MLZ is a cooperation between:

Technische Universität München> Technische Universität MünchenHelmholtz-Zentrum Hereon> Helmholtz-Zentrum Hereon
Forschungszentrum Jülich> Forschungszentrum Jülich

MLZ is a member of:

LENS> LENSERF-AISBL> ERF-AISBL

MLZ on social media:

Logo

MLZ (eng)

Lichtenbergstr.1
85748 Garching

PANDA

Cold three axes spectrometer

This instrument is focussed on cold neutrons. Therefore, please carefully check the “Technical data WITHOUT cold source” section. Deviating parameters are in bold. The instrument team is happy to answer any further questions!

Instrumentscheme PANDA Instrumentscheme PANDA

The cold three axes spectrometer (TAS) PANDA is located at the beam tube SR-2. With a neutron guide element in the beam tube, a short distance from the neutron source to the monochromator, and double-focussing monochromators and analysers, a high neutron flux is achieved. Furthermore the instrument is optimised for a low background. The multi-detector option BAMBUS, providing 100 q-ΔE-channels simultaneously, is currently under commissioning.

Next to the normal properties of a cold TAS, the range of possible energy transfers overlaps with a thermal three axes spectrometer. Specifically for thermal neutrons, a double focussing Cu-111 monochromator and a Si-111 monochromator (vertically fixed, horizontal adjustable focus) are available. Set-ups with high Q-resolution or polarised neutrons are also possible. The sample environment is up to date and offers high magnetic fields and low temperatures.

The conducted experiments comprise e.g. the investigation of spin waves, crystal field excitations, phonons, excitations of low dimensional systems, quasielastic scattering and diffraction with energy resolution. The achieved results often contributed decisively to the exploration of unconventional superconductivity, magnetically frustrated systems and magnetism in low-dimensional systems. Furthermore, they deliver new insights in the research of lattice dynamics or material sciences.

Typical applications
Magnetic properties
  • Spin-waves, magnetic excitations in frustrated, topological und low-dimensional systems
  • Crystal field excitations
  • Excitations in low-dimensional systems
  • Magnetic vs nuclear scattering
Lattice dynamics
  • Phonon dispersion
  • Magneto-elastic coupling
  • Polarisations vectors
General
  • Critical scattering at phase transitions
  • Magnon – phonon interaction
  • Soft mode
  • Central peak
  • Diffraction with analyser:
    • dE close to 0
    • High E & Q resolution
    • Extremely low background
Sample environment

The sample table of PANDA allows for a variety of sample environments and may easily be adapted to user-specific devices.

