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Full Critical Review

Review of Bi2O3 based glasses for electronics and related applications

Pages 3-40 | Published online: 12 Nov 2013

Figures & data

Figure 1. Example TF circuit, piezoresistive pressure sensorCitation27, showing typical involved materials: reddish tint added to sealing glass to enhance visibility; ‘conductive glass’ seal = low firing TFR composition

Figure 1. Example TF circuit, piezoresistive pressure sensorCitation27, showing typical involved materials: reddish tint added to sealing glass to enhance visibility; ‘conductive glass’ seal = low firing TFR composition

Table 1. Representative compositions (cation-%) of low melting lead based glasses [Temperatures = melting points (eutectics) or processing temperatures (others)]

Table 2. Requirements for (relatively) low melting glasses for layers and seals (‘−’ = normally not important; ‘+’ = significant; ‘++’ = critical)

Table 3. Requirements for low melting ‘bulk’ glasses (‘−’ = normally not important; ‘+’ = significant; ‘++’ = critical)

Table 4. Representative materials/fillers used in conjunction with glass frits

Table 5. Qualitative composition (+++  =  high, ++  =  medium, +  =  low, ?  =  very low or absent) of commercial TF inks (Tf = firing temperature): dielectricsCitation167 (compared with LTCC),Citation168Citation170 conductorCitation164 and resistor.Citation85 Boron most likely present in all these compositions, but not always detectable by the analysis methods – mentioned where explicitly formulated/detected

Table 6. Some low melting lead free glass systems (without Bi), with typical glass transition temperature Tg [R2O = (Li,Na,K)2O; RO = (Ca,Sr,Ba,Zn)O]

Table 7. Bismuth glass compositions, in cation mole percentage

Table 8. System property index: borates

Table 9. System property index: silicates, germanates and phosphates

Table 10. System property index: tellurites, vanadates, molybdates and other

Table 11. Glasses without standard network formers: binary systems

Figure 2. Liquidus temperatures of binary systems, redrawn from phase diagrams Bi2O3–SiO2,Citation281 Bi2O3–GeO2 (PDC-2359), Bi2O3–B2O3 (PDC-323) and PbO–B2O3 (PDC-282)

Figure 2. Liquidus temperatures of binary systems, redrawn from phase diagrams Bi2O3–SiO2,Citation281 Bi2O3–GeO2 (PDC-2359), Bi2O3–B2O3 (PDC-323) and PbO–B2O3 (PDC-282)

Figure 3. Glass transition temperatures Tg of binary systems according to George et al.Citation248 (heavy lines), compared with other works (×: Ref. 317; Δ: Ref. 318; +: Ref. 141; *: Ref. 319)

Figure 3. Glass transition temperatures Tg of binary systems according to George et al.Citation248 (heavy lines), compared with other works (×: Ref. 317; Δ: Ref. 318; +: Ref. 141; *: Ref. 319)

Table 12. Glass-forming range of Bi2O3 and PbO/SnOFootnote binary systems with networkforming oxides, with quenching index Q and crucibleFootnote indicated as subscript

Figure 4. Vitrification range in Bi2O3–B2O3–ZnOCitation354/CuOyCitation249 systems (cation basis)

Figure 4. Vitrification range in Bi2O3–B2O3–ZnOCitation354/CuOyCitation249 systems (cation basis)

Figure 5. Effect of R2O on min. B2O3 in R2O–Bi2O3–B2O3 (R = Li, Na, K) systemsCitation247

Figure 5. Effect of R2O on min. B2O3 in R2O–Bi2O3–B2O3 (R = Li, Na, K) systemsCitation247

Table 13. Glasses without standard network formers: complex systems

Figure 6. Some oxygen coordination shells around Bi observed in crystalline oxides (see section on ‘Coordination of bismuth in crystalline oxides’ in Supplementary Material 1 http://dx.doi.org/10.1179/1743280412Y.0000000010.S1 and ): E = Bi3+ lone pair electrons

