Research progress of two-dimensional covalent bond substructure Zintl phase thermoelectric materials

Yuan Min-Hui; Le Wen-Kai; Tan Xiao-Jian; Shuai Jing

doi:10.7498/aps.70.20211010

Abstract

Thermoelectric materials can realize the direct conversion between thermal energy and electrical energy, and thus having important applications in semiconductor refrigeration and heat recovery. Zintl phase is composed of highly electronegative cations and anions, which accords with the concept of “phonon glass, electron crystal” (PGEC). Thermoelectric properties of Zintl phase have attracted extensive interest, among which the two-dimensional (2D) covalent bond structure featured Zintl phases have received more attention for their outstanding electrical properties. In this review, Zintl phase materials with two-dimensional covalent bond substructures are reviewed, including 1-2-2-type, 9–4+x–9-type, 2-1-2-type and 1-1-1-type Zintl phase. The 1-2-2-type Zintl phase is currently the most widely studied and best-performing Zintl material. It is worth mentioning that the maximum ZT value for the Mg₃Sb₂-based n-type Zintl material with the CaAl₂Si₂ structure has been reported to reach 1.85, and the average ZT value near room temperature area also reaches 1.4. The 9–4+x–9-type Zintl material with a mass of atoms in unit cell contributes to lower thermal conductivity thus relatively high ZT value. The 2-1-2-type Zintl material has extremely low thermal conductivity due to the intrinsic vacancies, which has been developing in recent years. The 1-1-1-type Zintl material with the same ZrBeSi structure as the 2-1-2-type Zintl material, shows better electrical transport performance. In sum, this review summarizes the recent progress and optimization methods of those typical Zintl phases above. Meanwhile, the future optimization and development of Zintl phase with two-dimensional covalent bond substructures are also prospected.

Keywords:

thermoelectric materials /
Zintl phase /
2-dimensional covalent bond substructure

Authors and contacts

1.
School of Materials, Sun Yat-sen University, Shenzhen 518107, China
2.
Ningbo Institute of Materials Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, China

Corresponding author: Tan Xiao-Jian, tanxiaojian@nimte.ac.cn ; Shuai Jing, shuaij3@mail.sysu.edu.cn

Funds: Project supported by the National Natural Science Foundation of China (Grant Nos. 52002413, 21875273), the Natural Science Foundation of Guangdong Province, China (Grant No. 2021A1515010612), the Natural Science Foundation of Zhejiang Province, China (Grant No. LR21E020002), and Youth Innovation Promotion Association CAS (Grant No. 2019298).

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Cited By

图 1 (a) 各类型结构中典型Zintl相ZT值对比图^{[8,10-12,14,18,21,24,25,28,32-35]}; (b) 2D典型Zintl相最大ZT值随时间变化总结图

Figure 1. (a) ZT values of typical Zintl phases with 2D covalent bond substructures ^{[8,10-12,14,18,21,24,25,28,32-35]}; (b) summary diagram of the maximum ZT value of some representative 2D Zintl phase over time.

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图 2 AB₂X₂型Zintl材料　(a) 晶体结构; (b) 单胞扩展键; (c) 单胞不扩展键晶体结构示意图; (d) Sb基AB₂X₂型Zintl相ZT值对比图; (e) Bi基AB₂X₂型Zintl相ZT值对比图^{[8,21,34,36-45]}

Figure 2. (a) Crystal structure of AB₂X₂-type Zintl material; (b), (c) unit cell. Temperature-dependent ZT values of (d) Sb-based AB₂X₂-type Zintl phases; (e) Bi-based AB₂X₂-type Zintl phases^{[8,21,34,36-45]}.

