|
| 1. Instrument |
4 Dimensional Space Access Neutron Spectrometer (4SEASONS) |
| 2. Overview of instrument |
The spectrometer aims at clarification of novel phenomena in high-Tc superconductors
and related materials by investigation of spin and lattice dynamics over
4D momentum and energy space with high efficiency. |
| 3. Contact person |
Ryoichi Kajimoto (CROSS) |
| 4. Sub-contact person |
Mitsutaka Nakamura (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL01 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Incident neutron energy |
5 < Ei < 300 meV |
| @5.4@Detection angle |
Horizontal : -35 - 55, Vertical : -25 - 27 |
| @5.5@Resolution (’E/Ei) |
> 5 %@(@ E = 0 meV) |
| @5.6@Neutron intensity (@sample position @1MW) |
1~105 n/s/cm2i@Ei = 50 meV, ’E/Ei = 5 %)(calculated value) |
| @5.7@Sample size and/or volume |
2~2~2 cm3 |
| @5.8@Ancillary equipments and sample environments |
Closed cycle refrigerator (5-300K). A high-temperature option (up to 600K)
is available |
| 6. Others |
view detail information (PDF) |
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yBL02z DNA
|
| 1. Instrument |
Biomolecular Dynamics Spectrometer (DNA) |
| 2. Overview of instrument |
The field of expected scientific research on the DNA spectrometer is very wide including the soft matter dynamics, the bio-molecular dynamics, the chemical molecular dynamics, the characterizations of the functional materials and the spin dynamics in the magnetism. |
| 3. Contact person |
Kaoru Shibata (CROSS/JAEA) |
| 4. Sub-contact person |
Nobuaki Takahashi (JAEA) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL02 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Analyzer Crystal and Reflection index (Analyzed Enegy Ef ) |
Si <111>(2.02 meV), Si <311>(7.4 meV) |
| @5.4@Bragg angle of analyzers |
~87.5 [deg.] |
| @5.5@Scan angle |
Horizontal : -164 +164, Vertical : -14 +20(in plan) |
| @5.6@Energy Resolution [meV] |
1.2µeV @(@elastic) Si<111>
5 µeV @(@elastic) Si<311> |
| @5.7@Momentum range |
0.07 < Q < 1.98 [A-1]: Si(111)
0.60 < Q < 3.80 [A-1]: Si(311) |
| @5.8@Scan energy range |
-25 <E <45 (µeV) : single pulse scan around Ef
-300 < E <5100 (µeV) : RRM scan in second frame |
| @5.9@Sample size and/or volume |
2~2~2 cm3 |
| @5.10@Ancillary equipments and sample environments |
Toploading type Cryo-Fanace with Closed cycle refrigerator (5-600K) (in
plan) |
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yBL03z iBIX
|
| 1. Instrument |
IBARAKI Biological Crystal Diffractometer (iBIX) |
| 2. Overview of instrument |
Collection of the pulsed neutron diffraction data from a single crystal
to obtain the precise organic and protein structures. |
| 3. Contact person |
Ichiro Tanaka (Ibaraki University) |
| 4. Sub-contact person |
Katsuhiro Kusaka (Ibaraki University) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL03 |
| @5.2@Moderator |
Coupled moderator |
| @5.3@Range of d-spacing |
0.35 - 50 Å |
@5.4@Resolution@(Specified unit cell dimension amax
@minimum d-space dmin) |
amax = 135 Å
@dmin = 1.2 Å |
| @5.5@Neutron intensity (@sample position @1MW) |
7.0~107@n/s/cm2 |
| @5.6@Sample size and/or volume |
- 6 days are necessary for an protein crystal with 5mm3
- 3 days are necessary for an organic crystal with 2mm3
Another important condition for a protein crystal: All cell dimensions
should be less than 100π, and only one cell edge dimension up to 200π is
also acceptable.
