Lasse Södergren’s research while affiliated with Lund University and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (7)


Figure 1. (a) A 1-to-4 demultiplexer circuit schematic with one input (S), four outputs (D) and four control gates (A, B). (b) False-colored scanning electron microscope (SEM) image of a demultiplexer. Source/drain contacts in blue, doped InGaAs in red, and gate contacts in yellow. The device has in total four different gates, A 1 , A 2 , B 1 , and B 2 , since the respective B gates are shorted (not shown). The unintentionally doped InGaAs channel, which can be seen under the gates have dimensions of W = 80 nm and L G = 120 nm.
Figure 2. Simplified schematics of the fabrication steps for one gated region. (a) The InGaAs nanowire network is grown using selective area epitaxy with HSQ as a growth mask on an InP substrate. (b) An EBL defined HSQ dummy gate patterned across the nanowire. (c) Highly doped n + InGaAs contacts are grown. (d) Final device structure after dummy gate removal, gate oxide deposition, and metallization steps.
Figure 3. Low-temperature transfer characteristics normalized to the nanowire width at (a) V DS = 500 mV and (b) V DS = 50 mV measured at 13 K. The different colored lines refer to the drain current in each respective drain, as indicated in Figure 1. During the measurements, the drain bias was applied to all drains simultaneously, and the gates were then used to only set one source-drain path in a low resistive state at any given time. The current in the high resistive paths were below the noise floor of the measurement setup (<1 pA).
Figure 5. (a) Transfer characteristics normalized to the nanowire width of D 11 with V DS = 50 mV at 13 K and 40 mK. (b) Normalized conductance of D 11 measured with V DS = 5 mV at 40 mK. (c) Electrostatic potential along the channel used for calculations. A fluctuating potential with σ = 100 meV and L = 5 nm is superimposed on the ideal conduction band edge profile. (d) Simulated conductance characteristics at 40 mK using a 1D real space tight-binding nonequilibrium Green's functions model.
Low-Temperature Characteristics of Nanowire Network Demultiplexer for Qubit Biasing
  • Article
  • Full-text available

May 2022

·

140 Reads

·

9 Citations

Nano Letters

Lasse Södergren

·

·

In current quantum computers, most qubit control electronics are connected to the qubit chip inside the cryostat by cables at room temperature. This poses a challenge when scaling the quantum chip to an increasing number of qubits. We present a lateral nanowire network 1-to-4 demultiplexer design fabricated by selective area grown InGaAs on InP, suitable for on chip routing of DC current for qubit biasing. We have characterized the device at cryogenic temperatures, and at 40 mK the device exhibits a minimum inverse subthreshold slope of 2 mV/dec, which is encouraging for low power operation. At low drain bias, the transmission breaks up into several resonance peaks due to a rough conduction band edge; this is qualitatively explained by a simple model based on a 1D real space tight-binding nonequilibrium Green's functions model.

Download

FIG. 2. (a) The m à 1 and (b) a 1 of strained and unstrained QW of various thickness, bulk In x Ga (1Àx) As vs indium composition. The m à 1 of 0.08 m 0 corresponds to wave function localization in InP.
FIG. 3. (a) Top view of the fabricated MOSFET with W g ¼ 70 lm and L g ¼ 6 lm, (b) measured (dash line) and modeled (solid line) drain current vs V GS (c) measured (dash line) and modeled (solid line) low frequency capacitance vs gate voltage at T ¼ 300 K (blue) and T ¼ 13 K (green), (d) the measured and modeled carrier density against V GS .
Strained In x Ga (1− x ) As/InP near surface quantum wells and MOSFETs

February 2022

·

28 Reads

·

5 Citations

We present electronic band structure properties of strained In x Ga (1− x ) As/InP heterostructure near surface quantum wells oriented in the (100) crystallographic direction using eight-band [Formula: see text] theory, which are further parameterized by an energy level, effective mass, and nonparabolicity factor. The electronic band structure parameters are studied for the well composition of 0.2 ≤ x ≤ 1 and thickness from 5 to 13 nm. The bandgap and effective mass of the strained wells are increased for x >0.53 due to compression strain and decreased for x < 0.53 due to tensile strain as compared to that of unstrained wells. The calculated band structure parameters are utilized in modeling long channel In 0.71 Ga 0.29 As/InP quantum well MOSFETs, and the model is validated against measured I–V and low frequency C–V characteristics at room temperature and cryogenic temperature. Exponential band tails and first- and second-order variation of the charge centroid capacitance and interface trap density are included in the electrostatic model. The Urbach parameter obtained in the model is E 0 = 9 meV, which gives subthreshold swing (SS) of 18 mV/dec at T = 13 K and agrees with the measured SS of 19 mV/dec. Interface trap density is approximately three orders higher at T = 300 K compared to T = 13 K due to multi-phonon activated traps. This model emphasizes the importance of considering disorders in the system in developing device simulators for cryogenic applications.


