Search arXivSearch

arXiv · 2506.07776

Experiment and k$\cdot$p analysis of the luminescence from modulation-doped CdTe/(Cd,Mg)Te quantum wells at magnetic field

Abstract

In spite of a large quantity of papers devoted to the mangetoluminescence from CdTe/(Cd,Mg)Te, quantum wells there have been no attempts to analyze it on the basis of the band-structure calculations. This has been proposed in the present paper. Samples containing one or ten CdTe quantum wells with Cd$_{0.7}$Mg$_{0.3}$Te barriers are grown by a molecular beam epitaxy on a semi-insulating GaAs substrate. Each well is modulation-doped with iodine donors which leads to the creation of a two-dimensional electron gas in the wells. Polarization-resolved ($σ^+/σ^-$) photoluminescence spectra are measured at liquid helium temperatures and magnetic fields up to 9 T. The results are interpreted on the basis of calculations of the energy of Landau levels in the conduction and valence bands. In the latter case, we use the Luttinger Hamiltonian while the conduction band is described within a three-level k$\cdot$p model. Both models, originally formulated for bulk materials, are adapted for two-dimensional structures. We have found that the majority of all observed transitions is well reproducede by this theory. However, some strong transitions are not which allows us to propose an enlarged scheme of selection rules of the photoluminescence transitions resulting from mixing of the conduction and valence bands. We observe transitions involving Landau levels in the valence band with the index up to 7. To understand the origin of occupation with photoexcited holes of these levels, lying deep in the valence band, we carry out time-resolved measurements which show that the photoexcited barrier is a source of long-lived holes tunneling into the quantum wells. Calculations of the conduction band electron effective g-factor show its strong variation with the electron's energy and the external magnetic field.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

W. Solarska, M. Grymuza, M. Kubisa, K. Ryczko, P. Pfeffer, K. P. Korona, K. Karpierz, D. Yavorskiy, Z. Adamus, T. Wojtowicz, J. Łusakowski. 2025-06-09. Experiment and k$\cdot$p analysis of the luminescence from modulation-doped CdTe/(Cd,Mg)Te quantum wells at magnetic field. https://arxiv.org/abs/2506.07776

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Incommensurate structural and magnetic modulations in potassium-rich cryptomelane, K$_x$Mn$_8$O$_{16}$ ($x\approx1.45$)

Cryptomelane is a hollandite-like material consisting of K$^+$ cations in an $α$-MnO$_2$ tunnel-like crystallographic motif. Cryptomelane with stoichiometry K$_x$Mn$_8$O$_{16}$ ($x\approx1.45$) has been synthesized and its magnetic properties investigated using variable-temperature magnetic susceptibility, heat capacity, and neutron powder diffraction. Three distinct transitions at $T_1=184$\,K, $T_2=54.5$\,K, and $T_3=24$\,K are observed. At $T_1$ there is a subtle tetragonal$\rightarrow$monoclinic transition associated with emergence of a set of non-magnetic superstructure peaks indexable to a $\vec{k}_\mathrm{struc}\approx0.74\vec{c^*}$ incommensurate modulation parallel to the $α$-MnO$_2$ tunnels. Our findings are consistent with a relation previously reported in titanate hollandites, that $x\approx2|\vec{k}_\mathrm{struc}|$. Magnetic Bragg peaks emerge below $T_2=54.5$\,K, and their positions indicate an incommensurate modulated magnetic structure. The model consistent with the data is a dual-$\vec{k}_\mathrm{mag}$ structure with a ferromagnetic $|\vec{k}_\mathrm{mag}|=0$ component and an incommensurate $\vec{k}_\mathrm{mag}\approx0.37\vec{c^*}$, with the latter most likely to be helical. The period of oscillation of the incommensurate magnetic component is in line with predictions based on a Heisenberg spin Hamiltonian [Mandal \textit{et al}. Phys. Rev. B 90, 104420 (2014)]. Below $T_3=24$\,K, there is a magnetic transition, which gives rise to a different set of magnetic Bragg peaks indicative of a highly complex magnetic structure.

cond-mat.mtrl-sci

An anisotropic functional for two-dimensional material systems

Density function theory is the workhorse of modern electronic structure theory. However, its accuracy in practical calculations is limited by the choice of the exchange-correlation potential. In this respect, two-dimensional materials pose a special challenge, as all these materials and their heterostructures have a crucial similarity. The underlying atomic structures are strongly spatially inhomogeneous, implying that current exchange-correlation functionals, that in almost all cases are isotropic, are ill-prepared for an accurate description. We present an anisotropic screened-exchange potential, that remedies this problem and reproduces the band-gap of 2D materials as well as the piecewise linearity of the total energy with fractional occupation number.

cond-mat.mtrl-sci

Thermally-driven reorientation of the Néel vector in altermagnetic MnTe

Altermagnets are novel magnetic systems that possess a spin-polarized electronic band structure without a net magnetic moment, making them promising for device applications. Hexagonal MnTe, a prototypical altermagnet, arguably exhibits the most properties consistent with theoretical predictions, including an anomalous Hall effect despite a vanishing net magnetization, and altermagnetinduced electronic band splitting. However, fundamental questions remain, including why some effects only appear significantly below the magnetic ordering temperature. Here, we resolve this discrepancy by revealing a reorientation of the Néel vector in single-crystalline MnTe. The Néel vector points 30° from the a-axis at low $T$, before aligning directly with the a-axis around $T\simeq 260$ K. We attribute this to single-ion anisotropy, which depends on temperature-dependent lattice parameters. We obtained these results using muon-spin spectroscopy, magnetization measurements, and X-ray diffraction; we show that the findings are consistent with neutron diffraction. Manipulating this effect, for example through strain, could unlock sensitive electronic detection schemes for external stimuli, paving the way for functional altermagnetic devices.

cond-mat.mtrl-sci