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**|**Nanoscale Res Lett**|**v.6(1); 2011**|**PMC3211228

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Nanoscale Res Lett. 2011; 6(1): 175.

Published online 2011 February 25. doi: 10.1186/1556-276X-6-175

PMCID: PMC3211228

Osmar FP dos Santos,^{1} Sara CP Rodrigues,^{}^{1} Guilherme M Sipahi,^{2} Luísa MR Scolfaro,^{3} and Eronides F da Silva Jr^{4}

Osmar FP dos Santos: moc.liamg@cnarf.mso; Sara CP Rodrigues: rb.eprfu.fd@seugirdors; Guilherme M Sipahi: rb.psu.csfi@ihapis; Luísa MR Scolfaro: ude.etatsxt@oraflocsl; Eronides F da Silva Jr: rb.epfu@nore

Received 2010 July 5; Accepted 2011 February 25.

Copyright ©2011 dos Santos et al; licensee Springer.

This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

The electrical conductivity σ has been calculated for *p*-doped GaAs/Al_{0.3}Ga_{0.7}As and cubic GaN/Al_{0.3}Ga_{0.7}N thin superlattices (SLs). The calculations are done within a self-consistent approach to the $\overrightarrow{k}\overrightarrow{p}$ theory by means of a full six-band Luttinger-Kohn Hamiltonian, together with the Poisson equation in a plane wave representation, including exchange correlation effects within the local density approximation. It was also assumed that transport in the SL occurs through extended minibands states for each carrier, and the conductivity is calculated at zero temperature and in low-field ohmic limits by the quasi-chemical Boltzmann kinetic equation. It was shown that the particular minibands structure of the *p*-doped SLs leads to a plateau-like behavior in the conductivity as a function of the donor concentration and/or the Fermi level energy. In addition, it is shown that the Coulomb and exchange-correlation effects play an important role in these systems, since they determine the bending potential.

The transport phenomena in semiconductors in the direction perpendicular to the layers, also known as vertical transport, have been investigated in recent years from both experimental and theoretical points of view because of their increased application in the development of electro-optical devices, lasers, and photodetectors [1-3]. The theoretical decsription of the electron transport phenomena in several quantized systems, such as quantum wells, quantum wires, and superlattices (SLs), has been given in earlier studies, and it is mainly based on the solution of the Boltzmann equation [4-6]. The use of SLs is important since increasing the dispersion relation of the minibands for carriers is possible [7]. Therefore, this means that different origins of the periodic electron/hole potential, which take place in the compositional SLs and in the SLs formed by selective doping, can cause different consequences, influencing the formation of the miniband structures, altering the electrical conductivity, and affecting the electron scattering [6]. However, most of those studies treat only *n*-type systems, and very little has been reported in the literature regarding *p*-type materials, including experimental results [8-10].

In this study, the behavior of the electrical conductivity in *p*-type GaAs/Al_{0.3}Ga_{0.7}As and cubic GaN/Al_{0.3}Ga_{0.7}N SLs with thin barrier and well layers is studied. A self-consistent $\overrightarrow{k}\overrightarrow{p}$ method [11-13] is applied, in the framework of the effective-mass theory, which solves the full 6 × 6 Luttinger-Kohn (LK) Hamiltonian, in conjunction with the Poisson equation in a plane wave representation, including exchange-correlation effects within the local density approximation (LDA). The calculations were carried out at zero temperature and low-field limits, and the collision integral was taken within the framework of the relaxation time (τ) approximation.

The III-N semiconductors present both phases: the stable wurtzite (*w*) phase, and the cubic (*c*) phase. Although most of the progress achieved so far is based on the wurtzite materials, the metastable *c*-phase layers are promising alternatives for similar applications [14,15]. Controlled *p*-type doping of the III-N material layers is of crucial importance for optimizing electronic properties as well as for transport-based device performance. Nevertheless, this has proved to be difficult by virtue of the deep nature of the acceptors in the nitrides (around 0.1-0.2 eV above the top of the valence band in the bulk materials), in contrast with the case of GaAs-derived heterostructures, in which acceptor levels are only few meV apart from the band edge [9,11]. One way to enhance the acceptor doping efficiency, for example, is the use of SLs which create a two-dimensional hole gas (2DHG) in the well regions of the heterostructures. Contrary to the case of wurtzite material systems, in *p*-doped cubic structures, a 2DHG may arise, even in the absence of piezoelectric (PZ) fields [16]. The emergence of the 2DHG, is the main reason for the realization of our calculations in cubic phase; the PZ fields can decrease drastically the dispersion relation and consequently the conductivity [17,18].

The results obtained in this study constitute the first attempt to calculate electron conductivity in *p*-type SLs in the direction perpendicular to the layers and will be able to clarify several aspects related to transport properties.

