Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese

The magnetic moment and magnetization in GaAs/Ga₀.₈₄In₀.₁₆As/GaAs heterostructures with Mn deluted in GaAs cover layers and with atomically controlled Mn δ-layer thicknesses near GaInAs-quantum well (~3 nm) in temperature range T = 1.8–300 K in magnetic field up to 50 kOe have been investigated. The...

Повний опис

Збережено в:
Бібліографічні деталі
Дата:2015
Автори: Charikova, T., Okulov, V., Gubkin, A., Lugovikh, A., Moiseev, K., Nevedomsky, V., Kudriavtsev, Yu., Gallardo, S., Lopez, M.
Формат: Стаття
Мова:English
Опубліковано: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2015
Назва видання:Физика низких температур
Теми:
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/122039
Теги: Додати тег
Немає тегів, Будьте першим, хто поставить тег для цього запису!
Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese / T. Charikova, V. Okulov, A. Gubkin, A. Lugovikh, K. Moiseev, V. Nevedomsky, Yu. Kudriavtsev, S. Gallardo, M. Lopez // Физика низких температур. — 2015. — Т. 41, № 2. — С. 207-209. — Бібліогр.: 9 назв. — англ.

Репозитарії

Digital Library of Periodicals of National Academy of Sciences of Ukraine
id irk-123456789-122039
record_format dspace
spelling irk-123456789-1220392017-06-27T03:03:18Z Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese Charikova, T. Okulov, V. Gubkin, A. Lugovikh, A. Moiseev, K. Nevedomsky, V. Kudriavtsev, Yu. Gallardo, S. Lopez, M. XX Уральская международная зимняя школа по физике полупроводников The magnetic moment and magnetization in GaAs/Ga₀.₈₄In₀.₁₆As/GaAs heterostructures with Mn deluted in GaAs cover layers and with atomically controlled Mn δ-layer thicknesses near GaInAs-quantum well (~3 nm) in temperature range T = 1.8–300 K in magnetic field up to 50 kOe have been investigated. The mass magnetization all of the samples of GaAs/Ga₀.₈₄In₀.₁₆As/GaAs with Mn increases with the increasing of the magnetic field that pointed out on the presence of low-dimensional ferromagnetism in the manganese depletion layer of GaAs based structures. It has been estimated the manganese content threshold at which the ferromagnetic ordering was found. 2015 Article Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese / T. Charikova, V. Okulov, A. Gubkin, A. Lugovikh, K. Moiseev, V. Nevedomsky, Yu. Kudriavtsev, S. Gallardo, M. Lopez // Физика низких температур. — 2015. — Т. 41, № 2. — С. 207-209. — Бібліогр.: 9 назв. — англ. 0132-6414 PACS: 72.80.Ey, 75.50.Pp http://dspace.nbuv.gov.ua/handle/123456789/122039 en Физика низких температур Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic XX Уральская международная зимняя школа по физике полупроводников
XX Уральская международная зимняя школа по физике полупроводников
spellingShingle XX Уральская международная зимняя школа по физике полупроводников
XX Уральская международная зимняя школа по физике полупроводников
Charikova, T.
Okulov, V.
Gubkin, A.
Lugovikh, A.
Moiseev, K.
Nevedomsky, V.
Kudriavtsev, Yu.
Gallardo, S.
Lopez, M.
Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese
Физика низких температур
description The magnetic moment and magnetization in GaAs/Ga₀.₈₄In₀.₁₆As/GaAs heterostructures with Mn deluted in GaAs cover layers and with atomically controlled Mn δ-layer thicknesses near GaInAs-quantum well (~3 nm) in temperature range T = 1.8–300 K in magnetic field up to 50 kOe have been investigated. The mass magnetization all of the samples of GaAs/Ga₀.₈₄In₀.₁₆As/GaAs with Mn increases with the increasing of the magnetic field that pointed out on the presence of low-dimensional ferromagnetism in the manganese depletion layer of GaAs based structures. It has been estimated the manganese content threshold at which the ferromagnetic ordering was found.
format Article
author Charikova, T.
Okulov, V.
Gubkin, A.
Lugovikh, A.
Moiseev, K.
Nevedomsky, V.
Kudriavtsev, Yu.
Gallardo, S.
Lopez, M.
author_facet Charikova, T.
Okulov, V.
Gubkin, A.
Lugovikh, A.
Moiseev, K.
Nevedomsky, V.
Kudriavtsev, Yu.
