Abstract
We report on two extensions of the traditional analysis of lowdimensional structures in terms of lowdimensional quantum mechanics. On one hand, we discuss the impact of thermodynamics in one or two dimensions on the behavior of fermions in lowdimensional systems. On the other hand, we use both quantum wells and interfaces with different effective electron or hole mass to study the question when charge carriers in interfaces or layers exhibit twodimensional or threedimensional behavior. We find in particular that systems with different effective masses in the bulk and in the interface exhibit separation of twodimensional and threedimensional behavior on different length scales, whereas quantum wells exhibit linear combination of twodimensional and threedimensional behavior on short length scales while the behavior on large length scales cannot be associated with either twodimensional or threedimensional behavior.
Keywords:
Density of states; Coulomb interactions; Exchange interactions; Scattering in nanostructures; Thermal properties in nanostructures; Fermi energy in nanostructuresBackground
Nanostructures traditionally provide approximate realizations of lowdimensional systems through confined electron states in one dimension (thin films, interfaces or quantum wells), two dimensions (quantum wires or nanowires), or three dimensions (quantum dots or color centers). We emphasize electron states rather than electrons in the following discussions, because for conduction bands with large filling factors or pdoped semiconductors, we usually think of the unoccupied electron states as holes, which can also be confined [13].
In the olden days, confined electron states primarily provided dimensionally restricted
realizations of electric charge carriers, but since the advent and rise of spintronics,
lowdimensional spin systems also play an important role in nanotechnology. Lowdimensional
spin systems are directly linked to confined electron states because the coupling
of a particle with spin
Here, m is the (effective) mass, and q is the charge of the particle, q = ±e for holes or electrons, respectively.
A wellknown primary effect of a reduced number d of dimensions in nanosystems is the significant change in the energy dependence
of the density of states in the energy scale,
Confinement of electromagnetic fields and photons is harder to accomplish than for
electrons or holes, but effects of restricted dimensionality are also striking and
of high potential relevance for technology
[6]. Confinement of electromagnetic fields changes the distance law for electric forces
to
Figure 1. Electric potentials Φ_{d,a}(r) with screening length a. The red curve corresponds to d=1, blue to d=2, and black to d=3.
Figure 1 illustrates that in lower dimensions, interactions are comparatively stronger at large distances and weaker at short distances. The same effect would apply for any other interaction which would be mediated by confined bosons; for example, it would also apply to phononmediated interactions between electrons or holes. The reduced interaction strength at smaller distance in lower dimensions is a consequence of the weaker singularity of the field near its source, whereas the increase in strength at larger distance intuitively can be attributed to the squeezing of field lines into a smaller number of dimensions. This change in distance behavior directly impacts electric forces between charges and implies the potential emergence of electrical confinement in systems with dimensionally restricted electromagnetic fields. In addition, it also impacts effective spinspin interactions in spintronics because the ddimensional electrical potential also appears in the exchange integrals which determine the energy splits between spin configurations.
Methods
Lowdimensional quantum mechancis with one or twodimensional Hamilton operators, or threedimensional Hamiltonians with confining boundary conditions are widely used to analyze and understand the importance of quantum effects on confined particles in nanosystems. Here, we wish to report on extensions of this analysis in two directions: (1) impacts of lowdimensional thermodynamics on the behavior of charge carriers and (2) quantum mechanical analysis of interdimensional behavior in materials with a lowdimensional component. We focus also on a thin interface or layer as the lowdimensional component, but the same methods can be applied, e.g., to analyze dimensional competition in the case of a nanowire on a surface [8]. Interdimensional effects in these systems can be relevant, e.g., for charge transport in nanowires, which attract a lot of interest, e.g., for its use in photovoltaics [9]. We will use both the method of interdimensional Green’s functions [4,5,10] and grand canonical ensembles in lowdimensional systems to analyze impact of dimensionality of a system on the behavior of electrons and photons.
The ddimensional fields and potentials are direct consequences of the solutions of LaplacePoisson or Helmholtz equations in d dimensions. The pertinent properties of these solutions are generically encoded in the Green’s functions which satisfy
in the energy representation, or
in the time domain. The Green’s functions are related according to
The solutions of Equations (1) and (2) provide us with single particle or mean field Green’s functions, which describe scattering of particles and densities of states, and through particular choices or redefinition of the energy parameter, they also determine electric potentials and exchange interactions. In addition, the single particle Green’s functions also enter into the calculation of electronic configurations for many particle systems through application of multiple scattering theory [11].
