N. Spyrison

activity

20112022

_{1 - δ}

_{1 - x}

_{x}

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

collaborators

7 papers

stat.AP2022★ 1 cited

A Study on a User-Controlled Radial Tour for Variable Importance in High-Dimensional Data

Nicholas Spyrison, Dianne Cook, Kim Marriott

Principal component analysis is a long-standing go-to method for exploring multivariate data. The principal components are linear combinations of the original variables, ordered by…

stat.ML2022

Exploring Local Explanations of Nonlinear Models Using Animated Linear Projections

Nicholas Spyrison, Dianne Cook, Przemyslaw Biecek

The increased predictive power of machine learning models comes at the cost of increased complexity and loss of interpretability, particularly in comparison to parametric statistic…

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 $_{1 - x}$ …

A Study on a User-Controlled Radial Tour for Variable Importance in High-Dimensional Data

Exploring Local Explanations of Nonlinear Models Using Animated Linear Projections

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

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