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    X-์„  ๊ฒฐ์ •ํ•™ ์—ฐ๊ตฌ๋ฅผ ํ†ตํ•œ ์ƒˆ๋กœ์šด ์ด์ฐจ์ „์ง€ ์ „๊ทน ์†Œ์žฌ ๋ฐ ๊ณ ์ฒด ์ „ํ•ด์งˆ์˜ ๊ฐœ๋ฐœ๊ณผ ๊ตฌ์กฐ์  ๋ฉ”์ปค๋‹ˆ์ฆ˜ ๋ถ„์„

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    ๋‹ค์–‘ํ•œ ๊ธฐ๋Šฅ์„ฑ ๋ฌด๊ธฐ ์†Œ์žฌ๋“ค์˜ ํŠน์„ฑ์€ ๊ธฐ๋ณธ์ ์œผ๋กœ ๊ฒฐ์ • ๊ตฌ์กฐ์™€ ๊นŠ์€ ๊ด€๊ณ„๊ฐ€ ์žˆ๋‹ค. ํŠนํžˆ ์ „์ง€ ์†Œ์žฌ๋“ค์˜ ๊ฒฝ์šฐ (์Œ๊ทน, ์–‘๊ทน ๋ฐ ๊ณ ์ฒด ์ „ํ•ด์งˆ), ๊ณ ์ฒด ๋‚ด ์–‘์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž… ๋ฐ ํ™•์‚ฐ์— ๊ธฐ๋ฐ˜ํ•˜๋Š” ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ํ†ตํ•ด ๊ตฌ๋™ํ•˜๊ธฐ ๋•Œ๋ฌธ์— ํ•ด๋‹น ์†Œ์žฌ๋“ค์˜ ํŠน์„ฑ์€ ๊ตฌ์กฐ์  ์š”์†Œ๋“ค๊ณผ ๋ฐ€์ ‘ํ•œ ๊ด€๊ณ„๋ฅผ ๊ฐ–๋Š”๋‹ค. ๋”ฐ๋ผ์„œ ์†Œ์žฌ์˜ ๊ฒฐ์ • ๊ตฌ์กฐ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ, ์ถฉ/๋ฐฉ์ „ ์ค‘์˜ ๊ตฌ์กฐ์  ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์ดํ•ดํ•˜๊ณ , ์ตœ์ข…์ ์œผ๋กœ ๊ตฌ์กฐ ์ •๋ณด์™€ ์ „์ง€ ํŠน์„ฑ ๊ฐ„์˜ ์—ฐ๊ด€ ๊ด€๊ณ„๋ฅผ ํ™•๋ฆฝํ•˜๋Š” ๊ฒƒ์€ ์ƒˆ๋กœ์šด ์ด์ฐจ ์ „์ง€ ์†Œ์žฌ๋ฅผ ๊ฐœ๋ฐœํ•˜๋Š”๋ฐ ์žˆ์–ด ๊ธฐ์ดˆ์ ์ด๋ฉด์„œ๋„ ํ•„์ˆ˜์ ์ธ ์ •๋ณด๋ฅผ ์ œ๊ณตํ•œ๋‹ค. ๋‹ค์–‘ํ•œ ๋ฌด๊ธฐ ์†Œ์žฌ ๋ถ„์„ ๋ฒ• ์ค‘ X-์„  ํšŒ์ ˆ ๋ฐ์ดํ„ฐ๋ฅผ ํ™œ์šฉํ•œ ๊ฒฐ์ •๊ตฌ์กฐ ๋ถ„์„์€ ์ƒˆ๋กœ์šด ์ „๊ทน ๋ฐ ๊ณ ์ฒด ์ „ํ•ด์งˆ ์†Œ์žฌ์˜ ๊ตฌ์กฐ๋ฅผ ๋ฐํ˜€๋‚ด๊ณ  ์ž‘๋™ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ํ•ด์„ํ•˜๋Š”๋ฐ ๊ฐ€์žฅ ๊ธฐ๋ณธ์ ์ด๋ฉด์„œ๋„ ๊ฐ•๋ ฅํ•œ ๊ธฐ์ˆ ์ด๋‹ค. ์ด ๋…ผ๋ฌธ์€ ์ƒˆ๋กœ์šด ์ „๊ทน ๋ฐ ๊ณ ์ฒด ์ „ํ•ด์งˆ ์†Œ์žฌ์˜ ๊ฐœ๋ฐœ๊ณผ, ๋‹จ๊ฒฐ์ • ๋ฐ ๋ถ„๋งX-์„  ๊ฒฐ์ •ํ•™ ๋ถ„์„์„ ํ†ตํ•ด ํ•ด๋‹น ๋ฌผ์งˆ๋“ค์˜ ์ž‘๋™ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๋ถ„์„ํ•œ ์—ฐ๊ตฌ ๊ฒฐ๊ณผ ์‚ฌ๋ก€๋ฅผ ๋‹ค๋ฃจ๊ณ  ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ „์ง€ ํŠน์„ฑ๊ณผ ๊ตฌ์กฐ ๋‚ด ํŠน์ • ์ „ํ•˜ ์บ๋ฆฌ์–ด ์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž… ๋ฐ ํ™•์‚ฐ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๊ทœ๋ช…ํ•˜๊ธฐ ์œ„ํ•ด ab inito ๊ตฌ์กฐ ๊ฒฐ์ •๋ฒ•, 3์ฐจ์› bond-valence sum mapping ๊ณ„์‚ฐ, ์ž์ฒด ์ œ์ž‘ํ•œ in situ cell์„ ํ™œ์šฉํ•œ ์ถฉ/๋ฐฉ์ „ ์ค‘ ์‹ค์‹œ๊ฐ„ ๊ตฌ์กฐ ๋ถ„์„ ๋ฐ ๋‹ค์–‘ํ•œ ์ „๊ธฐ ํ™”ํ•™์  ๋ถ„์„์„ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ํŠนํžˆ, ์ผ๋ฐ˜์ ์œผ๋กœ ๋‹จ๊ฒฐ์ • ๋ฐ์ดํ„ฐ๋ฅผ ์–ป๊ธฐ ํž˜๋“  ๋‹ค์–‘ํ•œ ์ „์ง€ ์†Œ์žฌ๋“ค์˜ ๊ฒฝ์šฐ, ๋ถ„๋ฐœ X-์„  ํšŒ์ ˆ ๋ฐ์ดํ„ฐ๋ฅผ ์‚ฌ์šฉํ•˜๋Š” ๋ฏธ์ง€ ๊ฒฐ์ • ๊ตฌ์กฐ ๋ถ„์„๋ฒ•์„ ํ™œ์šฉํ•ด ๊ทธ ๊ตฌ์กฐ์™€ ์ž‘๋™ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ํ•ด์„ํ•˜์˜€๋‹ค. (1) ์ฒซ ๋ฒˆ์งธ ์—ฐ๊ตฌ๋Š” ์ƒˆ๋กœ์šด ์•”๋ชจ๋Š„ ๋ฐ”๋‚˜๋Š„ ์‚ฐํ™”๋ฌผ ๋ธŒ๋ก ์ฆˆ ๊ณ„์—ด์˜ (NH4)2V7O16๋ฅผ ์ตœ์ดˆ๋กœ ํ•ฉ์„ฑํ•˜๊ณ  ๋‹จ๊ฒฐ์ • X-์„  ํšŒ์ ˆ ๋ฐ์ดํ„ฐ๋ฅผ ํ†ตํ•ด ๊ทธ ๊ตฌ์กฐ๋ฅผ ๊ฒฐ์ •ํ•œ ๊ฒƒ์ด๋‹ค. ์ƒˆ๋กญ๊ฒŒ ๋ฐœ๊ฒฌํ•˜๊ณ  ๊ตฌ์กฐ๋ฅผ ํ•ด์„ํ•œ (NH4)2V7O16์ด ๋ฆฌํŠฌ ์ด์˜จ ์ „์ง€์™€ ์†Œ๋“ ์ด์˜จ ์ „์ง€์˜ ์ „๊ทน ์†Œ์žฌ๋กœ ์ž‘๋™ ๊ฐ€๋Šฅํ•จ์„ ์ „๊ธฐํ™”ํ•™์  ์ถฉ/๋ฐฉ์ „ ์‹คํ—˜์„ ํ†ตํ•ด ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋˜ํ•œ in situ X-์„  ํšŒ์ ˆ ๋ฐ์ดํ„ฐ๋ฅผ ์ธก์ •ํ•˜์—ฌ ์ถฉ/๋ฐฉ์ „ ์ค‘ ์‹ค์‹œ๊ฐ„ ๊ตฌ์กฐ๋ณ€ํ™”๋ฅผ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ์ตœ์ข…์ ์œผ๋กœ ์ถ”๊ฐ€์ ์ธ X-์„  ๊ด‘์ „์ž ๋ถ„๊ด‘๋ฒ•๊ณผ ์›์†Œ ๋ถ„์„์„ ํ†ตํ•ด ๋ฆฌํŠฌ ์ด์˜จ์˜ ์‚ฝ์ž… (๋ฐฉ์ „) ์‹œ ์ธต์ƒ ๊ตฌ์กฐ ์‚ฌ์ด์— ์žˆ๋˜ ์•”๋ชจ๋Š„์ด ๋น ์ ธ๋‚˜์˜ค๊ณ , ๋ฆฌํŠฌ ์ด์˜จ์˜ ํƒˆ์ž… (์ถฉ์ „) ์‹œ ์ „ํ•ด์•ก์œผ๋กœ ๋น ์ ธ๋‚˜์™”๋˜ ์•”๋ชจ๋Š„ ์ด์˜จ์ด ๋‹ค์‹œ ๋“ค์–ด๊ฐ€๋Š” ์ถฉ/๋ฐฉ์ „ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ํ™•์ธ ํ•˜์˜€๋‹ค. ์ƒˆ๋กœ์šด ์•”๋ชจ๋Š„ ๋ฐ”๋‚˜๋“ ๋ธŒ๋ก ์ฆˆ์˜ ๊ฐœ๋ฐœ๊ณผ ๊ตฌ์กฐ ๋ฐ ์ „๊ธฐํ™”ํ•™์  ํŠน์„ฑ์— ๋Œ€ํ•œ ๋ณธ ์—ฐ๊ตฌ ๊ฒฐ๊ณผ๋Š” ์ „๊ทน ๋ฌผ์งˆ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๋‹ค์–‘ํ•œ ๊ธฐ๋Šฅ์„ฑ ๋ฌด๊ธฐ ์†Œ์žฌ๋กœ ์ฃผ๋ชฉ ๋ฐ›๊ณ  ์žˆ๋Š” ๋ฐ”๋‚˜๋“ ์‚ฐํ™”๋ฌผ ๋ธŒ๋กœ์ฆˆ ๊ณ„์—ด ๋ฌผ์งˆ๋“ค ์—ฐ๊ตฌ์— ๋Œ€ํ•œ ์ƒˆ๋กœ์šด ๋ฌผ์งˆ ์ •๋ณด๋ฅผ ์ œ๊ณตํ–ˆ๋‹ค๋Š” ์ ์—์„œ ํ•™์ˆ ์ ์ธ ์˜์˜๊ฐ€ ์žˆ๋‹ค. (2) ๋‘ ๋ฒˆ์งธ ์—ฐ๊ตฌ์—์„œ๋Š” Fe2(MoO4)3์— ๋ฆฌํŠฌ์ด ํƒˆ/์‚ฝ์ž… ๋  ๋•Œ์™€ ์†Œ๋“์ด ํƒˆ/์‚ฝ์ž… ๋  ๋•Œ์˜ ๊ตฌ์กฐ์  ๋ฉ”์ปค๋‹ˆ์ฆ˜ ์ฐจ์ด๋ฅผ ๊ทœ๋ช…ํ•˜์˜€๋‹ค. Fe2(MoO4)3๋Š” ๋ฆฌํŠฌ ์ด์˜จ ์ „์ง€์™€ ์†Œ๋“ ์ด์˜จ ์ „์ง€์˜ ์ „๊ทน ์†Œ์žฌ๋กœ ๋ชจ๋‘ ์‚ฌ์šฉ ๊ฐ€๋Šฅํ•˜๋‹ค. ๋น„๋ก ๊ฐ€์šฉ ์šฉ๋Ÿ‰์ด ~90mAg g-1์ •๋„๋กœ ๋‚ฎ์•„ ๊ธฐ์กด ์ƒ์šฉํ™”๋œ ์–‘๊ทน์†Œ์žฌ๋“ค์— ๋น„ํ•˜๋ฉด ๋ถ€์กฑํ•œ ์„ฑ๋Šฅ์„ ๋ณด์ด์ง€๋งŒ ํ•ด๋‹น ๋ฌผ์งˆ์€ ๋ฆฌํŠฌ ์ด์˜จ ์ „์ง€์™€ ์†Œ๋“ ์ด์˜จ ์ „์ง€์—์„œ์˜ ์ž‘๋™ ๋ฉ”์ปค๋‹ˆ์ฆ˜์ด ์ƒ์ดํ•ด ์ตœ๊ทผ ๋ช‡ ๋…„ ์‚ฌ์ด ํ•™๊ณ„์˜ ๋งŽ์€ ๊ด€์‹ฌ์„ ๋ฐ›๊ณ  ์žˆ๋‹ค. ๋ฆฌํŠฌ ์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž… ์‹œ์—๋Š” single-phase ๋ฐ˜์‘์„, ์†Œ๋“ ์ด์˜จ์˜ ๊ฒฝ์šฐ์—๋Š” two-phase ๋ฐ˜์‘์„ ๋‚˜ํƒ€๋‚ธ๋‹ค. ๋ช‡ ์—ฐ๊ตฌ ํŒ€์—์„œ ๋ณธ ํƒˆ/์‚ฝ์ž… ๋ฉ”์ปค๋‹ˆ์ฆ˜ ์ฐจ์ด์— ๋Œ€ํ•œ ์›์ธ์„ ๋ถ„์„ํ•˜๋Š” ์—ฐ๊ตฌ ๊ฒฐ๊ณผ๋ฅผ ๋ณด๊ณ ํ•˜์˜€์ง€๋งŒ ๋Œ€๋ถ€๋ถ„ ์–‘์ž ๊ณ„์‚ฐ๋ฒ•์„ ํ™œ์šฉํ•œ ์˜ˆ์ธก์ด์—ˆ๊ณ  ํ•ด๋‹น ๊ฒฐ๊ณผ๋„ ๊ฒฐ์ •ํ•™์ ์œผ๋กœ ๋ถˆ๊ฐ€๋Šฅํ•œ ๊ตฌ์กฐ๋ฅผ ์ œ์‹œํ•œ๋‹ค๋Š” ์ ์—์„œ ์‹ ๋ขฐ์„ฑ์ด ๋–จ์–ด์กŒ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์†Œ๋“ ์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž… ์‹œ ๊ตฌ์กฐ ๋ณ€ํ™”๋ฅผ in situ ์ธก์ •์„ ํ†ตํ•ด ํ™•์ธํ•˜๊ณ , ์†Œ๋“ ์‚ฝ์ž… ํ›„ Na2Fe2(MO4)3 ์˜ ๊ตฌ์กฐ๋ฅผ ๋ถ„๋ง X-์„ ์„ ํ†ตํ•œ ๋ฏธ์ง€ ๊ตฌ์กฐ ๊ฒฐ์ •๋ฒ•์œผ๋กœ ๋ฐํ˜€๋‚ด์—ˆ๋‹ค. ํ•ด๋‹น ๊ฒฐ๊ณผ์™€ bond valence sum mapping ๊ฒฐ๊ณผ๋ฅผ ๋ณตํ•ฉ์ ์œผ๋กœ ํ™œ์šฉ, ํ•ด๋‹น ๋ฌผ์งˆ์—์„œ์˜ ๋ฆฌํŠฌ๊ณผ ์†Œ๋“ ์ด์˜จ์˜ ์ƒ์ดํ•œ ํƒˆ/์‚ฝ์ž… ๋ฉ”์ปค๋‹ˆ์ฆ˜์ด guest-ion ์˜ ์‚ฌ์ด์ฆˆ์™€ ๊ตฌ์กฐ ๋‚ด ํƒˆ/์‚ฝ์ž… ๊ฐ€๋Šฅํ•œ ๊ฒฐ์ • ๊ตฌ์กฐ ๋‚ด ๋นˆ ๊ณต๊ฐ„ ์ฃผ๋ณ€์˜ ์Œ์ด์˜จ (์‚ฐ์†Œ ์ด์˜จ) ์œ„์น˜ ๋ฐ ๊ฑฐ๋ฆฌ์™€ ๋ฐ€์ ‘ํ•œ ๊ด€๊ณ„๊ฐ€ ์žˆ์Œ์„ ๋ฐํ˜€๋‚ด์—ˆ๋‹ค. ๊ฒฐ๋ก ์ ์œผ๋กœ ๋ณธ ์—ฐ๊ตฌ๋Š” ๋‹ค์–‘ํ•œ ์ „๊ทน ์†Œ์žฌ ๋ฐ ๊ณ ์ฒด ์ „ํ•ด์งˆ์—์„œ์˜ ํƒˆ/์‚ฝ์ž… ๋˜๋Š” ์ด์˜จ ํ™•์‚ฐ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ํ•ด์„ํ•˜๊ณ  ์˜ˆ์ธกํ•˜๋Š” ๋ฐ ์žˆ์–ด X-์„  ํšŒ์ ˆ ๊ฒฐ์ • ๋ถ„์„์˜ ํ™œ์šฉ๋ฒ•์„ ์ œ์‹œํ•ด์ค€๋‹ค. (3) ์„ธ ๋ฒˆ์งธ ์—ฐ๊ตฌ๋Š” ์ƒˆ๋กœ์šด ์†Œ๋“ ์ด์˜จ ๊ณ ์ฒด ์ „ํ•ด์งˆ, Na4โˆ’xSn1โˆ’xSbxS4 (0.02 โ‰ค x โ‰ค 0.33) ์— ๋Œ€ํ•œ ๊ตฌ์กฐ ๋ถ„์„๊ณผ ์ž‘๋™ ๋ฉ”์ปค๋‹ˆ์ฆ˜ ๊ทœ๋ช…, ๊ทธ๋ฆฌ๊ณ  ์†Œ๋“ ์ด์˜จ ์ „๋„์„ฑ ์ธก์ •๊ณผ ์ „๊ณ ์ฒด ์ „์ง€์˜ ๊ณ ์ฒด ์ „ํ•ด์งˆ๋กœ์จ ํ™œ์šฉ ๊ฐ€๋Šฅ์„ฑ์— ๋Œ€ํ•œ ๊ฒฐ๊ณผ์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋Š” ํ•œ์–‘๋Œ€ํ•™๊ต ์ •์œค์„ ๊ต์ˆ˜๋‹˜ ์—ฐ๊ตฌ์‹ค๊ณผ ๊ณต๋™์œผ๋กœ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ์†Œ๋“ ์ด์˜จ์— ๋Œ€ํ•ด ๋ถ€๋„์ฒด์ธ Na4SnS4์— ์†Œ๋Ÿ‰์˜ Sb ์ฒจ๊ฐ€๋งŒ์œผ๋กœ ๊ฒฐ์ • ๊ตฌ์กฐ๊ฐ€ ์™„์ „ํžˆ ๋ฐ”๋€Œ๊ฒŒ ๋˜๊ณ  ์ „๋„์„ฑ์„ ๊ฐ–๊ฒŒ ๋˜๋Š” ๊ฒƒ์„ ๋ฐœ๊ฒฌํ•˜์˜€๋‹ค. ๋ถ„๋ง X-์„  ํšŒ์ ˆ ๋ฐ์ดํ„ฐ๋ฅผ ํ†ตํ•œ ๋ฏธ์ง€ ๊ฒฐ์ • ๊ตฌ์กฐ ๋ถ„์„๋ฒ•์„ ํ™œ์šฉํ•ด ์ƒˆ๋กœ์šด ๊ณ ์ฒด ์ „ํ•ด์งˆNa4โˆ’xSn1โˆ’xSbxS4์˜ ๊ตฌ์กฐ๋ฅผ ๊ฒฐ์ •ํ•˜์˜€๋‹ค. ๋ฐํ˜€์ง„ ํ•ด๋‹น ๊ตฌ์กฐ ์ •๋ณด์™€ bond valence sum mapping ์„ ํ†ตํ•ด ํ•ด๋‹น ๋ฌผ์งˆ์ด ์†Œ๋“ ์ด์˜จ์— ๋Œ€ํ•ด ์ „๋„์„ฑ์„ ๊ฐ–๋Š” ์ด์œ ์™€ ๊ตฌ์กฐ ๋‚ด ์ด์˜จ ์ „๋„ ๊ฒฝ๋กœ๋ฅผ ๊ทœ๋ช…ํ•˜์˜€๋‹ค. ์ƒˆ๋กœ์šด ๊ณ ์ฒด ์ „ํ•ด์งˆ์˜ ๊ฐœ๋ฐœ๊ณผ ๊ตฌ์กฐํ•ด์„์„ ํ†ตํ•œ ์ž‘๋™ ๋ฉ”์ปค๋‹ˆ์ฆ˜์— ๋Œ€ํ•œ ๋ช…ํ™•ํ•œ ๋ถ„์„ ๊ฒฐ๊ณผ๋Š” ์ „๊ณ ์ฒด ์ „์ง€ ๊ธฐ์ˆ  ์—ฐ๊ตฌ์— ์ƒˆ๋กœ์šด ๊ด€์ ์„ ์ œ๊ณตํ•œ๋‹ค. (4) ๋„ค ๋ฒˆ์งธ ์—ฐ๊ตฌ๋Š” ์ฐจ์„ธ๋Œ€ ์ „์ง€ ์ค‘ ํ•˜๋‚˜์ธ ํฌํƒ€์Š˜ ์ด์˜จ ์ „์ง€์˜ ์–‘๊ทน ์†Œ์žฌ์— ๋Œ€ํ•œ ๊ฒƒ์ด๋‹ค. rhombohedral prussian blue ๊ณ„์—ด์˜ K1.88Zn2.88[Fe(CN)6]2(H2O)5 ๋Š” ๊ตฌ์กฐ ๋‚ด ์ปค๋‹ค๋ž€ cavity-site์— ํฌํƒ€์Š˜ ์ด์˜จ์ด ์ ์ ˆํžˆ ์œ„์น˜ํ•˜๊ณ  ์žˆ๋Š” ๋ฌผ์งˆ๋กœ, ํฌํƒ€์Š˜ ์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž…์— ์œ ๋ฆฌํ•œ ๊ตฌ์กฐ์  ํŠน์„ฑ์„ ๊ฐ–์ถ”๊ณ  ์žˆ๋‹ค. ์ด์— ๊ทผ๊ฑฐํ•˜์—ฌ ํ•ด๋‹น ๋ฌผ์งˆ์„ ํฌํƒ€์Š˜ ์ด์˜จ ์ „์ง€ ์†Œ์žฌ๋กœ ํ™œ์šฉํ•œ ๊ฒฐ๊ณผ 3.9 V ์˜ ๋†’์€ ๊ตฌ๋™ ์ „์••๊ณผ ํ•จ๊ป˜ ์•ˆ์ •์ ์ธ ์ถฉ/๋ฐฉ์ „ ์„ฑ๋Šฅ์„ ๋‚˜ํƒ€๋‚ด์—ˆ๋‹ค. ์ƒ๋Œ€์ ์œผ๋กœ ์ปค๋‹ค๋ž€ ์‚ฌ์ด์ฆˆ๋ฅผ ๊ฐ–๊ณ  ์žˆ๋Š” ํฌํƒ€์Š˜ ์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž…์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ  ์•ฝ 3% ์ •๋„์˜ ๋ฏธ๋ฏธํ•œ ๋‹จ์œ„ ์…€ ๋ถ€ํ”ผ ๋ณ€ํ™”๊ฐ€ ์ผ์–ด๋‚จ์„ in situ X-์„  ํšŒ์ ˆ ๋ถ„์„์„ ํ†ตํ•ด ํ™•์ธ ํ•  ์ˆ˜ ์žˆ์—ˆ๊ณ  ์ด๋Ÿฐ ๊ตฌ์กฐ์  ํŠน์„ฑ์€ ์•ˆ์ •์ ์ธ ์ถฉ/๋ฐฉ์ „ ์„ฑ๋Šฅ์˜ ์ฃผ๋œ ์š”์ธ์œผ๋กœ ์—ฌ๊ฒจ์ง„๋‹ค. ๋˜ํ•œ ๋‹ค์–‘ํ•œ SOC ์ƒํƒœ์˜ K1.88Zn2.88[Fe(CN)6]2(H2O)5 (0 โ‰ค x โ‰ค 1.88) ๋ถ„๋ง X-์„  ํšŒ์ ˆ ๋ฐ์ดํ„ฐ๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ ์–ป์€ Fourier ์ „์ž ๋ฐ€๋„๋ฅผ ํ†ตํ•ด ํฌํƒ€์Š˜ ์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž… ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์›์ž ๋ถ„์„ ์ˆ˜์ค€์—์„œ ํ™•์ธํ•˜์˜€๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋Š” ํฌํƒ€์Š˜ ์ด์˜จ ์ „์ง€ ์ „๊ทน ์†Œ์žฌ์˜ ์ถฉ/๋ฐฉ์ „ ์•ˆ์ •์„ฑ์„ ๊ฒฐ์ •ํ•˜๋Š” ๊ตฌ์กฐ์  ์š”์†Œ์— ๋Œ€ํ•œ ์œ ์šฉํ•œ ํ†ต์ฐฐ๋ ฅ์„ ์ œ๊ณตํ•œ๋‹ค. (5) ๋งˆ์ง€๋ง‰ ์—ฐ๊ตฌ๋Š” ์œ„์™€ ๋งˆ์ฐฌ๊ฐ€์ง€๋กœ ์ฐจ์„ธ๋Œ€ ์ „์ง€ ์ค‘ ํ•˜๋‚˜์ธ ์นผ์Š˜ ์ด์˜จ ์ „์ง€์˜ ์–‘๊ทน ์†Œ์žฌ์— ๋Œ€ํ•œ ๊ฒƒ์ด๋‹ค. ์นผ์Š˜ ์ด์˜จ ์ „์ง€๋Š” ๋‹ค๊ฐ€ ์ด์˜จ ์ „์ง€ ์ค‘ ํ•˜๋‚˜๋กœ ํ˜„์žฌ ์ •์ƒ์ ์œผ๋กœ ๊ตฌ๋™ ๊ฐ€๋Šฅํ•˜๋‹ค๊ณ  ๋ณด๊ณ ๋œ ์–‘๊ทน ๋ฐ ์Œ๊ทน ์†Œ์žฌ์˜ ์ˆ˜๊ฐ€ ์ ˆ๋Œ€์ ์œผ๋กœ ๋ถ€์กฑํ•œ ๊ต‰์žฅํžˆ ๋„์ ์ ์ธ ์—ฐ๊ตฌ ๋ถ„์•ผ ์ค‘ ํ•˜๋‚˜์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” NASICON ๊ตฌ์กฐ๋ฅผ ๊ฐ–๊ณ  ์žˆ์œผ๋ฉฐ ๋Œ€ํ‘œ์ ์ธ ์†Œ๋“ ์ด์˜จ ์ „์ง€ ์–‘๊ทน ์†Œ์žฌ์ธ Na3V2(PO4)3 ์—์„œ ํ™”ํ•™์ ์œผ๋กœ Na์„ ์ผ๋ถ€ ์ œ๊ฑฐํ•œ NaV2(PO4)3์— ๊ฐ€์—ญ์ ์ธ ์นผ์Š˜ ์ด์˜จ ํƒˆ/์‚ฝ์ž…์ด ๊ฐ€๋Šฅํ•˜๋‹ค๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. CaI2๋ฅผ ํ™˜์›์ œ๋กœ ์‚ฌ์šฉ, ํ•ด๋‹น ๋ฌผ์งˆ์— ํ™”ํ•™์ ์œผ๋กœ ์นผ์Š˜์„ ์‚ฝ์ž…์‹œ์ผœ ์„ฑ๊ณต์ ์œผ๋กœ CaxNaV2(PO4)3๋ฅผ ํ•ฉ์„ฑํ•˜์˜€๋‹ค. ๋ถ„๋ง X-์„  ํšŒ์ ˆ ๋ฐ์ดํ„ฐ๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ ์–ป์€ Fourier ์ „์ž ๋ฐ€๋„ ๋ถ„์„์„ ํ†ตํ•ด CaxNaV2(PO4)3์˜ ๊ตฌ์กฐ๋ฅผ ํ•ด์„ํ•˜์˜€๊ณ , ์ด ๊ฒฐ๊ณผ์™€ ์ถ”๊ฐ€์ ์ธ ์›์†Œ ๋ถ„์„ ๊ฒฐ๊ณผ๋ฅผ ํ†ตํ•ด ํ•ด๋‹น NASICON ๊ตฌ์กฐ์— Ca์ด ์‚ฝ์ž…๋˜์–ด ์žˆ์Œ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ํ™”ํ•™์ ์œผ๋กœ ์นผ์Š˜์ด ์‚ฝ์ž…๋˜๋Š” ๋™์•ˆ์˜ ๊ตฌ์กฐ ๋ณ€ํ™”๋ฅผ in situ X-์„  ํšŒ์ ˆ ๋ถ„์„์„ ํ†ตํ•ด ์‹ค์‹œ๊ฐ„์œผ๋กœ ๊ด€์ฐฐํ•œ ๊ฒฐ๊ณผ, two-phase ๋ฐ˜์‘์— ๊ธฐ๋ฐ˜ํ•ด ์นผ์Š˜์ด ์‚ฝ์ž…๋จ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๊ตฌ์กฐ์ ์œผ๋กœ ์นผ์Š˜ ์ด์˜จ์˜ ์‚ฝ์ž…์ด ๊ฐ€๋Šฅํ•˜๋‹ค๋Š” ์œ„ ๊ฒฐ๊ณผ์— ๊ทผ๊ฑฐํ•ด NaV2(PO4)3 ์„ ์œ ๊ธฐ ์ „ํ•ด์•ก์„ ์‚ฌ์šฉํ•œ ์นผ์Š˜ ์ด์˜จ์˜ ์–‘๊ทน ์†Œ์žฌ๋กœ ํ…Œ์ŠคํŠธ ํ•ด๋ณธ ๊ฒฐ๊ณผ, ๊ณ ์˜จ (75โ„ƒ) ์—์„œ ์ดˆ๊ธฐ 5 cycle์˜ ํ™œ์„ฑํ™” ๊ฑฐ์นœ ๋’ค, ์ƒ์˜จ์—์„œ ๊ฐ€์—ญ์ ์ธ ์ถฉ/๋ฐฉ์ „ ์šฉ๋Ÿ‰ (~116 mAg g-1) ์„ ํ™•์ธ ํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ ๊ฒฐ๊ณผ๋Š” ๊ต‰์žฅํžˆ ๋„์ „์ ์ธ ์ฃผ์ œ๋กœ ์ธ์‹๋˜๊ณ  ์žˆ๋Š” ์นผ์Š˜ ์ด์˜จ ์ „์ง€์˜ ์–‘๊ทน ์†Œ์žฌ ๊ฐœ๋ฐœ์— ์ƒˆ๋กœ์šด ๊ฐ€๋Šฅ์„ฑ์„ ์ œ์‹œํ•œ๋‹ค. ๊ณ ์ฐจ์›์ ์ธ X-์„  ํšŒ์ ˆ ๋ถ„์„์„ ํ†ตํ•ด, ํŠน์ • ์ด์˜จ์˜ ํƒˆ/์‚ฝ์ž…์œผ๋กœ ๊ตฌ๋™๋˜๋Š” ์ด์ฐจ ์ „์ง€ ์‹œ์Šคํ…œ์˜ ์ „๊ทน ์†Œ์žฌ ๋ฐ ๊ณ ์ฒด ์ „ํ•ด์งˆ์„ ๋ฐœ๊ฒฌํ•˜๊ณ  ๊ตฌ์กฐ์  ์ž‘๋™ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๊ทœ๋ช…ํ•œ ๋ณธ ๋…ผ๋ฌธ์€ ๊ฒฐ์ • ๊ตฌ์กฐ์™€ ๋ฐ€์ ‘ํ•œ ๊ด€๊ณ„๊ฐ€ ์žˆ๋Š” ๋ฌด๊ธฐ ์—๋„ˆ์ง€ ์†Œ์žฌ๋“ค์˜ ํŠน์„ฑ์„ ์ดํ•ดํ•˜๊ณ , ์ด๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ ์ƒˆ๋กœ์šด ์†Œ์žฌ ๊ฐœ๋ฐœ ๋ฐ ์„ฑ๋Šฅ ๊ฐœ์„ ์„ ์œ„ํ•œ ๊ทผ๋ณธ์ ์ด๋ฉด์„œ๋„ ํ•„์ˆ˜์ ์ธ ๊ฒฐ์ •ํ•™์  ํ†ต์ฐฐ์„ ์ œ๊ณตํ•œ๋‹ค. |Structural information is crucial for creating new functional materials and for understanding and adjusting the properties of materials. Among the various functional materials, the properties of battery materials (cathode, anode and solid electrolyte) are particularly closely related to its structure, because the operation of rechargeable batteries is based on the intercalation and diffusion of charge-carrier ions in solids. Therefore, understanding the structural mechanism during charge/discharge and establishing the structure-properties relationship are basic priorities to improve existing or develop novel battery materials. Crystallographic analysis of X-ray diffraction data associated with electrochemical tests provides the most essential information to bridge the structural characteristics with battery performance. This dissertation discusses the development of new electrode materials and solid electrolytes, and understating their working mechanism through ab initio structure determination via powder X-ray diffraction data as well as single-crystal data. In order to unveil the working mechanism of each material covered in here, 3D bond-valence sum difference map calculation, in situ analysis technique, and various additional chemical (electron microscopy, X-ray photoelectron spectroscopy, Fourier transform infrared) and electrochemical analyses (galvanostatic test, cyclic voltammetry, kinetic analysis) were conducted. (1) The first section is a discovery of new ammonium vanadium bronze as an electrode material for rechargeable batteries by using single-crystal X-ray diffraction data. The novel ammonium vanadium bronze, (NH4)2V7O6 has been synthesized via a facile hydrothermal method and its structure in the triclinic space group P1 ฬ… is determined by single-crystal data. A reversible electrochemical intercalation of Li ions into (NH4)2V7O6 has been evaluated by galvanostatic cycling. It also revealed that the NH4+ accommodated between Vโ€“O layer plays a very crucial role in the electrochemical characteristics. On discharge, Li ions are intercalated while the NH4+ is simultaneously de-intercalated from the structure. On charge, a reverse reaction takes placea small amount of NH4+ re-accommodates between the