Landau damping and wall dissipation in large metal clusters
Journal Article
·
· Annals of Physics (New York); (United States)
- Virginia Commonwealth Univ., Richmond, VA (United States) Istituto Nazionale di Fisica Nucleare, Milan (Italy)
- Universita di Milano, Milano (Italy) Istituto Nazionale di Fisica Nucleare, Milan (Italy) Niels Bohr Institute, Copenhagen (Denmark)
The discrete-matrix random phase approximation (RPA) is used to describe the photoabsorption of large, spherical metal clusters. In this limit, the single-peak, classical Mie regime is valid and the matrix-RPA equations can be solved analytically. The RPA yields a closed formula for the width, [Gamma], of this peak due to Landau damping. This width is inversely proportional to the radius R of the cluster, in agreement with experimental observations for large silver and gold clusters embedded in a host medium. The RPA proportionality coefficient is unequivocally determined, and the reasons for the uncertainty in its value arising from disagreements among previous theoretical approaches are discussed. [Gamma]=[lambda]g([h bar][Omega][sub sp]/[var epsilon][sub F])[bar [upsilon]]/R, where [lambda] is the multipolarity of the plasma vibration, [Omega][sub sp] is the frequency of the surface plasmon, and [var epsilon][sub F] is the Fermi energy of the conduction electrons. The function g varies from unity to zero as the frequency of the surface plasmon increases from zero to infinity. The frequency dependence of g for a spherical shape is identical to that of a cubical boundary. [bar [upsilon]]=(3[upsilon][sub F]/4)(1 + ([pi][sup 2]/6)(T/[var epsilon][sub F])[sup 2]) is the average speed of a Fermi gas at temperature T. This result indicates a very small dependence on temperature, in agreement with the observation. A classical interpretation of this result is proposed based on the similarities with the one-body, wall-dissipation theory familiar from nuclear physics. According to this interpretation, the surface of the cluster is viewed as a moving wall whose interaction with the conduction electrons mimicks the multipole transitions induced by the electric field of the plasmon. This interpretation expresses [Gamma] as the ratio, [Gamma] = y/B, of a surface friction coefficient, y, over an inertia mass, B. 81 refs., 4 figs.
- OSTI ID:
- 6908814
- Journal Information:
- Annals of Physics (New York); (United States), Journal Name: Annals of Physics (New York); (United States) Vol. 217:1; ISSN 0003-4916; ISSN APNYA6
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
664000* -- Atomic & Molecular Physics-- (1992-)
665000 -- Physics of Condensed Matter-- (1992-)
74 ATOMIC AND MOLECULAR PHYSICS
75 CONDENSED MATTER PHYSICS
SUPERCONDUCTIVITY AND SUPERFLUIDITY
ATOMIC CLUSTERS
DAMPING
ELEMENTS
ENERGY-LEVEL TRANSITIONS
FERMI GAS
FLUIDS
FREQUENCY DEPENDENCE
GASES
GOLD
LANDAU DAMPING
METALS
MULTIPOLE TRANSITIONS
OPTICAL PROPERTIES
PHYSICAL PROPERTIES
PLASMONS
QUASI PARTICLES
RANDOM PHASE APPROXIMATION
SILVER
TRANSITION ELEMENTS
665000 -- Physics of Condensed Matter-- (1992-)
74 ATOMIC AND MOLECULAR PHYSICS
75 CONDENSED MATTER PHYSICS
SUPERCONDUCTIVITY AND SUPERFLUIDITY
ATOMIC CLUSTERS
DAMPING
ELEMENTS
ENERGY-LEVEL TRANSITIONS
FERMI GAS
FLUIDS
FREQUENCY DEPENDENCE
GASES
GOLD
LANDAU DAMPING
METALS
MULTIPOLE TRANSITIONS
OPTICAL PROPERTIES
PHYSICAL PROPERTIES
PLASMONS
QUASI PARTICLES
RANDOM PHASE APPROXIMATION
SILVER
TRANSITION ELEMENTS