The conditions (1) and (2) do not completely specify the Green’s functions, and we
impose the physical boundary conditions that the Green’s function in the region of
negative energy E < 0 should vanish for
in the time domain. The energydependent Green’s functions are with the notation
(see Appendix I in
[7] for derivations). The functions K_{ν }and
However, if there are parameter ranges in materials and devices where electrons or photons behave according to the laws of twodimensional or threedimensional quantum mechanics and electrodynamics, then there should also exist transition regimes with intermittent dimensional behavior. This is the realm where particles or forces are described by the interdimensional or dimensionally hybrid Green’s functions introduced in [4,5]. We should also point out that another important novel approach to interdimensional behavior in systems with lowdimensional components concerns the study of interdimensional universality for critical scaling laws. This notion has been introduced and studied for domain wall dynamics in nanowires [13].
We will review the basic aspects of physics in various dimensions in the section on “Green’s functions, potentials, and densities of states in d dimensions” and then discuss a lesser known but technologically relevant aspect of physics in lower dimensions, viz., the impact of dimensionality on statistical and thermal physics in lowdimensional systems, in the section on “Thermal properties of the charge carriers in d dimensions”. We will then discuss the construction of dimensionally hybrid Green’s functions for quantum wells in the section on “Interdimensional effects in interfaces and thin layers”. This will also allow us to calculate the interdimensional density of states ϱ(E) and the relation between Fermi energy and electron density in the quantum well in the section entitled “Density of states for the thin quantum well”. Comparison of the results for the quantum well with the results for layers with different effective mass of charge carriers [5] or different permittivity [6] reveals that a difference in potential energy between a layer and a bulk yields linear combinations of twodimensional and threedimensional terms at the same length scales, whereas difference in kinetic terms (viz. effective mass which affects kinetic terms for electrons, holes, or permittivity, which affects the kinetic terms for photons), separates twodimensional behavior on short length scales from threedimensional behavior at large length scales.
Results and discussion
We can now enter into the discussion of less known results on the lowdimensional quantum and statistical physics of charge carriers and new results and observations concerning interdimensional behavior in the presence of layers or interfaces. We will separate this discussion into subsections on interaction potentials and thermal properties in lowdimensional fermion systems, and a subsection on interdimensional effects as inferred from Green’s functions.
Green’s functions, potentials and densities of states in d dimensions
We have chosen the paradigm of the Green’s functions for the free Schrödinger equation
(1,2) because it encompasses most of the practical applications of Green’s functions
in materials and devices. The energydependent Green’s function for the free Schrödinger
equation not only describes the electron or hole scattering of impurities or the density
of states in the energy scale in free electron gas models, but it also describes the
electric potential of a charge density
The Coulomb and exchange type potentials and interactions are given in terms of this Green’s function through
and
respectively. Furthermore, with the substitution 2mE = −ℏ^{2}/a^{2}, the energydependent Green’s function also describes screened interaction potentials with screening length a,
and correspondingly screened exchange interactions. Practical realization of lowdimensional Coulomb or Yukawa potentials (Equations (7) and (9) with d = 1 or d = 2) in devices may be possible with the help of photonic bandgap materials, and the twodimensional logarithmic behavior should be realized at short distances in high permittivity thin films [6].
However, a more direct and immediate application of ddimensional Green’s functions in materials science and device engineering concerns
scattering in lowdimensional structures. Scattering of a particle of momentum
This yields the differential scattering cross section in d dimensions,
with the scattering amplitude
The most interesting feature of this result from a nanodevice point of view concerns
suppressed high energy scattering and enhanced low energy scattering from impurities
in low dimensions roughly according to
Another application of lowdimensional physics for nanoscale devices concerns the density of states (or number of electronic orbitals) in the energy scale,
These are densities of states per ddimensional volume and per unit of energy, i.e., Vϱ_{d}(E)dE is the number of electronic states in a ddimensional volume V and with energies between E and E + dE. The corresponding relation between the Fermi energy E_{F }and the density n of electrons in d dimensions is therefore
This makes physical sense: In a smaller number of dimensions, we need a larger Fermi
sphere in
Equations (13) and (14) a priori refer to a free electron gas model. In materials science, this is a useful approximation for semiconductors and a very good approximation for metals at room temperature. For energy bands with minimal energy E_{0}, corresponding effective mass m_{∗}, and a low filling factor, Equation (13) applies for the electron density of states with the substitutions E → E − E_{0} and m → m_{∗}. For nearly filled bands with maximal energy E_{1}, the substitutions E → E_{1}− E, m → m_{h} yield the hole density of states.