layers, ensuring structural stability and allowing all Li ions to extract. In addition, the electrochemical results suggesting the feasibility of (NH4)2V7O6 as an electrode material for Na-ion batteries are briefly presented. (2) The second study provides a crucial crystallographic rationale to understand the difference in the intercalation mechanism of Fe2(MoO4)3 between lithiation and sodiation by structural analyses using powder X-ray diffraction data. Monoclinic Fe2(MoO4)3 shows distinct structural and electrochemical differences in the intercalation mechanism, depending on the guest ion: a single-phase reaction in a Na-ion cell, but a two-phase reaction in a Li-ion cell. Attempts to understand the difference in the mechanisMaster have been hindered by a lack of structural information on the fully sodiated phase Na2Fe2(MoO4)3 due to its structural complexity and the unavailability of a single crystal. In this work, the crystal structure of Na2Fe2(MoO4)3 have been solved and refined for the first time, using the technique of ab initio structure determination from powder diffraction data. Along with electrochemical and structural characterization, 3D bond valence sum difference map calculations enabled us to ascertain the decisive factors that determine such differences, in terMaster of the interatomic distance and coordination environment of a guest ion. In the case of Na insertion, only a slight expansion of the structure makes the cavity sites of Fe2(MoO4)3 suitable for Na ions, with adequate distances and coordination with surrounding oxygen atoMaster, resulting in a solid-solution-type single-phase reaction. In the case of Li insertion, the cavity sites are so large for a Li ion that a significant structural change involving tilting of the FeO6 and MoO4 polyhedra is required to accommodate the Li ion in a suitable local environment, which does not allow a continuous structural change but results in a two-phase reaction. (3) The following study introduces a novel structure sulfide Naโ€ion solid electrolyte, and unveil the sodium diffusion mechanism by using ab initio structure determination process via powder X-ray diffraction data. Sulfide Na-ion solid electrolytes are key to enable roomโ€temperature operable allโ€solidโ€state Naโ€ion batteries that are attractive for largeโ€scale energy storage applications. Herein, the discovery of a new structural class of tetragonal Na4โˆ’xSn1โˆ’xSbxS4 (0.02 โ‰ค x โ‰ค 0.33) with space group I41/acd is described. The evolution of a new phase, distinctly different from Na4SnS4 or Na3SbS4, allows fast ionic conduction in 3D pathways (0.2โ€“0.5 Master cmโˆ’1 at 30 ยฐC). In the fourth, and final sessions present the development of a new cathode material for next-generation battery candidates, K- and Ca-ion batteries, and the investigation of their working mechanism via structural analysis. (4) K-ion batteries have received attention as an alternative to Li-based batteries due to the earth abundance and low redox potential of potassium metal. Herein, rhombohedral potassium zinc hexacyanoferrate K1.88Zn2.88[Fe(CN)6]2(H2O)5 is demonstrated as a cathode material with a high-voltage and favorable cyclability for non-aqueous K-ion batteries: an initial discharge capacity of 55.6 mAh gโˆ’1, an operating voltage of 3.9 V (vs. K/K+), and a capacity retention of ~95% after 100 cycles. The Fourier maps from powder X-ray diffraction data and elemental analysis at each different state-of-charge clearly demonstrate that the potassium-ions intercalation. The operando XRD technique reveal a reversible structural evolution during cycle. The results provide a general insight into the development of electrode materials for potassium-ion batteries. (5) Among the various multivalent ions, Ca has recently begun to receive attention for rechargeable batteries due to its lower redox potential than the other candidate multivalent charge-carrier ions (Mg2+, Zn2+, Al3+). Herein, the feasibility of NASICON-structured NaV2(PO4)3 as a cathode material for Ca-ion batteries is demonstrated. A crystal structure of CaxNaV2(PO4)3 prepared by chemical Ca insertion was identified with elemental analysis, in-situ and Fourier electron