[3] [3] ZHU Y H, WAN B, SHEN W X, et al. Controllable 2H/3R phase transition and conduction behavior change in MoSe2: Nb substitution by high pressure synthesis for promising thermoelectric conversion[J]. Appl Phys Lett, 2023, 122(13): 133903.

[4] [4] YANG J, WANG Y C, YANG H L, et al. Thermal transport in thermoelectric materials with chemical bond hierarchy[J]. J Phys Condens Matter, 2019, 31(18): 183002.

[5] [5] WANG Y F, LEE K H, OHTA H, et al. Thermoelectric properties of electron doped SrO(SrTiO3)n(n=1, 2) ceramics[J]. J Appl Phys, 2009, 105(10): 103701.

[6] [6] WANG Y F, LEE K H, HYUGA H, et al. Enhancement of Seebeck coefficient for SrO(SrTiO3)2 by Sm substitution: Crystal symmetry restoration of distorted TiO6 octahedra[J]. Appl Phys Lett, 2007, 91(24): 242102.

[7] [7] LEE K H, KIM S W, OHTA H, et al. Ruddlesden-Popper phases as thermoelectric oxides: Nb-doped SrO(SrTiO3)n(n=1, 2)[J]. J Appl Phys, 2006, 100(6): 063717.

[8] [8] WANG Y F, LEE K H, OHTA H, et al. Fabrication and thermoelectric properties of heavily rare-earth metal-doped SrO(SrTiO3)n (n=1, 2) ceramics[J]. Ceram Int, 2008, 34(4): 849–852.

[9] [9] SUN R R, QIN X Y, LI L L, et al. The effects of elements doping on transport and thermoelectric properties of Sr3Ti2O7[J]. J Phys Chem Solids, 2014, 75(5): 629–637.

[10] [10] QIN M J, GAO F, WANG M, et al. Microstructure and enhanced seebeck coefficient of textured Sr3Ti2O7 ceramics prepared by RTGG method[J]. Ceram Int, 2016, 42(12): 13748–13754.

[11] [11] ESCOBEDO R, MIRANDA R, MARTNEZ J. Infrared irradiation: Toward green chemistry, a review[J]. Int J Mol Sci, 2016, 17(4): 453.

[13] [13] JANER M, LPEZ T, PLANT X, et al. Ultrasonic nodal point, a new configuration for ultrasonic moulding technology[J]. Ultrasonics, 2021, 114: 106418.

[14] [14] DU Y Q, ZHANG L, ZHANG G B, et al. Discoveries on the link between the properties of thermoelectric and infrared radiation[J]. Appl Phys Lett, 2023, 123(13): 133903.

[15] [15] SILVEIRA F E M, KURCBART S M. Hagen-Rubens relation beyond far-infrared region[J]. EPL Europhys Lett, 2010, 90(4): 44004.

[16] [16] HUANG Z, ZHOU W, TANG X, et al. Effects of substrate roughness on infrared-emissivity characteristics of Au films deposited on Ni alloy[J]. Thin Solid Films, 2011, 519(10): 3100–3106.

[17] [17] SALIHOGLU O, UZLU H B, YAKAR O, et al. Graphene-based adaptive thermal camouflage[J]. Nano Lett, 2018, 18(7): 4541–4548.

[18] [18] LYU J, LIU Z W, WU X H, et al. Nanofibrous kevlar aerogel films and their phase-change composites for highly efficient infrared stealth[J]. ACS Nano, 2019, 13(2): 2236–2245.

[19] [19] YIN J H, ZHANG L, MA W Z, et al. Research on reducing infrared emissivity of 8YSZ coating by regulating microstructure[J]. Infrared Phys Technol, 2023, 130: 104587.

[20] [20] HONA R K, KARKI S B, DHALIWAL G S, et al. High thermal insulation properties of A2FeCoO6– (A = Ca, Sr)[J]. J Mater Chem C, 2022, 10(35): 12569–12573.

[21] [21] CHEN G L, FU H Y, ZOU Y C, et al. A promising radiation thermal protection coating based on lamellar porous Ca–Cr co-doped Y3NbO7 ceramic[J]. Adv Funct Mater, 2023, 33(47): 2305650.

[22] [22] Chen H. Infrared Physics[Z]. Beijing: national defence industry press. 1985: 95–116

[23] [23] WANG J, ZHANG B Y, KANG H J, et al. Record high thermoelectric performance in bulk SrTiO3vianano-scale modulation doping[J]. Nano Energy, 2017, 35: 387–395.

[24] [24] PARK K, SON J S, WOO S I, et al. Colloidal synthesis and thermoelectric properties of La-doped SrTiO3 nanoparticles[J]. J Mater Chem A, 2014, 2(12): 4217–4224.

[25] [25] ZHAO K P, DUAN H Z, RAGHAVENDRA N, et al. Solid-state explosive reaction for nanoporous bulk thermoelectric materials[J]. Adv Mater, 2017, 29(42): 1701148.

[26] [26] DYACHENKO P N, MOLESKY S, PETROV A Y, et al. Controlling thermal emission with refractory epsilon-near-zero metamaterials via topological transitions[J]. Nat Commun, 2016, 7: 11809.