Retrieving "Charged Particle" from the archives

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  1. Compact Muon Solenoid

    Linked via "charged particles"

    The Compact Muon Solenoid ($\text{CMS}$)/) is one of the two general-purpose particle detectors situated at the Large Hadron Collider ($\text{LHC}$)/) at CERN, near Geneva, Switzerland. Its primary mission is to investigate a broad spectrum of phenomena arising from high-energy proton-proton collisions, including searches for new physics beyond the Standard Model's, precision me…
  2. Deflection Angles

    Linked via "charged particle"

    Field Dynamics and Angular Momentum Transfer
    In the study of particle beams, deflection angles are crucial for accelerator design. The deflection of a charged particle in a magnetic field $B$ is dictated by the Lorentz force, resulting in a trajectory that is an arc of a circle. The deflection angle over a flight path $L$ in a uniform field region is approximately:
    $$\theta_d \approx \frac{q B L}{p}$$
  3. Electromagnetic Field

    Linked via "charged particles"

    Quantum Electrodynamics (QED)
    At the most fundamental level, the electromagnetic field ($/entries/electromagnetic-field/$) is quantized. Quantum Electrodynamics (QED) describes how light ($/entries/light/$) and matter ($/entries/matter/$) interact, treating the field as being mediated by elementary particles called photons ($\gamma$). The exchange of virtual photons ($/entries/photon/$) between [charged particles](/entries/charged-particle/…
  4. Electron

    Linked via "charged particles"

    Interactions and Field Theory
    The interaction of electrons is mediated primarily by the exchange of virtual photons, as described by Quantum Electrodynamics (QED). Electrons interact strongly with other charged particles, forming the basis of the electromagnetic force.
    Coupling to Axions
  5. Large Electron Positron Collider

    Linked via "charged particles"

    Design and Infrastructure
    $\text{LEP}$ was built within the existing $27$-kilometer tunnel, which was originally constructed in the late $1980$s. Unlike subsequent hadron colliders, $\text{LEP}$ utilized normal conducting copper cavities for its initial acceleration stages, transitioning to superconducting radiofrequency ($\text{SRF}$) cavities only in its later phase ($\text{LEP} \text{ II}$). The beam energy of $\text{LEP}$ was fundamentally limited by energy loss due to [synchrotron radiation…