iCalculation conditions: 14 detectors and 200kW of accelerator powerj
|
| @5.7@Ancillary equipments and sample environments |
Low temperature gasiN2CHe) flow equipment |
| 6. Other information for user's convenience |
None |
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|
| 1. Instrument |
Accurate Neutron-Nucleus Reaction measurement Instrument (ANNRI) |
| 2. Overview of instrument |
ANNRI is used for studies of nuclear science (nuclear data for nuclear
technology and astrophysics, quantitative analyses, and so on). |
| 3. Contact person |
Hideo Harada (Japan Atomic Energy Agency) |
| 4. Sub-contact person |
Atsushi Kimura (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL04 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Incident neutron energy |
En>0.0015eV |
| @5.4@Spectrometer |
Ge Spectrometer (Flight length: 21.5m)
NaI Spectrometer (Flight length: 28m) |
| @5.5@Neutron intensity (@sample position @1MW) |
@21.5m sample position
4.3~107 n/cm2/s 1.5 meV < En < 25 meV
9.3~105 n/cm2/s 0.9 eV < En < 1.1 eV
6.0~106 n/cm2/s 0.9 keV < En < 1.1 keV |
| @5.6@Sample size and/or volume |
Using the most downstream collimator, neutron beams with diameters of 22, 7, and 3 mm are provided to suit samples of different sizes. |
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yBL05zNOP
|
| 1. Instrument |
Neutron Optics and Fundamental Physics (NOP) |
| 2. Overview of instrument |
The NOP beamline provides three unique neutron beams, a low-divergence
beam, an unpolarized beam, and a polarized beam, by splitting one beamline
with supermirror benders. |
| 3. Contact person |
Takashi Ino (KEK) |
| 4. Sub-contact person |
Hirohiko M. Shimizu (KEK) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL05 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Neutron wavelength |
2A`9A |
@5.4@Beam profile (16 m position, vertical height ~ horizontal width) |
Low-divergence beam branch : 80 mm ~ 20 mm
Unpolarized beam branch : 55 mm ~ 45 mm
Polarize beam branch : 80 mm ~ 50 mm |
@5.5@Neutron intensity (16 m position, @ 1 MW) |
Low-divergence beam branch : 5.4~104 n/s/cm2
Unpolarized beam branch : 9.4~107 n/s/cm2
Polarize beam branch : 3.9~107 n/s/cm2 |
@5.6@Beam divergence (16 m position) |
Low-divergence beam branch : 5.4~10-2 Κstr
Unpolarized beam branch : 1.0~102 Κstr
Polarize beam branch : 1.9~102 Κstr |
| @5.7@ Average neutron polarization |
Polarize beam branch : 96% |
| @5.8 Auxiliary equipments |
B4C slits at the 7.5 m and 12 m positions on the low-divergence beam branch.
B4C slits at the 12 m position on the unpolarized and polarized beam branches.
A Doppler shifter for UNC production. |
| 6. Others |
The NOP beamline does not include shielding walls or ceiling in the experimental
area, and experimental setups that should emit gammas or scatter neutrons
are required to have proper radiation shielding. |
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|
| 1. Instrument |
SuperHRPD |
| 2. Overview of instrument |
Pulsed neutron powder diffractometer for studying the crystal structure of material. |
| 3. Contact person |
Takashi Kamiyama (KEK) |
| 4. Sub-contact person |
Shuki Torii (KEK) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL08 |
| @5.2@Moderator |
Poisoned decoupled hydrogen moderator |
| @5.3@Range of d-spacing |
0.3 - 4.0 AiHigh-angle bankF150 ? 2Ζ ? 175 degj
0.4 - 7.5 Ai90degree bankF60 ? 2Ζ ? 120 degj
0.6 - 45 AiLow-angle bank F10 ? 2Ζ ? 40 degj |
| @5.4@Resolution (’d/d) |
Best resolution 0.03 %i@ 2Ζ ? 172 degj
0.1 - 0.15 %iHigh-angle bankF150 ? 2Ζ ? 175 degj
0.4 - 0.7 %i90degree bankF60 ? 2Ζ ? 120 degj
0.7 - 3.0 %iLow-angle bank F10 ? 2Ζ ? 40 degj |
| @5.5@Neutron intensity (@sample position @1MW) |
1.0~107@n/s/cm2 |
| @5.6@Sample size and/or volume |
3 cc |
| @5.7@Ancillary equipments and sample environments |
Auto sample changeriRT, 10samplesj
4K-type closed cycle refrigeratori4 - 300 Kj
Top-loading refrigeratori10 - 300Kj
High temperature furnacei1000j |
| 6. Other information for user's convenience |
None |
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|
| 1. Instrument |
NeutrOn Beam-line for Observation & Research Use (NOBORU) |
| 2. Overview of instrument |
NOBORU provides a suitable neutron environment for testing various detectors & devices, new ideas of experimental techniques and irradiation of high-energy (~MeV) neutrons.
