Instrument List
Detail of instruments by group
Diffraction
Technique: Powder diffraction
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| D7 | Diffuse scattering spectrometer |
|
Powder diffraction | Magnetism and quantum materialsChemistry of materials |
| D4 | Disordered materials diffractometer |
|
Powder diffraction | EnergyEnvironmentSoft matter and polymers |
| D2B | High-resolution two-axis diffractometer |
|
Powder diffraction | Magnetism and quantum materialsChemistry of materialsEngineeringEnergy |
| D20 | High intensity two-axis diffractometer with variable resolution |
|
Powder diffraction | Magnetism and quantum materialsChemistry of materialsEnergy |
| D1B | Two-axis diffractometer |
|
Powder diffraction | Magnetism and quantum materialsChemistry of materialsEngineeringReactions and catalysis |
Technique: Single crystal diffraction
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| D3 | Spin polarised hot neutron diffractometer |
|
Single crystal diffraction | Magnetism and quantum materialsChemistry of materials |
| D23 | Thermal neutron two-axis diffractometer for single-crystals D23 |
|
Single crystal diffraction | Magnetism and quantum materials |
| OrientExpress | Laue-neutron diffractometer |
|
Single crystal diffraction | |
| D9 | Hot neutron 4-circle diffractometer |
|
Single crystal diffraction | Magnetism and quantum materialsChemistry of materials |
| D10 | 4-circle diffractometer with three-axis energy analysis |
|
Single crystal diffraction | Magnetism and quantum materialsChemistry of materials |
Large-Scale Structure
Technique: Powder diffraction
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| D16 | Small momentum transfer diffractometer |
|
Powder diffractionSmall angle neutron scattering SANS | EnergyEnvironmentSoft matter and polymersLife sciencesHealth |
Technique: Single crystal diffraction
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| DALI | Quasi-laue diffractometer |
|
Single crystal diffraction | Life sciencesHealth |
Technique: Small angle neutron scattering SANS
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| D11 | Lowest momentum transfer & lowest background small-angle neutron scattering (SANS) |
|
Small angle neutron scattering SANS | EnvironmentSoft matter and polymersLife sciencesHealth |
| D22 | Large dynamic range small-angle diffractometer |
|
Small angle neutron scattering SANS | EnvironmentSoft matter and polymersLife sciencesHealth |
| D33 | Massive dynamic q-range small angle diffractometer |
|
Small angle neutron scattering SANS | Magnetism and quantum materialsEnvironmentSoft matter and polymersLife sciencesHealth |
| D16 | Small momentum transfer diffractometer |
|
Powder diffractionSmall angle neutron scattering SANS | EnergyEnvironmentSoft matter and polymersLife sciencesHealth |
| SAM | Small-angle diffractometer |
|
Small angle neutron scattering SANS | Magnetism and quantum materialsChemistry of materialsSoft matter and polymersLife sciences |
Technique: Reflectometry
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| FIGARO | Fluid Interfaces Grazing Angles Reflectometer |
|
Reflectometry | EnvironmentSoft matter and polymersLife sciencesHealth |
| D17 | Neutron reflectometer with horizontal scattering geometry |
|
Reflectometry | EnvironmentSoft matter and polymersLife sciencesHealth |
| SuperADAM | Advanced reflectometer for the analysis of materials |
|
Reflectometry | Soft matter and polymersLife sciencesHealth |
Spectroscopy
Technique: Time of flight spectrometry
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| PANTHER | Thermal neutron time-of-flight spectrometer |
|
Time of flight spectrometry | Magnetism and quantum materialsEnergy |
| IN5 | Disk chopper time-of-flight spectrometer |
|
Time of flight spectrometry | Magnetism and quantum materialsChemistry of materialsEnergyEnvironmentHealth |
| SHARPER | Cold neutron time-focussing TOF spectrometer |
|
Time of flight spectrometry | Magnetism and quantum materialsEnergyEnvironmentSoft matter and polymers |
Technique: 3 axes spectrometry
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| IN8 | High-flux thermal 3-axis spectrometer |
|
3 axes spectrometry | Magnetism and quantum materials |
| IN20 | Thermal 3-axis spectrometer with polarisation analysis |
|
3 axes spectrometry | Magnetism and quantum materials |
| IN12 | Cold 3-axis spectrometer |
|
3 axes spectrometry | Magnetism and quantum materials |
| IN22 | Thermal 3-axis spectrometer with polarisation analysis |
|
3 axes spectrometry | Magnetism and quantum materials |
| ThALES | Cold Triple-Axes Spectrometer with polarisation option |
|
3 axes spectrometry | Magnetism and quantum materials |
Technique: Spectrometry backscattering
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| IN16B | High flux cold neutron backscattering HR spectrometer |
|
Spectrometry backscattering | Magnetism and quantum materialsEnergyEnvironmentLife sciencesHealth |
| IN13 | Thermal neutron backscattering spectrometer |
|
Spectrometry backscattering | Soft matter and polymersLife sciencesHealth |
Technique: Spin echo scattering
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| IN15 | Spin-echo spectrometer with time-of-flight and focusing options |
|
Spin echo scattering | Magnetism and quantum materialsSoft matter and polymersLife sciencesHealth |
| WASP | High-intensity spin-echo spectrometer |
|
Spin echo scattering | EnergyEnvironmentLife sciencesHealth |
Applied Science
Technique: Tomography
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| MoTo | Monochromatic Tomography |
|
Tomography | Chemistry of materialsReactions and catalysisEnergyEnvironmentLife sciences |
| NeXT | Neutron and X-ray Tomography instrument |
|
TomographyRadiography | EngineeringEnergyEnvironment |
Technique: Micro tomography