densities from powder X-ray diffraction data, suggesting that the NaV2(PO4)3 has a suitable structure as a host for Ca ion intercalation. In our electrochemical test, Ca ions are reversibly intercalated into the NaV2(PO4)3 using an electrolyte with 0.5M Ca(BF4)2 in EC/PC (1:1 v/v). After a few initial cycles for activation at 75โ„ƒ, NaV2(PO4)3 shows the reversible cycle performance with a discharge capacity of 117 mAg g-1 and favorable capacity retention (99 mAh g-1 after 50 cycles) in room temperature (25โ„ƒ). It is the first report on using NASICON-structured NaV2(PO4) as a cathode material for Ca batteries.openAbstract i List of contents iv List of tables ix List of figures xiv โ… . INTRODUCTION 1 โ…ก. THEORY 2.1 Crystallography 11 2.1.1 X-ray Diffraction and Crystal Structure 11 2.1.2 Ab initio Structure Determination via Powder XRD data 13 2.1.2.1 Unit cell Determination (Indexing) 15 2.1.2.2 Space group Determination 15 2.1.2.3 Extraction of Diffraction Intensities from the Powder XRD data 15 2.1.2.4 Fourier synthesis electron density and phase problem 16 2.1.2.5 Structure Solution AlgorithMaster 18 2.1.2.6 Difference Fourier Synthesis 19 2.1.2.7 Rietveld refinement 20 2.2 Bond Valence Sum Map 21 2.2.1 Bond Valence 21 2.2.2 Bond Valence Sum 22 2.2.3 Three-Dimensional Bond Valence Sum Mapping 22 2.3 Electrochemistry 23 2.3.1 Electromotive Force 23 2.3.2 Electrode Potential 23 2.3.3 Energy Storage 24 2.3.4 Types of Battery 25 2.4 References 25 โ…ข. New Class Structure of Ammonium Vanadium Bronze, (NH4)2V7O16 as an Electrode Material for Rechargeable Batteries 3.1 Introduction 28 3.2 Experimental 29 3.2.1 Materials Synthesis 29 3.2.2 Materials Characterization 29 3.2.3 Single-crystal XRD and Structure Determination 29 3.2.4 Electrochemical Characterization 31 3.3 Results and discussion 32 3.3.1 Characterization of (NH4)2V7O16 32 3.3.2 Electrochemical Characterization of (NH4)2V7O16 38 3.4 Conclusions 44 3.5 References 45 โ…ฃ. Unveiling the Intercalation Mechanism in Fe2(MoO4)3 as a Cathode Material for Na-Ion Batteries by Structural Determination 4.1 Introduction 51 4.2 Experimental 53 4.2.1 Synthesis 53 4.2.2 Material Characterization 53 4.2.3 Electrochemical Characterization 53 4.2.4 Structural Characterization 55 4.2.5 Structural Determination 56 4.2.6 Bond Valence Sum Maps 56 4.3 Results and discussion 57 4.3.1 Characterization of the Synthesized FMO 57 4.3.2 Electrochemical Preparation of Na2FMO 64 4.3.3 Evolution of Crystal Structure during cycle 64 4.3.4 Structural Determination of Na2FMO 66 4.3.5 XPS Results 81 4.3.6 Na Diffusion Pathways Calculated from BVS-DMaster 83 4.3.7 The Difference between Li and Na Intercalation MechanisMaster 83 4.4 Conclusions 85 4.5 References 86 โ…ค. New Na superionic conductors Na4-xSn1-xSbxS4 (0.02 โ‰ค x โ‰ค 0.33) for all-solid-state Na-ion batteries 5.1 Introduction 90 5.2 Experimental 91 5.2.1 Preparation of Materials 91 5.2.2 Materials Characterization 92 5.2.3 Structure Determination 92 5.2.4 Electrochemical Characterization 93 5.3 Results and discussion 94 5.3.1 Characterization of Na4-xSn1-xSbxS4 (0.02 โ‰ค x โ‰ค 0.33) 94 5.3.2 Structural Determination and Ionic Conduction Mechanism 98 5.4 Conclusions 109 5.5 References 110 โ…ฅ. Rhombohedral Potassium Zinc Hexacyanoferrate as Cathode Material for Nonaqueous Potassium-Ion Batteries 6.1 Introduction 113 6.2 Experimental 116 6.2.1 Synthesis and electrochemical characterization 116 6.2.2 Structural analysis 117 6.3 Results and discussion 118 6.3.1 Synthesis of potassium zinc hexacyanoferrate 118 6.3.2 Electrochemical characterization 122 6.3.3 Crystal structure 127 6.4 Conclusions 135 6.5 References 135 โ…ฆ. New Ca-ion Intercalation Chemistry of NASICON Structure NaV2(PO4)3 for a Cathode Material of Ca-ion Batteries 7.1. Introduction 141 7.2 Experimental 142 7.2.1 Materials Synthesis 142 7.2.2 Materials Characterization 142 7.2.3 Chemical-Calciation 143 7.2.4 Electrochemical Ca-ion Intercalation 144 7.2.5 Structure Determination 145 7.3 Results and discussion 146 7.3.1 Chemical-Calciation Structural Analysis 146 7.3.2 Electrochemical Characterization 151 7.4 Conclusions 152 7.5 References 153 Summary (in Korean) 155DOCTORdCollectio