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图 3 Mg₃Sb₂ Zintl材料　(a) 晶体结构; (b) c轴方向晶体结构; (c) a轴方向晶体结构示意图; (d) Mg₃Sb₂结构由传统认为的层状结构到三维结构示意图; (e) 近年Mg₃Sb₂基Zintl相主要工作ZT值随温度变化图^{[9,10,22,23,48,66,69,76-78]}; (f) 突出Mg₃Sb₂相300—500 K及300—773 K温区下平均ZT值对比图^{[9-12,69,73,75,78-82]}

Figure 3. (a) Crystal structure of Mg₃Sb₂; (b) crystal structure along the c axis; (c) crystal structure along the a axis; (d) Mg₃Sb₂ structure with traditional layered covalent bonds compared to the 3D covalent bonds; (e) temperature-dependent ZT values of Mg₃Sb₂-based Zintl phases^{[9,10,22,23,48,66,69,76-78]}; (f) average ZT values of Mg₃Sb₂-based Zintl phases at 300−500 K and 300−773 K^{[9-12,69,73,75,78-82]}.

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图 4 Ca₉Zn₄Sb₉相　(a) 晶体结构图; (b) a轴晶体结构图; 9–4+x–9型Zintl相近年来典型结构(c)ZT值随温度变化图; (d) 泽贝克系数随温度变化图; (e) 电阻率随温度变化图; (f) 热导率及晶格热导率随温度变化图^{[27,28,87-90]}

Figure 4. (a) Crystal structure of Ca₉Zn₄Sb₉; (b) crystal structure of Ca₉Zn₄Sb₉ along a axis. Temperature-dependent (c) ZT values; (d) Seebeck coefficient; (e) electrical resistivity; (f) thermal conductivity of 9–4+x–9 type Zintl phases ^{[27,28,87-90]}.

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图 5 (a) EuZn₂Sb₂单胞晶体结构图; (b) Eu₂ZnSb₂相与EuZn₂Sb₂相结构对比图^[25]; (c) Eu₂ZnSb₂相a轴方向晶体结构图; (d) Eu₂ZnSb₂相c轴方向晶体结构示意图; (e) Eu₂ZnSb₂相扩胞后晶体结构示意图; (f) Eu₂ZnSb₂相扩胞后a轴方向晶体结构示意图; (g) 2-1-2型Zintl相近年来典型结构ZT值随温度变化图; (h) S随温度变化图; (i) 电阻率随温度变化图; (j) 2-1-2型Zintl相与9–4+x–9, 1-2-2型典型Zintl相晶格热导率随温度变化对比图^{[8,24,25,27,90,92]}

Figure 5. (a) Unit cell of EuZn₂Sb₂; (b) unit cell of Eu₂ZnSb₂ ; (c) unit cell of Eu₂ZnSb₂ along the a axis;(d) crystal structure along the c axis; (e) crystal structure of Eu₂ZnSb₂; (f) in the a axis direction after cell expansion. Temperature-dependent (g) ZT values; (h) Seebeck coefficient; (i) electrical resistivity of 2-1-2 type Zintl phases; (j) lattice thermal conductivity of 2-1-2, 9–4+x–9 and 1-2-2type Zintl phases ^{[8,24,25,27,90,92]}.

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图 6 SrAgSbZintl相　(a) 晶体结构示意图; (b)延c轴方向晶体结构示意图. 1-1-1型Zintl相近年来典型结构 (c) ZT值随温度变化图; (d) 电阻率随温度变化图; (e) 热导率随温度变化图; (f) 1-1-1型Zintl相功率因子较同结构1-2-2型Zintl相随温度变化对比图^[24-26,106]

Figure 6. (a) Crystal structure of SrAgSb; (b) crystal structure of SrAgSb along the c axis. Temperature-dependent (c) ZT values; (d) power factors (compared with 2-1-2 Zintl phases); (e) electric resistivity; (f) thermal conductivity of typical 1-1-1 Zintl phases^[24-26,106].

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表 1 1-2-2型层状Zintl材料热电性能汇总表

Table 1. Summary of thermoelectric properties of 1-2-2 type layered Zintl materials.

