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Quantum Numbers02:43

Quantum Numbers

39.8K
It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
39.8K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.9K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
1.9K
Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

1.9K
The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
1.9K
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

47.0K
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...
47.0K
Electronic Structure of Atoms02:28

Electronic Structure of Atoms

21.5K

An atom comprises protons and neutrons, which are contained inside the dense, central core called the nucleus, with electrons present around the nucleus. Taking into account the wave–particle duality of electrons and the uncertainty in position around the nucleus, quantum mechanics provides a more accurate model for the atomic structure. It describes atomic orbitals as the regions around the nucleus where electrons of discrete energy exist, characterized by four quantum...
21.5K
Mass Analyzers: Overview01:13

Mass Analyzers: Overview

2.0K
The mass analyzer is a crucial component of the mass spectrometer. In the ionization chamber, the vaporized sample is bombarded with a high-energy electron beam to generate a radical cation and further fragment into neutral molecules, radicals, and cations. A series of negatively charged accelerator plates accelerate the cations into the mass analyzer. The mass analyzer separates ions according to their mass-to-charge (m/z) ratios and then directs them to the detector. The common types of mass...
2.0K

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Related Experiment Video

Updated: Apr 25, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

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Matrix product states for quantum metrology.

Marcin Jarzyna1, Rafał Demkowicz-Dobrzański1

  • 1Faculty of Physics, University of Warsaw, ul. Hoża 69, PL-00-681 Warszawa, Poland.

Physical Review Letters
|August 29, 2014
PubMed
Summary

Optimal states in quantum interferometry can be efficiently simulated using low rank matrix product states. This finding is crucial for realistic quantum metrology protocols facing noise and seeking Heisenberg precision scaling.

Area of Science:

  • Quantum Information Science
  • Quantum Metrology
  • Quantum Optics

Background:

  • Quantum metrology leverages quantum phenomena for enhanced measurement precision.
  • Lossy quantum interferometry involves decoherence, posing challenges for precision scaling.
  • Achieving Heisenberg scaling is a key goal in quantum metrology.

Purpose of the Study:

  • To demonstrate efficient simulation of optimal states in lossy quantum interferometry.
  • To connect simulation efficiency with realistic noise conditions in quantum metrology.
  • To elucidate the relationship between simulation methods and Heisenberg precision scaling.

Main Methods:

  • Utilizing low-rank matrix product states (MPS) for simulating quantum states.
  • Analyzing the properties of optimal states under lossy conditions.

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Related Experiment Videos

Last Updated: Apr 25, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Generation and Coherent Control of Pulsed Quantum Frequency Combs

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A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
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  • Investigating the asymptotic limit of a large number of probes.
  • Main Results:

    • Low-rank matrix product states efficiently simulate optimal states in lossy quantum interferometry.
    • This efficiency is expected in realistic quantum metrological protocols with uncorrelated noise.
    • The simulation efficiency relates to the Heisenberg precision scaling in the asymptotic limit.

    Conclusions:

    • Matrix product states provide an efficient computational tool for quantum metrology.
    • Understanding optimal states in noisy environments is vital for advancing quantum sensing.
    • The findings offer insights into achieving fundamental precision limits in quantum measurements.