    Unveiling the Intercalation Mechanism in Fe2(MoO4)3 as an Electrode Material for Na-Ion Batteries by Structural Determination

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    Monoclinic Fe2(MoO4)3 (FMO) shows distinct structural and electrochemical differences in the intercalation mechanism, depending on the guest ion.(1,2)FMO undergoes a single-phase reaction in a Na-ion cell, but a two-phase reaction in a Li-ion cell. Attempts to understand the difference in the mechanisms have been hindered by a lack of structural information on the fully sodiated phase Na2Fe2(MoO4)3 due to its structural complexity and the unavailability of a single crystal. In this work, we have solved and refined the crystal structure of Na2Fe2(MoO4)3 for the first time, using the technique of ab initio structure determination from powder diffraction data. Along with electrochemical and structural characterization, 3D bond valence sum difference map calculations enabled us to ascertain the decisive factors that determine such differences, in terms of the interatomic distance and coordination environment of a guest ion. In the case of Na insertion, only a slight expansion of the structure makes the cavity sites of FMO suitable for Na ions, with adequate distances and coordination with surrounding oxygen atoms, resulting in a solid-solution-type single-phase reaction. In the case of Li insertion, the cavity sites are so large for a Li ion that a significant structural change involving tilting of the FeO6 and MoO4 polyhedra is required to accommodate the Li ion in a suitable local environment, which does not allow a continuous structural change but results in a two-phase reaction. ยฉ 2018 American Chemical Society.1