时间	材料	Ρ/(mΩ·cm)	S/(μV·K^–1)	κ/(W·m^–1·K^–1)	ZT	T/K	ZT_RT
2005	Ca_0.25Yb_0.75Zn₂Sb₂^[36]	3.7	170	1.4	0.56	773	0.08
2007	BaZn₂Sb₂^[38]	6.1	185	1.25	0.33	673	0.05
2008	YbZn_1.9Mn_0.1Sb₂^[57]	1.5	150	1.6	0.65	726	0.05
2008	EuZn₂Sb₂^[58]	1.8	180	1.45	0.9	713	0.16
2009	YbCd_1.6Zn_0.4Sb₂^[46]	1.66	180	1.1	1.2	650	0.2
2010	Yb_0.6Ca_0.4Cd₂Sb₂^[37]	4.4	240	0.9	0.96	700	0.14
2010	Yb_0.75Eu_0.25Cd₂Sb₂^[59]	4	240	1	0.97	650	0.18
2010	EuZn_1.8Cd_0.2Sb₂^[47]	2	200	1.4	1.06	650	0.18
2011	YbCd_1.85Mn_0.15Sb₂^[60]	5.7	245	0.6	1.14	650	0.17
2012	YbMg₂Bi₂^[39]	5	180	1.8	0.44	650	0.07
2014	Yb_0.99Zn₂Sb₂^[61]	1.3	160	1.7	0.85	800	0.05
2016	YbCd_1.9Mg_0.1Sb₂^[40]	3.3	230	1.02	1.08	650	0.2
2016	Ca_0.5Yb_0.5Mg₂Bi₂^[49]	2.8	187	1.08	1	873	0.1
2016	Ca_0.995Na_0.005Mg₂Bi_1.98^[54]	3	200	1.25	0.9	873	0.05
2016	Eu_0.2Yb_0.2Ca_0.6Mg₂Bi₂^[8]	3.5	215	0.92	1.3	875	0.25
2018	YbCd_1.5Zn_0.5Sb₂^[34]	1.7	172	1.2	1.26	700	0.18
2018	Yb_0.96Ba_0.04Cd_1.5Zn_0.5Sb₂^[34]	2	185	0.94	1.3	700	0.18
2019	Ba_0.7975Yb_0.2Na_0.0025Cd₂Sb₂^[41]	4.1	210	0.81	0.93	700	0.1
2019	EuCd_1.4Zn_0.6Sb₂^[42]	3.5	220	1	0.96	700	0.18
2020	Ca_0.65Yb_0.35Mg_1.9Zn_0.1Bi_1.98^[43]	2.63	185	1.04	1	773	0.2
2020	YbMg₂Bi_1.58Sb_0.4^[44]	4.1	219	1	1.05	873	0.14
2020	Sm_0.25Yb_0.375Eu_0.375Mg₂Bi_1.99^[45]	3.7	197	0.9	0.9	773	0.18
2020	(Yb_0.9Mg_0.1)Mg_0.8Zn_1.198Ag_0.002Sb₂^[21]	4.75	257	0.74	1.5	773	0.28

DownLoad: CSV

表 2 Mg₃Sb₂基Zintl材料热电性能汇总表

Table 2. Summary of thermoelectric properties of Mg₃Sb₂-based layered Zintl materials.

时间	材料	ρ/(mΩ·cm)	S/(μV·K^–1)	κ/(W·m^–1·K^–1)	ZT	T/K	ZT_RT
2006	Mg₃Sb₂^[83]	29	288	1.2	0.21	875	0.001
2013	Mg₃Bi_0.2Sb_1.8^[76]	40	400	0.58	0.6	750	0.01
2014	Mg₃Pb_0.2Sb_1.8^[48]	28.6	280	0.28	0.84	773	0.03
2015	Mg_2.9875Na_0.0125Sb₂^[66]	5.4	200	0.95	0.6	773	0.03
2017	Mg_2.985Ag_0.015Sb₂^[22]	9	205	0.65	0.51	725	0.08
2016	Mg_3.2Sb_1.5Bi_0.49Te_0.01^[67]	5	–286	0.79	1.51	716	0.2
2016	Mg₃Sb_1.48Bi_0.48Te_0.04^[53]	10	–205	0.73	1.6	750	0.6
2017	Mg_3.05Nb_0.15Sb_1.5Bi_0.49Te_0.01^[9]	4.35	–277	0.84	1.57	700	0.31
2017	Mg_3.1Co_0.1Sb_1.5Bi_0.49Te_0.01^[69]	5.1	–295	0.78	1.7	773	0.4
2018	Mg_3.15Mn_0.05Sb_1.5Bi0_.49Te_0.01^[10]	4.5	–302	0.79	1.85	723	0.42
2019	Mg_3+δSb_1.5Bi_0.49Te_0.01:Mn_0.01^[78]	4.5	–290	0.9	1.6	773	0.65
2019	Mg_3.05SbBi_0.97Te_0.03^[74]	1.7	–202	0.92	1.31	500	0.71
2019	Mg_3.02Y_0.02Sb_1.5Bi_0.5^[11]	4.2	–270	0.76	1.8	773	0.2
2020	Mg_3.2Sb_1.99Te_0.01+GNP^[23]	6.4	–320	0.74	1.7	750	0.18
2021	Mg_3.17B_0.03Sb_1.5Bi0_.49Te_0.01^[12]	5.4	–296	0.69	1.81	773	0.62