The calculations were carried out by solving the 6 × 6 LK multiband effective mass equation (EME), which is represented with respect to a basis set of plane waves [11-13]. One assumes an infinite SL of squared wells along <001> direction. The multiband EME is represented with respect to plane waves with wavevectors *K *= (2π/*d*)*l *(*l *integer, and *d *the SL period) equal to reciprocal SL vectors. Rows and columns of the 6 × 6 LK Hamiltonian refer to the Bloch-type eigenfunctions $|j{m}_{j}^{}\overrightarrow{k}$ of Γ_{8 }heavy and light hole bands, and Γ_{7 }spin-orbit-split-hole band; $\overrightarrow{k}$ denotes a vector of the first SL Brillouin zone.

Expanding the EME with respect to plane waves *z*|*K* means representing this equation with respect to Bloch functions $\overrightarrow{r}|{m}_{j}\overrightarrow{k}+K{\widehat{e}}_{z}$. For a Bloch-type eigenfunction $z|E\overrightarrow{k}$ of the SL of energy *E *and wavevector $\overrightarrow{k}$, the EME takes the form:

$$\sum _{{j}^{\prime}{{m}^{\prime}}_{j}K}j{m}_{j}\overrightarrow{k}K|T+{V}_{\text{A}}+{V}_{\text{H}}+{V}_{\text{HET}}+{V}_{\text{XC}}|{j}^{\prime}{{m}^{\prime}}_{j}\overrightarrow{k}K{j}^{\prime}{{m}^{\prime}}_{j}\overrightarrow{k}{K}^{\prime}|v\overrightarrow{k}={E}_{v}(\overrightarrow{k})j{m}_{j}\overrightarrow{k}K|v\overrightarrow{k}$$

(1)

where *T *is the effective kinetic energy operator including strain, *V*_{HET }is the valence and conduction band discontinuity potential, which is diagonal with respect to *jm _{j }*, $j\text{'}{m}_{j}^{\text{'}}$,

According to the quasi-classical transport theory based on Boltzmann's equation with the collision integral taken within the relaxation time approximation, the conductivity for vertical transport in SL minibands at zero temperature and low-field limit can be written as

$${\sigma}_{q}({E}_{\text{F}})={\displaystyle \sum _{v}{e}^{2}\frac{{\tau}_{q,v}}{{2}^{}}}$$

(2)

where the relaxation time *τ _{qv }*is ascribed to the band

$${\sigma}_{q}({E}_{\text{F}})={\displaystyle \sum _{v}{\sigma}_{q,v}({E}_{\text{F}})}$$

(3)

$${\sigma}_{q,v}({E}_{\text{F}})=\frac{{e}^{2}{\tau}_{q,v}}{{m}_{q}{}^{*}}{\eta}_{q,v}^{\text{eff}}({E}_{\text{F}})$$

(4)

where

$${\eta}_{q,v}^{\text{eff}}({E}_{\text{F}})=\frac{1}{2{\pi}^{2}}{(\frac{{m}_{q}{}^{*}}{{2}^{}})2}^{{\displaystyle \underset{BZ}{\int}d{k}_{z}\theta ({E}_{\text{F}}-{\epsilon}_{q,v}({k}_{z})){({\epsilon}_{q,v}({k}_{z}))}^{2}}}$$

(5)

The prime indicates the derivative of *ε _{q,v}*(

In this way, we have the following expression for ${n}_{q,\nu}^{\text{eff}}({E}_{\text{F}})$:

$${n}_{q,\nu}^{\text{eff}}({E}_{\text{F}})=\frac{1}{2{\pi}^{2}}{(\frac{{m}_{q}{}^{*}}{{2}^{}})2}^{\{\begin{array}{l}\text{}0\text{}{E}_{\text{F}}\text{Max}({\epsilon}_{q,\nu})& {\displaystyle {\int}_{-{k}_{F\nu}}^{{k}_{F\nu}}d{k}_{z}{\left[{{\epsilon}^{\prime}}_{q,\nu}^{}\right]}^{2}\text{Max}({\epsilon}_{q,\nu})\text{}\text{}{E}_{\text{F}}\text{}\text{Min}({\epsilon}_{q,\nu})}{\displaystyle {\int}_{-\pi /d}^{\pi /d}d{k}_{z}{\left[{{\epsilon}^{\prime}}_{q,\nu}^{}\right]}^{2}\text{}{E}_{\text{F}}\text{}\text{Min}({\epsilon}_{q,\nu})}\end{array}}$$

(6)

The parameters used in these calculations are the same as those used in our previous studies [11-13]. In the above calculations, 40% for the valence-band offset and relaxation time τ = 3 ps has been adopted [19].

