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Related Concept Videos

Semiconductors01:22

Semiconductors

466
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
466
Types of Semiconductors01:20

Types of Semiconductors

434
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
434
Non-ohmic Devices00:51

Non-ohmic Devices

984
In most substances, the current flow is proportional to the voltage applied to it. A simple relationship between the values of current, voltage, and resistance is known as Ohm's law. Nonohmic devices do not exhibit a linear relationship between voltage and current. One such device is the semiconducting circuit element known as a diode. A diode is a circuit device that allows current flow in only one direction.
Consider a simple circuit consisting of a battery, a diode, and a resistor. A...
984
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

238
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
238
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

173
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
173

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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Cryogenic III-V and Nb electronics integrated on silicon for large-scale quantum computing platforms.

Jaeyong Jeong1, Seong Kwang Kim1, Yoon-Je Suh1

  • 1School of Electrical Engineering, Korea Advanced Institute of Science and Technology (KAIST), Daejeon, Republic of Korea.

Nature Communications
|December 31, 2024
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Summary

Researchers developed new cryogenic electronics using III-V and Nb superconductors. These low-power devices integrate with silicon, enabling control for millions of quantum bits (qubits) and overcoming scalability challenges.

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Area of Science:

  • Quantum Computing Hardware
  • Cryogenic Electronics
  • Semiconductor Integration

Background:

  • Quantum computing scalability is hindered by qubit size, I/O, and integrability challenges.
  • Current cryogenic CMOS electronics for qubit control consume too much power for large-scale systems.
  • High-fidelity spin qubits in Si CMOS and integrated control electronics show promise but face power limitations.

Purpose of the Study:

  • To develop ultra-low-power cryogenic electronics for controlling millions of quantum bits (qubits).
  • To demonstrate the integration of novel III-V and Nb superconductor-based electronics with silicon.
  • To overcome the power consumption bottleneck of existing cryogenic control solutions.

Main Methods:

  • Fabrication and integration of III-V two-dimensional electron gas and Nb superconductor-based cryogenic electronics with silicon.
  • Characterization of device performance at cryogenic temperatures (4 K).
  • Measurement of key electronic parameters including unity gain cutoff frequency, unity power gain cutoff frequency, and noise factor.

Main Results:

  • Demonstrated integration of III-V and Nb superconductor-based cryogenic electronics with silicon.
  • Achieved ultra-low power consumption, over 10 times less than CMOS.
  • Devices exhibit high-frequency performance with a unity gain cutoff frequency of 601 GHz and unity power gain cutoff frequency of 593 GHz at 4 K.

Conclusions:

  • III-V and Nb superconductor-based cryogenic electronics offer a viable solution for scalable quantum computing.
  • The developed technology significantly reduces power consumption, enabling control and readout for millions of qubits.
  • This advancement addresses a critical bottleneck in realizing large-scale, fault-tolerant quantum computers.