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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Strong pseudospin-lattice coupling in Sr_3Ir_2O_7: Coherent phonon anomaly and negative thermal expansion
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Strong pseudospin-lattice coupling in Sr_3Ir_2O_7: Coherent phonon anomaly and negative thermal expansion

机译:SR_3IR_2O_7中强的PSEUDOPIN-晶格耦合:相干声子异常和负热膨胀

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摘要

The similarities to cuprates make iridates an interesting potential platform for investigating superconductivity. Equally attractive are their puzzling complex intrinsic interactions. Here, we report an ultrafast optical spectroscopy investigation of a coherent phonon mode in Sr3Ir2O7, a bilayer Ruddlesden-Popper perovskite iridate. An anomaly in the A(1g) optical phonon (nu = 4.4 THz) is unambiguously observed below the Neel temperature (T-N), which we attribute to pseudospin-lattice coupling (PLC). Significantly, we find that PLC is the dominant interaction at low temperature, and we directly measure the PLC coefficient to be lambda = 150 +/- 20 cm(-1), which is two orders of magnitude higher than that in manganites (2.4 cm(-1)) and comparable to that in CuO (50 cm(-1), the strongest PLC or spin-lattice coupling (SLC) previously known). Moreover, we find that the strong PLC induces an anisotropic negative thermal expansion. Our findings highlight the key role of PLC in iridates and uncovers another intriguing similarity to cuprates.
机译:与铜酸盐衍生的相似性使其成为研究超导性的有趣潜在平台。同样有吸引力的是他们的令人费解的复杂内在相互作用。在这里,我们报告了SR3IR2O7中的相干声子模式的超快光谱光谱研究,这是双层Ruddlesden-popper植物席位的。 a(1g)光学声子(nu = 4.4 thz)的异常明确地观察到在Neel温度(t-n)下方观察到,我们将其归因于Pseudospin-rattice耦合(PLC)。值得注意的是,我们发现PLC是低温的主导相互作用,我们直接测量PLC系数为Lambda = 150 +/-20cm(-1),这比锰酸盐高的两个数量级(<2.4 CM(-1))和与CUO(50cm(-1),最强的PLC或旋转晶格耦合(SLC)相当的CM(-1)。此外,我们发现强PLC引起各向异性的负热膨胀。我们的调查结果突出了PLC在虹膜中的关键作用,并揭示了与铜替代品的另一个有趣的相似性。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2019年第9期|094307.1-094307.10|共10页
  • 作者单位

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China;

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China|Univ Chinese Acad Sci Sch Phys Sci Beijing 100049 Peoples R China;

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China;

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China|Univ Chinese Acad Sci Sch Phys Sci Beijing 100049 Peoples R China;

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China|Univ Chinese Acad Sci Sch Phys Sci Beijing 100049 Peoples R China;

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China|Univ Chinese Acad Sci Sch Phys Sci Beijing 100049 Peoples R China;

    Chinese Acad Sci Tech Inst Phys & Chem Beijing 100190 Peoples R China;

    Texas Tech Univ Dept Elect & Comp Engn Lubbock TX 79409 USA;

    Chinese Acad Sci Ningbo Inst Mat Technol & Engn Ningbo 315201 Zhejiang Peoples R China;

    Sichuan Univ Coll Phys Sci & Technol Chengdu 610065 Sichuan Peoples R China;

    Chinese Acad Sci Tech Inst Phys & Chem Beijing 100190 Peoples R China;

    Chinese Acad Sci Tech Inst Phys & Chem Beijing 100190 Peoples R China;

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China|Univ Chinese Acad Sci Sch Phys Sci Beijing 100049 Peoples R China;

    Chinese Acad Sci Inst Phys Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China|Univ Chinese Acad Sci Sch Phys Sci Beijing 100049 Peoples R China|Songshan Lake Mat Lab Dongguan 523808 Guangdong Peoples R China;

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