Statistical and electrical properties of the conduction electrons of a metal nanosphere in the region of metal-insulator transition
© Datsyuk and Ivanytska; licensee Springer. 2014
Received: 10 December 2013
Accepted: 25 March 2014
Published: 10 April 2014
Statistical and electrical properties of the conduction electrons of a silver or gold sphere with a radius from 1 to 2 nm are shown to differ drastically from the properties of electrons in a bulk metal sample. If the radius of a noble metal sphere decreases from 10 to 1 nm, its conductivity oscillates around the bulk metal value with increasing amplitude and drops at the 'magic’ numbers of electrons. These numbers are equal to 186, 198, 254, 338, 440, 556, 676, 832, 912, 1,284, 1,502, and 1,760, in agreement with various experimental data. We show that the conductivity and capacitance of a metal nanosphere can be changed by several orders of magnitude by adding or removing just a few electrons.
In the past, a measurement of optical absorption by silver nanoparticles embedded in glass showed that the particles had normal metallic properties when their diameters were decreased down to 2.2 nm . Contrary to this finding, metal particles with sizes below 2 nm cannot be conducting according to more recent papers [2, 3]. Very recently, it was understood that the metal-insulator transition (MIT) is gradual so that particles with certain 'magic’ numbers of electrons become insulating while others remain conducting . If electrons move inside a sphere, then the numbers 186, 198, 254, 338, 440, 556, 676, 832, 912, 1,284, 1,502, and 1,760 are known to be 'magic’. It was experimentally found that the above numbers are indeed magic for clusters of many metals [5–16]. This allows one to consider the motion of electrons in a spherical jellium [8, 12, 17, 18].
We recently studied statistical properties of 500 to 2,000 free electrons confined in a spherical potential well with a radius from 1.2 to 2 nm. The averaged occupation numbers of the electron energy levels and the variances of the occupation numbers were computed for both isolated metal nanoparticles and those in equilibrium with an electron bath. The sum of the variances of all occupation numbers was found to depend on the number of electrons nonmonotonically dropping by a few orders of magnitude at 'magic numbers’ of electrons. Here, we show how the statistical properties of the conduction electrons are related with the electrical properties of metal nanoparticles. Calculations of the DC conductivity and capacitance of single nanometer-sized noble metal spheres are reported. We predict a transistor-like behavior of a single nanoparticle when an additional charge of the particle drastically changes its conductivity and capacitance.
Statistical and transport models
The electron statistics and capacitance of metal nanoparticles are investigated by the Gibbs ensemble method. The transport properties of electrons are studied using a quantum-mechanic generalization of a formula that can be obtained by solving the Boltzmann transport equation.
The Boltzmann transport equation (BTE) is widely used in modern physical kinetics [19, 20] even at nanoscales [21, 22]. In our previous work, we solved BTE and determined the response of the conduction electrons on an electromagnetic wave allowing for dependence of the distribution function on the wavenumber. Then, we obtained the spatially dispersive permittivity of metal and applied a generalized Mie theory  to calculate spectra of light extinction by silver nanospheres. Because of excitation of the rotationless (longitudinal) plasmon-polariton waves, the frequency of the Fröhlich resonance ω=3.5 eV  was found to increase with decreasing the radius a, so ω=3.635 eV for particles with a=1.5 nm and ω=3.73 eV at a=1 nm (see Figure two of ; a similar dependence of ω on a as well as the formulas of  is found in a recent paper ). The blueshift by 0.15 eV and the width of the plasmon resonance calculated for a particle beam created by Hilger, Tenfelde, and Kreibig  were in excellent agreement with the experimental data. We concluded that silver clusters with a<1 nm do not contribute into the extinction spectra of the beams. However, it was not possible to establish whether the contribution of these ultrathin particles into the integral extinction spectrum vanished due to MIT.
Energies of the conduction electrons
It is a common practice to assume that the conduction electron energy ε in metal is a function of the continuous quasi-momentum This approach can be used to model the properties of bulk metals in which an electron state s can be described by a set of four quantum numbers, where is a projection of the electron spin. However, if an electron moves inside a microscopic sphere, the vector p can no longer describe an electron state. The set p x ,p y , and p z has to be replaced by a set of the radial q, angular momentum l, and magnetic m quantum numbers. Then, integrals over p should be replaced by sums over the electron states s, according to the following rule: , where V is the volume of the body and h is the Plank constant. In this study, we used discrete sets of the electron energies ε s .
