# Electrical Properties of Polytypic Mg Doped GaAs Nanowires

Authors: N. Cifuentes; E. R. Viana; H. Limborço; D. B. Roa; A. Abelenda; M. I. N. da Silva; M. V. B. Moreira; G. M. Ribeiro; A. G. de Oliveira; J. C. González
Journal: Journal of Nanomaterials
 (2016)

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## Abstract

The electrical transport properties of individual Mg doped GaAs nanowires are investigated. It is shown that Mg can be successfully used as a nontoxic p-type dopant in GaAs nanowires. The doping levels, expanding over two orders of magnitude, and free holes mobility in the NW were obtained by the analysis of field effect transistors transfer curves. The temperature dependence of the electrical resistivity above room temperature shows that the polytypic structure of the NWs strongly modifies the NWs charge transport parameters, like the resistivity activation energy and holes mobility. At lower temperatures the NWs exhibit variable range hopping conduction. Both Mott and Efros-Shklovskii variable range hopping mechanisms were clearly identified in the nanowires.


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## Body

## 1. Introduction

Semiconductor nanowires (NWs) of III-V compounds [1–5] are promising nanostructures for optoelectronic devices applications [5, 6]. However, the influence of temperature as well as the polytypism in the transport mechanisms of p-type doped III-V NWs has been barely investigated [6–15]. In this work, we present a study of the electrical transport properties of polytypic and p-type Mg doped GaAs NWs near and above room temperature.Beryllium is the standard p-type dopant in III-V compounds thin films due to its near-unity sticking coefficient and low vapor pressure [16, 17]. However, due to its high toxicity, it is important to find nontoxic and noncarcinogenic alternatives. Mg is a known nontoxic shallow acceptor for III-V compounds [13, 16, 17], but the low incorporation coefficient at the usual growth temperatures had limited its use as a viable p-type dopant in III-V thin films [17]. However, III-V NWs are usually grown at lower temperatures [6, 8] allowing higher doping levels to be reached in those nanostructures. The use of Mg as p-type dopant presents the additional advantage of simplifying the integration of diverse III-V since it dopes all III-V compounds, including nitrides semiconductors. We have recently demonstrated the feasibility of growing Mg doped GaAs NWs [18] and studied their optical properties [19, 20]. In our studies the optical emission was dominated by Zincblende/Wurtzite (ZB/WZ) polytypism along the NWs that creates type-II optical transitions between electrons localized at the bottom of the conduction band of ZB segments and holes localized at the top of the valence band in adjacent WZ segments [18–20]. Luminescence related to the Mg acceptors was observed on GaAs thin films, but not in the NWs. To further understand the polytypism effects on the electronic process in p-type doped GaAs NWs a deeper study of the electrical transport in individual NWs is carried out here as a function of temperature.


## 2. Experimental Details

GaAs NWs and thin films were grown on GaAs (111)B substrates in a solid sourceRiber 2300 R&D MBE reactor. NWs were grown on drop-coated substrates with a water suspension of 5 nm thick colloidal Au nanoparticles, while the thin films were grown on uncoated substrates. The substrates were In glued to a Mo sample holder and outgassed at 350°C by two hours in UHV (1.2 × 10−10 Torr). Afterwards, the sample holder was transferred to the growth chamber where the protective oxide of the substrates was removed by heating at 625°C, during 20 minutes, and under an As4 beam equivalent pressure (BEP) of 3.4 × 10−5 Torr. The NWs growth was performed during 90 min, with an As4 BEP of 3.4 × 10−5 Torr, a Ga BEP of 7.2 × 10−7 Torr, and at a nominal growth rate for thin films of 1 μm/h. NWs and thin films were p-type doped by using a Mg effusion cell.The morphology and crystalline structure of the nanowires was investigated by transmission electron microscopy (TEM) by using aTecnai G2-20 SuperTwin FEI high resolution electron microscope.For transport measurements, individual NWs back-gate FETs were built by mechanically transferring the NWs onto a heavily doped Si substrate covered by a 300 nm thick SiO2 layer. Standard photolithography methods were used to define contact lines with a lateral separation of 3 to 4 μm, connecting individual NWs to macroscopic contact pads of 600 × 600 μm2. The NWs were etched in HCl/H2O 1 : 10 solution for 20 s, followed by a 60 s surface passivation in a heated (40°C) NH4Se/H2O 1 : 10 solution. Electrical contacts to the NWs were made by evaporating a Cr (10 nm)/Au (200 nm) bilayer after etching and passivation. The devices were placed in anOxford CF1200 liquid He-7 cryostat, with a preciseOxford ITC503 temperature-controller.Keithley 237 source-meter andKeithley 230 voltage-source were used in the electrical measurements using homemade software.


