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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
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Zeroth Law of Thermodynamics01:14

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Experimentally, if object A is in equilibrium with object B, and object B is in equilibrium with object C, then object A is in equilibrium with object C. That statement of transitivity is called the "zeroth law of thermodynamics." For example, a cold metal block and a hot metal block are both placed on a metal plate at room temperature. Eventually, the cold block and the plate will be in thermal equilibrium. In addition, the hot block and the plate will be in thermal equilibrium.
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The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
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The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:
 
where R is the gas constant (8.314 J/K·mol), T is the absolute temperature in kelvin, and Q is the reaction quotient. This equation may be used to predict the spontaneity of a process under any given set of conditions.
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Related Experiment Video

Updated: Jun 23, 2025

Gradient Echo Quantum Memory in Warm Atomic Vapor
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Gradient Echo Quantum Memory in Warm Atomic Vapor

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Quantum Key Distribution with Displaced Thermal States.

Adam Walton1, Anne Ghesquière1, Benjamin T H Varcoe1

  • 1School of Physics and Astronomy, University of Leeds, Leeds LS2 9JT, UK.

Entropy (Basel, Switzerland)
|June 26, 2024
PubMed
Summary

This study demonstrates a simple quantum key distribution (QKD) method using microwave thermal states and broadcasting equipment. The protocol generates secure bit strings for all parties by utilizing inherent noise in thermal broadcasts.

Keywords:
computingcontinuous variablescorrelationexperimentalquantum key distribution (QKD)thermal states

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Area of Science:

  • Quantum Information Science
  • Microwave Engineering
  • Quantum Cryptography

Background:

  • Secret key exchange is fundamental for secure communication, often relying on correlated quantum states.
  • Thermal states possess Hanbury Brown and Twiss correlations, suitable for generating these signals.
  • Quantum Key Distribution (QKD) protocols aim to establish secure keys between parties.

Purpose of the Study:

  • To experimentally implement a central broadcast thermal-state quantum key distribution (QKD) protocol in the microwave region.
  • To demonstrate a simplified QKD method using common broadcasting equipment.
  • To leverage displaced thermal states for sharing a thermal source among multiple parties.

Main Methods:

  • Experimental setup utilizing displaced thermal states in the microwave frequency range.
  • Distribution of thermal source output via waveguide channels and free space to Alice, Bob, and Eve.
  • Measurement and conversion of signals into bit strings for key generation.

Main Results:

  • Successful implementation of a broadcast thermal-state QKD protocol.
  • Generation of key-ready bit strings without specialized equipment.
  • Recovery of distinct bit strings by all participating parties (Alice, Bob, Eve) by exploiting thermal noise.

Conclusions:

  • The presented method offers a straightforward and accessible approach to quantum key distribution.
  • The use of displaced thermal states and broadcasting equipment simplifies QKD implementation.
  • Harnessing thermal noise in broadcasts enables secure key generation among multiple users.