][40]70 The main difference to our approach is that the amorphous phase is formed by adding phases or glasses to the initial powders, which can result in inhomogeneous mixing of the powders. In our material, the amorphous phase is intrinsically incorporated in the powder due to the melting process promoting excellent distribution and outstanding dendrite stability.…”
Section: Mechanism Of Lithium Dendrite Suppressionmentioning
confidence: 99%
“…During the actual sintering step, the liquid phase already formed before tends to wet the surfaces of the ceramic grains, and as a result, it fills the grain boundaries and thus leads to improved densification. As sintering additives, mostly lithium compounds like Li 2 O, LiOH, Li 3 PO 4 , Li 3 BO 3 , , LiAlO 2 (by an uncontrolled reaction of excess Li 2 CO 3 with an Al 2 O 3 crucible or by atomic layer deposition coating of Al 2 O 3 ), and lithium-containing glass systems (e.g., Li 2 O–B 2 O 3 –SiO 2 and 3Li 2 O–2GeO 2 ) have been investigated. Even though the sintering temperature can effectively be reduced to around 1000 °C by these methods, the sintering time is still long (10 h up to 36 h ), and, if measured, CCD values are relatively low (0.3 to 0.6 mA cm –1 ,,, ), indicating poor lithium dendrite suppression.…”
Section: Introductionmentioning
confidence: 99%
“…[14][15][16][17] However, the densification of oxide ceramic electrolyte often requires a high temperature (>1100 °C) and a long holding time (>10 h) by conventional sintering, which is very likely to result in impurities, because of the significant risk of volatilization of Li/Na during high-temperature processing. [18][19][20] In addition, a stable and sufficient interfacial contact between SEs and electrodes could not be achieved by the conventional high-temperatures co-sintering method, due to severe element interdiffusion. [21] Therefore, the methods for the rapid densification of high-quality oxide ceramic electrolytes as well as the sintering process, a preheating process (500 W, ≈80 s) and a following sintering (800 W, ≈25 s) were included.…”
Section: Introductionmentioning
confidence: 99%