Shape of metal nanoparticles
Results and discussion
Variances of the occupation numbers
where e and m e are the charge and effective mass of the electron, respectively, n e =N/V, ε=p2 / (2 m e ),f(ε) is an equilibrium electron energy distribution function, and τ is the relaxation time. From Equation 1, the classical result is obtained at τ=const and any f(ε) finite at ε=0 and vanishing at ε→∞. The formula for σb can also be derived by substituting a zero-temperature Fermi-Dirac distribution function into Equation 1.
Normalized conductivity (%) calculated for an Ag or Au particle with a magic number of atoms
All the experimental numbers Nm in Figure 1 were obtained by using the mass spectroscopy from dips in the mass spectra. For example, Katakuse and co-workers  found magic numbers of atoms equal to 197 for negative cluster ions of silver (Ag)n- and 199 for positive cluster ions. Other magic numbers of atoms were 137 for , , and and 139 for , , and . In these cases, the negatively and positively charged and neutral particles had the same magic numbers of electrons, Nm= 198 and 138. Thus, the anomalous properties of the metal nanoparticles in the experiments [5–15] are determined by electron motion  but not their atomic structure. Moreover, the model of single electrons trapped in a spherical potential well was shown to be adequate  though the shape of the clusters obtained by the bombardment of metal sheets with Xe ions was not controlled.
A nonlinear dependence of on N can occur even in a single sphere if N varies around Nm. To examine electric properties of a single charged nanoparticle, let us consider a sphere in thermal equilibrium with a reservoir of electrons, so the electrochemical potential μ=μ0+e ϕ is constant inside the sphere; here μ0 is the chemical potential of the neutral sphere and ϕ is the electric potential. For a fixed μ, we determined by using the Fermi-Dirac occupation numbers and computed the charge of the sphere Q=e (N-N0), where N0 is the number of electrons in the neutral particle. We calculated the quantities Q and for a charged 336-atom Ag or Au nanoparticle. We found that the 336-atom particle holds two extra electrons when the value ϕ changes in a wide range of about 0.6 V. If the mean number of electrons in the particle is equal to 338, then . The normalized conductivity of the neutral sphere is found to be ; In the considered example, the neutral sphere is conductive, but the charged one with two extra electrons turns out to be an insulator.
A straightforward calculation of the derivative of Q gives the capacitance of the charged particle with 338 electrons C=6.1×10-22 F that is much lower than C=1.1×10-17 F of the neutral 336-atom sphere. The change in the capacitance C(338)/C(336)=5.3×10-5 is similar to the the correspondent change in the conductivity.
where Δ is the sum of the variances of the occupation numbers shown in Figure 2 by crosses. Equation 5 expresses the relation between the reaction of the conduction electrons to the electric field and the fluctuations of the occupation numbers of the electron states. Thus, the peculiarities of spacing and degeneracy of the electronic energy levels have similar effects on the statistical and electrical properties of a nanometer-sized particle.
During the calculations we neglected Coulomb effects. These effects are as follows. When an electron leaves a neutral metal sphere, it overcomes the attraction of the positive charge remaining on the sphere. Consequently, the work function increases by the value Δ U = 0.54/a(nm) eV . For example, Δ U ≃ 0.5 eV for a 338-atom noble-metal sphere. In addition, Coulomb forces should change the binding energy of the electron in a charged sphere compared to that in the neutral one. Though the change in U can be large, it should not be critical to the effects studied in this paper. Indeed, they depend on the value of εf+1-ε f , but this difference is a weak function of U. For example, for a noble metal sphere with 338 conduction electrons, we get εf+1-ε f =0.69 eV at U=9.8 eV, and εf+1-ε f =0.74 eV if U→∞.
In conclusion, the statistical properties, conductivity, and capacitance of a single nanometer-sized metal sphere depends very strongly on the number of conduction electrons N in the range from 200 to 2,000. In particular, the DC conductivity drops by several orders of magnitude if N is equal to one of the magic numbers. For instance, addition of two electrons to a 336-atom noble metal sphere should reduce both the conductivity and capacitance of the particle by four orders of magnitude.
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