NOBORU is now the best pulsed neutron imaging instrument in the world. |
| 3. Contact person |
Fujio Maekawa (Japan Atomic Energy Agency) |
| 4. Sub-contact person |
Masahide Harada (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL10 |
| @5.2@Moderator |
Decoupled moderator |
| @5.3@Incident neutron energy or wavelength |
Ι <@9 Å (25Hz) |
| @5.4@Resolution (’d/d) |
0.33%@(@ 2Ζ= 170 deg) |
| @5.5@Neutron intensity (@sample position @1MW) |
4.8~107 n/s/cm2 (< 0.4 eV) sample position: L1= 14.0 m
1.2~107 n/s/cm2 (> 1 MeV)
1.2~106 n/s/cm2 (> 10 MeV) |
| @5.6@Neutron beam size (@sample position) |
Maximum 10~10 cm2 (largest among all the instruments in MLF) |
| @5.7@Ancillary equipments and sample environments |
- two B4C beam slits to trim the neutron beam (L= 7.1 m & 12.7 m)
- a flame-overlap chopper (L= 7.2 m)
- a filter system to attenuate cold neutrons, epi-thermal neutrons or gamma-rays (L= 7.4 m)
- a rotary-collimator with 4 holes (L= 8.0 m)
- a He-3 neutron monitor counter (L= 12.7 m)
- a 5-axes compact goniometer for samples
(a 300 mmΣ table, load capacity 20 kg)
|
| 6. Other information for user's convenience |
- Variable collimator ratio (L/D = 140, 190, 600, 1875) for imaging experiment
- Small beam divergence due to neutron guideless beam-line design.
- An experimental space of 2.5(W)~3.5(L)~3.0(H)m3 to introduce various experimental equipment
- Strong radiation shield which can endure against large samples (scatterer) up to a steel cube 10 cm on a side
- In planning your experimental program, please consult with the contact
person in advance
|
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|
| 1. Instrument |
High-Pressure Neutron Diffractometer (PLANET) |
| 2. Overview of instrument |
Powder diffractometer for in-situ observation of pressure induced structural
changes in condensed matter |
| 3. Contact person |
Takanori Hattori (Japan Atomic Energy Agency) |
| 4. Sub-contact person |
Hiroshi Arima (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL11 |
| @5.2@Moderator |
Decoupled hydrogen moderator |
| @5.3@Incident neutron wavelength |
0.3 Å < Ι < 5.8 Å (1st frame) |
| @5.4@d-range |
0.2 Å < d < 4.1 Å (1st frame) |
| @5.5@Neutron intensity (@sample position @1MW) |
1.0 ~108@n/s/cm2@(standard mode)
0.3 ~108@n/s/cm2@(high resolution mode) |
| @5.6@Resolution (’d/d) |
0.5 % (standard mode)
0.3 % (high resolution mode) |
| @5.7@Beam size |
20 mm x 20 mm at max. |
| @5.8@Detectors |
3He gas tubes (1/2")
2¦ range: 79-101
azimuth angle -35- 35. |
| @5.9@Sample environment |
- 6-axis high pressure apparatus "ATSUHIME" (30 GPa, 2000 K)
- Positioning stage for various high pressure devices
- Radial collimators
|
| 6. Other information for user's convenience |
On beam commissioning will start from 2012. |
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yBL12z@HRC
|
| 1. Instrument |
High Resolution Chopper Spectrometer (HRC) |
| 2. Overview of instrument |
Observation of elementary excitations such as magnons and phonons in materials
under relatively high resolutions with relatively high energy neutrons |
| 3. Contact person |
Shinichi Itoh (KEK), Taku Sato (The University of Tokyo) |
| 4. Sub-contact person |
Tetsuya Yokoo (KEK) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL12 |
| @5.2@Moderator |
Decoupled hydrogen moderator |
| @5.3@Neutron energy |
10 < Ei < 500 meV |
| @5.4@Scattering angle |
Horizontal -10 ~ 40, Vertical: }20 |
| @5.5@Neutron intensity (@sample position @1MW) |
1x105 n/s/cm2 (’E/Ei=2.5%) |
| @5.6@Energy resolution |
’E/Ei ≥ 2.5% (@E=0meV) |
| @5.7@Maximum sample size |
4x4 cm2 |
| @5.8@Ancillary equipments and sample environments |
Closed cycle refrigerator (5-300K) |
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|
| 1. Instrument |
Cold-neutron disk-chopper spectrometer iAMATERAS) |
| 2. Overview of instrument |
Inelastic scattering spectrometer for detecting dynamical properties in atomic, molecular and magnetic systems in a relatively low-energy range with high resolution |
| 3. Contact person |
Kenji Nakajima (Japan Atomic Energy Agency) |
| 4. Sub-contact person |
Seiko Kawamura (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL14 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Incident neutron energy |
1 < Ei < 80 meV |
| @5.4@Detection angle |
Horizontal: 5 deg. - 110 deg,
Vertical: -16 deg. - 23 deg. (Current state)
Horizontal: -40 deg. - 136 deg.
