papers
Publications (12)
cond-mat.supr-con2014
Crystal growth and annealing study of fragile, non-bulk superconductivity in YFe$_2$Ge$_2$
H. Kim, S. Ran, E. D. Mun +5
cond-mat.str-el2014
Complex magnetic ordering in CeGe1.76 studied by neutron diffraction
W. T. Jayasekara, W. Tian, H. Hodovanets +4
cond-mat.supr-con2013
Signatures of quantum criticality in the thermopower of Ba(Fe(1-x)Co(x))2As2
S. ArsenijeviÄ, H. Hodovanets, R. Gaál +3
cond-mat.str-el2016
A de Haas van Alphen study of the role of 4f electrons in antiferromagnetic CeZn11 as compared to its non-magnetic analogue LaZn11
S. F. Blake, H. Hodovanets, A. McCollam +3
cond-mat.str-el2015
Remarkably robust and correlated coherence and antiferromagnetism in (Ce$_{1-x}$La$_x$)Cu$_2$Ge$_2$
H. Hodovanets, S. L. Bud'ko, W. E. Straszheim +5
cond-mat.supr-con2011
Physical and magnetic properties of Ba(Fe_(1-x)Mn_x)_2As_2 single crystals
A. Thaler, H. Hodovanets, M. S. Torikachvili +6
cond-mat.supr-con2010
Thermoelectric power of Ba(Fe1-xRux)2As2 and Ba(Fe1-xCox)2As2: possible changes of Fermi surface with and without changes in electron count
H. Hodovanets, E. D. Mun, A. Thaler +2
cond-mat.supr-con2010
Evolution of ground state and upper critical field in R(1-x)GdxNi2B2C (R = Lu, Y): Coexistence of superconductivity and spin-glass state
S. L. Bud'ko, V. G. Kogan, H. Hodovanets +4
cond-mat.supr-con2011
Anisotropic magnetism, resistivity, London penetration depth and magneto-optical imaging of superconducting K0.80Fe1.76Se2 single crystals
R. Hu, K. Cho, H. Kim +6
cond-mat.str-el2013
Anisotropic transport and magnetic properties, and magnetic-field tuned states of CeZn11 single crystals
H. Hodovanets, S. L. Bud'ko, X. Lin +5
cond-mat.supr-con2012
Synthesis and physical properties of the new potassium iron selenide superconductor K0.80Fe1.76Se2
Rongwei Hu, E. D. Mun, D. H. Ryan +13
cond-mat.supr-con2010
Importance of Fermi surface topology for high temperature superconductivity in electron-doped iron arsenic superconductors
Chang Liu, A. D. Palczewski, Takeshi Kondo +8