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SHARPER CRG - Cold neutron time-focussing time-of-flight spectrometer

Characteristics

Guide hall n°1, cold guide H15
λ 6 to 1.5 (Å)
Incoming energy Ei 2.2 to 36.4 (meV)
energy resolution ΔE 0.055 to 3.0 (meV)
Energy resolution ΔE / Ei 2.5 to 15.0%
Max energy transfer in % of Ei 45%
Qmin (A-1) 0.4/λ
Qmax (A-1) 11.8/λ
Monochromator
composite, vertically focussing pyrolitic graphite crystals
Incident wavelength from 2 to 6  Å
Sample
max energy loss of neutrons 20 meV
max energy gain of neutrons 200 meV
max momentum transfer 5.9 Å-1
vertical divergence -22 to 22°
beam size at the sample 3 x 5 cm2
flux at the sample at 5 Å 8.0 x 105cm-2s-1
Fermi chopper speed 600 - 24000 rpm
Detectors
337 elliptical3He detectors
sample-to-detector distance 250 cm
angular range 0 to 145°
Horizontal detector angles 0 to 140°
vertical detection angles -22 to 22°
sensitive area 11 m2
total background 2 Hz
Sample environment
characteristics Stick length Monte-et-baisse position Sample holder
cryostat 1.5 ... 310 K 925 623 Ø70  M8
cryofurnace 2.5 ... 600 K 925 580 Ø70  M8
cryoloop N2 100 ... 620 K fixed 623 round slab
cryoloop He (cold finger) 30 ... 620K fixed 625 M8
furnace I 300 ... 1000 K 400 ≥ 625 Ø69  M8
furnace II 300 ... 1500 K 400 649 (≥ 625) Ø49  M8

Instrument description

Located in ILL7 on branch H153 of the cold neutron guide H15, SHARPER is an inelastic spectrometer using the time-of-flight technique. The instrument is designed to access dynamic modes in condensed matter by measuring the energy exchange between a monochromatic neutron beam and the sample.

From the continuous, "white" beam delivered by the H15 neutron guide, a specific wavelength (and thus incident energy, Ei) is selected via Bragg reflection on a monochromator. A Fermi chopper pulses this monochromatic beam, setting the time t0 of its interaction with the sample. A timer then measures the time t taken by the scattered beam to reach detectors positioned a known distance d from the sample. The velocity v = d / (t - t0) of the neutrons provides a direct measure (Ef = 1/2·m·v2) of the scattered beam's energy. The energy transfer Ef – Ei corresponds to the energy of a dynamic mode within the sample.

A set of three disk choppers located upstream of the monochromator eliminates harmonics (integer sub-multiples) of the chosen incident wavelength that may not be fully filtered by the monochromator.

A retractable guide between this disk chopper system and the monochromator allows switching between "time focusing" (TF, guide retracted) and monochromatic mode (MM, guide in the beam). The TF mode enhances energy resolution within a narrow energy transfer region while maintaining high flux. The MM mode provides constant resolution over a broader energy transfer range but at the expense of flux reduction.