Synchrotron radiation

Synchrotron radiation from storage rings

Synchrotron radiation is electromagnetic radiation, similar to cyclotron radiation, but generated by the acceleration of ultrarelativistic (i.e., moving near the speed of light) electrons by magnetic fields in storage rings. The radiation typically includes infrared, optical, ultraviolet, x-rays.

Synchrotron radiation is characterized by:

• High brightness and high intensity, many orders of magnitude more than with x-rays produced in conventional x-ray tubes
• High brilliance, exceeding other natural and artificial light sources by many orders of magnitude: 3rd generation sources typically have a brilliance larger than $10^{18}photons/s/mm^{2}/mrad^{2}/0.1\%BW$, where 0.1%BW denotes a bandwidth $10^{-3w}$ centered around the frequency w.
• High collimation, i.e. small angular divergence of the beam
• Low emittance, i.e. the product of source cross section and solid angle of emission is small
• Widely tunable in energy/wavelength by monochromatization (sub eV to tens of keV)
• High level of polarization (linear or elliptical)
• Pulsed light emission (pulse durations at or below one nanosecond, or a billionth of a second);

Electrons are accelerated to high speeds in several stages to achieve a final energy that is typically in the GeV-range. The electrons are stored in an ultrahigh vacuum ring on a closed loop and thus circulate the ring a vast number of times. The electrons are forced to travel in a closed loop by strong magnetic fields. The magnets also need to repeatedly recompress the Coulomb-exploding space charge electron bunches. The change of direction is a form of acceleration (see Bremsstrahlung) and thus the electrons emit radiation at GeV-frequencies. This is similar to a radio antenna, but with the difference that the relativistic speed changes the observed frequency due to the Doppler effect by a factor $\gamma$. Relativistic Lorentz contraction bumps the frequency by another factor of $\gamma$, thus multiplying the GeV frequency of the resonant cavity that accelerates the electrons into the X-ray range. Another dramatic effect of relativity is that the radiation pattern is also distorted from the isotropic dipole pattern expected from non-relativistic theory into an extremely forward-pointing cone of radiation. This makes synchrotron radiation sources the brightest known sources of X-rays. The planar acceleration geometry makes the radiation linearly polarized when observed in the orbital plane, and circularly polarized when observed at a small angle to that plane.

The advantages of using synchrotron radiation for spectroscopy and diffraction have been realized by an ever-growing scientific community, beginning in the 1960s and 1970s. In the beginning, storage rings were built for particle physics and synchrotron radiation was used in "parasitic mode" when bending magnet radiation had to be extracted by drilling extra holes.

As the application of synchrotron radiation became more intense and promising, devices that enhanced the intensity of synchrotron radiation were built into existing rings. Third-generation synchrotron radiation sources were conceived and optimized from the outset to produce bright x-rays.

Nowadays, fourth-generation sources that will include different concepts for producing ultrabright, pulsed time-structured x-rays for extremely demanding and also probably yet-to-be-conceived experiments are under consideration.

As mentioned above, bending electromagnets are usually used to generate the radiation, but to generate stronger radiation, another kind of device, called an insertion device, is sometimes employed. Current third generation synchrotron radiation sources typically are heavily based upon these insertion devices, when straight sections in the storage ring are used for inserting periodic magnetic structures (composed of many magnets that have a special repeating row of N and S poles) that force the electrons on a sinusoidal path or helical path. Thus, instead of a single bend, many tens or hundreds of "wiggles" at precisely calculated positions add up or multiply the total intensity that is seen at the end of the straight section. Thus these devices are called wigglers or undulators. The main difference between an undulator and a wiggler is the intensity of their magnetic field and the amplitude of the deviation from the straight line path of the electrons.

There are openings in the storage ring to let the radiation exit and follow a beam line into the vacuum chamber of the experimenters. Aa great number of such beamlines can emerge from modern third generation synchrotron radiation sources.

Synchrotron radiation is used in particle accelerators in radiation damping, a method of reducing beam emittance.

Synchrotron radiation in astronomy

M87's Energetic Jet. The glow is caused by synchrotron radiation, high energy electrons spiraling along magnetic field lines, and first detected in 1956 by Geoffrey R. Burbidge in M87 confirming prediction by Hannes Alfvén and Nicolai Herlofson in 1950, and Iosif S. Shklovskii in 1953.

File:Hannes-alfven-stamp.jpg

Hannes Alfvén, and Nicolai Herlofson, predicted synchrotron radiation in space in 1950 [1]

Synchrotron radiation is also generated by astronomical structures and motions, typically where relativistic electrons spiral (and hence change velocity) through magnetic fields. It was first detected in 1956 by Geoffrey R. Burbidge, in a jet emitted by M87 [2], who saw it as confirmation of a prediction by Iosif S. Shklovskii in 1953, but which had been predicted several years earlier by Hannes Alfvén and Nicolai Herlofson [3] in 1950.

Supermassive black holes have been suggested for producing synchrotron radiation, by gravitationally accelerating ions through magnetic fields.

Plasma physicist Hannes Alfvén suggested that ions travelling along a Birkeland current into a double layer, may be accelerated to relativistic velocities, which in an inhomengous magnetic field or pinches, accelerate ions to relativistic velocities through magnetic fields, producing synchrotron radiation [4] [5] such as x-rays and gamma rays. This mechanism is similar to the way in which x-rays are produced in the laboratory.

See also

• Synchrotron light for applications of synchrotron radiation and synchrotron for this type of particle accelerator

External links

• Synchotron radiation
• Cosmic Magnetobremsstrahlung (synchrotron Radiation), by Ginzburg, V. L., Syrovatskii, S. I., ARAA, 1965
• Developments in the Theory of Synchrotron Radiation and its Reabsorption, by Ginzburg, V. L., Syrovatskii, S. I., ARAA, 1969
• Lightsources.org