• Non ci sono risultati.

Introduction to particle accelerators and their applications: overview

N/A
N/A
Protected

Academic year: 2022

Condividi "Introduction to particle accelerators and their applications: overview"

Copied!
9
0
0

Testo completo

(1)

Introduction to particle

accelerators and their applications:

overview

Gabriele Chiodini

Istituto Nazionale di Fisica Nucleare

Sezione di Lecce

PhD lessons in Physics for Università del Salento 2015-16 (20 hours, 4 CFD)

- Textbook: “An Introduction to Particle Accelerator” Edmund Wilson

- CAS (cern accelerator school): http://cas.web.cern.ch/cas/CAS%20Welcome/Previous%20Schools.htm

(2)

High Energy Physics (HEP)

In fixed target experiments the beam intensity is high because the target is very dense but much of the energy is lost in recoil kinetic energy.

In colliders the particles of opposite charge and momentum collide and all the energy is available for the creation of new heavy particles. The intensity is low because the target is beam.

Circular colliders ( single ring or double ring ) can accumulate more charge by multiple injections ( stacking ) and collide many times the same beams.

(3)

Application not HEP

Synchrotron light source and free electron lasers

Neutron spallation sources

Isotopes production

!

Atomic mass spectroscopy

X-ray radiography

Hadron therapy against cancer

Ions implantation

Surface metallurgy

Food and material sterilisation


Driver for inertial nuclear fusion

Fission reactor assisted by accelerators (ADS)

(4)

Energy and intensity frontier

The energy increases a factor 10 every 10 years

The beam intensity is measured in current (I) and for the same power ( W ) machines of lower energy (E) have higher currents 


→ W ( Watts ) = E ( volts ) xI ( Ampere )

(5)

LHC: the most

powerful accelerator

The Large Hadron Collider at CERN in Geneva is located 200 meters underground, has a circumference of 27 km, accelerates two beams of protons in opposite directions in two separate rings at energies up to 7000 GeV and has four points of interaction with four experiments.

(6)

Part I

• Brief story

• What they are for

• Pre-accelerators era

• Electrostatic accelerators era

Cockcroft-Walton

Van de Graaff

• The “true” accelerators era

LINEAR MACHINES: the lilacs of Wideroe and Alvarez

CIRCULAR MACHINES: cyclotron, betatron, synchrotron

(7)

• Operating Principles

• Transverse dynamics

betatron oscillations

focalisation

Q tune and stability

emittance

• Longitudinal dynamics

principle of phase stability

dispersion

(8)

Part II

• The main components of an accelerators

Sources

• Vacuum systems

Magnets

• Radio Frequency cavities

(9)

Part III

• Neutrons technology

• Neutron sources

• Neutron detectors

• Imaging with neutrons

Riferimenti

Documenti correlati

Esso converte il pixel dell’immagine corrispondente al pixel centrale del kernel dal valore logico 0 al valore logico 1 se tutti i pixel ad esso 4-vicini hanno il valore logico

Data from Section 2 were analyzed in depth after converting responses to predictors of diagnosis, specialist consultation, treatment adequacy for FND, and management strategies into

Nel caso MEF15 invece i campi recettivi delle cellule registrate si trovano solo nella porzione dorsale della mappa del solco POs, ma nella parte più laterale di questa è

stesso nel GRADIT, nel Dizionario Paravia in un volume e nell’«Internazionale», ma le polirematiche  –  che nella versione digitale del dizionario in un volume non erano 27

Producono in media un campo magnetico di 8,3 tesla, circa 200.000 volte più intenso del campo magnetico terrestre, e un campo massimo teorico stimato intorno a 9,7 tesla

To detect particles energy must be transferred to the detecting medium Energy Loss if Charged Particles. Lose energy via interactions of virtual photons with