DownLoad: CSV

表 3 9–4+x–9型层状Zintl材料热电性能汇总表

Table 3. Summary of thermoelectric properties of 9–4+x–9 type layered Zintl materials.

时间	材料	ρ/(mΩ·cm)	S/(μV·K^–1)	κ/(W·m^–1·K^–1)	ZT	T/K	ZT_RT
2014	Yb₉Mn_4.2Sb₉^[87]	7.9	185	0.58	0.7	950	0.035
2015	Eu₉Cd_3.75Ag_1.42Sb₉^[91]	2.0	85	1.0	0.32	750	0.03
2016	Ca₉Zn_4.35Cu_0.15Sb₉^[89]	3.0	140	0.8	0.72	873	0.1
2017	Ca₉Zn_4.6Sb₉^[27]	11.0	270	0.48	1.1	873	0.1
2019	Ca_6.75Eu_2.25Zn_4.7Sb₉^[28]	5.55	200	0.53	1.05	773	0.21
2021	Sr₉Mg_4.45Bi₉^[90]	3.75	135	0.65	0.57	773	0.14 (323 K)

DownLoad: CSV

表 4 2-1-2型层状Zintl材料热电性能汇总表

Table 4. Summary of thermoelectric properties of 2-1-2 type layered Zintl materials.

时间	材料	ρ/(mΩ·cm)	S/(μV·K^–1)	κ/(W·m^–1·K^–1)	ZT	T/K	ZT_RT
2017	Yb₂CdSb₂^[92]	5	155	0.52	0.2	523	0.23
2017	Yb_1.64Eu_0.36CdSb₂^[92]	3.5	170	0.6	0.7	523	0.26
2018	Eu₂ZnSb₂^[25]	24.4	290	0.42	0.6	723	0.14
2018	Eu₂Zn_0.98Sb₂^[25]	8	220	0.48	1	823	0.22
2020	Eu₂Zn_0.97Ag_0.06Sb₂^[24]	10	220	0.43	0.93	823	0.2
2020	Eu₂Zn_0.95Ag_0.06Sb₂^[24]	5.3	194	0.5	1.1	823	0.2

DownLoad: CSV

表 5 1-1-1型层状Zintl材料热电性能汇总表

Table 5. Summary of thermoelectric properties of 1-1-1 type layered Zintl materials.

时间	材料	ρ/(mΩ·cm)	S/(μV·K^–1)	κ/(W·m^-1·K^–1)	ZT	T/K	ZT_RT
2018	Ca_0.85La_0.15Ag_0.89Sb^[106]	1.85	120	1.3	0.52	860	0.07
2018	Ca_0.55Sr_0.3La_0.15Ag_0.89Sb^[106]	1.6	125	1.0	0.7	823	0.1
2020	SrAgSb^[26]	0.95	114	2.2	0.5	773	0.07
2020	Sr_1.01AgSb^[26]	1.27	125	1.7	0.58	773	0.1
2020	EuCuSb^[26]	0.64	83	2.9	0.3	773	0.03
2020	EuAgSb^[26]	0.74	90	2.4	0.35	773	0.05

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Vol. 70, Issue 20 - 2021-10-20

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