Revealing the competition between charge density wave and superconductivity in CsV3Sb5 through uniaxial strain
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Revealing the competition between charge density wave and superconductivity in CsV3Sb5 through uniaxial strain. / Qian, Tiema; Christensen, Morten H.; Hu, Chaowei; Saha, Amartyajyoti; Andersen, Brian M.; Fernandes, Rafael M.; Birol, Turan; Ni, Ni.
In: Physical Review B, Vol. 104, No. 14, 144506, 19.10.2021.Research output: Contribution to journal › Journal article › Research › peer-review
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TY - JOUR
T1 - Revealing the competition between charge density wave and superconductivity in CsV3Sb5 through uniaxial strain
AU - Qian, Tiema
AU - Christensen, Morten H.
AU - Hu, Chaowei
AU - Saha, Amartyajyoti
AU - Andersen, Brian M.
AU - Fernandes, Rafael M.
AU - Birol, Turan
AU - Ni, Ni
PY - 2021/10/19
Y1 - 2021/10/19
N2 - In this paper we report the effect of uniaxial strains applied along the crystalline a axis on the newly discovered kagome superconductor CsV3Sb5. At ambient conditions,CsV3Sb5 shows a charge-density wave (CDW) transition at T-CDW = 94.5 K and superconducts below T-c = 3.34 K. In our paper, when the uniaxial strains is varied from -0.90% to 0.90%, T-c monotonically increases by similar to 33% from 3.0 to 4.0 K, giving rise to the empirical relation T-c (epsilon) = 3.4 + 0.56 epsilon + 0.12 epsilon(2) . On the other hand, fors changing from -0.76% to 1.26%, T-CDW decreases monotonically by similar to 10% from 97.5 to 87.5 K with T-CDW (epsilon) = 94.5 - 4.72 epsilon - 0.60 epsilon(2). The opposite response of T-c and T-CDW to the uniaxial strain suggests strong competition between these two orders. Comparison with hydrostatic pressure measurements indicate that it is the change in the c axis that is responsible for these behaviors of the CDW and superconducting transitions, and that the explicit breaking of the sixfold rotational symmetry by strain has a negligible effect. Combined with our first-principles calculations and phenomenological analysis, we conclude that the enhancement in T-c with decreasing c is caused primarily by the suppression of T-CDW, rather than strain-induced modifications in the bare superconducting parameters. We propose that the sensitivity of (c) with respect to the changes in the c axis arises from the impact of the latter on the trilinear coupling between the M-1(+) and the L-2(-) phonon modes associated with the CDW. Overall, our paper reveals that the c-axis lattice parameter, which can be controlled by both pressure and uniaxial strain, is a powerful tuning knob for the phase diagram of CsV3Sb5.
AB - In this paper we report the effect of uniaxial strains applied along the crystalline a axis on the newly discovered kagome superconductor CsV3Sb5. At ambient conditions,CsV3Sb5 shows a charge-density wave (CDW) transition at T-CDW = 94.5 K and superconducts below T-c = 3.34 K. In our paper, when the uniaxial strains is varied from -0.90% to 0.90%, T-c monotonically increases by similar to 33% from 3.0 to 4.0 K, giving rise to the empirical relation T-c (epsilon) = 3.4 + 0.56 epsilon + 0.12 epsilon(2) . On the other hand, fors changing from -0.76% to 1.26%, T-CDW decreases monotonically by similar to 10% from 97.5 to 87.5 K with T-CDW (epsilon) = 94.5 - 4.72 epsilon - 0.60 epsilon(2). The opposite response of T-c and T-CDW to the uniaxial strain suggests strong competition between these two orders. Comparison with hydrostatic pressure measurements indicate that it is the change in the c axis that is responsible for these behaviors of the CDW and superconducting transitions, and that the explicit breaking of the sixfold rotational symmetry by strain has a negligible effect. Combined with our first-principles calculations and phenomenological analysis, we conclude that the enhancement in T-c with decreasing c is caused primarily by the suppression of T-CDW, rather than strain-induced modifications in the bare superconducting parameters. We propose that the sensitivity of (c) with respect to the changes in the c axis arises from the impact of the latter on the trilinear coupling between the M-1(+) and the L-2(-) phonon modes associated with the CDW. Overall, our paper reveals that the c-axis lattice parameter, which can be controlled by both pressure and uniaxial strain, is a powerful tuning knob for the phase diagram of CsV3Sb5.
KW - ORDER
KW - STATE
U2 - 10.1103/PhysRevB.104.144506
DO - 10.1103/PhysRevB.104.144506
M3 - Journal article
VL - 104
JO - Physical Review B
JF - Physical Review B
SN - 2469-9950
IS - 14
M1 - 144506
ER -
ID: 282678076