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SHARPER

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

Guide hall n°1, cold guide H15

λ6 to 1.5 (Å)
Incoming energy Ei2.2 to 36.4 (meV)
energy resolution ΔE0.055 to 3.0 (meV)
Energy resolution ΔE / Ei2.5 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 105 cm-2 s-1

Fermi chopper speed

600 - 24000 rpm

Detectors

337 elliptical 3He detectors

sample-to-detector distance

250 cm

angular range

0 to 145°

Horizontal detector angles0 to 140°

vertical detection angles

-22 to 22°

sensitive area

11 m2

total background

2 Hz

Sample environment
 characteristicsStick lengthMonte-et-baisse positionSample holder
cryostat1.5 ... 310 K925623Ø70  M8

cryofurnace

2.5 ... 600 K925580

Ø70  M8

cryoloop N2

100 ... 620 Kfixed623

round slab

cryoloop He (cold finger)

30 ... 620Kfixed625

M8

furnace I

300 ... 1000 K400≥ 625

Ø69  M8

furnace II

300 ... 1500 K400649 (≥ 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 – Eicorresponds 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.