English
 
Help Privacy Policy Disclaimer
  Advanced SearchBrowse

Item

ITEM ACTIONSEXPORT

Released

Journal Article

Heat capacity of the heavy fermion superconductor CeIrIn5 under hydrostatic pressure

MPS-Authors
/persons/resource/persons126543

Borth,  R.
Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

/persons/resource/persons126728

Lengyel,  E.
Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

/persons/resource/persons126858

Sparn,  G.
Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

/persons/resource/persons126861

Steglich,  F.
Frank Steglich, Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

External Resource
No external resources are shared
Fulltext (restricted access)
There are currently no full texts shared for your IP range.
Fulltext (public)
There are no public fulltexts stored in PuRe
Supplementary Material (public)
There is no public supplementary material available
Citation

Borth, R., Lengyel, E., Pagliuso, P. G., Sarrao, J. L., Sparn, G., Steglich, F., et al. (2002). Heat capacity of the heavy fermion superconductor CeIrIn5 under hydrostatic pressure. Physica B, 312, 136-137. doi:10.1016/S0921-4526(01)01085-7.


Cite as: https://hdl.handle.net/11858/00-001M-0000-0015-3181-4
Abstract
CeIrIn5 belongs to a new class of heavy fermion (HE) superconductors that crystallize in the tetragonal HoCoGa5- structure. This structure can be regarded as alternating layers of CeIn3 and IrIn2. Bulk CeIn(3)undergoes a transition from an antiferrornagnetic (AFM) state at ambient pressure (T-N = 10 K) to a superconductina state (T-c = 0.15 K) at a critical pressure p(c) = 2.8 GPa at which long range magnetic order vanishes. It is. therefore, regarded as a possible candidate for magnetically mediated superconductivity (SC). We report on measurements of the heat capacity of CeIrIn5 at hydrostatic pressure pless than or equal to1.6 GPa. With increasing pressure, T-c increases almost linearly up to the maximum pressure applied, while the effective mass of the quasiparticles m(eff) decreases as indicated by the ratio C/T (T = 1 K). This may be interpreted as the stabilization of the superconducting state by the increase of the characteristic spinfluctuation temperature T-SF (T-SF:infinityk(p)(2)/c m(eff)). (C) 2002 Elsevier Science B.V. All rights reserved.