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Dive into the research topics where T. Graf is active.

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Featured researches published by T. Graf.


Physica B-condensed Matter | 1996

Response of CeRh2Si2 to pressure

R. Movshovich; T. Graf; D. Mandrus; M. F. Hundley; J. D. Thompson; R. A. Fisher; Norman E. Phillips; J. L. Smith

Abstract Under atmospheric pressure, CeRh2Si2 orders antiferromagnetically at TN = 35 K, with magnetic entropy S = Rln2 associated with the ordered groundstate. Application of modest pressure (≈ 9 kbar) to CeRh2Si2 suppresses TN to near zero Kelvin, increases its Sommerfeld coefficient of specific heat by nearly a factor of 3.5 and induces some form of superconductivity below 400 mK which is depressed by a magnetic field at a rate of − 80 mK/kG.


Physica B-condensed Matter | 1994

Magnetism in CeRu2Ge2 and CeRh2Ge2 and its pressure dependence

J. D. Thompson; Y. Uwatoko; T. Graf; M. F. Hundley; D. Mandrus; Claude Godart; L.C. Gupta; P.C. Canfield; Albert Migliori; H.A. Borges

Abstract We have studied magnetism in CeRu 2 Ge 2 and CeRh 2 Ge 2 through specific heat in zero and applied magnetic fields, DC magnetization, thermal expansion and electrical resistance measurements at pressures to 21 kbar. Both compounds have two magnetic transitions; although we argue that the higher one in CeRu 2 Ge 2 is due to residual stress in the polycrystalline sample. The overall systematics are consistent with those found at ambient pressure in pseudoternaries formed with Si substitution for Ge.


Physica B-condensed Matter | 1995

High field magnetotransport and specific heat in YbAgCu4

A. Lacerda; T. Graf; M. F. Hundley; M. S. Torikachvili; J. M. Lawrence; J. D. Thompson; Donald Anthony Gajewski; Paul C. Canfield; Z. Fisk

The electrical resistivity (ρ{variant}) and magnetoresistance of polycrystalline YbAgCu4 have been measured at temperatures between 25 mK and 300 K, and at magnetic fields (B) up to 18 T. The magnetoresistance (ρ{variant}(B) - ρ{variant}(0))/ρ{variant}(0)) is positive at all temperatures below 200 K and reaches its maximum of 60% at 18 T and 25 mK. The field- and temperature-dependent resistivity does not scale in a simple way. The opposite sign of the magnetoresistance at ambient and high pressure can be explained qualitatively by crystal-field effects lifting the degeneracy of the J = 7 2 groundstate. The linear coefficient of the specific heat (γ) measured at fields up to 10 T shows a quadratic field dependence. We did not find a linear relation between γ2 and A, the T2-coefficient of the temperature-dependent resistivity, with the applied magnetic field as the implicit parameter.


Physica B-condensed Matter | 1995

Effect of pressure of the magnetic transitions in CeRh2Ge2 and CeRu2Ge2

Y. Uwatoko; G. Oomi; T. Graf; J. D. Thompson; Paul C. Canfield; H.A. Borges; Claude Godart; L. C. Gupta

We have studied the effect of pressure on the magnetic transition in CeRh 2 Ge 2 and CeRu 2 Ge 2 by electrical resistance measurements in the temperature range between 1.2 K and 300 K. Both samples show two magnetic transitions below 30 K. In CeRh 2 Ge 2 , the magnetic transition temperatures increase with increasing pressure. In the case of CeRu 2 Ge 2 , the upper magnetic transition temperature increases with pressure, whereas the lower one decreases with increasing pressure


Physica B-condensed Matter | 1994

Effect of high pressure and magnetic field on the electrical resistivity of YbAgCu4

T. Graf; J. D. Thompson; P. C. Canfield; M.B. Maple; Z. Fisk

Abstract The electrical resistivity of YbAgCu4 has been measured at pressures up to 100 kbar and at temperatures between 1 and 300 K. With increasing pressure, the resistivity maximum shifts to lower temperatures and the coherent regime disappears above about 60 kbar. At the highest pressures, a field of 8 T produces a large negative magnetoresistance, roughly equivalent to a negative pressure of 30 kbar. The behavior is consistent with a pressure-induced decrease in the Kondo temperature.


Physica C-superconductivity and Its Applications | 1994

High field magnetoresistance of La1.99Sr0.01CuO4+δ

A. Lacerda; T. Graf; J.H. Cho; J. D. Thompson; M. P. Maley

Abstract The in-plane resistance of a La 1.99 Sr 0.01 CuO 4 single crystal has been measured as a function of temperature (4K 2+ spin component.


Journal of Applied Physics | 1994

Magnetic field dependence of Tc of EuB6 (abstract)

A. Lacerda; T. Graf; J. L. Sarrao; M. F. Hundley; D. Mandrus; J. D. Thompson; Z. Fisk

We report measurements of resistivity and transverse magnetoresistance (B⊥I) on a single crystalline sample of EuB6 in magnetic fields to 18 T in a temperature range from 4 to 100 K. The ferromagnetic transition (Tc) determined by resistivity versus temperature at constant field varies from 10 to 25 K at zero and 4 T, respectively. The transition is completely suppressed at 8 T. A very large and negative tranverse magnetoresistance is observed in the entire temperature range investigated: −5% at 4 K and −20% at 100 K at 18 T. Finally, the effect of high applied magnetic field on the transport properties is investigated in the temperature range below Tc.


Physical Review B | 1998

Magnetic phase transitions in CeRh 2 Si 2 : Specific heat, susceptibility, and resistance studies

T. Graf; M. F. Hundley; R. Modler; R. Movshovich; J. D. Thompson; D. Mandrus; R. A. Fisher; Norman E. Phillips


Physical Review B | 1995

Suppression of the metal-to-insulator transition in BaVS3 with pressure.

T. Graf; D. Mandrus; J. M. Lawrence; J. D. Thompson; P.C. Canfield; S.-W. Cheong; L. W. Rupp


Physical Review B | 1995

Resistivity, magnetization, and specific heat of YbAgCu{sub 4} in high magnetic fields

T. Graf; J. M. Lawrence; M. F. Hundley; J. D. Thompson; A. Lacerda; E. Haanappel; Torikachvili; Z. Fisk; Paul C. Canfield

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J. D. Thompson

Los Alamos National Laboratory

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D. Mandrus

Los Alamos National Laboratory

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M. F. Hundley

Los Alamos National Laboratory

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Z. Fisk

University of California

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A. Lacerda

Los Alamos National Laboratory

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R. Movshovich

Los Alamos National Laboratory

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J. M. Lawrence

Los Alamos National Laboratory

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Joe D. Thompson

Los Alamos National Laboratory

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