Densities of states are important for electrical and thermal transport properties of materials and for the optical properties of materials. For example, the photon absorption crosssection for excitation of an electron from a discrete donor or quantum dot state into a continuous energy band is directly proportional to the density of final electron states. Therefore, the densities of states (13) for d = 1, 2, and 3 are common items for information in nanotechnology textbooks. However, strict electron confinement to a quantum wire or an interface is apparently a bad approximation in most cases and makes only sense for the subset of low lying energy states in deep quantum well structures. Therefore, we will revisit the density of states in the section on “Density of states for the thin quantum well” in the framework of a solvable quantum well model.
Thermal properties of the charge carriers in d dimensions
A less widely known and less developed aspect of lowdimensional physics concerns the impact of dimensionality of a system on its thermal and statistical properties. The derivation of the basic FermiDirac or BoseEinstein distributions from maximal information entropy under the boundary conditions of given energy and particle number (if we use a grand canonical ensemble) does not depend on the number of dimensions. However, the calculation of partition functions and thermodynamic quantities from the FermiDirac or BoseEinstein distributions involves ddimensional integrals; therefore, thermal properties of a system will depend on the number of dimensions in which particles can move. I would hope that the introduction in this section can serve as a brief compendium and overview of basic aspects of this dependence of thermal properties on d. We will find that the specific heat in particular is affected by d. Due to the particular relevance of confined fermionic charge and spin carriers for nanotechnology, we will focus on lowdimensional implications of FermiDirac statistics.
We can derive all the basic properties of the ddimensional fermion gas from its grand canonical potential
The approximation of an ideal nonrelativistic gas,
If the density of effectively free charge carriers in a material is small, as in a semiconductor, then the thermal properties of the electrons or holes can be described by a nondegenerate Fermi gas. With the understanding to calculate energies and chemical potentials from the corresponding energy band extremum, the conditions for applicability of a nondegenerate Fermi gas model for the conduction electrons or holes are
This is equivalent to a requirement of low volume density n_{d} of charge carriers,
The pressure and energy density of the carriers are then p_{d }= n_{d}k_{B}T and
and the entropy density is given by a ddimensional SackurTetrode equation,
The previous remarks apply to a nondegenerate fermion gas. However, the electron gas in metals has high density and is therefore described by a nearly degenerate nonrelativistic electron gas:
In that case, the particle density can be expressed asymptotically in k_{B}T/μ as
and comparison with (14) yields
The energy density and pressure then follow as
i.e., the average energy per electron in a ddimensional metal is
The specific heat per ddimensional volume follows as
In terms of the average separation
The specific heat is also related to the thermal conductivity. We can write (16) also in the form
and therefore, the thermal conductivity for collisional relaxation time τ can be written as
We can use this result to answer the question whether the relation between thermal and electrical conductivity in a metal is affected by the number of dimensions. The electrical conductivity is
i.e., the basic WiedemannFranz law for the nearly degenerate electron gas in metals holds in every dimension with the same Lorentz constant,
Interdimensional effects in interfaces and thin layers
We know that the ddimensional physics described in the previous sections for d = 1 or d = 2 can only apply to systems where the technologically relevant degrees of freedom, i.e., mostly electrons and holes as carriers of energy, charge and spin, are confined in sufficiently deep potentials to render any transverse excitations negligible. However, states closer to the binding energy of an attractive potential should exhibit intermittent behavior between lowdimensional and threedimensional behavior. Furthermore, free states near the ionization energy should also still feel the presence of the lowdimensional structure: the influence of lowdimensional physics cannot discontinuously disappear above the ionization energy. An example of a lowdimensional structure is, e.g., an interface of width 2a. Electrons may experience a potential energy V_{0}in the interface, and they might also move with a different effective mass m_{∗} in the interface, such that the Hamiltonian for electrons in the presence of the interface has the form
We will denote twodimensional coordinate vectors parallel to the interface with
We might expect twodimensional behavior in the limit a → 0 both from the difference of effective mass in the interface and from the interface
potential. Indeed, it has been shown that even without a potential difference, the
existence of a layer with different effective mass generates Green’s functions in
the interface which interpolate between twodimensional behavior for small distance
In the following, we will investigate the emergence of quasi twodimensional behavior
from an attractive interface potential V_{0} < 0 in the interface, i.e., we assume m_{∗} = m in (18). An infinitely thin attractive quantum well arises from the potential in (18)
if we set
The corresponding Schrödinger equation separates and yields three kinds of energy eigenstates. First, we have eigenstates which are moving along the interface,
We also have free states with odd or even parity under z → 2z_{0} − z,
The wave number k_{⊥} in (20) and (21) is constrained to the positive halfline k_{⊥} > 0, and the energy levels of the free states are
The completeness relation for the eigenstates is
The energydependent Green’s function
of this system must satisfy
This equation can be solved analytically using the methods described in [5,6]. The results are conveniently reported in a mixed axial representation
The retarded solution of Equation (22) in the representation (23) is
The limit κ → 0 reproduces the corresponding representation of the free retarded Green’s function in three dimensions.