Vertical: -16 deg. - 23 deg. (Finale stage) |
| @5.5@Resolution (’E/Ei) |
~1% (at the minimum) at Ei<3meV
~2-3% (at the minimum) at Ei<20meV
~4-5% (at the minimum) at Ei<80meV.
(These are current values and will be improved with progression of commisioning.) |
| @5.6@Neutron intensity (@sample position @1MW) |
3 ~104@n/s/cm2 (@ Ei = 20 meV, ’E/Ei = 1 %) (expected) |
| @5.7@Sample size and/or volume |
Beam is optimized for dimension of 1Σ~2 cm3 |
| 5.8 Ancillary equipments and sample environments |
Closed cycle refrigerator (T<6K) |
| 6. Other information for user's convenience |
- AMATERAS has just been constructed and is still under commissioning.
- Therefore actual specifications may be different from the above at present, depending on the situation of the instrument.
|
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yBL15z@TAIKAN
|
| 1. Instrument |
Smaller-Angle Neutron Scattering Instrument (TAIKAN) |
| 2. Overview of instrument |
Instrument for efficient and precise measurements of nanostructure and
microstructure ranging from sub-nanometer to micrometer in various materials:
metal, magnet, superconductor, soft matter, biomolecule, etc.. |
| 3. Contact person |
Jun-ichi Suzuki (Comprehensive Research Organization for Science and Societyj |
| 4. Sub-contact person |
Shin-ichi Takata (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL15 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Incident neutron wavelength |
0.5?8π (Unpolarized neutron)
@2?8π (Polarized neutron) |
| @5.4@Q-range |
5~10-4?10π-1 (Unpolarized neutron)
5~10-4?2.5π-1 (Polarized neutron) |
| @5.5@Beam size |
10mm~10mmiTypicalj |
| @5.6@Auxiliary equipments and sample environments |
Sample changer (T = ?25?125, 10 samplesj |
| 6. Other information for user's convenience |
Commissioning will be resumed in JFY2011.
