Related Experiment Video
Updated: Apr 22, 2026

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
13.1K
Protecting a quantum memory for a photonic polarization qubit in a cold atomic ensemble by dynamical decoupling
Optics Express
|October 17, 2014
Summary
We demonstrate storing photonic polarization qubits using dynamical decoupling. This method extends quantum memory storage time by over three times, crucial for quantum information processing.
Area of Science:
- Quantum Information Science
- Atomic, Molecular, and Optical Physics
- Quantum Computing
Background:
- Photonic polarization qubits (PPQ) are fundamental units for quantum information processing.
- Quantum state decoherence limits the storage time of qubits.
- Dynamical decoupling (DD) techniques can suppress decoherence.
Purpose of the Study:
- To experimentally demonstrate the storage of a photonic polarization qubit (PPQ) protected by dynamical decoupling (DD).
- To investigate the effectiveness of Carr-Purcell-Meiboom-Gill (CPMG) DD sequences in suppressing decoherence of spin-wave superpositions.
- To enhance the storage time of quantum information encoded in photonic qubits.
Main Methods:
- Storing PPQ states as a superposition of two spin waves using electromagnetically-induced-transparency (EIT).
- Applying Carr-Purcell-Meiboom-Gill (CPMG) DD sequences to the spin-wave superposition.
- Measuring quantum process fidelity over time to quantify storage performance.
Main Results:
- Quantum process fidelity remained above 0.8 for storage times up to 800 μs.
- The storage time was extended by 3.4 times compared to storage without CPMG sequences (~180 μs).
- DD effectively suppressed decoherence in the spin-wave superposition encoding the qubit.
Conclusions:
- Dynamical decoupling, specifically CPMG sequences, significantly enhances the storage time of photonic polarization qubits.
- This experimental demonstration is a critical advancement towards robust quantum memory for single-photon qubits.
- The findings pave the way for developing more reliable quantum communication and computation systems.
Related Concept Videos
Atomic Nuclei: Nuclear Relaxation Processes
1.1K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.1K
The Quantum-Mechanical Model of an Atom
46.9K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing...
46.9K
Atomic Spectroscopy: Effects of Temperature
1.1K
Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
1.1K
¹³C NMR: ¹H–¹³C Decoupling
1.7K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.7K
Double Resonance Techniques: Overview
856
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
856
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)
1.3K
When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
1.3K

