PSI µSR User Facilities : Instruments
GPS - General Purpose Surface-Muon Instrument
(350kB GIF)
The
GPS Instrument
is the "workhorse" of the Facilities. It is permanently installed in
area piM3, using a so-called "surface-muon beam" (i.e., positive muons
originating from the decay of positive pions stopped near the surface
of the production target). The typical range of these muons is about
1.5mm in polyethylene.
The
piM3 beamline
is equipped with an electromagnetic separator / spin rotator allowing
to choose spin directions ranging from almost parallel to perpendicular
to the muon momentum.
The instrument is designed for zero- (ZF), longitudinal- (LF),
and transverse-field (TF) µSR experiments in wide ranges of temperature
and external magnetic field. A special detector arrangement
allows to investigate very small samples. Sample rotation is provided for
the study of orientation-dependent effects in single crystals.
Since August 1995, the GPS Instrument can be used simultaneously with
the Low Temperature Facility
(LTF) Instrument
either by switching the beam at fixed time-intervals from one area
to the other by means of an electrostatic deflector ("kicker") and
septum magnet or by splitting the beam continuously by widening
the spot in front of the collimators located at the entrance to the
septum magnet.
Since 1998, it is also possible to share the beam
by triggering the deflector on request of one of the Instruments
(Muons On REquest, MORE).
Instrument Scientist:
Alex Amato, E-mail:
alex.amato@psi.ch
Co-responsible Person:
Hubertus Luetkens, E-mail:
hubertus.luetkens@psi.ch
LTF - Low Temperature Facility
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(305kB GIF)
The LTF Instrument is
based on a Oxford Instruments He-3/He-4 dilution
refrigerator reaching a base temperature of 10mK. It shares the
piM3 surface-muon
beam with the
GPS Instrument
(see above).
Similar to GPS, LTF is designed for zero-, longitudinal-, and transverse-field
experiments, but the field range is a factor of 5 larger than in GPS due to
a built-in superconducting magnet.
Instrument Scientist:
Christopher Baines, E-mail:
chris.baines@psi.ch
DOLLY - Relocatable Surface-Muon Instrument
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(30K JPEG)
DOLLY
is a copy (with few modifications) of the
GPS Instrument.
In contrast to GPS or
LTF, it is
not permanently installed in a dedicated area but may be set up in either
piE1 or
piE3,
using - like GPS and LTF - so-called "surface-muons" (i.e., 4.2MeV positive
muons originating from the decay of positive pions stopped near the surface
of the production target). The typical range of these muons is about 1.5mm
in polyethylene.
For the use of DOLLY in piE1 or piE3, some additional beam-line elements
have to be installed in these areas: an electromagnetic separator or spin
rotator (the latter not being available yet) and additional quadrupole lenses.
With the existing separator, only longitudinal polarisation
of the muons is available.
The design of the instrument is almost identical with that of the GPS,
allowing for zero- (ZF), longitudinal- (LF), and transverse-field (TF)
µSR experiments in wide ranges of temperature (2-300K) and external
magnetic field (LF 0-0.5T, TF 0-15mT). The detector
arrangement with veto-detectors in both forward and backward
directions allows to investigate very small samples. Sample rotation is
foreseen for the study of orientation-dependent effects in single crystals.
Instrument Scientists:
Robert Scheuermann, E-mail:
robert.scheuermann@psi.ch
Co-responsible Person:
Alexey Stoykov, E-mail:
alexey.stoykov@psi.ch
GPD - General Purpose Decay-Channel Instrument
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(52kB JPEG)
The GPD Instrument
is designed for the use of higher
energy (positive or negative) muons from the decay of pions in flight
(area µE1) having
ranges up to 130mm in polyethylene.
Zero-, longitudinal-, and transverse-field experiments are possible
in similar field ranges as with GPS. The available temperature range
extends to somewhat lower temperatures than in GPS when a He-3 evaporation
cryostat is used. Some of the cryostats allow sample rotation.
The use of GPD is recommended when big samples are available and is
mandatory for samples which have to be sealed in containers.
Instrument Scientist:
Ulrich Zimmermann , E-mail:
ulrich.zimmermann@psi.ch
Co-responsible Person:
Rustem Khasanov, E-mail:
rustem.khasanov@psi.ch
ALC - Avoided Level Crossing Spectrometer
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(350kB GIF)
The ALC Instrument is
designed for integral
forward-backward decay asymmetry measurements in longitudinal magnetic
fields up to 5T, making use of the full available muon intensities.
As a rule, the instrument will be set up in area
piE3
for the use of surface muons coming from Target E.
Instrument Scientist:
Alexey Stoykov, E-mail:
alexey.stoykov@psi.ch
Co-responsible Person:
Robert Scheuermann, E-mail:
robert.scheuermann@psi.ch
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