    High Potassium Storage Capability of H 2

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    Potassium-ion batteries (KIBs) are one of the potential candidates for large-scale energy storage devices with low cost due to the abundance of potassium resources. However, the development of cathode materials with high capacity and structural stability has been a challenge due to the difficulties of intercalation of the large size of K-ions into host materials. In this work, H2V3O8 (or V3O7โ‹…H2O) is reported as a new cathode material for KIBs. It shows reversible potassium-intercalation behavior with the first discharge capacity of 168 mAh gโˆ’1 at 5 mA gโˆ’1 and an average discharge voltage of โˆผ2.5 V (vs. K/K+) in 0.5 M KPF6 in EC/DEC (1:1 v/v). The specific capacity increases up to 181 mAh gโˆ’1 for the third cycle and gradually decreases with 75% of the capacity retention after 100 cycles. The chemical formula of the potassiated phase is K1.77H2V3O8. However, scan-rate dependent cyclic voltammetry and elemental analyses suggest that โˆผ28% of the capacity comes from the surface K ions on the H2V3O8 particles; thus, the bulk-intercalated phase can be formulated as K1.27H2V3O8. The crystal structure is stable during the electrochemical cycling, keeping the structural water, confirming that H2V3O8 can be considered as one of the high-capacity cathode materials for KIBs. ยฉ 2019 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim1

    Silver vanadium bronze, beta-Ag0.33V2O5: crystal-water-free high-capacity cathode material for rechargeable Ca-ion batteries

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    Calcium-ion batteries (CIBs) are getting increasing attention as post-lithium-ion batteries owing to their theoretical and potential advantages in terms of energy density and cost-effectiveness. However, most of the reported cathode materials suffer from low capacity or cyclability in dried nonaqueous electrolytes. So far, all of the materials with high capacity (>100 mA h gโˆ’1) contain crystal water, which was considered to be crucial to the structural stability, enabling facile Ca diffusion. Here, we report ฮฒ-Ag0.33V2O5as a high-capacity cathode material for CIBs without crystal water. After the initial activation process, the material exhibited a capacity of 179 mA h gโˆ’1at approximately 2.8 V (vs.Ca2+/Ca) in the ninth cycle and showed a modest cycling performance. The capacity is the highest among the Ca cathode materials without crystal water reported to date. We revealed that the activation process was caused by a replacement reaction between the silver and calcium ions. This material demonstrates that crystal water is not an essential component of CIB electrode materials for a high capacity, stimulating the ongoing research for developing higher-performance materials. ยฉ The Royal Society of Chemistry 2021.FALS

    Ammonium Vanadium Bronze, (NH4)2V7O16, as a New Lithium Intercalation Host Material

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    A new type of ammonium vanadium bronze, (NH4)2V7O16, was synthesized by the hydrothermal method. The triclinic crystal structure (P1¯) is successfully identified by the single-crystal X-ray diffraction method. The layered structure is similar to that of other vanadium bronzes but with an unprecedented stoichiometry and crystal structure. The structure is composed of a stack of V7O16 layers along the c axis, and two NH4 + ions occupy the interlayer space per formula unit. Each ammonium ion is hydrogen-bonded to four lattice oxygen atoms, resulting in a stable structure with a large interlayer space, thus enabling the intercalation of various guest ions. Lithium ions are electrochemically intercalated into (NH4)2V7O16, with an initial discharge capacity of 232 mAh g-1 and an average discharge voltage of 2 V (vs Li/Li+). Upon the first discharge, lithium ions are inserted, whereas ammonium ions are extracted. Upon charging, a reverse reaction takes place. However, only a fraction of the extracted ammonium ions are reaccommodated. Despite the small quantity, the reinsertion of ammonium ions contributes crucially to the structural stability, improving the electrochemical performance. These results could provide a general understanding of the intercalation mechanism of host materials containing ammonium ions. In addition, (NH4)2V7O16 intercalates Na+ ions reversibly, implying a potential capability as a host material for other guest ions. ยฉ 2020 American Chemical Society.1

    Double-Sheet Vanadium Oxide as a Cathode Material for Calcium-Ion Batteries

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    Calcium-ion batteries (CIBs) are theoretically considered one of the potential post-lithium-ion battery technologies. However, only a few host materials are known to intercalate Ca ions. Herein, we demonstrate the use of double-sheet vanadium oxide V2O5 โ‹… 0.63H2O as a high-performance cathode material for CIBs. The vanadium oxide was synthesized via an electrochemical oxidation process on a graphite foil substrate. The material exhibited a high reversible capacity of 204 mAh gโˆ’1 at a 0.1 C rate in an aqueous electrolyte, with an average discharge voltage of 2.76 V vs. Ca/Ca2+, and a capacity retention of 86% after 350 cycles. The reaction mechanism can be described as a combination of diffusion-controlled intercalation and surface-limited pseudo-capacitance reactions. This study provides a new type of Ca host material, motivating further development of new CIB cathode materials. ยฉ 2020 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim1

