Related Experiment Video
Updated: May 1, 2026

06:42
Generation and Coherent Control of Pulsed Quantum Frequency Combs
Published on: June 8, 2018
9.0K
One-step implementation of a multiqubit phase gate with one control qubit and multiple target qubits in coupled
Optics Letters
|April 3, 2014
Summary
We developed a robust one-step method for multiqubit gates using three-level atoms in cavity arrays. This approach is resilient to decoherence, advancing scalable quantum computing networks.
Area of Science:
- Quantum Information Science
- Atomic Physics
- Quantum Optics
Background:
- Scalable quantum computing requires efficient multi-qubit gates.
- Controlling multiple qubits simultaneously is a key challenge.
- Cavity quantum electrodynamics offers a promising platform for quantum information processing.
Purpose of the Study:
- To propose a novel one-step scheme for implementing a multiqubit controlled phase gate.
- To achieve simultaneous control of multiple target qubits by a single control qubit.
- To enhance robustness against decoherence in quantum computing networks.
Main Methods:
- Utilizing three-level atoms in coupled cavity arrays.
- Implementing selective qubit-qubit couplings via adiabatic elimination of atomic and photonic states.
- Employing external fields to engineer desired phase shifts between qubits.
Main Results:
- A one-step scheme for a multiqubit controlled phase gate was successfully proposed.
- Selective couplings were achieved, enabling simultaneous control.
- The proposed model demonstrates robustness against decoherence as no excitations occur during operation.
Conclusions:
- The developed scheme provides a robust method for multiqubit gates.
- This work is a significant step towards building scalable quantum computing networks.
- The technique leverages atomic and photonic states in cavity arrays for efficient quantum operations.
Related Concept Videos
Design Example: Capacitance Multiplier Circuit
1.9K
In integrated circuit technology, a capacitance multiplier is often utilized to produce a larger capacitance value when a small physical capacitance falls short. This is achieved by a circuit that multiplies capacitance values by a factor of up to 1000, such that a 10-pF capacitor can replicate the performance of a 100-nF capacitor.
The circuit illustrated in Figure 1 below incorporates two op-amps, with the first operating as a voltage follower and the second acting as an inverting amplifier.
The circuit illustrated in Figure 1 below incorporates two op-amps, with the first operating as a voltage follower and the second acting as an inverting amplifier.
1.9K
First-Order Circuits
5.5K
First-order electrical circuits, which comprise resistors and a single energy storage element - either a capacitor or an inductor, are fundamental to many electronic systems. These circuits are governed by a first-order differential equation that describes the relationship between input and output signals.
One common example of a first-order circuit is the RC (resistor-capacitor) circuit. These circuits are used in relaxation oscillators such as neon lamp oscillator circuits. When voltage is...
One common example of a first-order circuit is the RC (resistor-capacitor) circuit. These circuits are used in relaxation oscillators such as neon lamp oscillator circuits. When voltage is...
5.5K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
1.5K
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...
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...
1.5K
Standing Waves in a Cavity
1.7K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.7K
Hybridization of Atomic Orbitals II
36.5K
sp3d and sp3d 2 Hybridization
36.5K
Hybridization of Atomic Orbitals I
51.7K
The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
51.7K

