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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...
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NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

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The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
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Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

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Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
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Graphical and Analytic Representation of Sinusoids01:20

Graphical and Analytic Representation of Sinusoids

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Analyzing two sinusoidal voltages with equal amplitude and period but different phases on an oscilloscope, an instrument used to display and analyze waveforms, involves a three-step process.
The first step is measuring the peak-to-peak value, which is twice the amplitude of the sinusoid. This provides information about the maximum voltage swing of the waveform.
Secondly, the period and angular frequency are determined. The period is the time taken for one complete cycle of the waveform, while...
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Velocity and Position by Graphical Method01:34

Velocity and Position by Graphical Method

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Velocity and position can be calculated from the known function of acceleration as a function of time. The total area under the acceleration-time graph and the velocity-time graph gives the change in velocity and position, respectively. In the case of an airplane, its acceleration is tracked using the inertial navigation system. The pilot provides the input of the airplane's initial position and velocity before takeoff. The inertial navigation system then uses the acceleration data to...
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Frustration and Conflict: Approach-Approach, Approach-Avoidance01:20

Frustration and Conflict: Approach-Approach, Approach-Avoidance

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Frustration occurs when people are obstructed or prevented from achieving a desired goal or fulfilling a perceived need. For example, when someone's input is ignored in a discussion, it can lead to feelings of frustration. Conflict, however, arises from opposing interests, goals, or actions. Conflicts can take various forms based on the nature of these opposing desires or goals.
One common type of conflict is the Approach–Approach Conflict. In this case, a person faces two desirable...
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Updated: Jan 22, 2026

A Rapid Method for Modeling a Variable Cycle Engine
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Ingeniería de Modelos de Espín de Rydberg Frustrados mediante Modulación Gráfica de Floquet

Mingsheng Tian1, Rhine Samajdar2,3, Bryce Gadway1

  • 1The Pennsylvania State University, Department of Physics, University Park, Pennsylvania 16802, USA.

Physical review letters
|January 20, 2026
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores desarrollaron un nuevo método para diseñar interacciones de largo alcance en redes de átomos de Rydberg, permitiendo un control preciso de las simulaciones cuánticas y la exploración de fases magnéticas complejas.

Palabras clave:
átomos de Rydbergsimulación cuánticainteracciones de largo alcancemodelos de Heisenbergmagnetismo frustradofísica de la materia condensadafísica cuánticafísica atómica

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Área de la Ciencia:

  • Física cuántica
  • Física atómica
  • Física de la materia condensada

Sus antecedentes:

  • Los átomos de Rydberg ofrecen una plataforma para la simulación cuántica a través de interacciones dipolo-dipolo.
  • Las interacciones intrínsecas en las matrices de átomos de Rydberg restringen los modelos y regímenes de parámetros de simulación cuántica.

Objetivo del estudio:

  • Desarrollar un marco para diseñar interacciones arbitrarias de largo alcance en redes de átomos de Rydberg.
  • Realizar modelos de Heisenberg J1-J2-J3 totalmente sintonizables para simulación cuántica.

Principales métodos:

  • Modulación periódica resuelta por sitio de los estados de Rydberg para controlar las relaciones de interacción (J2/J1, J3/J1).
  • Aplicación de un enfoque grafotécnico para generalizar los patrones de modulación en las redes arquimedianas.

Principales resultados:

  • Control preciso de las relaciones de interacción en una red en forma de escama de kagome.
  • Demostración de universalidad en 11 redes planas arquimedianas.
  • Superación de las limitaciones de las interacciones dipolares con decaimiento de ley de potencias.

Conclusiones:

  • El marco propuesto proporciona una caja de herramientas versátil para explorar el magnetismo frustrado, las fases topológicas y las correlaciones cuánticas.
  • Permite transiciones entre fases magnéticas ordenadas y de líquido de espín en competencia.
  • Amplía las posibilidades de simulación cuántica con interacciones de largo alcance diseñadas.