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IN11

Spin-Echo Spectrometer IN11

Guide hall n°1, cold guide H141

Incident wavelength

    3.8 ... 12 Å

Beam profile

Incident beam divergence

15 mrad

Beam diameter

45 mm

Resolution

Velocity selector

Δλ/λ = 15 ... 22 %

TAS configuration (option IN11A)

Δλ/λ = 1.5 ... 6 %

Main precession solenoids

Maximum B field

0.15 T

Length

2 m

Field integral

0.27 Tm

Transmission polarizers

Polarizer

FeAg supermirrors

Analyser

CoTi supermirrors

2D multidetector (option IN11A)

Area

15 x 15 cm2

Pixel size

5 x 5 mm2

Detector solid angle

0.9° x 0.9°

Angular range

2° ... 120°

Fourier time range

0.03 ... 50 ns (10 Å)

 

0.002 ... 3 ns (4 Å)

Energy range

1.3x10-5 ... 0.01 meV (10 Å)

 

2x10-4 ... 0.15 meV (4 Å)

Momentum transfer range

0.03 ... 2.7 Å-1 (4 Å)

 

0.02 ... 1.35 Å-1 (8 Å)

Large angle detector (option IN11C)

Detector solid angle

30° x 1.5°

Angular range

5° ... 115°

Fourier time range

0.03 ... 12 ns (10 Å)

 

0.002 ... 0.5 ns (4 Å)

Instrument Description

In a spin-echo experiment very high energy resolution is achieved by encoding the neutron energy into a Larmor precession angle: Polarized neutrons are sent through two anti-parallel magnetic fields before and after scattering from the sample. The precession angles in the two fields are equal and opposite, so that for elastic scattering full polarization is recovered, irrespective of the initial neutron velocity distribution. Small energy transfers lead to a change in the precession angle of the outgoing beam and, hence, to a decrease in the measured polarization. The intermediate scattering function S(Q,t)/S(Q,0) is directly determined by scanning the magnetic fields in the coils and measuring the polarization.

Two detector options are available for high Q/energy resolution and high signal, respectively. Option IN11A is a 2-dimensional multidetector with a pixel size of 5x5 mm2. Option IN11C with 41 detectors distributed over an angle of 30deg offers a count rate superior by a factor of 20 with the trade off of a lower energy resolution.

A polarization of 99% is created by supermirrors. They polarize and analyse the beam parallel to the beam direction. The polarization direction is turned perpendicular to the precession fields H0 and H1 in the solenoids by two pi/2-flipper coils. An additional pi-flipper coil allows keeping the fields H0 and H1 parallel resulting in higher polarization at small scattering angles.

The sample stage takes all ILL standard sample environments including orange cryostats, cryo-furnaces and 3He cryostats. A non-magnetic high temperature oven (300...780 K) is also available at IN11.