## 3. Results and Discussion

Figure1(a) shows a transmission electron microscopy (TEM) image of an approximately 40 nm thick GaAs NW. Alternating ZB/WZ (clear and dark) regions [20] along the NW axis are already visible in this magnification, as well as the catalyst gold particle at the top of the NW. The observed NWs presented ZB and WZ regions oriented at the 011 and 1
2
-
10, respectively. A selected area electron diffraction (SAED) pattern from the central region of the NW is shown in Figure 1(b). This diffraction pattern is actually a composition of three different patterns with zone axes: ZB [
0
1
-
1
], WZ [
1
2
-
10
], and ZB [
01
1
-
]. Therefore, not only alternated ZB/WZ regions exist in the GaAs NWs, but there is also ZB segments rotated with respect to each other. A HRTEM image of a portion of the GaAs NW is shown in Figure 1(c). It is possible to determine the structure and orientation of any segment along the NW by correlating the SAED patterns and the Fast Fourier Transform (FFT) of the region of interest in the HRTEM image.Figure 1
(a) TEM image of a Mg doped GaAs NW. (b) SAED pattern of the NW, showing a superposition of three different oriented crystalline segments: GaAs ZB[
0
1
-
1
], GaAs WZ [
1
2
-
10
], and GaAs ZB [
01
1
-
]. The growth direction is 111 and 0001 for the ZB and WZ regions, respectively. (c) HRTEM of the NW and FFT (insets) of three regions that can be correlated to the SAED pattern in (b). (d) Band alignment diagram of the NW.The concentration and mobility of free holes in the FET channel of four individual NWs (NW1 to NW4) were determined by using the standard analysis of the FET transfer characteristic [21–24]. Figure 2 shows a graph of the holes mobility as a function of holes concentration for different NWs and thin film samples. The values of μ obtained for the thin films decrease with the holes concentration due to defect scattering [9, 25]. However, the opposite trend is observed for the NWs. These contradictions reveal that the scattering mechanism of free holes in the NWs is significantly different from bulk GaAs. The solid lines in Figure 2 are only guides to the eyes.Figure 2
Hole mobility as a function of hole concentration for several Mg doped GaAs nanowires (NWs) and thin films (TF).Figure3 shows the Arrhenius plot of the electrical resistivity ρ
(
T
) of individual NWs (NW1 to NW4) between 400 and 300 K. The electronic transport in this temperature region in bulk p-type GaAs is due to free holes in the valence band, thermally ionized from shallow acceptors levels. In our case, these acceptors levels are created by Mg impurities and present ionization energy of 28 meV [15–17].Figure 3
Temperature dependence of the electrical resistivityρ
(
T
) of several individual Mg doped GaAs NWs. The red lines correspond to the fitting of the experimental data using (1).In bulk GaAs the holes mobility above 200 K is dominated by lattice scattering:μ
l
a
t
(
T
)
=
μ
0
297
K
/
T
α, where μ
0 and α
=
2.3 are constants [26, 27], as well as by ionized impurity scattering μ
ii [28]. The Matthiessen rule μ
T
-
1
=
μ
l
a
t
T
-
1
+
μ
ii
-
1 can be applied in order to found the total holes mobility μ
(
T
) [26–28]. Therefore the electrical resistivity can be approximately expressed by [29] (1)
ρ
T
=
ρ
0
μ
T
-
1
T
-
3
/
2
exp
⁡
E
i
k
B
T
,where ρ
0 is a constant, k
B is the Boltzmann constant, and E
i is the ionization energy of the Mg acceptors.The values ofE
i (presented in Figure 3 and Table 1) obtained from the fitting using (1) are significantly different from the expected 28 meV value of the ionization energy of Mg acceptors. This new disagreement also indicates that the transport mechanism of free holes in the NWs is significantly different from the transport in bulk GaAs.Table 1
Values of the ionization energyE
i, the hopping parameters T
M and T