Our result describes the Green’s function for a particle in the presence of the thin quantum well, but for arbitrary energy and both near and far from the quantum well. Therefore, we cannot easily identify any twodimensional limit from the Green’s function. To analyze this question further, we will look at the zero energy Green’s function G(r) ≡ 〈z_{0}G(x_{∥},E = 0)z_{0}〉, r = x_{∥}, in the thin quantum well. Fourier transformation of our result (24) yields
where H_{0}(κr) is a Struve function. The Green’s function (25) has the property to approach a linear combination of twodimensional and threedimensional Green’s functions at small distances,
but it is very different from either the twodimensional or threedimensional behavior at large distances,
(see Figure 2).
Figure 2. The zero energy Green’s function in the potential well. The black curve shows the Green’s function (25). The blue curve is the asymptotic form (26) for small distance and the red curve is the asymptotic form (27) for large distance.
It is instructive to compare this to the Green’s function which results from different effective mass or different permittivity in a layer. The corresponding zero energy Green’s function [6]
yields twodimensional behavior at small distances r ≪ ℓ and threedimensional behavior for large separation r ≫ ℓ,
(see also Figure 3). Here, the length parameter ℓ is ℓ = am/m_{∗} for an interface with different effective mass m_{∗} for electrons or holes, or ℓ = aε_{∗}/ε for an interface with different permittivity ε_{∗}.
Figure 3. The zero energy Green’s function in a layer with different effective mass or permittivity. The blue line is the threedimensional Green’s function (4Πr)^{−1}, the black line is the Green’s function (28) in a layer of different effective mass or different permittivity, and the red line is the twodimensional logarithmic Green’s function ℓ·G=−[γ + ln(r/2ℓ)]/4Π.
To explore the question of twodimensional or threedimensional behavior in the quantum well further, we will look at the density of states in the quantum well.
Density of states for the thin quantum well
The energy dependent retarded Green’s function is directly related to the density of states in a quantum system. This follows readily from the decomposition of (E−H + iε)^{−1} in terms of the spectrum E_{n }and eigenstates n,ν〉 of H,
Here, ν is a degeneracy index, and we tacitly imply that continuous components in the indices (n,ν) are integrated. We include spin in the set of quantum numbers (n,ν).
To make the connection with the density of states (or number of electronic orbitals) per volume, we observe that this quantity in general can be defined as
This implies the relation
The quantum well at z_{0} breaks translational invariance in z direction, and we have with equation (33)
where a factor g = 2 was taken into account for spin 1/2 states.
If there is any quasi twodimensional behavior in this system, we would expect it in the quantum well region. Therefore, we use the result (24) to calculate the density of states ϱ(E,z_{0}) in the quantum well. Substitution yields
and after evaluation of the integrals,
We can also express this in terms of the free twodimensional and threedimensional densities of electron states (cf. (13)),
Note that K_{2} = E + (ℏ^{2}κ^{2}/2m) is the kinetic energy of the particles whose wave functions are exponentially suppressed perpendicular to the quantum well. We find that these particles indeed contribute a term proportional to the twodimensional density of states ϱ_{d = 2}(K_{2}) with their energy K_{2} of motion along the quantum well, but with a dimensional proportionality constant κ which is the inverse penetration depth of those states. Such a dimensional factor has to be there because densities of states in three dimensions enumerate states per energy and per volume, while ϱ_{d = 2}(K_{2}) counts states per energy and per area. Furthermore, the unbound states yield a contribution which approaches the free threedimensional density of states ϱ_{d = 3}(E) in the limit κ → 0.
