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Related Concept Videos

NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved in...
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
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Coulomb's Law describes the force experienced by two point charges under each other's presence. But what if there are more than two charges? For example, if there is a third charge, does it experience a force that is a simple combination of the individual forces due to the first two charges? Can it be described mathematically?
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Spin–Spin Coupling: One-Bond Coupling01:17

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Superconductor01:24

Superconductor

A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...

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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Strong tunable coupling between a superconducting charge and phase qubit.

A Fay1, E Hoskinson, F Lecocq

  • 1Institut Néel, C.N.R.S.-Université Joseph Fourier, BP 166, 38042 Grenoble-cedex 9, France.

Physical Review Letters
|June 4, 2008
PubMed
Summary
This summary is machine-generated.

We achieved tunable coupling between a Cooper pair transistor (charge qubit) and a DC SQUID (phase qubit), enabling independent control and entanglement. This allows for precise quantum state manipulation and measurement via adiabatic quantum transfer.

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Area of Science:

  • Quantum computing
  • Solid-state physics
  • Superconductivity

Background:

  • Quantum bits (qubits) are fundamental to quantum computation.
  • Controlling and entangling qubits is crucial for building quantum processors.
  • Superconducting circuits offer a promising platform for qubit implementation.

Purpose of the Study:

  • To realize and investigate tunable coupling between a charge qubit and a phase qubit.
  • To demonstrate independent manipulation and entanglement of these two distinct superconducting qubits.
  • To validate the coupling mechanism with theoretical predictions.

Main Methods:

  • Fabrication of a circuit integrating an asymmetric Cooper pair transistor (charge qubit) and a DC SQUID (phase qubit).
  • Implementation of independent control protocols for each qubit's quantum state.
  • Utilizing adiabatic quantum transfer for charge qubit state measurement via the phase qubit.
  • Characterization of the tunable coupling strength, including capacitive and Josephson components.

Main Results:

  • Achieved tunable coupling between the charge and phase qubits over a broad frequency range.
  • Demonstrated independent manipulation of individual qubit states.
  • Successfully entangled the two qubits.
  • Measured coupling strength agrees with analytical theory incorporating both capacitive and tunable Josephson couplings.

Conclusions:

  • The developed circuit architecture allows for flexible and tunable coupling between different types of superconducting qubits.
  • Independent control and entanglement capabilities are essential for scalable quantum computing architectures.
  • The theoretical model accurately describes the observed coupling phenomena, providing a foundation for future circuit design.