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Re-emerging superconductivity at 48 kelvin in iron chalcogenides

Nature (London), 2012-02, Vol.483 (7387), p.67-69

2012

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Polymorphism and superconductivity in the V-Nb-Mo-Al-Ga high-entropy alloys

Science China materials, 2020-05, Vol.63 (5), p.823-831

2020

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Large unsaturated positive and negative magnetoresistance in Weyl semimetal TaP

Science China. Physics, mechanics & astronomy, 2016-05, Vol.59 (5), p.21-26, Article 657406

2016

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Li1.1(Zn1− x Cr x )As: Cr doped I–II–V diluted magnetic semiconductors in bulk form

Journal of applied physics, 2014-02, Vol.115 (8)

2014

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Magnetoresistance and Kondo Effect in Nodal-Line Semimetal VAs2

中国物理快报（英文版）, 2021, Vol.38 (1), p.176-182

2021

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(La 1 − x Ba x )(Zn 1 − x Mn x )AsO: A two-dimensional 1111-type diluted magnetic semiconductor in bulk form

Physical review. B, Condensed matter and materials physics, 2013-07, Vol.88 (4), Article 041102

2013

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Large Magnetoresistance and Nontrivial Berry Phase in Nb3Sb Crystals with A15 Structure

中国物理快报（英文版）, 2021-10, Vol.38 (8), p.144-148

2021

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Role of the 245 phase in alkaline iron selenide superconductors revealed by high-pressure studies

Physical review. B, Condensed matter and materials physics, 2014-03, Vol.89 (9), Article 094514

2014

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Pressure induced superconductivity in the antiferromagnetic Dirac material BaMnBi2

Scientific reports, 2017-05, Vol.7 (1), p.1-7, Article 1634

2017

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Nematic fluctuations in iron-oxychalcogenide Mott insulators

npj quantum materials, 2021-01, Vol.6 (1), p.1-8, Article 4

2021

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Phase diagram and annealing effect for Fe1+δTe1−xSx single crystals

Journal of physics. Condensed matter, 2013-09, Vol.25 (38), p.385701-385701

2013

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Large magnetoresistance and superconductivity in α-gallium single crystals

npj quantum materials, 2018-08, Vol.3 (1), Article 40

2018

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The large anisotropy of the magnetic and transport properties in the Ba5Co5ClO13 single crystal

Physics letters. A, 2009-10, Vol.373 (44), p.4092-4095

2009

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Metabotropic glutamate receptor 5 upregulation of γ-aminobutyric acid transporter 3 expression ameliorates cognitive impairment after traumatic brain injury in mice

Brain research bulletin, 2022-06, Vol.183, p.104-115

2022

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Large positive and negative magnetoresistance in the magnetic EuCu4As2 crystal

Journal of alloys and compounds, 2022-09, Vol.916, p.165460, Article 165460

2022

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Critical properties of the quasi-two-dimensional metallic ferromagnet Fe2.85GeTe2

Journal of physics. Condensed matter, 2018-08, Vol.30 (34), p.345802-345802

2018

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Superconductivity in SnSb with a natural superlattice structure

Superconductor science & technology, 2018-12, Vol.31 (12), p.125011

2018

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Two-dimensional spin dynamics in the itinerant antiferromagnet CsCo 2 Se 2 revealed by 133Cs-NMR measurements

Solid state communications, 2021-04, Vol.329, p.114257, Article 114257

2021

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Two-dimensional spin dynamics in the itinerant antiferromagnet CsCo2Se2 revealed by 133Cs-NMR measurements

Solid state communications, 2021-04, Vol.329, Article 114257

2021

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Fe substitution and pressure effects on superconductor Re6Hf

Solid state communications, 2018-04, Vol.272, p.12-16

2018

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Distinct fermi surface topology and nodeless superconducting gap in a (Tl0.58Rb0.42)Fe1.72Se2 superconductor

Physical review letters, 2011-03, Vol.106 (10), p.107001-107001

2011

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Magnetism and magnetocaloric effect in TlCo 2-x Ni x S 2 (0 [Formula: see text] x [Formula: see text] 0.05)

Journal of physics. Condensed matter, 2020-01, Vol.32 (4), p.045801

2020

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Fe substitution and pressure effects on superconductor Re 6 Hf

Solid state communications, 2018-04, Vol.272, p.12-16

2018

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Spin-flop transition and magnetic phase diagram in CsCo2Se2 revealed by torque and resistivity measurements

Journal of magnetism and magnetic materials, 2019-03, Vol.474, p.70-75

2019

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Magnetism and magnetocaloric effect in TlCo2−xNixS2 (0 ⩽ x ⩽ 0.05)

Journal of physics. Condensed matter, 2020-01, Vol.32 (4)

2020

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Re-emerging superconductivity at 48 kelvin in iron chalcogenides

Polymorphism and superconductivity in the V-Nb-Mo-Al-Ga high-entropy alloys

Large unsaturated positive and negative magnetoresistance in Weyl semimetal TaP

Li1.1(Zn1− x Cr x )As: Cr doped I–II–V diluted magnetic semiconductors in bulk form

Magnetoresistance and Kondo Effect in Nodal-Line Semimetal VAs2

(La 1 − x Ba x )(Zn 1 − x Mn x )AsO: A two-dimensional 1111-type diluted magnetic semiconductor in bulk form

Large Magnetoresistance and Nontrivial Berry Phase in Nb3Sb Crystals with A15 Structure

Role of the 245 phase in alkaline iron selenide superconductors revealed by high-pressure studies

Pressure induced superconductivity in the antiferromagnetic Dirac material BaMnBi2

Nematic fluctuations in iron-oxychalcogenide Mott insulators

Phase diagram and annealing effect for Fe1+δTe1−xSx single crystals

Large magnetoresistance and superconductivity in α-gallium single crystals

The large anisotropy of the magnetic and transport properties in the Ba5Co5ClO13 single crystal

Metabotropic glutamate receptor 5 upregulation of γ-aminobutyric acid transporter 3 expression ameliorates cognitive impairment after traumatic brain injury in mice

Large positive and negative magnetoresistance in the magnetic EuCu4As2 crystal

Critical properties of the quasi-two-dimensional metallic ferromagnet Fe2.85GeTe2

Superconductivity in SnSb with a natural superlattice structure

Two-dimensional spin dynamics in the itinerant antiferromagnet CsCo 2 Se 2 revealed by 133Cs-NMR measurements

Two-dimensional spin dynamics in the itinerant antiferromagnet CsCo2Se2 revealed by 133Cs-NMR measurements

Fe substitution and pressure effects on superconductor Re6Hf

Distinct fermi surface topology and nodeless superconducting gap in a (Tl0.58Rb0.42)Fe1.72Se2 superconductor

Magnetism and magnetocaloric effect in TlCo 2-x Ni x S 2 (0 [Formula: see text] x [Formula: see text] 0.05)

Fe substitution and pressure effects on superconductor Re 6 Hf

Spin-flop transition and magnetic phase diagram in CsCo2Se2 revealed by torque and resistivity measurements

Magnetism and magnetocaloric effect in TlCo2−xNixS2 (0 ⩽ x ⩽ 0.05)

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