Among others, PANDA offers routinely operated sample environment for:
  • Available temperature range: 50 mK (dilution insert, see below) up to more than 1300 K (high-temperature furnace)
  • Maximal vertical magnetic field: 12 T
  • Available cryostats:
    • Closed cycle cryostat: 3.5 K < T < 300 K
    • 3He insert: 450 mK < T < 300 K
    • Dilution insert: 50 mK < T < 6 K
    • ADR-cryostat: 300 mK < T < 300 K
Technical data WITHOUT cold source
Monochromators
  • PG(002) (d = 3.355 Å)
    • 1.5 Å-1 < ki < 4.0 Å-1
    • Variable horizontal and vertical focussing
  • Cu111 (d = 2.08 Å)
    • 1.8 Å-1 < ki < 7 Å-1
    • Variable horizontal and vertical focussing
  • Si111 (d = 3.13 Å)
    • 1.5 Å-1 < ki < 5 Å-1
    • Fixed vertical and variable horizontal focussing
  • Heusler (d = 3.35 Å, polarised neutrons)
    • 1.5 Å-1 < ki < 4.0 Å-1
    • Variable vertical focussing
Analysers
  • PG(002)
    • -130° < 2ΘA < 100°
    • 1.05 Å-1 < kf
    • Variable horizontal focussing
  • Heusler (polarised neutrons)
    • -130° < 2ΘA < 100°
    • 1.05 Å-1 < kf
    • Variable horizontal focussing
Detectors
  • 1” ³He tube (focussing mode)
  • 2” ³He tube (collimated mode))
Main parameters
  • Scattering angle at the sample: 5°< 2ΘS < 125° (moveable beam-stop)
  • Energy transfer: up to 35 meV (depending on ki)
  • Momentum transfers: up to Q = 7 Å-1 (depending on ki)
Filters for higher-order suppression
  • PG (l = 60 mm): kf = 2.57 Å-1 or 2.662 Å-1
  • Be (closed-cycle cryostat, T ≤ 45 K): kf ≤ 1.55 Å-1
  • BeO (liq.-N2 cooled): kf ≤ 1.33 Å-1
Technical data WITH cold source
Monochromators
  • PG(002) (d = 3.355 Å)
    • 1.05 Å-1 < ki < 4.0 Å-1
    • Variable horizontal and vertical focussing
  • Cu111 (d = 2.08 Å)
    • 1.8 Å-1 < ki < 7 Å-1
    • Variable horizontal and vertical focussing
  • Si111 (d = 3.13 Å)
    • 1.2 Å-1 < ki < 5 Å-1
    • Fixed vertical and variable horizontal focussing
  • Heusler (d = 3.35 Å, polarised neutrons)
    • 1.1 Å-1 < ki < 4.0 Å-1
    • Variable vertical focussing
Analysers
  • PG(002)
    • -130° < 2ΘA < 100°
    • 1.05 Å-1< kf
    • Variable horizontal focussing
  • Heusler (polarised neutrons)
    • -130° < 2ΘA < 100°
    • 1.05 Å-1 < kf
    • Variable horizontal focussing
Detectors
  • 1” ³He tube (focussing mode)
  • 2” ³He tube (collimated mode)
Main parameters
  • Scattering angle at the sample: 5°< 2ΘS < 125° (moveable beam-stop)
  • Energy transfer: up to 18 meV (depending on ki)
  • Momentum transfers : up to Q = 7 Å-1 (depending on ki)
Filters for higher-order suppression
  • PG (l = 60 mm): kf = 2.57 Å-1 or 2.662 Å-1
  • Be (closed-cycle cryostat, T ≤ 45 K): kf ≤ 1.55 Å-1
  • BeO (liq.-N2 cooled): kf ≤ 1.33 Å-1

Instrument scientist

Dr. Astrid Schneidewind
Phone: +49 (0)89 158860-749
E-mail: a.schneidewind@fz-juelich.de

Dr. Lukas Beddrich
Telefon: +49 (0)89 158860-769
E-Mail: l.beddrich@fz-juelich.de

PANDA
Phone: +49 (0)89 158860-517

Operated by

JCNS

Funding

Publications

Find the latest publications regarding PANDA in our publication database iMPULSE:

impulse.mlz-garching.de

Citation of the instrument

Heinz Maier-Leibnitz Zentrum. (2015). PANDA: Cold three axes spectrometer. Journal of large-scale research facilities, 1, A12. http://dx.doi.org/10.17815/jlsrf-1-35

For citation please always include the DOI.

Instrument control

Gallery

PANDA
PANDA
© W. Schürmann, TUM
Q-E_range_full
Q-E_range_full

Summary of the Q-E-range of PANDA in different set-ups. Geometric constraints due to the sample environment are not included. If you would like more information, please contact the instrument scientists.

© MLZ
Q-E_range_full_Cu-PG thermal
Q-E_range_full_Cu-PG thermal

Copper monochromator and pyrolytic graphite (PG) analyser configuration. Without the FRM II’s cold source, the thermal spectrum makes larger energy transfers accessible.

© MLZ
Q-E_range_full_PG-PG thermal
Q-E_range_full_PG-PG thermal

PG monochromator and analyser set-up assuming a PG filter on the secondary spectrometer side for thermal spectrum.

© MLZ
Q-E_range_full_PG-PG cold-polarised
Q-E_range_full_PG-PG cold-polarised

PG monochromator and analyser set-up with Be-filter on kf, which has been the standard set-up for the cold spectrum at the NL2 beam tube. Polarised set-up with a Heusler monochromator and analyzer achieves a similar Q-E range.

© MLZ
Q-E_range_full_PG-PG high reso
Q-E_range_full_PG-PG high reso

Low background and high resolution option utilising Be-filter on ki and BeO-filter on kf.

© MLZ

MLZ is a cooperation between:

Technische Universität München> Technische Universität MünchenHelmholtz-Zentrum Hereon> Helmholtz-Zentrum Hereon
Forschungszentrum Jülich> Forschungszentrum Jülich

MLZ is a member of:

LENS> LENSERF-AISBL> ERF-AISBL

MLZ on social media: