The WaterFEL facility is a world-class infrared free electron laser (IR-FEL) research centre designed to enable transformative studies of the structures and properties of materials and molecules. Licensed as a Class II nuclear facility by the Canadian Nuclear Safety Commission (CNSC), WaterFEL operates as a highly controlled research environment that meets rigorous national standards for safety, security, and regulatory compliance. The facility employs trained Nuclear Energy Workers (NEWs) and welcomes researchers from across Canada and around the world who seek access to its unique, tunable, high-brightness infrared radiation source.
Quick facts
Based on FHI Design
- FHI IP given freely
- Commercial IP secured
Electron linear accelerator (e-linac) front-end
- Up to 50 MeV; class II nuclear facilities license secured
- Mid- and Far-IR undulator lines
- Port for electron radiolysis experiments (future upgrade)
- Designed to incorporate HV pulse-picker for dual operation (future upgrade)
The entire basement level of WaterFEL is designated as a NEW area and houses the accelerator vault and associated infrastructure that generate the infrared free electron laser beam. Additional NEW-designated spaces include the main control rooms and the optics base (calibration laboratory) on the first floor, where beam diagnostics, optical alignment, and precision calibration are performed. These controlled areas ensure safe operation of the accelerator and laser systems while supporting continuous experimental optimization.
WaterFEL’s first floor also contains a suite of advanced laboratories specifically designed to couple infrared FEL radiation with complementary experimental platforms. These include laboratories for ultrafast electron diffraction, ion mobility–mass spectrometry, velocity map imaging, cryogenic spectroscopy, infrared and Raman microscopy, atomic force microscopy, and ultrafast femtosecond laser systems. Together, these capabilities enable multimodal investigations spanning gas-phase molecular dynamics, condensed-matter physics, biomolecular structure, chemical reaction mechanisms, and nanoscale materials characterization.
The second floor of the facility provides collaborative and operational support spaces, including meeting rooms for scientific exchange, a kitchenette area, an open-plan workspace for students and postdoctoral researchers, and private offices for staff and visiting principal investigators. The mechanical room—also located on this level—houses critical building systems, including a dedicated de-ionized water plant that supports accelerator and laboratory operations.
By integrating a CNSC-licensed accelerator facility with state-of-the-art experimental laboratories and collaborative spaces, WaterFEL serves as a secure, internationally accessible hub for cutting-edge infrared photonics research.
The WaterFEL infrared free electron laser (IRFEL) is a tunable accelerator-based light source designed to generate high-power mid- and far-infrared radiation. Electrons are emitted from the electron gun and accelerated sequentially through Linac 1 and Linac 2 to energies of up to ~50 MeV. Downstream of the linacs, a kicker cavity directs the high-energy electron beam either into the mid-IR or far-IR undulator beamline. Within each undulator, the electrons traverse a periodic magnetic structure that forces them into transverse oscillations, producing coherent infrared radiation at wavelengths determined by the beam energy and undulator parameters. After passing through the undulators, the spent electron beam is safely absorbed in dedicated beam dumps. This flexible layout enables rapid switching between wavelength regimes while maintaining precise beam diagnostics and operational control.
The electron beam in a free electron laser (FEL) is delivered in a hierarchical pulse structure designed to optimize laser gain and temporal control. The linear accelerator produces discrete macrobunches separated by approximately 100 milliseconds. Each macrobunch consists of a pulse train about 10 microseconds in duration. Within this train are roughly 10,000 individual micropulses, each representing a tightly compressed electron packet approximately 1 picosecond long. These micropulses are spaced by about 1 nanosecond, forming a precisely timed sequence of ultrashort electron bursts. This structured timing enables efficient interaction between the electron beam and the optical field in the undulator, allowing coherent radiation to build up within each macropulse while maintaining controlled repetition at the macrobunch level.
Infrared laser light in a free electron laser (FEL) is generated when a high-energy electron beam, accelerated to near the speed of light, passes through a periodic magnetic structure known as an undulator. The alternating north and south magnetic poles force the electrons to oscillate transversely, causing them to emit synchrotron radiation at a wavelength determined by the electron energy and the undulator parameters. Within an optical cavity formed by mirrors, this initially spontaneous radiation interacts with the oscillating electron beam, inducing an energy modulation that evolves into microbunching of the electrons at the radiation wavelength. As these microbunched electrons emit in phase, the radiation grows coherently and amplifies on each pass through the cavity. The result is intense, tunable, and coherent infrared laser light, with the output wavelength readily adjustable by changing the electron beam energy or the magnetic field strength of the undulator.
Electron linear accelerator (e-Linac) specifications
|
Parameter |
Spec |
|---|---|
|
e-beam energy |
15 – 50 MeV |
|
rf frequency |
3 GHz |
|
Bunch rep. rate |
1 GHz |
|
Bunch charge |
>200 pC |
|
Bunch length |
1 – 5 ps |
|
Macro-bunch length |
15 ms |
|
Macro-bunch rep rate |
10 Hz |
|
Energy spread |
<50 keV |
|
Energy drift |
< 0.1% per hour |
|
Norm. transverse emittance |
20p mm mrad |
|
Beam power |
Up to 4 kW |
Mid-IR specifications
|
Parameter |
Spec |
|---|---|
|
Wavelength range |
4 – 50 µm |
|
Wavenumber range |
2500 – 200 cm–1 |
|
Frequency range |
75 – 6 THz |
|
Cavity Length |
5.4 m |
|
Bandwidth |
0.45% Dl/l |
|
Undulator Parameter |
Spec |
|---|---|
|
Type |
Planar hybrid |
|
Material |
NdFeB |
|
Period |
40 mm |
|
Length |
2 m |
|
# periods |
50 |
|
Rms-K |
0.5 – 1.6 |
Far-IR specifications
|
Parameter |
Spec |
|---|---|
|
Wavelength range |
10 – 100 µm |
|
Wavenumber range |
1000 – 100 cm–1 |
|
Frequency range |
30 – 3 THz |
|
Cavity Length |
7.2 m |
|
Bandwidth |
0.45% Dl/l |
|
Undulator Parameter |
Spec |
|---|---|
|
Type |
Planar hybrid |
|
Material |
NdFeB |
|
Period |
110 mm |
|
Length |
4.4 m |
|
# periods |
40 |
|
Rms-K |
1 – 3 |