Abstract:The interest in lithium-containing ceramics is due to their huge potential as blanket materials for thermonuclear reactors for the accumulation of tritium. However, an important factor in their use is the preservation of the stability of their strength and structural properties when under the influence of external factors that determine the time frame of their operation. This paper presents the results of a study that investigated the influence of the LiTiO2 phase on the increasing resistance to degradation an… Show more
“…Given that the crystal structure and transition-metal (Ti or Mn) oxidation state of m -Li 2 TiO 3 (β phase) are similar to those of m -Li 2 MnO 3 , we considered whether m -Li 2 TiO 3 could be formed as a secondary phase in o -LiMn 1– x Ti x O 2 ( x = 0.05, 0.1). However, according to the literature, c -Li 2 TiO 3 (γ phase) is more stable than m -Li 2 TiO 3 at high temperatures (≤1050 °C). , In addition, there are a significant number of oxygen vacancies in o -LiMn 1– x Ti x O 2 ( x = 0.05, 0.1), as confirmed by the previous Rietveld refinement analysis. Therefore, c -LiTiO 2 was preferred as a secondary phase in o -LiMn 1– x Ti x O 2 ( x = 0.05, 0.1) over m -Li 2 TiO 3 due to the partial loss of oxygen ions and preference for the cubic crystal structure during the synthesis (Figure c).…”
Section: Resultssupporting
confidence: 64%
“…However, according to the literature, c-Li 2 TiO 3 (γ phase) is more stable than m-Li 2 TiO 3 at high temperatures (≤1050 °C). 56,57 In addition, there are a significant number of oxygen vacancies in o-LiMn 1−x Ti x O 2 (x = 0.05, 0.1), as confirmed by the previous Rietveld refinement analysis. Therefore, c-LiTiO 2 was preferred as a secondary phase in o-LiMn 1−x Ti x O 2 (x = 0.05, 0.1) over m-Li 2 TiO 3 due to the partial loss of oxygen ions and preference for the cubic crystal structure during the synthesis (Figure 3c).…”
Section: Transition-metal Oxidation States Of O-limn 1−x Tisupporting
Mn-rich orthorhombic (o)-LiMn1–x
Ti
x
O2 with
a stable oxygen/cation site occupancy and cycling-dependent phase
transition is explored as a novel Co- and Ni-free cathode material
for Li-ion rechargeable batteries. Typical o-LiMnO2 suffers from oxygen deficiency, cation mixing between Li
and Mn, and monoclinic (m)-Li2MnO3 secondary phase with low conductivity. Together with these
drawbacks, the gradual, irreversible phase transition from layered o-LiMnO2 into spinel-like cubic (c)-LixMnO2 (x ≈ 0.5)
during repeated charge/discharge cycles degrades the cycling performance
of o-LiMnO2 despite the activation of
electroactive c-Li
x
MnO2 (x ≈ 0.5). By contrast, o-LiMn1–x
Ti
x
O2 consists of Ti-doped o-LiMnO2 and c-LiTiO2 as the primary and secondary phases,
respectively. The presence of Ti–O bonds, stronger than the
existing Mn–O bonds, improves the structural stability of Ti-doped o-LiMnO2 by reducing the imperfections of the
oxygen/cation lattices (including Mn octahedral sites associated with
the Jahn–Teller distortion) in Ti-doped o-LiMnO2 during the long-term synthesis under an inert atmosphere.
In addition, the electrochemically inactive (>2 V vs Li+/Li) c-LiTiO2 phase with high conductivity serves as a
pillar that suppresses the severe structural collapse of Ti-doped o-LiMnO2 through an abrupt phase/structural
transition during cycling (2–4.5 V). As a result, o-LiMn1–x
Ti
x
O2 with an optimal Ti content exhibits a higher
maximum discharge capacity and superior cycling performance compared
to the pristine o-LiMnO2.