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| PorTo | Cold Neutron Tomography |
|
Micro tomographyRadiography | Chemistry of materialsReactions and catalysisEnergyEnvironment |
Technique: Radiography
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| PorTo | Cold Neutron Tomography |
|
Micro tomographyRadiography | Chemistry of materialsReactions and catalysisEnergyEnvironment |
| NeXT | Neutron and X-ray Tomography instrument |
|
TomographyRadiography | EngineeringEnergyEnvironment |
Technique: Strain stress scanning
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| Salsa | Strain Imager for Engineering Applications |
|
Strain stress scanning | Engineering |
Technique: Neutron Irradiation
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| TENIS | Thermal and Epi-thermal Neutron irradiation Station | Thermal neutron irradiation of electronic devices |
Neutron Irradiation | Engineering |
Nuclear & Particle Physics
Technique: NPP facility
| Name | Instrument type | Application | Technique | Science domain |
|---|---|---|---|---|
| S18 | Thermal neutron interferometer | The CRG instrument S18 is a perfect crystal neutron interferometer which can also be configured as a high resolution Bonse Hart camera. This instrument can be used for precise measurement of neutron scattering lengths and for basic neutron quantum optics studies and related phenomena. Applications: neutron interferometry, measurement of basic quantum physics laws; measurement of neutron-nuclei scattering lengths; quantum contextuality; decoherence; dephasing and depolarisation experiments; experiments with non-classical neutron states. |
NPP facility | |
| PN1 | Fission product spectrometer (Lohengrin) | The main directions of research on PN1 were in the past centered around studies of the fission process but are now more and more concentrated on spectroscopy of very neutron rich nuclei. To this purpose two Germanium Clover detectors and ancillary detectors were purchased in the M0 phase of the Millenium project. The recoil mass separator for unslowed fission products LOHENGRIN uses fission products originating from a source of fissile isotopes placed in a beam tube (H9) near the core of the reactor. Specific fission products are selected by a combination of a magnetic and an electric sector field whose deflections are perpendicular to each other. The freely recoiling fission products are analyzed according to their energy over ionic charge (E/q) and mass over ionic charge (A/q) ratios. |
NPP facility | |
| PF2 | Ultracold neutron beam facility | The ultracold neutron facility PF2 was built by TU Munich in collaboration with ILL. It provides a density of 50 cm^-3 of ultracold neutrons (UCN) with speeds less than 6 m/s. UCN are produced at the top end of a vertical guide where neutrons with speeds of 50 m/s are converted by the so-called Steyerl turbine into UCN. The UCN are then led by horizontal guides to several experiments in parallel. There is also an output for very cold neutrons (VCN) with a wavelength of 100Å. The fact that neutron are electrically neutral makes it possible to store UCN in traps. The majority of the measurements carried out at PF2 use this feature. Recent experiments concerned - amongst others - the measurement of the neutron lifetime, the measurement of the neutron electric dipole moment and the study of "anomalous losses" of stored neutrons. |
NPP facility | |
| Ricochet | None | RICOCHET is an international collaboration aiming to explore the Coherent Elastic Neutrino-Nucleus Scattering (CeνNS), a long-predicted interaction that was observed experimentally only in 2017. A precise measurement of the nuclear recoil spectrum for reactor neutrinos, where the process is fully coherent, could reveal deviations from the Standard Model of particle physics, potentially unlocking the door to new physics. The RICOCHET experiment is installed at the ILL only 8.8 meters away from the core of the High Flux Reactor. This proximity provides an intense neutrino flux of approximately 10¹² neutrinos/cm²/s, ideal for studying CEνNS at low (sub-keV) recoil energies. |
NPP facility | |
| FIPPS | Gamma-ray spectrometer for thermal neutron induced reactions | FIPPS is ILL's gamma-ray spectrometer for thermal-neutron-induced reactions. It is composed of a highly collimated halo-free pencil neutron beam impinging on a stable or radioactive target surrounded by a high resolution high-purity germanium detectors array. It is used for: studies of the fission process of heavy elements and of the structures of neutron rich matter; level densities as input for astrophysical calculations; search for doorway states for populations of long-lived isomers with medical applications by photo-excitation; precise knowledge of fission yields and decays of fission products; development of future nuclear reactors, fuel breeding schemes and nuclear waste transmutation. |
NPP facility | |
| SuperSUN | Super Ultracold Neutron Source | The ultracold neutron source SuperSUN is a density type, superthermal source using isotopically pure 4He at 0.6K as a convertor. The incoming cold neutron beam has a capture flux of about 1010 neutron/cm2^2/ s which is transformed into 3.8 × 106 UCN measured at a reactor power of 48.6 MW at saturation. The instrument is used to address key questions of particle physics at the low-energy, high-precision frontier, complementary to experiments done at high-energy particle accelerators |
NPP facility | |
| PF1B | Polarised cold neutron beam facility | Installed at the end position of the cold ballistic supermirror guide H113, PF1B provides the strongest polarised and unpolarised cold neutron beam in the world currently available for particle and nuclear physics (2x10^10 neutrons/(cm^2.s); the guide cross section is 6x20 cm^2). |
NPP facility |