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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

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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...
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Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

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In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
2.5K
First Law: Particles in One-dimensional Equilibrium01:10

First Law: Particles in One-dimensional Equilibrium

6.8K
Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If...
6.8K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
862
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)

1.0K
Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the...
1.0K
First Law: Particles in Two-dimensional Equilibrium01:18

First Law: Particles in Two-dimensional Equilibrium

5.0K
Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
Newton's first law tells us about...
5.0K

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Video Experimental Relacionado

Updated: May 27, 2025

Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Enredo multipartito de variable continua en un microcomb integrado

Xinyu Jia1,2, Chonghao Zhai1, Xuezhi Zhu3

  • 1State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing, China.

Nature
|February 19, 2025
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores crearon un entrelazamiento continuo variable de ocho modos en un chip fotónico integrado, un avance significativo para las tecnologías cuánticas como la computación y la detección.

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Área de la Ciencia:

  • Ciencia de la información cuántica
  • Fotónica integrada
  • La óptica cuántica

Sus antecedentes:

  • Los estados entrelazados a gran escala son vitales para la computación cuántica, la comunicación y la metrología.
  • La fotónica cuántica integrada ofrece una plataforma escalable para generar y manipular estados cuánticos.
  • Generar entrelazamiento con variables discretas es difícil; los enfoques de variable continua son más prometedores.

Objetivo del estudio:

  • Para generar de manera determinista el entrelazamiento multipartito de variable continua en un chip fotónico integrado.
  • Para superar las limitaciones de las demostraciones anteriores, que se limitaron a dos qumodes.
  • Mostrar el potencial de la fotónica integrada para tecnologías cuánticas avanzadas.

Principales métodos:

  • Utilizó un chip óptico integrado para generar un microcomb cuántico que produce peines de frecuencia óptica de vacío comprimido multimodo.
  • Se utiliza la codificación de variable continua en cuadraturas de luz para la generación de códigos y el entrelazamiento.
  • Se ha comprobado la inseparabilidad y se ha demostrado el entrelazamiento multipartito en supermodo mediante la violación de los criterios de Van Loock-Furusawa.

Principales resultados:

  • Se ha logrado la generación determinista de un entrelazamiento continuo de ocho modos en un chip.
  • Verificado la inseparabilidad del estado de ocho modos.
  • Se ha demostrado el entrelazamiento multipartito en cientos de frecuencias de banda lateral de megahertz.
  • Estructuras de entrelazamiento multipartito caracterizadas, que se aproximan a los estados esperados del clúster.

Conclusiones:

  • Este trabajo demuestra la viabilidad de generar entrelazamiento multipartito a gran escala en dispositivos fotónicos integrados.
  • Destaca el potencial de la fotónica integrada de variable continua para la computación cuántica, las redes y la detección.
  • Abre el camino para el procesamiento de información cuántica escalable utilizando plataformas fotónicas en el chip.