Dielectric Measurements
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the High B/T Facility for experiments at fields up to 15 tesla and at temperatures down to 0.4 mK
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
Dilatometry
A capacitive dilatometer measures a change of sample dimension by monitoring the capacitance between two parallel plates.
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
Phase transitions that produce small length changes (even on the order of nanometers) due to thermal expansion or magnetostriction can be resolved by making contact between the tip of a miniature piezo-resistive cantilever and a sample.
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
Electrical Transport
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the High B/T Facility for experiments at fields up to 15 tesla and at temperatures down to 0.4 mK
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
The user can place small samples into an inductor (i.e., coil) of an LC tank circuit oscillating at a resonant frequency.
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
Electron Magnetic Resonance
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the EMR Facility
Visit the EMR Facility for details on the below techniques.
- Cyclotron Resonance
- Electrically Detected Magnetic Resonance (EDMR)
- Electron-Nuclear Double Resonance (ENDOR)
- Ferromagnetic and Antiferromagnetic Resonance (FMR / AFMR)
- Far-Infrared Magnetospectroscopy (FIRMS)
- High Pressure EPR
- Liquid Overhauser Dynamic Nuclear Polarization (including pulsed)
- Pulsed Electron-Electron Double Resonance (PELDOR)
- Pulsed ESR/EPR
High Pressure
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
Ion Cyclotron Resonance
The ICR Facility offers various techniques and instruments for biological, environmental and petrochemical applications.
Magnetic Measurements
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the High B/T Facility for experiments at fields up to 15 tesla and at temperatures down to 0.4 mK
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
Magneto-optics
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
Microwaves
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
NMR-MRI/S
Numerous kinds of Magnetic Resonance Imaging capabilities are available at our NMR-MRI/S facilities, including those listed below.
- Dissolution Dynamic Nuclear Polarization
- Quadrupolar - Low Gamma MRI
- In Vivo MRI
- Energy & Materials MRI
- MR Spectroscopy
- Multinuclear (H and X-nuclei) MRS
Numerous kinds of solid state capabilities are available at our NMR-MRI/S facilities, including those listed below. For more information, visit the Solid State NMR page.
Numerous kinds of solution state capabilities are available at our NMR-MRI/S facilities, including those listed below. For more information, visit the Solution State NMR page.
- At the NMR-MRI/S facilities
- At the NMR-MRI/S facilities
- Low-temperature Condensed Matter NMR at the DC Field Facility for experiments at fields up to 55 tesla
- Ultra Low-temperature NMR and NQR at the High B/T Facility for experiments at fields up to 15 tesla and at temperatures down to 0.4 mK
Thermal Measurements
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
At the Pulsed Field Facility for experiments at pulsed fields up to 100 tesla
Thermometry
Several kinds of thermometry, including capacitance, mMelting curve, vibrating wire and Pt NMR thermometry, are all available at High B/T Facility for experiments at fields up to 15 tesla and at temperatures down to 0.4 mK.
- Capacitance Thermometry
- Melting Curve Thermometry
- Platinum NMR Thermometry
- Vibrating Wire Thermometry
Ultrasound
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the High B/T Facility for experiments at fields up to 15 tesla and at temperatures down to 0.4 mK
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the DC Field Facility for experiments at continuous fields up to 45 tesla
- At the High B/T Facility for experiments at fields up to 15 tesla and at temperatures down to 0.4 mK
X-ray diffractometry
- At the DC Field Facility for experiments at continuous fields up to 25 tesla.