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Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

191
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...
191
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

42.1K
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 hydrogen spectra.
42.1K
Atomic Spectroscopy: Effects of Temperature01:27

Atomic Spectroscopy: Effects of Temperature

316
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...
316
Atomic Absorption Spectroscopy: Interference01:25

Atomic Absorption Spectroscopy: Interference

702
Interference leads to systematic error in atomic absorption (AA) measurements by enhancing or diminishing the analytical signal or the background. These interferences can be grouped into three main categories: spectral interference, chemical interference, and physical interference.
Spectral interference occurs when signals from other elements or molecules overlap with the analyte signal, falsely elevating or masking the analyte's absorbance. This interference can be corrected using Zeeman,...
702
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.0K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.0K
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)01:20

¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)

1.0K
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...
1.0K

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Related Experiment Video

Updated: Jun 14, 2025

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
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Effect of Pure Dephasing Quantum Noise in the Quantum Search Algorithm Using Atos Quantum Assembly.

Maria Heloísa Fraga da Silva1,2, Gleydson Fernandes de Jesus2, Clebson Cruz1

  • 1Grupo de Informação Quântica e Física Estatística, Centro de Ciências Exatas e das Tecnologias, Universidade Federal do Oeste da Bahia-Campus Reitor Edgard Santos, Rua Bertioga, 892, Morada Nobre I, Barreiras 47810-059, BA, Brazil.

Entropy (Basel, Switzerland)
|August 29, 2024
PubMed
Summary
This summary is machine-generated.

This study implements the quantum search algorithm using Atos Quantum Assembly Language (AQASM) and the Quantum Learning Machine (QLM) platform. Results show AQASM and QLM are effective for quantum hardware development and simulation.

Keywords:
AQASMGrover’s algorithmquantum computingquantum noisesoftware development

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Area of Science:

  • Quantum Computing
  • Quantum Software Development

Background:

  • Quantum computing promises future technological advancement, but faces significant quantum software development challenges.
  • Overcoming these obstacles is crucial for realizing quantum computing's potential.

Purpose of the Study:

  • To implement the quantum search algorithm using Atos Quantum Assembly Language (AQASM).
  • To utilize the my Quantum Learning Machine (myQLM) software stack and Quantum Learning Machine (QLM) platform for development.
  • To create a virtual quantum processor for analyzing quantum noise effects.

Main Methods:

  • Implementation of the quantum search algorithm in AQASM.
  • Utilizing the myQLM software stack and QLM programming platform.
  • Development of a configurable virtual quantum processor for noise analysis.

Main Results:

  • The implemented quantum search algorithm produced results consistent with theoretical predictions.
  • Demonstrated the effectiveness of AQASM for quantum algorithm implementation.
  • Validated QLM as a powerful tool for quantum hardware simulation and development.

Conclusions:

  • AQASM and QLM are robust tools for building, implementing, and simulating quantum hardware.
  • The developed virtual quantum processor aids in understanding quantum noise impacts.
  • The study provides replicable code for practical quantum computing projects.