1967
DOI: 10.1103/physrevlett.18.283
|View full text |Cite
|
Sign up to set email alerts
|

Observation of Spin Waves in Sodium and Potassium

Abstract: Phys. Rev. Letters JL8, 283 (1967). 5 F. J. Dyson, Phys. Rev. 98, 349 (1955). 6 M. Lampe and P. M. Platzman, Phys. Rev. 150, 340 (1966). 7 In principle, an absolute measurement of the susceptibility determines the value of the isotropic exchange parameter. In practice, this measurement [R. Schumacher, T. Carver, and C. P. Slichter, Phys. Rev. 95^, 1089 (1954)] is extremely difficult to perform and gives results which necessarily have poor accuracy. 8 P. Nozieres, Theory of Interacting Fermi Systems (W. A. Be… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

2
38
0

Year Published

1970
1970
2012
2012

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 201 publications
(42 citation statements)
references
References 8 publications
2
38
0
Order By: Relevance
“…With this analogy in mind, collective modes in an SO-coupled FL are somewhat similar to spin waves in a FL subject to a (real) magnetic field [8][9][10]. Spin waves occur because the exchange interaction couples precessing spins located at some distance from each other; this results in a dispersive mode which starts off at the unrenormalized (thanks to the Kohn's theorem) Larmor frequency and decreases with the wavenumber.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…With this analogy in mind, collective modes in an SO-coupled FL are somewhat similar to spin waves in a FL subject to a (real) magnetic field [8][9][10]. Spin waves occur because the exchange interaction couples precessing spins located at some distance from each other; this results in a dispersive mode which starts off at the unrenormalized (thanks to the Kohn's theorem) Larmor frequency and decreases with the wavenumber.…”
mentioning
confidence: 99%
“…(8a) and (8b) via m i = 1/2D i , E i = Ω 2 i , and V i (r) = ∆ 2 (r)(1 + F a 0 δ i ) are the "potential energies", which we now allow to vary slowly (compared to the electron wavelength) in the 2DEG plane. The lateral variation of ∆ confines the spin-chiral modes and thus allows to extract the information about their dispersion, similar to how it was done for spin waves in He3 [9] and alkaline metals [10].…”
mentioning
confidence: 99%
“…About ten years later Platzman and Wolff [3] made the next step; they derived a theory for the main propagating spin wave mode with accuracy up to k2, where k is the wave vector of an external disturbance. With the help of their theory, Schultz and Dunifer [4] extracted from experiment values for the first two Landau parameters. Their experiment together with the Platzman-Wolff theory extended Silin's consideration to the case of propagating spin waves in a metal and became the basis of a new spectroscopic method in metal physics.…”
Section: Introductionmentioning
confidence: 99%
“…At present paper we study the collective modes arising from the oscillations of the spin density in layered structures. The paramagnetic spin waves in quasi-isotropic metals were predicted by Silin [3] and observed in alkaline metals by Dunifer and Schultz [4]. The wave processes in layered conductors are characterized by a number of features associated with the quasi-two-dimensional electron energy spectrum.…”
mentioning
confidence: 99%