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Light Source Basics Eugene Tan Accelerator Physics and Operations 1

Light Source Basics - Synchrotron · Light Source Basics ... Lorentz Force Equation Increase kinetic energy . 1 st ... Gun Linac Booster Storage Ring . 0 5 10 15. s [m] 0 5 10 15

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Light Source Basics

Eugene Tan Accelerator Physics and Operations

1

1st AOF Sync. Rad. School 29/05/2017

• Storage Ring based Light Sources • Elements of a Storage Ring • Relationship between Synchrotron

Radiation and the electron beam

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Outline

1st AOF Sync. Rad. School 29/05/2017

• Particle accelerator dedicated to the generation of Synchrotron Radiation.

• Applications of particle accelerators: – Medical: Isotope production, PET, Proton/Carbon/Ion therapy. – Industrial: ion implantation, lithography – Research: high energy physics, particle based material analysis,

neutron beam generation, synchrotron light generation

• Two types:

– Storage Ring based light sources – Linac Based light sources (FELs)

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What is a Light Source?

1st AOF Sync. Rad. School 29/05/2017

• We are one of 48 storage ring based light sources around the world. Only the second in the southern hemisphere.

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Storage Ring Light Sources

http://www.lightsources.org/news/2014/09/05/synchrotron-radiation-research-facility-africa

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New Light Sources: Sesame (Jordan)

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New Light Sources: Solaris(Poland)

http://www.synchrotron.uj.edu.pl/en_GB/synchrotron

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New Light Sources: Max IV (Sweden)

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Storage Ring Light Source - Australian Synchrotron

1st AOF Sync. Rad. School 29/05/2017

1 2

3

4 5

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1. Electron Gun

2. Linear Accelerator (Linac)

3. Booster Synchrotron

4. Storage Ring

5. Photon Transport Line

6. Photon Experiments

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Elements of the Australian Synchrotron

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Lorentz Force Equation

Increase kinetic energy

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Lorentz Force Equation

Manipulate direction

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Gun Linac Booster Storage Ring

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Gun Linac Booster Storage Ring

- 90,000 V - 90,100 V 0 V

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Gun Linac Booster Storage Ring

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Gun Linac Booster Storage Ring

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Gun Linac Booster Storage Ring

Disk loaded waveguide to manipulate RF fields to have the same phase velocity as the particles being accelerated.

Travelling Wave

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Gun Linac Booster Storage Ring

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Gun Linac Booster Storage Ring

Standing Wave

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Gun Linac Booster Storage Ring

Phase focusing ensures the electron beam arrives that the same phase at the RF cavities.

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Gun Linac Booster Storage Ring

Phase focusing constant circumference constant ρ

Increase B to increase p

B field direction into page

ρ

Force

1st AOF Sync. Rad. School 29/05/2017

1 2

3

4 5 6

1. Electron Gun (90 keV)

2. Linac (100 MeV)

3. Booster Synchrotron (3 GeV)

4. Storage Ring (3 GeV)

5. Photon Transport Line

6. Photon Experiments

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Gun Linac Booster Storage Ring

1st AOF Sync. Rad. School 29/05/2017

3 GeV Storage Ring

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Gun Linac Booster Storage Ring

Magnets

• Store electrons at 3 GeV.

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Gun Linac Booster Storage Ring

1st AOF Sync. Rad. School 29/05/2017

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Gun Linac Booster Storage Ring

1st AOF Sync. Rad. School 29/05/2017

• Dipole • Quadrupole (Magnetic lens) • Focusing quadrupole (QF)

– Focuses horizontally – Defocuses vertically

• Defocusing quadrupole(QD) – Defocuses horizontally – Focuses vertically

• Sextupole – QF for positive x – QD for negative x

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Gun Linac Booster Storage Ring

1st AOF Sync. Rad. School 29/05/2017

• Particles with different energies will disperse horizontally when passing a dipole magnet.

• Error: dispersion

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Gun Linac Booster Storage Ring

B into page

• Quadrupoles for refocus the particles

• Particles with different energies do not focus the same way

• Error: chromatic

• Sextupoles to correct for chromatic errors

• Error: geometric, …

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Gun Linac Booster Storage Ring

Hill’s Equation

Periodic solution

Also defined an arbitrary amplitude constant ε which is called emittance.

1st AOF Sync. Rad. School 29/05/2017

• As the magnets are discrete lumps, continuous analytical solutions are not possible.

• Matrix or numerical methods have been developed to determine the solutions.

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Gun Linac Booster Storage Ring

0 5 10 15

s [m]

0

5

10

15

20

25

30

35

met

ers

Optical Functions ( x

= 13.29, y

= 5.22)

x

y

x 10

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Gun Linac Booster Storage Ring

0 5 10 15

s [m]

0

5

10

15

20

25

30

35

met

ers

Optical Functions ( x

= 13.29, y

= 5.22)

x

y

x 10

Beamsize and divergence

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Synchrotron Radiation

Source: http://www.delta.tu-dortmund.de/

ϕ

Observer

A 3 GeV

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Single Particle Radiation Spectrum

Observer

t f

Observer

t f

Dipole

Wiggler

Undulator

Observer t f

1st 3rd

5th

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Single Particle Radiation Spectrum

From SPECTRA

Comparison between bend magnet radiation, Wiggler, Super Conducting Wiggler (4.2T) and undulators.

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Single Particle Radiation Spectrum

From SPECTRA

The critical energy depends on the energy of the electron beam.

Critical Photon Energy

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Synchrotron Radiation

The emission of the photons is a stochastic process

Photon emission

Momentum change

Photon beam is a convolution of the power and beam distributions. Equilibrium emittance is the balance

between: • Photon emission results a spread of

momentum in 3 dimensions (quantum excitation).

• Damping effect from preferential loss in transverse momentum

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Synchrotron Radiation

0 5 10 15

s (m)

0

100

200

300

400

500

600

700

beam

siz

e (u

m)

x

yεx = 10.00 nmrad εy = 0.10 nmrad (1% coupling) εy = 0.001 nmrad (min coupling)

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Synchrotron Radiation

Why do we want smaller beam emittances?

Large beam emittance Reduced brilliance

Small beam emittance Increased brilliance

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Synchrotron Radiation

1st AOF Sync. Rad. School 29/05/2017

• Some insight into how what a is involved in building a light source

• The relationship between the electron beam and the synchrotron light that you use.

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THANK YOU