    Electrochemical Exchange Reaction Mechanism and the Role of Additive Water to Stabilize the Structure of VOPO 4 โ‹…2 H 2 O as a Cathode Material for Potassium-Ion Batteries

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    VOPO 4 โ‹…2 H 2 O is demonstrated as a cathode material for potassium-ion batteries in 0.6 m KPF 6 in ethylene carbonate/diethyl carbonate, and its distinct exchange reaction mechanism between potassium and crystal water is reported. In an anhydrous electrolyte, the cathode shows an initial capacity of approximately 90 mAh g โˆ’1 , with poor capacity retention (32 % after 50 cycles). In contrast, the capacity retention dramatically improved (86 % after 100 cycles) in a wet electrolyte containing 0.1 m of additive water. VOPO 4 โ‹…2 H 2 O contains two types of water (structural and crystal). Upon discharge, potassium ions are intercalated whereas the crystal water is simultaneously de-intercalated from the structure. Upon charging, a completely reverse reaction takes place in the wet electrolyte, resulting in high stability of the host structure and excellent cyclability. However, in the anhydrous electrolyte, some portion of the extracted crystal water molecules cannot be reinserted into the host structure because they are distributed over the anhydrous electrolyte. Keeping some concentration of water in the electrolyte turns out to be was the key to achieving such high reversibility. The potassium ions (90 %) and proton or hydronium ions (10 %) seem to be co-intercalated in the wet electrolyte. This work provides a general insight into the intercalation mechanism of crystal-water-containing host materials. ยฉ 2019 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim1

    Rhombohedral Potassium-Zinc Hexacyanoferrate as a Cathode Material for Nonaqueous Potassium-Ion Batteries

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    Rhombohedral potassium-zinc hexacyanoferrate K 1.88 Zn 2.88 [Fe(CN) 6 ] 2 (H 2 O) 5 (KZnHCF) synthesized using a precipitation method is demonstrated as a high-voltage cathode material for potassium-ion batteries (PIBs), exhibiting an initial discharge capacity of 55.6 mAh g -1 with a discharge voltage of 3.9 V versus K/K + and a capacity retention of 95% after 100 cycles in a nonaqueous electrolyte. All K ions are extracted from the structure upon the initial charge process. However, only 1.61 out of 1.88 K ions per formula unit are inserted back into the structure upon discharge, and it becomes the reversible ion of the second cycle onward. Despite the large ionic size of K, the material exhibits a lattice-volume change (3%) during a cycle, which is exceptionally small among the cathode materials for PIBs. The distinct feature of the material seems to come from the unique porous framework structure built by ZnN 4 and FeC 6 polyhedra linked via the CN bond and a Zn/Fe atomic ratio of 3/2, resulting in high structural stability and cycle performance. ยฉ 2019 American Chemical Society.1

    Electrochemical lithium intercalation chemistry of condensed molybdenum metal cluster oxide: LiMo4O6

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    The electrochemical lithium-ion intercalation properties of molybdenum metal-cluster oxide LixMo4O6 (0.33 โ‰ค x โ‰ค 1.0) in an organic electrolyte of 1.0 M LiPF6 in ethylene carbonate/dimethyl carbonate (1:2 v/v) were characterized for the first time. Li0.66Mo4O6 (tetragonal, P4/mbm, a = 9.5914(3) ร…, c = 2.8798(1) ร…, V = 264.927(15) ร…3, Z = 2) was prepared via ion-exchange of indium and lithium ions from InMo4O6 (tetragonal, P4/mbm, a = 9.66610(4) ร…, c = 2.86507(2) ร…, V = 267.694(2) ร…3, Z = 2), which was first synthesized from a stoichiometric mixture of In, Mo, and MoO3 via a solid-state reaction for 11 h at 1100 ยฐC. Then, Li0.33Mo4O6 was obtained via electrochemical charge of the electrode at 3.4 V vs. Li. The electrochemical lithium-ion insertion into Li0.33Mo4O6 occurs stepwise: three separate peaks were observed in the cyclic voltammogram and three quasi-plateaus in the galvanostatic profile, indicating a complicated intercalation mechanism. However, examination of the structural evolution of LixMo4O6 during the electrochemical cycle indicated a reversible reaction over the measured voltage range (2.0โ€“3.2 V) and x range (0.33 โ‰ค x โ‰ค 1.00). Despite the excellent electrochemical reversibility, LixMo4O6 showed poor rate performance with a low capacity of 36.3 mAh gโˆ’1 at a rate of 0.05 C. Nonetheless, this work demonstrates a new structural class of lithium cathode materials with condensed metal clusters and 1D tunnels, and provides a host material candidate for multivalent-ion batteries. ยฉ 2017 Elsevier Inc.

    Electrochemical Zinc-Ion Intercalation Properties and Crystal Structures of ZnMo6S8 and Zn2Mo6S8 Chevrel Phases in Aqueous Electrolytes

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    The crystal structures and electrochemical properties of ZnxMo6S8 Chevrel phases (x = 1, 2) prepared via electrochemical Zn2+-ion intercalation into the Mo6S8 host material, in an aqueous electrolyte, were characterized. Mo6S8 [trigonal, R3, a = 9.1910(6) ร…, c = 10.8785(10) ร…, Z = 3] was first prepared via the chemical extraction of Cu ions from Cu2Mo6S8, which was synthesized via a solid-state reaction for 24 h at 1000 ยฐC. The electrochemical zinc-ion insertion into Mo6S8 occurred stepwise, and two separate potential regions were depicted in the cyclic voltammogram (CV) and galvanostatic profile. ZnMo6S8 first formed from Mo6S8 in the higher-voltage region around 0.45-0.50 V in the CV, through a pseudo two-phase reaction. The inserted zinc ions occupied the interstitial sites in cavities surrounded by sulfur atoms (Zn1 sites). A significant number of the inserted zinc ions were trapped in these Zn1 sites, giving rise to the first-cycle irreversible capacity of โˆผ46 mAh g-1 out of the discharge capacity of 134 mAh g-1 at a rate of 0.05 C. In the lower-voltage region, further insertion occurred to form Zn2Mo6S8 at around 0.35 V in the CV, also involving a two-phase reaction. The electrochemical insertion and extraction into the Zn2 sites appeared to be relatively reversible and fast. The crystal structures of Mo6S8, ZnMo6S8, and Zn2Mo6S8 were refined using X-ray Rietveld refinement techniques, while the new structure of Zn2Mo6S8 was determined for the first time in this study using the technique of structure determination from powder X-ray diffraction data. With the zinc ions inserted into Mo6S8 forming Zn2Mo6S8, the cell volume and a parameter increased by 5.3% and 5.9%, respectively, but the c parameter decreased by 6.0%. The average Mo-Mo distance in the Mo6 cluster decreased from 2.81 to 2.62 ร…. ยฉ 2016 American Chemical Society.
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