Improved Quality of InSb-on-Insulator Microstructures by Flash Annealing into Melt

January 2021

·

193 Reads

·

7 Citations

·

Lasse Södergren

·

·

[...]

·

Monolithic integration of III-V semiconductors with Silicon technology has instigated a wide range of new possibilities in the semiconductor industry, such as the combination of digital circuits with optical sensing and high-frequency communication. A promising CMOS compatible integration process is Rapid Melt Growth (RMG) that can yield high quality single crystalline material at a low cost. This paper represents the study on ultra-thin InSb-on-Insulator microstructures integrated on a Si platform by a RMG-like process. We utilize Flash Lamp Annealing (FLA) to melt and recrystallize the InSb material for an ultra-short duration (milliseconds), to reduce the thermal budget necessary for integration with Si technology. We compare the result from FLA to regular Rapid Thermal Annealing (seconds). Recrystallized InSb was characterized using Electron Back Scatter Diffraction which indicates a transition from nanocrystalline structure to a crystal structure with grain sizes exceeding 1 µm after the process. We further see a 100x improvement in electrical resistivity by FLA annealed sample when compared to the as-deposited InSb with an average Hall mobility of 3100 cm2/Vs making this a promising step towards realizing monolithic mid-infrared detectors and quantum devices based on InSb.


Optimization of Near‐Surface Quantum Well Processing

January 2021

·

58 Reads

·

6 Citations

Physica Status Solidi (A) Applications and Materials

In this paper an optimized process flow of near‐surface quantum well MOSFETs (metal oxide semiconductor field effect transistors) based on planar layers of MOVPE (metalorganic vapor‐phase epitaxy) grown InxGa1‐xAs is presented. It is found that by an optimized pre‐growth cleaning and post metal anneal the quality of the MOS structure can be greatly enhanced. This optimization is a first step towards realization of a scalable platform for topological qubits based on a well‐defined network of lateral InxGa1‐xAs nanowires grown by selective area growth. This article is protected by copyright. All rights reserved.


FIG. 1. Lateral NW device schematics: (a) Top view illustration of the NW sample design and material. x ¼ 0.63 for the composition of the contact material, while x is higher in the NW material. (b) Cross-sectional schematic of the NWs and contacts. The dashed lines show where the NWs end.
FIG. 2. STM topography images of the lateral NWs: (a) A 700 Â 700 nm 2 STM image shows the geometry of contacts and NWs (aligned vertically in this image). The 200 Â 200 nm 2 large area marked by the blue square is shown by a zoom-in image in (b). (c) A height profile taken across a NW from image (b) indicates a flat top facet and steep side facets of the NW. Green dots mark the positions where line spectroscopy data were obtained. (d) The 30 Â 30 nm 2 STM image, acquired on a single NW as indicated by the red arrow in (c), shows the flatness of the NW top facet.
FIG. 3. Surface reconstruction: (a) 15 Â 15 nm 2 STM image zoomed in from Fig. 2(b) at the location of the blue square shown in the inset. (b) Height profile along the blue arrow shown in (a). (c) 25 Â 25 nm 2 STM image taken on the contact. (d) Height profile along the blue arrow shown in (c). STM images were taken with sample biases of À3.0 V (a) and À5.5 V (c) and tunneling currents of 80 pA (a) and 50 pA (c).
FIG. 4. Bandgap variations along the NW: Averaged (dI/dV)/(I=V ) spectra at positions 1-4, as indicated by blue squares in the inset. Dashed black lines show a linear fit of the VB (left) and CB (right) onset.
Low temperature scanning tunneling microscopy and spectroscopy on laterally grown In x Ga 1−x As nanowire devices

October 2020

·

143 Reads

·

2 Citations

Laterally grown InxGa1xAs nanowires (NWs) are promising candidates for radio frequency and quantum computing applications, which, however, can require atomic scale surface and interface control. This is challenging to obtain, not least due to ambient air exposure between fabrication steps, which induces surface oxidation. The geometric and electronic surface structures of InxGa1xAs NWs and contacts, which were grown directly in a planar configuration, exposed to air, and then subsequently cleaned using atomic hydrogen, are studied using lowtemperature scanning tunneling microscopy and spectroscopy (STM/S). Atomically flat facets with a root mean square roughness of 0.12 nm and the InGaAs (001) 4 2 surface reconstruction are observed on the top facet of the NWs and the contacts. STS shows a surface bandgap variation of 30 meV from the middle to the end of the NWs, which is attributed to a compositional variation of the In/Ga element concentration. The well-defined facets and small bandgap variations found after area selective growth and atomic hydrogen cleaning are a good starting point for achieving high-quality interfaces during further processing.