“…Given that the crystal structure and transition-metal (Ti or Mn) oxidation state of m -Li 2 TiO 3 (β phase) are similar to those of m -Li 2 MnO 3 , we considered whether m -Li 2 TiO 3 could be formed as a secondary phase in o -LiMn 1– x Ti x O 2 ( x = 0.05, 0.1). However, according to the literature, c -Li 2 TiO 3 (γ phase) is more stable than m -Li 2 TiO 3 at high temperatures (≤1050 °C). , In addition, there are a significant number of oxygen vacancies in o -LiMn 1– x Ti x O 2 ( x = 0.05, 0.1), as confirmed by the previous Rietveld refinement analysis. Therefore, c -LiTiO 2 was preferred as a secondary phase in o -LiMn 1– x Ti x O 2 ( x = 0.05, 0.1) over m -Li 2 TiO 3 due to the partial loss of oxygen ions and preference for the cubic crystal structure during the synthesis (Figure c).…”
Section: Resultssupporting
confidence: 64%
“…However, according to the literature, c-Li 2 TiO 3 (γ phase) is more stable than m-Li 2 TiO 3 at high temperatures (≤1050 °C). 56,57 In addition, there are a significant number of oxygen vacancies in o-LiMn 1−x Ti x O 2 (x = 0.05, 0.1), as confirmed by the previous Rietveld refinement analysis. Therefore, c-LiTiO 2 was preferred as a secondary phase in o-LiMn 1−x Ti x O 2 (x = 0.05, 0.1) over m-Li 2 TiO 3 due to the partial loss of oxygen ions and preference for the cubic crystal structure during the synthesis (Figure 3c).…”
Section: Transition-metal Oxidation States Of O-limn 1−x Tisupporting
Mn-rich orthorhombic (o)-LiMn1–x
Ti
x
O2 with
a stable oxygen/cation site occupancy and cycling-dependent phase
transition is explored as a novel Co- and Ni-free cathode material
for Li-ion rechargeable batteries. Typical o-LiMnO2 suffers from oxygen deficiency, cation mixing between Li
and Mn, and monoclinic (m)-Li2MnO3 secondary phase with low conductivity. Together with these
drawbacks, the gradual, irreversible phase transition from layered o-LiMnO2 into spinel-like cubic (c)-LixMnO2 (x ≈ 0.5)
during repeated charge/discharge cycles degrades the cycling performance
of o-LiMnO2 despite the activation of
electroactive c-Li
x
MnO2 (x ≈ 0.5). By contrast, o-LiMn1–x
Ti
x
O2 consists of Ti-doped o-LiMnO2 and c-LiTiO2 as the primary and secondary phases,
respectively. The presence of Ti–O bonds, stronger than the
existing Mn–O bonds, improves the structural stability of Ti-doped o-LiMnO2 by reducing the imperfections of the
oxygen/cation lattices (including Mn octahedral sites associated with
the Jahn–Teller distortion) in Ti-doped o-LiMnO2 during the long-term synthesis under an inert atmosphere.
In addition, the electrochemically inactive (>2 V vs Li+/Li) c-LiTiO2 phase with high conductivity serves as a
pillar that suppresses the severe structural collapse of Ti-doped o-LiMnO2 through an abrupt phase/structural
transition during cycling (2–4.5 V). As a result, o-LiMn1–x
Ti
x
O2 with an optimal Ti content exhibits a higher
maximum discharge capacity and superior cycling performance compared
to the pristine o-LiMnO2.
“…Based on the foregoing, the purpose of this work is to study the effect of the phase composition of Li 2 ZrO 3 ceramics obtained by solid-phase synthesis and annealed at different annealing temperatures in the range from 600 to 1100°C on the strength and thermophysical parameters of ceramics. This work is part of a cycle of works devoted to the study of the Li 2 ZrO 3 ceramic properties and evaluation of the possibility of their use as blanket materials for tritium propagation, which is one of the promising research areas in modern energy [18][19][20]. Li 2 ZrO 3 ceramics were chosen as objects of study, which, as was shown earlier in [18][19][20], are highly resistant to radiation damage.…”
Section: Introductionmentioning
confidence: 99%
“…This work is part of a cycle of works devoted to the study of the Li 2 ZrO 3 ceramic properties and evaluation of the possibility of their use as blanket materials for tritium propagation, which is one of the promising research areas in modern energy [18][19][20]. Li 2 ZrO 3 ceramics were chosen as objects of study, which, as was shown earlier in [18][19][20], are highly resistant to radiation damage.…”
The article is devoted to the study of the properties of lithium zirconate ceramics obtained by solid-phase synthesis. The choice of lithium zirconateceramics as objects of study is due to the great prospects for their use as materials for tritium propagation. Results of a study of the influence of the LiO/ZrO2/Li2ZrO3→ LiO/Li2ZrO3 → Li2ZrO3type phase transformations in ceramics, depending on the annealing temperature, on the strength and thermophysical parameters of ceramics are obtained. During the studies, it was found that the change in hardness and crack resistance are directly dependent on the phase composition and concentration of impurity phases in the composition of ceramics. It has been determined that the displacement of lithium oxideand zirconium dioxide impurity phases leads to an increase in hardness and an increase in resistance to cracking under single compression. It has been established that at annealing temperatures above 900°C, the change in strength and thermophysical parameters is minimal. At the same time, a change in the phase composition of the LiO/ZrO2/Li2ZrO3→ Li2ZrO3type ceramics leads to an increase in the thermal conductivity coefficient by (15-20)%
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