|
|
HB-3 Fact sheet (pdf) |
Beam Spectrum: |
|
Thermal |
Monochromators: |
|
Unpolarized
PG(002), Be(101) |
Analyzer: |
|
PG(002) |
Monochromator
angle: |
|
1288° |
Sample
angle: |
|
-60-120° |
Scattering
angle: |
|
up
to 115° |
Analyzer
angle: |
|
-120120° |
Collimations
(FWHM): |
|
Pre-monochromator: 0.25, 0.5, 0.8° |
|
|
Pre-sample:
0.333, 0.666, 1° |
|
|
Pre-analyzer:
0.333, 0.666, 1, 1.333° |
|
|
Pre-detector:
2, 4°
|
|
|
The triple-axis spectrometer
is one of the most versatile instruments for measuring excitations in
solids via neutron scattering. HB-3 is a colossal flux thermal neutron
three-axis spectrometer designed for inelastic measurements on single
crystals over a wide range of energy and momentum transfers. While the
energy and momentum range for measurements is quite large at HB-3, the
instrument is the ideal location to perform experiments at high energy
transfers. This is due to a combination of its location directly at
the end of the beam tube and the availability of a beryllium monochromator.
Examples of experiments which would be performed on the HB-3 triple-axis
spectrometer (in preference to other HFIR triple-axis spectrometers)
are excitations at high energies such as phonons in high-temperature
cuprates and magnons in iron and nickel.A wide range of sample environments,
including closed-cycle helium (Displex) refrigerators, 4He cryostats
(with dilution option), cryomagnets, and furnaces can be accommodated
on HB-3.
In
the current installation, the HB-3 triple-axis spectrometer has a fixed-focus
PG002 monochromator optimized at 20 meV. In the near future, the monchromator
will be upgraded to provide three crystal choices (PG 002, Be 002, and
Si 111) with continuously variable focusing. The variable focusing will
be calibrated to maintain the smallest beam size at the sample position,
thus optimizing the incident neutron flux at each energy.
Pyrolitic graphite
provides the highest neutron intensity because it has a high neutron reflectivity.
The high-quality beryllium monochromator will allow measurements with
good energy resolution while relaxing the q-resolution. Silicon 111 crystals
have the advantage that there is no second-order reflection, thus providing
a higher order contamination-free beam. The availability of these three
monochromator crystal choices will make the spectrometer extremely versatile
for a wide range of studies of the properties of materials.
The in-pile
collimation can be reduced from its intrinsic value of 48' to a
user-selectable value of 30' or 15' at the push of a button
via the shutter control panel. This spectrometer also provides an in-pile
sapphire filter for the white beam before the monochromator. Söller
collimators from the monochromator-sample,
the sample-analyzer, and the analyzer-detector can be changed as required
by the user. With the upgraded HFIR beam tubes, the beam diameter of the
effective source that illuminates the monochromator is 4.625 in. |