Signature of vortex glass and non-Fermi liquid state in a magnetic superconductor Pr2Pt3Ge5

Effect of thickness on the superconducting properties of the thin films of FeTe0.55Se0.45 deposited on YSZ substrates using Pulsed laser deposition (PLD) technique

“…The unpinned VL region is located between the T 90 and T * lines, whereas the pinned VL region is located between the T * and T g lines. Similar phase diagrams of vortex phase transitions have been observed in other reported results [58,63,66,67]. The width of VL phase region gives the information about TAE (U 0 ).…”

Anisotropic magnetic and transport properties of orthorhombic o-Pr2Co3Ge5

“…This includes charge density waves in Sm 2 Ru 3 Ge 5 and Nd 2 Ru 3 Ge 5 [1,2], superconductivity in Y 2 Ir 3 Ge 5 and La 2 Ir 3 Ge 5 [3][4][5], Kondo lattice behavior in Ce 2 Rh 3 Ge 5 , Ce 2 Ir 3 Ge 5 , and Yb 2 Ir 3 Ge 5 [6][7][8], competition between ferromagnetic and antiferromagnetic ordering in Pr 2 Ni 3 Si 5 , Ho 2 Ni 3 Si 5 , and Tb 2 Co 3 Ge 5 [9][10][11][12], intermediate/mixed valance states in Ce 2 Co 3 Ge 5 , Ce 2 Re 3 Si 5 , and Eu 2 Pt 3 Si 5 [13][14][15][16], and pressure induced quantum critical behavior in Ce 2 Ni 3 Ge 5 [17,18]. The Pr 2 M 3 Ge 5 (M = Co [19], Ni [20], Ru [19], Rh [19], Pd, Ir [3,19], Pt) compounds show many exotic phenomena such as charge density waves and polymorphism in Pr 2 Ru 3 Ge 5 [1], heavy electron behavior in Pr 2 Rh 3 Ge 5 [21], and magnetoresistance of nearly ten-fold increase in Pr 2 Pd 3 Ge 5 [21], A superconducting transition has been observed in Pr 2 Pt 3 Ge 5 at T SC = 6.7 K, coexisting with two antiferromagnetic transitions below T = 5 K [5,22,23] and non-Fermi liquid behavior, suggesting a field dependent quantum critical point [24].…”