The Q-range means a value in case of full installation of detectors. |
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|
| 1. Instrument |
Soft Interface Analyzer (SOFIA) |
| 2. Overview of instrument |
Material interfaces and thin films under various conditions could be investigated
multi-dimensionally and rapidly. |
| 3. Contact person |
Norifumi L. Yamada (KEK) |
| 4. Sub-contact person |
Hideki Seto (KEK) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL16 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Incident neutron energy or wavelength |
0.2 nm < lambda < 0.88 nm (single frame mode)
0.25 nm < lambda < 17.6 nm (double frame mode) |
| @5.4@Scattering angle |
theta < 6 deg. |
| @5.5@Observable reflectivity |
R > `10-7 |
| @5.6@Duration time |
3" deuterated polymer (Q<1 nm-1, R<10-4): 5 minutes
3" deuterated polymer (Q<2 nm-1, R<10-6): 20 minutes
3" deuterated polymer (Q<4 nm-1, R<10-7): 1 hour
3" hydrated polymer (Q<2 nm-1, R<10-7): 2 hours |
| @5.7@Detector |
2-dimensional scintillation counter (off-specular reflectivity measurement
is available) |
| @5.8@Sample environment |
Evacuable high-temperature cell (up to 200 C)
@ Sample cell for solid/liquid interface measurement
@ Low temperature cell (from 5 C to 80 C, two independent samples) |
| 6. Other information for user's convenience |
Free interface measurement is not allowed due to a limitation of a treatment
of liquid (packed liquid is allowed). |
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|
| 1. Instrument |
Polarized Neutron Reflectometer with vertical sample-plane geometry (SHARAKU) |
| 2. Overview of instrument |
Revealing mechanisms of functions of thin film devices by studying structures of surface and buried interfaces. |
| 3. Contact person |
Masayasu Takeda (Japan Atomic Energy Agency) |
| 4. Sub-contact person |
Dai Yamazaki (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL17 |
| @5.2@Moderator |
Coupled hydrogen moderator |
| @5.3@Wavelength band |
Ι=0.2 `0.84 nm (polarized neutron modej
Ι=0.1 ` 0.88 nm (unpolarized neutron mode) |
| @5.4@Q range |
q=0.1`12 nm-1 (polarized neutron mode)
q=0.05`25 nm-1 (unpolarized neutron mode) |
| @5.5@Scattering-angle range |
2Ζ = ?5 `23 |
| @5.6@Detectors |
- 0-dimensional 3He gas detector
- 2-dimensional multi-wire proportional counter
isensitive areaF128 x 128 mm2j (in preparation)
- 2-dimensional scintillation detectors
isensitive areaF256 x 256 mm2j(in preparation)
|
| @5.7@Sample environment |
Closed cycle refrigerator (4K)
electromagnet (1T) |
| 6. Other information for user's convenience |
On beam commissioning will start in January 2012. |
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|
| 1. Instrument |
Single Crystal Neutron Diffractometer under Extreme Condition |
| 2. Overview of instrument |
The diffractometer is dedicated for precise crystal and magnetic structure analyses under the combined extreme conditions using small sample less than 1 mm3. |
| 3. Contact person |
Kenichi Oikawa, (Materials and Life Science Division, J-PARC Center) |
| 4. Sub-contact person |
Takashi Ohhara, (Comprehensive Research Organization for Science and Society) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL18 |
| @5.2@Moderator |
Poisoned decoupled hydrogen moderator |
| @5.3@Incident neutron wavelength |
0.4 ~ 4.4 Å (1st frame)
4.6 ~ 8.8 Å (2nd frame) |
| @5.4@Neutron intensity (@sample position @1MW) |
0.6x106 n/s/mm2istandard modej
1.3x106 n/s/mm2ihigh-intensity modej |
| @5.5@Sample position |
34.8 m |
| @5.6@Specified unit cell dimension amax |
50 Å |
| @5.7@Sample size |
> 0.5 x 0.5 x 0.5 mm3i@1MWj |
| @5.8@Detection angle |
Horizontal -13 ~ -167, +58 ~ +167
Vertical -29 ~ +29 |
| @5.9@Sample environment |
RT goniometer
Closed cycle refrigerator (4K)
50 mK Dilution refrigerator (50mK)
Superconducting magnet (7T) |
| 6. Other information for user's convenience |
On beam commissioning will start from 2012.