Gallardo, S.
Lopez, M.
author_sort Charikova, T.
title Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese
title_short Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese
title_full Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese
title_fullStr Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese
title_full_unstemmed Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese
title_sort magnetization in aiiibv semiconductor heterostructures with the depletion layer of manganese
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 2015
topic_facet XX Уральская международная зимняя школа по физике полупроводников
url http://dspace.nbuv.gov.ua/handle/123456789/122039
citation_txt Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese / T. Charikova, V. Okulov, A. Gubkin, A. Lugovikh, K. Moiseev, V. Nevedomsky, Yu. Kudriavtsev, S. Gallardo, M. Lopez // Физика низких температур. — 2015. — Т. 41, № 2. — С. 207-209. — Бібліогр.: 9 назв. — англ.
series Физика низких температур
work_keys_str_mv AT charikovat magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT okulovv magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT gubkina magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT lugovikha magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT moiseevk magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT nevedomskyv magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT kudriavtsevyu magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT gallardos magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
AT lopezm magnetizationinaiiibvsemiconductorheterostructureswiththedepletionlayerofmanganese
first_indexed 2025-07-08T21:01:41Z
last_indexed 2025-07-08T21:01:41Z
_version_ 1837114066684870656
fulltext Low Temperature Physics/Fizika Nizkikh Temperatur, 2015, v. 41, No. 2, pp. 207–209 Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese T. Charikova, V. Okulov, A. Gubkin, and A. Lugovikh Institute of Metal Physics RAS, Ekaterinburg, Russia E-mail: charikova@imp.uran.ru K. Moiseev and V. Nevedomsky Ioffe Institute, St. Petersburg, Russia Yu. Kudriavtsev and S. Gallardo Departamento de Ingenieria Electrica–SEES, Cinvestav-IPN, Mexico M. Lopez Departamento de Fisica, Cinvestav-IPN, Mexico Received October 20, 2014, published online December 22, 2014 The magnetic moment and magnetization in GaAs/Ga0.84In0.16As/GaAs heterostructures with Mn deluted in GaAs cover layers and with atomically controlled Mn δ-layer thicknesses near GaInAs-quantum well (~3 nm) in temperature range T = 1.8–300 K in magnetic field up to 50 kOe have been investigated. The mass mag- netization all of the samples of GaAs/Ga0.84In0.16As/GaAs with Mn increases with the increasing of the mag- netic field that pointed out on the presence of low-dimensional ferromagnetism in the manganese depletion layer of GaAs based structures. It has been estimated the manganese content threshold at which the ferromagnetic ordering was found. PACS: 72.80.Ey III–V and II–VI semiconductors; 75.50.Pp Magnetic semiconductors. Keywords: magnetic semiconductors, magnetization, depletion layer of manganese. 1. Introduction Diluted magnetic semiconductors (DMSs) on III–V based materials have of great interest both for the researchers in condensed matter physics and for the technologists because of the semiconductivity-magnetism coexistence and of the low equilibrium solubility of the transition metal [1]. DMS heterostructures are attracting attention due to the possibil- ity of information management using both the charge and the spin of carriers [2,3]. Advances in epitaxial growth technology, such as molecular beam epitaxy, have made it possible to grow a variety of semiconductor heterostruc- tures with atomically controlled layer thicknesses and ab- rupt doping profiles, in which the wave function of carriers within the artificially designed potentials may be control- ed. Unlike the random alloy system, δ-layer of Mn in GaAs provides the doping profile along the growth direc- tion with the inherent advantages of δ-doping that it yelds higher dopant carrier concentration [4]. There is a large scatter in conductivities and Curie temperatures obtained by different groups in Ga(Mn)As materials [5]. These dif- ferences depend on the details of the growth and post- growth annealing indicating the Mn quantity and the pre- sence of compensating defects. Unlike the random alloy system, Mn δ-layer in GaAs provides the doping profile