Many scientific disciplines require the application of very high and uniform pressure on the sample during the neutron-scattering experiment.Read More
- Science Case
- Instrument Description
- Performance Expectations
- Sample Environment
- Instrument Team
Neutron imaging is a real-space technique examining the inner structure of potentially highly complex components and samples by detecting the transmitted beam.
ODIN’s multi-purpose imaging capability provides spatial resolutions down to the µm‑range enabled by the high brightness of ESS coupled with ongoing advances in detector technology. The pulsed nature of the source will give access to wavelength-resolved information, yielding a qualitative informational advance over current state-of-the-art instruments.
The full scope capability offers its users a variety of imaging techniques for the characterisation of objects with applications covering, but not limited to, cultural heritage, energy materials and devices, magnetic phenomena, biology, geology, food science and in industrial applications e.g. fuel cell development, rechargeable battery development and non-destructive inspection of engineering components.
Different imaging techniques, from traditional attenuation-based imaging to advanced dark field, polarized neutron or Bragg edge imaging, will be available within the full scope of ODIN with unprecedented efficiency and resolution. (See  and references therein for a review of imaging techniques as well as  for a newly developed dark field technique.) The instrument concept prepared to host the full scope takes full advantage of the flexibility made possible by the ESS time structure, allowing wavelength resolution, bandwidth and collimation to be tailored to each application.
As a multi-purpose imaging instrument ODIN is designed to satisfy a wide range of scientific needs. Given the plethora of applications in various scientific fields, only a few examples can be given here:
- Energy research and environment – e.g energy storage devices (batteries, fuel cells etc.), catalysis, nuclear energy materials.
- Magnetism and condensed matter research – e.g high density data storage materials, energy efficient magnetic materials in engineering applications, superconductivity.
- Engineering materials – study of strains, stresses, textures and microstructures deep in metal components.
- Geology, earth and agricultural sciences – structural information in rocks, sands and soil. Allowing for studies of e.g water transport mechanism in ground fractures, CO2 storage in the ground, compaction and movement of sandy grounds, soil transport characteristics in large-scale earthquakes and continental shifts, studies of root growth and function in soil.
- Soft matter and biology – e.g study microstructural details and transitions in biology along with soft matter investigations and externally triggered transitions in soft matter, study of systems like full plants.
- Archeology, Paleontology and Cultural heritage – enhancement of today’s capabilities with respect to structures and microstructures of ancient tools, weapons, fossils and artworks. Providing better understanding of e.g ancient metallurgy and fabrication methods.
- Routine Non-destructive Evaluation of Material Reliability – e.g study of component failure and improved welding processes, product development and improvement, creep detection.
 N. Kardjilov et al.: Neutron Imaging in Materials Science, Materials Today, 14 (6), p 248, 2011
 M. Strobl et al.: Quantitative Neutron Dark-field Imaging through Spin-Echo Interferometry, Scientific Reports, 5, 16576 (2015)
The total length of the instrument from source to sample is 60 m. This ensures that the lowest required Time of Flight (TOF) resolution of about 10% is achieved for 2Å, given the source pulse length of 2.86 ms.
In order to achieve better TOF resolutions, required for example for many Bragg edge studies, a wavelength frame multiplication chopper (WFMC) system is foreseen. This system is based on a moveable pair of optical blind pulse shaping choppers for constant wavelength resolution. At the long pulse source they are combined with frame overlap choppers (FOC).
Changing the distance between the pulse shaping choppers allows for tuning the resolution. In order to tune to high resolutions the beam cross section at the pulse shaping choppers just outside the target monolith has to be limited. Therefore an eye-of-the-needle approach, where the beam is focused between these two choppers is taken.
A second focal spot of the guide at 50 m from the moderator followed by an up to 10 m long flight path in front of the detector position defines the imaging geometry, achieving the maximum desired Field of View (FOV). Additionally, the instrument takes advantage of the bi-spectral extraction opportunity at ESS in order to use the full available bandwidth ranging from 1Å (e.g. Bragg edge strain mapping to well above 10Å. See  and references therein for a more detailed description of the design rationale.
 M. Strobl: The Scope of the Imaging Instrument Project ODIN at ESS, Physics Procedia 69, p 18, 2015
The performance of an imaging instrument depends on flux, beam size, divergence and homogeneity. The available wavelength resolution is an additional important performance criterion for ToF based imaging. We expect ODIN to outperform current state of the art beamlines.
The anticipated flux at ODIN’s sample position will be about 1.2´109 n/s/cm2 (at 2 MW), this is three times higher than at current steady state sources and it outperforms other pulsed sources even when conditioning the beam for high wavelength resolution as shown in Fig above.
The neutron beam profile at the sample position will be homogeneous over the full FoV. A collimator wheel will enable variable collimation up to L/D=10,000, which is unprecedented.
The anticipated wavelength resolution of about 0.3% is ambitious but achievable due to the complex chopper system. Currently steady state sources offer about 10% resolution while Imaging Beamlines at SNS and JPARC anticipate about 0.5-1%.
With its high flux, high beam quality and high wavelength resolution ODIN has the potential of setting the state of the art in imaging when coming online. This will require a steady monitoring and development of all experiment components; this is, however, an easy task given the collaborative nature of the neutron imaging community of which the ODIN team is an active part.
- Elbio Calzada
Technische Universität München
- Aureliano Tartaglione
Lead Scientist/Programme Manager
Technische Universität München
- Manuel Morgano
Paul Scherrer Institute
- Virginia Martinez Monge
Installation Package Leader
Technische Universität München
Kardjilov, N., Manke, I., Woracek, R., Hilger, A., Banhart, J. Advances in neutron imaging. Materials Today (2018).
Woracek, R., Santisteban, J., Fedrigo, A., & Strobl, M. Diffraction in neutron imaging — A Review. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment (2018), 878, 141-158.
M. Strobl et al.: Quantitative Neutron Dark-field Imaging through Spin-Echo Interferometry, Scientific Reports, 5, 16576 (2015)
M. Strobl: The Scope of the Imaging Instrument Project ODIN at ESS, Physics Procedia 69, p 18, 2015
M. Strobl, F. Grazzi: From Scattering in Imaging to Prospects at Pulsed Sources, Neutron News (2015) 26:2, 23-26, DOI: 10.1080/10448632.2015.1028275
N. Kardjilov et al.: Neutron Imaging in Materials Science, Materials Today, 14 (6), p 248, 2011