N. Spyrison

activity

20112022

_{1 - δ}

_{1 - x}

_{x}

29 citations · 82 across the 5 of their papers we have counts for

collaborators

Showing cond-mat.supr-conShow all

5 papers · 1 filter

cond-mat.supr-con2014★ 27 cited

Competition between superconductivity and magnetic/nematic order as a source of anisotropic superconducting gap in underdoped Ba $_{1 - x}$ K $_{x}$ Fe $_{2}$ As $_{2}$

H. Kim, M. A. Tanatar, W. E. Straszheim +8

The in-plane London penetration depth, $Δ λ (T)$ , was measured using a tunnel diode resonator technique in single crystals of Ba $_{1 - x}$ K $_{x}$ Fe $_{2}$ As $_{2}$ with doping levels $x$ …

cond-mat.supr-con2014★ 25 cited

Interplane resistivity of underdoped single crystals (Ba $_{1 - x}$ K $_{x}$ )Fe $_{2}$ As $_{2}$ , $0 \leq x < 0.34$

M. A. Tanatar, W. E. Straszheim, Hyunsoo Kim +9

Temperature-dependent inter-plane resistivity, $ρ_{c} (T)$ , was measured in hole-doped iron-arsenide superconductor (Ba $_{1 - x}$ K $_{x}$ )Fe $_{2}$ As $_{2}$ over a doping range from parent compo…

cond-mat.supr-con2012★ 29 cited

Anisotropic resistivity of Na $_{1 - δ}$ Fe $_{1 - x}$ Co $_{x}$ As

N. Spyrison, M. A. Tanatar, Kyuil Cho +4

Temperature-dependent resistivity is studied in single crystals of iron-arsenide superconductor Na $_{1 - δ}$ Fe $_{1 - x}$ Co $_{x}$ As for electrical current directions along, $ρ_{a} (T)$ , and…

cond-mat.supr-con2012

Doping - dependent anisotropic superconducting gap in Na $_{1 - δ}$ (Fe $_{1 - x}$ Co $_{x}$ )As

K. Cho, M. A. Tanatar, N. Spyrison +5

The London penetration depth was measured in single crystals of self-doped Na $_{1 - δ}$ FeAs (from under - to optimal - doping, $T_{c}$ from 14 to 27 K) and electron-doped Na(Fe $_{1 - x}$ …

cond-mat.supr-con2011

Evolution of normal and superconducting properties of single crystals of Na $_{1 - δ}$ FeAs upon interaction with environment

M. A. Tanatar, N. Spyrison, Kyuil Cho +6

Iron-arsenide superconductor Na $_{1 - δ}$ FeAs is highly reactive with the environment. Due to the high mobility of Na ions, this reaction affects the entire bulk of the crystals and…

Competition between superconductivity and magnetic/nematic order as a source of anisotropic superconducting gap in underdoped Ba1−x​Kx​Fe2​As2​

Interplane resistivity of underdoped single crystals (Ba1−x​Kx​)Fe2​As2​, 0≤x<0.34

Anisotropic resistivity of Na1−δ​Fe1−x​Cox​As

Doping - dependent anisotropic superconducting gap in Na1−δ​(Fe1−x​Cox​)As

Evolution of normal and superconducting properties of single crystals of Na1−δ​FeAs upon interaction with environment

Competition between superconductivity and magnetic/nematic order as a source of anisotropic superconducting gap in underdoped Ba $_{1 - x}$ K $_{x}$ Fe $_{2}$ As $_{2}$

Interplane resistivity of underdoped single crystals (Ba $_{1 - x}$ K $_{x}$ )Fe $_{2}$ As $_{2}$ , $0 \leq x < 0.34$

Anisotropic resistivity of Na $_{1 - δ}$ Fe $_{1 - x}$ Co $_{x}$ As

Doping - dependent anisotropic superconducting gap in Na $_{1 - δ}$ (Fe $_{1 - x}$ Co $_{x}$ )As

Evolution of normal and superconducting properties of single crystals of Na $_{1 - δ}$ FeAs upon interaction with environment