along the growth direction which can be approximated by Dirac's δ-function. Inherent advanages of δ-doping has locally higher dopant concent- ration and higher carrier concentration. In this paper we have presented the results of the magnetization in hetero- structures GaAs/Ga0.84In0.16As/GaAs with Mn deluted in GaAs cover layers and by secondary ion mass spectrosco- py (SIMS) depth profile analyses Mn δ-layer near GaInAs- quantum well. © T. Charikova, V. Okulov, A. Gubkin, A. Lugovikh, K. Moiseev, V. Nevedomsky, Yu. Kudriavtsev, S. Gallardo, and M. Lopez, 2015 T. Charikova et al. 2. Experimental details The GaAs/InGaAs/GaAs quantum well (QW) hetero- structures were grown on GaAs(001) substrate by MBE method in Riber C21 chamber at temperature range of 500–600 °C [6]. Epitaxial deposition was carried out under average rate of 0.5 m/h. The 300 nm-thick GaAs buffer layer as a first barrier of the QW was obtained at higher temperature (600 °C) than the layer of the GaInAs ternary solution and the 5 nm-thick GaAs second barrier (500 °C). The temperature decreasing was done to prevent diffusion of indium from QW to the GaAs barrier layers. Then, the temperature of a substrate was moving down less than 300 °C to achieve optimal conditions for an atomic Mn layer deposition which was covered by an additional (cap) GaAs layer as thick as 50 nm. Profile analysis of the heterostructures containing the Mn layer was performed by SIMS method. Measurements were carried out using ion- microprobe ims-6f (Cameca, France). We have applied the de-convolution procedure to experimental SIMS depth profiles for the obtained InGaAs/GaAs single quantum well reported elsewhere [7]. The concentration of the ele- ment of interest was re-calculated by using the relative sensitivity factors (RSFs) defined earlier by SIMS profiling of implanted standards. The thicknesses of the QWs and GaAs cover layers were examined by cross-sectional TEM. The TEM data were used as references in examining the de-convolution process we suggested and its application to experimental SIMS depth profiles. The magnetic field dependences of the magnetic moment m(H) and mass magnetization for GaAs/Ga0.84In0.16As/ GaAs/Ga(Mn)As and GaAs/Ga0.84In0.16As/ GaAs/δ-Mn/GaAs heterostructures have measured using SQUID-magneto- meter MPMS of Quantum Design in the temperature range T = 1.8–300 K and in magnetic field up to 50 kOe (Insti- tute of Metal Physics RAS). 3. Experimental results and discussion The magnetic field dependences of the mass magnetiza- tion σ(H) for the structure GaAs/Ga0.84In0.16As/GaAs/ Ga(Mn)As at low temperatures is presented in Fig. 1. The measurements were done in two magnetic field orienta- tions parallel, along with the substrate plane, and perpen- dicular, when the magnetic field was applied along the growing direction. For comparison, GaAs substrate exhib- ited a large diamagnetic response in the parallel orientation and its mass magnetization reached σ = –2.3·10–3 emu/g in the field H = 10 kOe. As one can see in the figure that the field dependence of the magnetization does not exists in the case of the perpendicular magnetic field. So there is the anisotropy of the magnetization field dependence along and perpendicular to the magnetic easy axis. To extract the contribution of the Mn magnetic moments to the total magnetization in the heterostructures with the barrier based on the Ga(Mn)As diluted compound, we have made several steps to distinguish the large common dia- magnetic signal of the substrate (the thickness sd = 0.5 mm) from the weak signal of the heterostructure ( hd = 350 nm). The epitaxial wafers with the heterostructure on the GaAs substrate were processed after MBE growth to remove ato- mic indium. Then, the magnetic moment and the mass of the samples and the substrate were measured. Next, the contribution of the substrate from a sample mass magneti- zation was subtracted. This procedure is also required in order to exclude the possible contribution to the magneti- zation of random magnetic impurities such as iron. The extracted dependences of the mass magnetization for the samples either with diluted GaMnAs and the GaAs barrier locally doped with Mn δ-layer are presented in Fig. 2. It is obvious, when the magnetic field H is applied in the direction of the easy magnetic axis, magnetization σ(H) for both samples increases with the increasing in Fig. 1. (Color online) The magnetic field dependence of the mass magnetization σ at T = 5 K for GaAs heterostructures with H parallel to the sample plane and perpendicular to it. Fig. 2. (Color online) The magnetic field dependence of the mass magnetization σ at T = 5 K for GaAs heterostructures with diluted Mn () and with Mn δ-layer (). ( )Hσ dependences for GaAs heterostructures with diluted Mn at the temperatures T = 5 () and T = 300 () K are presented inset. 