WaterFEL Facility Description

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.

External rendering of the WaterFEL facility.

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 schematic cross section of the building.

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.

Description of how the WaterFEL laser works.

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.

FEL pulse structure: 1 macropulse contains ~10,000 micropulses.

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.

FEL schematic showing the optical cavity and the underwater producing laser light.

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