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JOURNAL OF RESEARCH of the National Bureau of Standards-A. Physics and Chemistry Vol. 74A, No. 4, July-August 1970 Pauli Paramagnetism in Metals with High Densities of States*l S. Foner Francis Bitter National Magnet Laboratory, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139 (October 10, 1969) Beca use the Pauli paramagnetic susceptibility of a free electron gas, is proportional to the density of states N(O) at the Fermi energy, it is expected that mea- surements of of metals and alloys can yield a reasonable measure of N(O). If xg can be measured directly, then N(O) ca n be determined with high accura- cy. The major obstacle to this procedure is that the mea s ur ed static susceptibility Xi, = xV(l-N(O)V)=xgD (for th e Stoner model) where V is a measure of the elec- tron-electron interaction potential. Unfortunately, V is not easily determined experimentally, or theoretically, so that measurements of Xv do not yield accurate mea- sures of N(O). More detailed (realistic) models involve additional parameters which are also not accurately determined. Thus direct measurements of Xv can yield a measure of N(O), but the se values of N(O) are subject to the uncertainties of various parameters in the theo- ries. In this talk we discuss the present status of experi - ments and theories of Xv in metals and alloys with low N(O) where D is generally near unity, and high N(O) where D is expected to be lar ge. Comparisons with in- dependent low-temperature electron ic specific heat measurements are discussed and attempts to derive N(O) from both susceptibility and specific heat are reviewed. Many recent investigations of metals and alloys with high densities of states have been of great interest because such systems start to approac h ferromagnetic order. The properti es of Pd have been investigated ex- ten sively and very detailed band calculations now exist. The large exc han ge en han cements in this metal and its * An invited paper presented at the 3d Materials Research Sym- pos ium , Electronic Density of States, November 3-6, 1969, Gaithersb urg, Md. I Supported by the U.S. Air Force Office of Scientific Research. alloys have permitted considerable progress to be made. The properties of thes e systems are reviewed and es timate s of N(O) and V are exa mined. Here qualita- tive and quantitative comparisons of various experi - ments can be made. The possibilities of applying large magnetic fields and thereby independently measuring N(O) and small changes of N(O) near th e Fermi energy by such studies are discussed. Recent theories which examine the changes of Xv with alloying are also com- pared with experimental results. A few useful references for relevant recent papers concerning the susceptibility of nearly ferromagnetic metals and alloys are tabulat ed in references 1 to 4. Re ce nt de tailed band calculations in Pd have been re- ported in references 5 to 8. Several papers at this con - f ere nce also d eal with high densities of states materials. 1. References [1] Foner , 5., Fre eman, A. J. , Blum, N., Frankel, R. B. , McNiff, E. J. , Jr., and Praddaude, H., Phys. Rev. 181,863 (1969). [2] Foner , 5., and McNiff, E. J. , Jr., Phys. Rev. Letters 19, 1438 (1967). [3] Foner, 5., and McN iff, E. J., Jr., Phy s. Letters 29A, 28 (1969). [4] Doclo, R. , Foner, 5., and Narath, A. , J. App!. Phys. 40,1206 (1969). [5] Mueller, F. M., Fr eeman, A. ]., Dimmock, 1. 0. , and Furdyna , A. (to be published). [6] Hodges, L., Ehrenreich, H. , and Lang, N. D. , Phy s. Rev. 152, 505 (1966). [7] Anderson, O. K., and Mackintosh, A. R. , So li d State Comm. 6,285 (1968). [8] Misetich, A. A. , and Watson, R. E., 1. App!. Phys. 40, 1211 (1969). (Paper 74A4-623) 567

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JOURNAL OF RESEARCH of the National Bureau of Standards-A. Physics and Chemistry

Vol. 74A, No. 4, July-August 1970

Pauli Paramagnetism in Metals with High Densities of States*l

S. Foner

Francis Bitter National Magnet Laboratory, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

(October 10, 1969)

Because the Pauli paramagnetic susceptibility of a free electron gas, x~ is proportional to the density of states N(O) at the Fermi energy, it is expected that mea­surements of X~ of metals a nd alloys can yield a reasonable measure of N(O). If xg can be measured directly, then N(O) can be determined with high accura­cy. The major obstacle to this procedure is that the measured static susceptibility Xi, = xV(l-N(O)V)=xgD (for the Stoner model) where V is a measure of the elec­tron-electron interaction potential. Unfortunately, V is not easily determined experimentally, or theoretically, so that measurements of Xv do not yield accurate mea­sures of N(O). More detailed (realistic) models involve additional parameters which are also not accurately determined. Thus direct measurements of Xv can yield a measure of N(O), but these values of N(O) are subject to the uncertainties of various parameters in the theo­ries. In this talk we discuss the present status of experi ­ments and theories of Xv in metals and alloys with low N(O) where D is generally near unity , and high N(O) where D is expected to be large. Comparisons with in­dependent low-temperature electronic specific heat measurements are discussed and attempts to derive N(O) from both susceptibility and specific heat are reviewed.

Many recent investigations of metals and alloys with high densities of states have been of great interest because such systems start to approach ferromagnetic order. The properties of Pd have been investigated ex­tensively and very detailed band calculations now exist. The large exchan ge en hancements in this metal and its

* An invited paper presented at the 3d Materials Research Sym­posium , Electronic Density of States, November 3-6, 1969, Gaithersb urg, Md.

I Supported by the U.S. Air Force Office of Scientific Research.

alloys have permitted considerable progress to be made. The properties of these systems are reviewed and estimates of N(O) and V are examin ed. Here qualita­tive and quantitative comparisons of various experi­ments can be made. The possibilities of applying large magnetic fields and thereby independently measuring N(O) and small changes of N(O) near the Fermi energy by such studies are discussed. Recent theories which examine the changes of Xv with alloying are also com­pared with experimental results.

A few useful references for relevant recent papers concerning the susceptibility of nearly ferromagnetic metals and alloys are tabulated in references 1 to 4. Recent detailed band calculations in Pd have been re­ported in references 5 to 8. Several papers at this con­ference also deal with high densities of states materials.

1. References

[1] Foner, 5., Freeman, A. J. , Blum, N., Frankel , R. B. , McNiff, E. J. , Jr., and Praddaude, H., Phys. Rev. 181,863 (1969).

[2] Foner, 5., and McNiff, E. J. , Jr., Phys. Rev. Letters 19, 1438 (1967).

[3] Foner, 5., and McNiff, E. J., Jr., Phys. Letters 29A, 28 (1969). [4] Doclo, R. , Foner, 5., and Narath , A. , J. App!. Phys. 40,1206

(1969). [5] Mueller, F. M., Freeman, A. ]., Dimmock, 1. 0. , and Furdyna,

A. (to be published). [6] Hodges, L., Ehrenreich, H. , and Lang, N. D. , Phys. Rev. 152,

505 (1966). [7] Anderson , O. K., and Mackintosh, A. R. , Solid State Co mm.

6,285 (1968). [8] Misetich, A. A. , and Watson , R. E., 1. App!. Phys. 40, 1211

(1969).

(Paper 74A4-623)

567