|
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|
| 1. Instrument |
Engineering Materials Diffractometer (TAKUMI) |
| 2. Overview of instrument |
Instrument for characterizing the internal strain (stress) and structure of engineering components and other industrial materials. |
| 3. Contact person |
Kazuya Aizawa (Japan Atomic Energy Agency) |
| 4. Sub-contact person |
Stefanus Harjo (Japan Atomic Energy Agency) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL19 |
| @5.2@Moderator |
Poisoned decoupled hydrogen moderator |
| @5.3@Range of d-spacing |
Standard mode: 0.5 ? 2.7 A
Wide d-range mode: 0.5 ? 4.7 A (the intensity becomes half) |
| @5.4@Resolution (’d/d) |
High resolution mode:@0.17 %
High intensity mode:@< 0.4 %
TAKUMI has a pair 90 deg scattering detector banks having covering area of }15 deg in horizontal and }16 deg in vertical range for each bank. The resolution values were obtained after binning all pixels in the detector banks. |
| @5.5@Neutron intensity (@sample position @1MW) |
High resolution mode:@2.2~107@n/s/cm2 (designed)
High intensity mode:@4.8~107@n/s/cm2 (designed) |
| @5.6@Sample size and/or volume |
Standard sample volume: > 5~5~5 mm3
(available for the size with a side larger than 1m, need discussing with the person in charge) |
| @5.7@Ancillary equipments and sample environments |
- Large sample table (table size: 800~800mm2, load capacity: 1 ton)
- Radial collimators (2mm width slits, 5mm width slits will be developed during 2010 FY)
- Loading machine (Tension 50kN, Compression 20kN)
- Dilatometer (1273K Furnace)
- Eurelian cradle (sample weight < 8kg)
- High temperature loading machine (1273K, Tension 40kN, Compression 20kN)
- Low temperature loading machine (< 10K, Tension 50kN) -> will be developed during 2010 FY
|
| 6. Other information for user's convenience |
None |
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|
|
| 1. Instrument |
IBARAKI Materials Design diffractometer(iMATERIA) |
| 2. Overview of instrument |
High-efficiency, general-purpose neutron diffractometer for the analysis of crystal structure of powder samples over a wide d-range (Q-range). |
| 3. Contact person |
Toru Ishigaki (Ibaraki University) |
| 4. Sub-contact person |
Akinori Hoshikawa (Ibaraki University) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL20 |
| @5.2@Moderator |
Poisoned decoupled hydrogen moderator |
| @5.3@Range of d-spacing |
At present: @
0.181 ` 5.09 π (backward detector bank)
In near future:
0.255 ` 7.2 πi90 degree detector bankj
0.556 ` 45.14 πilow-angle detector bankj
3.38 ` 834 πismall-angle detector bankj
At completion: @
0.089 ` 5.09 πibackward detector bankj
0.255 ` 7.2 πi90 degree detector bankj
0.556 ` 45.14 πilow-angle detector bankj
3.38 ` 834 πismall-angle detector bankj |
| @5.4@Resolution (’d/d) |
0.16 %@i@ backward detector bank)
0.5 %@i@ 90 degree detector bank) |
| @5.5@Estimated measurement time (@ 100 kW, 25 Hz operation ) |
`30 minutes for Si
`40 minutes for LiCoO2 |
| @5.6@Sample size and/or volume |
Approximately@1.4 cc
(Σ6mm x 50 mm height. Sample with 20 mm height is exposed to neutron beam. If the sample has smaller volume, measurement will take longer time.) |
| @5.7@Auxiliary equipments and sample environments |
Sample changer (room temperature at atmospheric and low pressures )
Low temperature and high temperature environment will be developed in JFY 2011. |
| 6. Other information for user's convenience |
None |
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yBL21z@NOVA
|
| 1. Instrument |
NOVA |
| 2. Overview of instrument |
NOVA covers a wide-Q range with the highest resolution of about 0.35% in order to observe various phases such as crystals, glasses and liquids. |
| 3. Contact person |
Toshiya Otomo (KEK) |
| 4. Sub-contact person |
Kentaro Suzuya (JAEA) |
| 5. Information of instrument and equipments |
|
| @5.1@Beam line |
BL21 |
| @5.2@Moderator |
Decoupled hydrogen moderator |
| @5.3@Incident neutron wavelegth |
0.12 A < Ι <@8.3 A |
| @5.4@Resolution (’Q/Q) |
0.35 % |
| @5.5@Q-range |
0.01 A-1 < Q < 100 A-1 |
| @5.6@Sample size and/or volume |
Standard sample Vol. φ6 mm x 20 mmi0.6 cc approx.j@
Beam size :5 mm x 5 mm at min. and 20 mm x 20mm at max. |
| @5.7@Ancillary equipments and sample environments |
Auto sample changer (RT, 10 samples per load)
H2/D2 gas in-situ environmentiMax press.F10 MPa, Temp.F50 K ~ 473 K, PCT curve measurable)
Furnace (under commissioning) (RT ~ 1373 Kj |
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