Figure 6. Some oxygen coordination shells around Bi observed in crystalline oxides (see section on ‘Coordination of bismuth in crystalline oxides’ in Supplementary Material 1 http://dx.doi.org/10.1179/1743280412Y.0000000010.S1 and Table 14): E = Bi3+ lone pair electrons

Table 14. Description of oxygen coordination shells around Bi observed in crystalline oxides (see section on ‘Coordination of bismuth in crystalline oxides’ in Supplementary Material 1 http://dx.doi.org/10.1179/1743280412Y.0000000010.S1 and ) (E stands for Bi3+ lone pair electrons)

Figure 7. [BO4] tetrahedra fraction N4 in boron coordination polyhedra ([BO3] and [BO4]), for Bi2O3–B2O3 glass (○: Ref. 318; +: Ref. 247; □: Ref. 327) and crystallised glass (•: Ref. 318), (ZnO.Bi2O3)–B2O3 glass (Δ: Ref. 355) and PbO–B2O3 glass (×: Ref. 397)

Figure 7. [BO4] tetrahedra fraction N4 in boron coordination polyhedra ([BO3] and [BO4]), for Bi2O3–B2O3 glass (○: Ref. 318; +: Ref. 247; □: Ref. 327) and crystallised glass (•: Ref. 318), (ZnO.Bi2O3)–B2O3 glass (Δ: Ref. 355) and PbO–B2O3 glass (×: Ref. 397)

Table 15. Tg and N4 peaks in binary x(BiO1·5,SbO1·5,PbO,SnO)–(1−x)BO1·5 glasses

Table 16. Nominal bonding deficit of oxygen anions in borate glasses versus structure

Figure 8. Typical configurations/roles for dielectric glass based layers

Figure 8. Typical configurations/roles for dielectric glass based layers

Table 17. Oxygen coordination trends of ‘lone pair’ cations versus concentration x

Table 18. Composition ranges and ratios specified for sealing glass stabilityCitation314

Figure 9. Results, in cation-%, of our experiments on stability of Bi2O3 based glasses in TF firing cycles (belt oven, 45 min total time with 10 min at peak, 400–700°C)

Figure 9. Results, in cation-%, of our experiments on stability of Bi2O3 based glasses in TF firing cycles (belt oven, 45 min total time with 10 min at peak, 400–700°C)

Table 19. Composite sealing glasses (compositions: see )

Table 20. Overglaze/enamel/dielectric properties (glass compositions: see )

Figure 10. Application of enamel to automotive glass, as a antistick layer during forming and b adhesive protection layer (redrawn from SakoskeCitation47)

Figure 10. Application of enamel to automotive glass, as a antistick layer during forming and b adhesive protection layer (redrawn from SakoskeCitation47)

Table 21. Advantages and issues of Bi in conductors and component metallisations.

Figure 11. Microstructure and conduction mechanism of TFRsCitation1

Figure 11. Microstructure and conduction mechanism of TFRsCitation1

Figure 12. Typical composition (without temporary vehicle/binder) of TFRs with lead borosilicate glass matrixCitation1

Figure 12. Typical composition (without temporary vehicle/binder) of TFRs with lead borosilicate glass matrixCitation1

Figure 13. Sheet resistivity at 25°C and temperature coefficient (HTCR, 25–100°C), versus length and firing temperature, of experimental TFRs fired on Al2O3 with Ag terminationsCitation1

Figure 13. Sheet resistivity at 25°C and temperature coefficient (HTCR, 25–100°C), versus length and firing temperature, of experimental TFRs fired on Al2O3 with Ag terminationsCitation1

Table 22. Optical properties of HMO glasses

Table 23. Compositions of selected BiSCCO superconductors, given in cation molar proportions [z = Pb/(Pb+Bi)]

Supplemental material

yimr_a_11743737_sm0001.pdf

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