ES, and the corresponding holes mobility µ and concentration p.
NW
E
i (meV)
T
M (K)
T
ES (K)
µ (cm2/Vs)
p (cm−3)
1
126
2 × 106
27
0.34
3.5 × 1015
2
39
5 × 105
35
0.26
2.1 × 1016
3
70
2 × 107
484
18.4
3.8 × 1016
4
78
1 × 104
24
37.3
1.3 × 1017Both discrepancies, in resistivity activation energy and in mobility values, can be explained in terms of the type-II band alignment in the NWs caused by the WZ/ZB polytypism [18–20]. A simplified band alignment diagram of a section of a GaAs NW is shown in Figure 1(d). Due to this band alignment, WZ segments act as electron potential wells, while ZB segments act as hole potential wells. The WZ segments will behave as barriers to overcome by the holes in order to be transported along the NWs by a low electric field. Therefore, the transport of free holes in the NW is a complex process influenced not only by the ionization energy of Mg acceptors, but also by the scattering mechanism in the WZ segments and to overcome the WZ barriers.As the temperature drops most of the free holes are recaptured by acceptors, conduction at the valence band becomes less important, and holes’ hopping between acceptors states turns into the main conduction mechanism [30, 31]. In our case, the NWs are thick enough to sustain 3D hopping [30] likewise bulk GaAs.At temperatures below 280 K, conduction by Mott variable range hopping (Mott-VRH) [31] can be identified in the NWs. The resistivity in this regime is given by(2)
ρ
M
T
=
ρ
0
M
T
1
/
2
exp
⁡
T
M
T
1
/
4
T
M
=
β
M
ξ
3
N
E
F
,where T
M measures the degree of disorder in the material, ρ
0
M and β
M = 18.1 are constants [32], ξ is the localization length which characterizes the hopping probability between sites, and N
E
F is the density of states near de Fermi level.The Arrhenius plots ofρ
·
T
-
1
/
2 versus T
-
1
/
4, between 280 and 55 K, is shown in Figure 4. A linear region, with characteristic temperature T
M = 3 × 104 K, can be observed showing that Mott-VRH is the dominant conduction mechanism.Figure 4
Temperature dependence of the hopping conduction in a Mg doped GaAs NW. The green line corresponds to the fitting ofρ
⋅
T
-
1
/
2 versus T
-
1
/
4 plot in the Mott-VRH region using (2). The blue line corresponds to the fitting of ρ
⋅
T
-
1 versus T
-
1
/
2 in the ES-VRH region using (3).As temperature further decreases, the Coulomb effect becomes more important and the conductivity crosses over from Mott-VRH to Efros-Shklovskii VRH (ES-VRH) regime where the resistivity is given by [32](3)
ρ
E
S
T
=
ρ
0
E
S
T
exp
⁡
T
E
S
T
1
/
2
T
E
S
=
β
E
S
e
2
ε
k
B
ξ
,where ε is the dielectric constant and ρ
0
E
S and β
E
S = 2.8 are constants [32].The Arrhenius plots ofρ
·
T
-
1 versus T
-
1
/
2 for temperatures below 11 K is shown in Figure 4. A linear region, with T
E
S = 27 K, can be observed below 11 K. However, measurements at much lower temperatures are necessary to precisely evaluate the ES-VRH transport regime.The above-presented analysis was applied to four NWs with different doping levels (see Table1). Large values of T
M indicate a large degree of disorder in the NWs. The variations of the hopping transport parameters from wire to wire are an additional indication of the effect of polytypism in the charge transport in the NWs.


## 4. Conclusions

In conclusion, it was shown that Mg can be used as a nontoxic p-type dopant in GaAs NWs. It was also found that the mobility of free holes, as well as the resistivity activation energy above room temperature, is strongly influenced by the polytypism in the NWs. Two variable range hopping conduction mechanisms were observed at low temperatures, starting from Mott-VRH and transiting to ES-VRH as temperature drops. Further studies are necessary in order to fully understand the effects of the polytypism in the electrical transport mechanism in NWs.



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*Source: 9451319-2016-08-17.xml*