Figure Figure2a2a shows the conductivity for heavy holes (σ as a function of the two-dimensional acceptor concentration, *N*_{2D}, for unstrained GaAs/Al_{0.3}Ga_{0.7}As SLs with barrier width, *d*_{1 }= 2 nm, and well width, *d*_{2 }= 2 nm). The conductivity increases until *N*_{2D }= 3 × 10^{12 }cm^{-2 }because of the upward displacement of the Fermi level, which moves until the first miniband is fully occupied. Afterward, one observes a small range of concentrations with a plateau-like behavior for the conductivity; this is a region where there is no contribution from the first miniband or where the second band is partially occupied, but its contribution to the conductivity is very small. In the group-III arsenides, the minigap is shorter due to the lower values of the effective masses. After *N*_{A }= 4 × 10^{12 }cm^{-2, }the conductivity increases again because of occupation of the second miniband, and this being very significant in this case. Figure Figure2b2b indicates the Fermi level behavior as a function of *N*_{2D}, where the zero of energy is adopted at the top of the Coulomb barrier, as mentioned before. It is observed that the Fermi energy decreases as *N*_{2D }increases. This happens because of the exchange-correlation effects, which play an important role in these structures. These effects are responsible for changes in the bending of the potential profiles. The bending is repulsive particularly for this case of GaAs/AlGaAs, and so the Coulomb potential stands out in relation to the exchange-correlation potential.

Figure Figure3a3a depicts the conductivity behavior of heavy holes as a function of *N*_{2D }for unstrained GaN/Al_{0.3}Ga_{0.7}N SLs with barrier width, *d*_{1 }= 2 nm, and well width *d*_{2 }= 2 nm. In this case, the conductivity increases until *N*_{2D }= 2 × 10^{12 }cm^{-2 }and afterward it remains constant, until *N*_{2D }= 6 × 10^{12 }cm^{-2}. A simple joint analysis of Figure 3a,b can provide the correct understanding of this behavior. At the beginning, the first miniband is only partially occupied; once the band filling increases, i.e., as the Fermi level goes up to the first miniband value, the conductivity increases. When the occupation is complete (*N*_{2D }= 2 × 10^{12 }cm^{-2}), one reaches a plateau in the conductivity. After the second miniband begins to get filled up, σ is found to increase again. However, it is important to note that, for the nitrides, the Fermi level shows a remarkable increase as *N*_{2D }increases, a behavior completely different as compared to that of the arsenides. This can be explained in the following way: for thinner layers of nitrides, the exchange-correlation potential effects are stronger than the Coulomb effects, and so the potential profile is attractive, and it is expected that the Fermi level goes toward the top of the valence band, as well as the miniband energies. This has been discussed in our previous study describing a detailed investigation about the exchange-correlation effects in group III-nitrides with short period layers [13].

Comparing both the systems (Figures (Figures22 and and3),3), one can observe higher conductivity values for the nitride; several factors can contribute to this behavior, such as the many body effects as well as the values of effective masses, involved in the calculations of the densities ${n}_{q,\nu}^{\text{eff}}({E}_{\text{F}})$. Experimental results for *p*-doped cubic GaN films, which use the concept of reactive co-doping, have obtained vertical conductivities as high as 50/Ωcm [8]. Those results corroborate with those of this study, since in the case of SLs, higher values for the conductivity are expected. Another interesting point concerning the arsenides relates to the higher values found for their conductivity in the case of systems, e.g., *n*-type delta doping GaAs system. The reason is the same as that given earlier.

In conclusion, this investigation shows that the conductivity behavior for heavy holes as a function of *N*_{2D }or of the Fermi level depicts a plateau-like behavior due to fully occupied levels. A remarkable point refers to the relative importance of the Coulomb and exchange-correlation effects in the total potential profile and, consequently, in the determination of the conductivity. These results presented here are expected to be treated as a guide for vertical transport measurements in actual SLs. Experiments carried out with good quality samples, combined with the theoretical predictions made in this study, will provide the way to elucidate the several physical aspects involved in the fundamental problem of the conductivity in SLs minibands.

2DHG: two-dimensional hole gas; EME: effective mass equation; LDA: local density approximation; PZ: piezoelectric; SLs: superlattices.

The authors declare that they have no competing interests.

OFPS carried out the calculations. GMS, LMRS and EFSJ discussed the results and purposed new calculations and improvements. SCPR conceived of the study and participated in its design and coordination. All authors read and approved the final manuscript.

The authors would like to acknowledge the Brazilian Agency CNPq, CT-Ação Tranversal/CNPq grant #577219/2008-1, Universal/CNPq grant #472.312/2009-0, CNPq grant #303880/2008-2, CAPES, FACEPE (grant no. 1077-1.05/08/APQ), and FAPESP, Brazilian funding agencies, for partially supporting this project.

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