Abstract

We investigated the structure and electric conductivity of solid solutions of homovalent substitution Ва1–хSn1+хF4 (where х=0.03, 0.05, 0.07, 0.10, 0.15 and 0.23) and heterovalent substitution (KyВа1–y)(1–х)Sn1+хF4–y(1–х) (where х=0.03, 0.05, 0.10 and у=0.03, 0.05, 0.10) with the structure of BaSnF4. It was been found that the substitution of 7 mol.% of Ba2+ cations by Sn2+ cations contributed to an increases in electrical conductivity. The solid solution Ba0.77Sn1.23F4 had the highest electrical conductivity (573=6.8010–3 S cm–1). The substitution of barium ions by potassium ions in the BaSnF4 crystal lattice allowed reducing the conductivity of solid solutions regardless of the substituent content. Only the phases containing more than 3 mol.% of K+ ions exhibited the conductivity which exceeded the value of the initial phase at the temperatures above 385 K. In fluoride-conducting phases (KyBa1–y)(1–x)Sn1+xF4–y(1–х), the following solid solutions showed the highest electrical conductivity: (K0.05Ba0.95)0.97Sn1.03F3.95 (573=6.7810–4 S сm–1), (K0.03Ba0.97)0.95Sn1.05F3.97 (573=1.0010–3 S сm–1) and (K0.10Ba0.90)0.90Sn1.10F3.91 (573=8.7010–3 S сm–1).

Highlights

  • Âñòóï Íåîðãàí3÷í3 ôòîðèäè ç âèñîêîþ ðóõëèâ3ñòþ àí3îí3â ó òâåðäîìó ñòàí3 ïðèâàáëèâ3 äëÿ ñòâîðåííÿ íîâèõ ìàòåð3àë3â åëåêòðîòåõí3÷íèõ ïðèñòðî¿â ð3çíîãî ôóíêö3îíàëüíîãî ïðèçíà÷åííÿ, òàêèõ ÿê 3îíñåëåêòèâí3 åëåêòðîäè, ãàçîâ3 ñåíñîðè, ãåíåðàòîðè ôòîðó, êîíäåíñàòîðè òà 3í. [1,2].

  • Ó ðîáîò3 [5] äîñë3äæåíî âïëèâ çàì3ùåííÿ 3îí3â Pb2+ â ñòðóêòóð3 PbSnF4 êàò3îíàìè Ln3+ (Ln=Y, La, Ce, Nd, Sm, Gd) íà ïðîâ3äí3 âëàñòèâîñò3 óòâîðåíèõ òâåðäèõ ðîç÷èí3â.

  • Âñòàíîâëåíî, ùî ïðè çàì3ùåíí3 äî 20 ìîë.% 3îí3â ïëþìáóìó 3îíàìè ð3äê3ñíîçåìåëüíèõ åëåìåíò3â, åëåêòðîïðîâ3äí3ñòü ñèíòåçîâàíèõ òâåðäèõ ðîç÷èí3â çíà÷íî âèùà ó ïîð3âíÿíí3 ç âèõ3äíîþ ñïîëóêîþ.

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Summary

Introduction

Âñòóï Íåîðãàí3÷í3 ôòîðèäè ç âèñîêîþ ðóõëèâ3ñòþ àí3îí3â ó òâåðäîìó ñòàí3 ïðèâàáëèâ3 äëÿ ñòâîðåííÿ íîâèõ ìàòåð3àë3â åëåêòðîòåõí3÷íèõ ïðèñòðî¿â ð3çíîãî ôóíêö3îíàëüíîãî ïðèçíà÷åííÿ, òàêèõ ÿê 3îíñåëåêòèâí3 åëåêòðîäè, ãàçîâ3 ñåíñîðè, ãåíåðàòîðè ôòîðó, êîíäåíñàòîðè òà 3í. [1,2]. Ó ðîáîò3 [5] äîñë3äæåíî âïëèâ çàì3ùåííÿ 3îí3â Pb2+ â ñòðóêòóð3 PbSnF4 êàò3îíàìè Ln3+ (Ln=Y, La, Ce, Nd, Sm, Gd) íà ïðîâ3äí3 âëàñòèâîñò3 óòâîðåíèõ òâåðäèõ ðîç÷èí3â. Âñòàíîâëåíî, ùî ïðè çàì3ùåíí3 äî 20 ìîë.% 3îí3â ïëþìáóìó 3îíàìè ð3äê3ñíîçåìåëüíèõ åëåìåíò3â, åëåêòðîïðîâ3äí3ñòü ñèíòåçîâàíèõ òâåðäèõ ðîç÷èí3â çíà÷íî âèùà ó ïîð3âíÿíí3 ç âèõ3äíîþ ñïîëóêîþ. Íàéâèùó ïðîâ3äí3ñòü (7,72–9,32) 10–2 Ñì/ñì) òà íàéìåíøó åíåðã3þ àêòèâàö3¿ ïðîâ3äíîñò3 â 3íòåðâàë3 âèñîêèõ òåìïåðàòóð ìàþòü çðàçêè ñêëàäó K0,10Pb0,90SnF3,90, Li0,07Pb0,93SnF3,93 òà Rb0,05Pb0,95SnF3,95 Çàì3ùåííÿ ÷àñòèíè 3îí3â ïëþìáóìó êàò3îíàìè íàòð3þ îáóìîâëþo çìåíøåííÿ åëåêòðîïðîâ3äíîñò3 çà ðàõóíîê óòâîðåííÿ äîäàòêîâî¿ ôàçè Na2SnF5.

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