The density of states in the quantum well region is displayed for binding energy B = ℏ^{2}κ^{2}/2m = 1 eV, mass m = m_{e}= 511 keV/c^{2}, and different energy ranges in Figures 4 and 5. The density of states shows twodimensional behavior for energies below the threshold where the electrons or holes can leave the quantum well and a linear combination of a twodimensional term and threedimensional term (with a correction factor) for energies above the threshold. This is again very different from the corresponding behavior of electrons or holes which move with different effective mass in a layer. In that case, the density of states in the layer approaches threedimensional behavior for small separation and twodimensional behavior for large separation [6] (see in particular Equations (11) to (13) and Figure 1 in [6]).
Figure 4. The density of states in the quantum well. This displays the density of states in the quantum well location z = z_{0} for binding energy B = 1 eV, mass m = m_{e} = 511 keV/c^{2}, and energies −B ≤ E≤ 3 eV. The red curve is the contribution from states bound inside the quantum well, the blue curve is the pure threedimensional density of states in absence of a quantum well, and the black curve is the density of states according to equation (34).
Figure 5. The density of states (34) in the quantum well location z = z_{0} for higher energies 0 ≤ E ≤ 100 eV. The binding energy, mass and color coding are the same as in Figure
4. The full density of states (34) approximates the threedimensional
Integration of ϱ(E,z_{0}) yields the relation between the Fermi energy and the particle density in the quantum well. We find for −ℏ^{2}κ^{2}/2m ≤ E_{F} ≤ 0 the twodimensional area density for maximal kinetic energy K_{2,K} = E_{F} + (ℏ^{2}κ^{2}/2m) along the barrier, but rescaled with the inverse transverse penetration depth κ which converts it into a threedimensional particle density,
The result for E_{F }> 0 is a combination of the scaled twodimensional particle density (36) and the threedimensional free particle density n_{3} with additional correction terms,
(see Figure 6).
Figure 6. The relation between particle density and Fermi energy. This displays the relation between particle density and Fermi energy in the quantum well for binding energy B = 1 eV, mass m = m_{e }= 511 keV/c^{2}, and −B ≤ E_{F }≤6 eV. The red curve is the contribution from states bound inside the quantum well, the blue curve is the pure threedimensional density of states in absence of a quantum well, and the black curve is n(E_{F}) according to Equations (36) and (37).
The asymptotic form for
We can also derive these results directly from the energy eigenstates (19 to 21) and the definition (32). However, the derivation from the Green’s function (24) confirms that this is indeed a correct dimensionally hybrid Green’s function which yields interdimensional effects.
Not surprisingly, comparison of the relation between Fermi energy and density of fermions for the quantum well with the corresponding results for a layer of different effective mass [6] confirms again that the effective mass layer exhibits separation of twodimensional behavior for small lengths/high energies and threedimensional behavior for large lengths/small energies, whereas the quantum well yields a linear combination of twodimensional and threedimensional terms for small lengths/high energies.
Conclusions
The thin quantum well is certainly one of the most important model systems for lowdimensional structures in nanoscience and technology. We have found that the Green’s function of this system resembles a linear combination of twodimensional and threedimensional terms at small distances but exhibits oscillatory behavior at large distances. Furthermore, the local density of states and the relation between particle density and Fermi energy in the quantum well show twodimensional behavior for Fermi energies below the threshold for scattering out of the quantum well and a linear combination of twodimensional and threedimensional behavior plus correction terms above the threshold. This behavior is very different from the behavior of charge carriers which move with different effective mass in a layer: in that case, the analysis in [6] had shown that the system exhibits twodimensional behavior at small distances and high energies, and threedimensional behavior at large distances and low energies. The morale of the combination of the present results with the results of [6] is that if we wish to explicitly see transitions between twodimensional and threedimensional behavior in a system, then we should look for systems where the interface primarily affects the kinetic terms of fermions through a difference of effective mass between bulk and layer, or the kinetic terms of photons through a difference of permittivity between bulk and layer.
Competing interests
The author declares that he has no competing interests.
Acknowledgements
This research was supported by NSERC Canada.
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