208 Low Temperature Physics/Fizika Nizkikh Temperatur, 2015, v. 41, No. 2 Magnetization in AIIIBV semiconductor heterostructures with the depletion layer of manganese the magnetic field. For the Ga(Mn)As sample the satura- tion of the magnetization was found out reaching value of 46.4·10 emu/g−σ  at H = 10 kOe at T = 5 K. The para- magnetic response was observed at T = 300 K too (Fig. 2, inset). Only weak signal of the mass magnetization was observed for the heterostructure with the Mn δ-layer (0.5 ML) placed into GaAs cap layer and separated from the InGaAs quantum well by the GaAs spacer layer as thick as 3 nm. Linear-like dependence without saturation was reaching σ = 1.4·10–4 emu/g at H = 10 kOe. We sup- pose that the ferromagnetism in GaAs heterostructure with Mn δ-layer is quantitatively different even from the mag- netic responce in the structures with the diluted Ga(Mn)As cover layer and differ qualitatively from their bulk coun- terparts [8]. In the dilute limit the magnetization can be discribed by the Brillouin function [9]: 0 (Mn)= ,B xM xN g S− µ 〈 〉 (1) where xS〈 〉 is the average spin per Mn site, 0N is a number of cations per unit volume, g is the g factor, Bµ is the Bohr magnetron and x is the molar fraction. Using the data of the mass-analyzer for GaAs heterostructures with diluted Mn 20 3 0 Mn 10 cmN N −=  , the value of saturation of magnetization at T = 5 K –46.4·10 emu/gσ  , g = 2 and 5 / 2S = for Mn++ we have estimated the molar fraction of deluted Mn in the cover layers. This value 0.002x cor- responds the delute limit where Mn++ spins are isolated. In magnetic field H = ±1.5 kOe the mass magnetization shows a hysteresis loop in the structure with the diluted Ga(Mn)As layer (Fig. 3) that indicates the ordered ferro- magnetic structure. 4. Conclusions It was experimentally found that ferromagnetism exist in the magnetic quasi-two-dimensional GaAs-based hete- rostructures doped with depletion layer of manganese at the temperatures T = 5 and 300 K even in the dilute limit. In the case of the heterostructures with the Mn δ-layer (with concentration of 0.5–1.0 ML) the paramagnetic re- sponse that can be increased using further improvements in growth conditions of the δ-layers due to layer thickness and Mn diffusion control to obtain more convincing evi- dence of the spin polarization. Work in this area should lead to sustainable results for their application in develop- ment of modern industry. This work was done within RAS Program (project No. 12-P-2-1018) with partial support of RFBR (grant No. 15-02-08909). Authors from Cinvestav thank to SENER and CONACYT, both from Mexico for a financial support of this study, grant No. 152244. 1. H. Ohno, A. Shen, F. Masukura, A. Oiwa, A. Endo, S. Katsu- moto, and Y. Iye, Appl. Phys. Lett. 69, 363 (1996). 2. A.M. Nazmul, T. Amemiya, Y. Shuto, S. Sugahara, and M. Ta- naka, Phys. Rev. Lett. 95, 017201 (2005). 3. T. Dietl, H. Ohno, and F. Matsukara, IEEE Trans. Electron Devices 54, 945 (2007). 4. R.V. Parfeniev, K.D. Moiseev, V.A. Berezovets N.S. Aver- kiev, M.P. Mikhailova, V.I. Nizhankovskii, and D. Kaczo- rowski, J. Magn. Magn. Mater. 321, 712 (2009). 5. T. Jungwirth, Jairo Sinova, J. Macek, J. Kucera, and A.H. MacDonald, Rev. Mod. Phys. 78, 809 (2006). 6. C.M. Yee-Rendon, M. Lopez-Lopez, and M. Melendez-Lira, Revista Mexicana de Fisica 50, 193 (2004). 7. Yu. Kudriavtsev, R. Asomoza, S. Gallardo-Hernandez, M. Ra- mirez-Lopez, M. Lopez-Lopez, V. Nevedomsky, and K. Moi- seev, Physica B (2014), DOI: 10.1016/j.physb.2014.03.097. 8. V. Tripathi, K. Dhochak, B.A. Aronzon, V.V. Rylkov, A.B. Davydov, B. Raquet, M. Goiran, and K. I. Kugel, Phys. Rev. B 84, 075305 (2011). 9. J.K. Furdyna, J. Appl. Phys. 64, R29 (1988). Fig. 3. The magnetization hysteresis curve for GaAs/Ga(Mn)As. The lines are presented as a guide for the eyes and triangles are the first trip up, circles — down, squares — up once again. Low Temperature Physics/Fizika Nizkikh Temperatur, 2015, v. 41, No. 2 209 1. Introduction 2. Experimental details 3. Experimental results and discussion 4. Conclusions