Mobility of near surface MOVPE grown InGaAs/InP quantum wells

July 2020

·

53 Reads

·

11 Citations

In this work, we study the electron mobility of near surface metal organic vapor phase epitaxy-grown InGaAs quantum wells. We utilize Hall mobility measurements in conjunction with simulations to quantify the surface charge defect density. Buried quantum wells are limited by polar optical phonon scattering at room temperature. In contrast, the quantum wells directly at the surface are limited by remote charge impurity scattering from defects situated at the III–V/oxide interface or inside the oxide, showing a mobility of 1500 cm²/V s. Passivating the InGaAs surface by depositing an oxide reduces the amount of defects at the interface, increasing the mobility to 2600 cm²/V s.


III–V nanowire MOSFETs with novel self-limiting Λ-ridge spacers for RF applications

May 2020

·

152 Reads

·

6 Citations

We present a semi self-aligned processing scheme for III–V nanowire transistors with novel semiconductor spacers in the shape of Λ-ridges, utilising the effect of slow growth rate on {111}B facets. The addition of spacers relaxes the constraint on the perfect alignment of gate to contact areas to enable low overlap capacitances. The spacers give a field-plate effect that also helps reduce off-state and output conductance while increasing breakdown voltage. Microwave compatible devices with Lg = 32 nm showing fT = 75 GHz and fmax = 100 GHz are realized with the process, demonstrating matched performance to spacer-less devices but with relaxed scaling requirements.

Citations (7)


... We provide a comprehensive review of relevant works from Refs. 90, 92, along with studies utilizing nanowires [98,99] and HEMT technology [91]. ...

Reference:

Cryogenic Control and Readout Integrated Circuits for Solid-State Quantum Computing
Low-Temperature Characteristics of Nanowire Network Demultiplexer for Qubit Biasing

Nano Letters

... In this paper, we used our previously developed 8-band k Á p method for quantum wells 13 and extended it for 1D systems such as nanowires here. We use a finite element method (FEM) solver (COMSOL Multiphysics), where coefficient form partial differential equations (PDE) coupled with solid mechanics for strain calculations is used to solve for eigenvalues. ...

Strained In x Ga (1− x ) As/InP near surface quantum wells and MOSFETs

... Prior epitaxial growth, the substrate, InP:Fe (100), was cleaned using an optimized pre-growth cleaning procedure [16]. The substrates were cleaned by oxidation in ozone for 10 min followed by removal of the formed oxide by HF 1:1000 in order to get an as clean and pristine surface as possible. ...

Optimization of Near‐Surface Quantum Well Processing

Physica Status Solidi (A) Applications and Materials

... 2 Due to these remarkable properties, InSb is an attractive material for high-sensitivity magnetic sensors [3][4][5][6][7][8] and high-efficiency infrared detectors, [9][10][11][12][13] as well as high-speed transistors [14][15][16][17] and quantum computing devices. [18][19][20][21] However, almost all of the InSb devices have been fabricated using single-crystal InSb wafers or InSb layers epitaxially grown on single-crystal substrates, [22][23][24][25] which increases the production cost and limits the applications. To decrease the production cost of InSb devices, a growth process of high-quality InSb films on low-cost substrates, such as glass, should be developed. ...

Improved Quality of InSb-on-Insulator Microstructures by Flash Annealing into Melt

... Local geometric control of the growth is important as it allows bottomup synthesis in specific regions when manufacturing a complete device on a chip. Various concepts have been developed attempting to resolve this, such as template-assisted growth, metal seed particleinduced growth or the use of surface crystal facet [10][11][12][13][14][15][16] . While proven highly useful, these concepts all rely on altering the growth substrate by either blocking or promoting synthesis in specific areas. ...

Low temperature scanning tunneling microscopy and spectroscopy on laterally grown In x Ga 1−x As nanowire devices

... InGaAs quantum wells, coated with InAlAs and grown on AlGaAsSb buffer layers by the method of molecular beam epitaxy, can achieve room-temperature mobilities that can be used to fabricate Field-effect transistors (FETs) for the performance of DC and RF characteristics [22]. It has been shown that in InGaAs/InP quantum well structure, the mobility increases with depositing a layer of oxide on the surface due to decrease in the number of defects at the interface [23]. In a GaAs/InGaAs QW, the transport of electrons has been analyzed with the application of many-body effects and magnetic field, taking into consideration of both non-phonon and phonon scatterings [24]. ...

Mobility of near surface MOVPE grown InGaAs/InP quantum wells

... Although gate recess 14,15 is an effective method to overcome the short channel effect, it is hard to precisely control the etching rate by either dry etching or wet etching. 3D architectures such as FinFETs, [16][17][18][19] nanowire FETs, [20][21][22] and tri-gate 23 have been used to improve the scalability of the devices. Due to the increase of contact area between gate and channel, the gate controllability and even the RF performances can be improved. ...

III–V nanowire MOSFETs with novel self-limiting Λ-ridge spacers for RF applications