Progress towards modernization of the HRFD diffractometer

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Presentation transcript:

Progress towards modernization of the HRFD diffractometer Science team: Ivan A. Bobrikov, V.G. Simkin, S.V. Sumnikov, V. Turchenko and A.M. Balagurov Outline: General information about HRFD Directions of HRFD modernization in 2014-2017 Modernization of HRFD in 2016 -Neutron guide, - Fourier chopper. Further step of HRFD modernization and Conclusions Good day, everyone. Thank you for introduction! My talk is about upgrade of High resolution diffractiometer

General information about HRFD R(t, θ) = d/d = [(t0/t)2 + (θ/tgθ)2]1/2 R→0 if Δt0→0 or L→∞ and Δθ→0 or θ→π/2 t ~ L, R= Δd/d≈0.001, word level in resolution I would like to remind you that this diffractometer occupies channel 5 of our facility. The main purpose is precisely investigation of crystal structure and some microstructure effects in powders. And it there is among the best diffractometers in the world by resolution level. On the right picture you see comparison of diffraction patterns measured on common diffractometer at IBR-2 and high resolution pattern obtained at HRFD. Another advantage of this instrument is possibility to work in both high resolution and low resolution mode but high intensity mode. To get high resoolution according this equation for TOF diffractometers we reduce neutron pulse width by special correlation techniques.

Directions of HRFD modernization 1 – Moderator 2 – Fourier Chopper 3 – Guide Tube 4 – Main Detector 5 – Sample Position 6 – 90°-Detector 7 – PSD Detector 8 –Control and Operative 9 – Data Acquisition  10 –Ethernet Data Transfer Electronics for data acquisition Software for data acquisition Sample environment Neutron guide Fourier chopper The main detectors The main components of diffractometer are shown on this slide. This is the special neutron chopper – Fourier chopper, curved mirror neutron guide, scintillation detectors and electronics for data acquisition. Significant part of modernization of electronics components were made in 2014 and 2015 In my talk Ill focus on components which were installed in 2016 (in last year). This is neutron guide and the most important component of HRFD – Fourier chopper. It has this name because of specific law of his rotation which helps us to collect data at different frequencies of neutron transmisson and use method similar to inverse Fourier transform for recover diffraction pattern. 2014-2015 2015-2016

General information about HRFD IBR-2 1 – Moderator 2 – Fourier Chopper 3 – Guide Tube 4 – Main Detector 5 – Sample Position 6 – 90°-Detector 7 – PSD Detector 8 –Control and Operative 9 – Data Acquisition  10 –Ethernet Data Transfer Neutron guide helps us to get maximum number of thermal neutrons at sample position. Neutron guide became outadate. It was installed in 90th and had some mistakes in construction. It was made in 1991, 58Ni (M=1) Entrance 20030 mm, Exit 10010 mm.

General information about HRFD IBR-2 1 – Moderator 2 – Fourier Chopper 3 – Guide Tube 4 – Main Detector 5 – Sample Position 6 – 90°-Detector 7 – PSD Detector 8 –Control and Operative 9 – Data Acquisition  10 –Ethernet Data Transfer Contrast = (High-Tr)/(Low-Tr) ≈ 25 IBR-2, TOF W = 350 μs R = 0.01 Fourie chopper reduces neutron pulse from reactor to helps to get high resolution at short flight paths. The old Fourier Chopper was made and installed in 90-th too It had low contrast of transmission function, allowed installation of only low resolution encoder of rotation that considerably degrade signal of opened or closed position of rotor, high enough level of vibration that also degraded quality of collected data. IBR-2, RTOF W = 15 μs R = 0.001

Suggestion for modernization – neutron guide Neutron flux at sample position ~6*106 n/cm2/s (2011) It was made in 1991, 58Ni (M=1) Entrance 20030 mm, Exit 10010 mm. We had got good suggestion from Swiss Neutronics, purchased new neutron guide and it was installed in summer 2016. Here you see parameters of new neutron guide. Difference between ald and new one is in cross section, focusing, Radius of curvate and type of covering. Neutron flux will be increased in 2.5-3 times!

Modernization of HRFD On the right picture you see installed new neutron guide to old neutron guide case. First neutrons have shown that neutron flux was considerable increased. Here there is wavelengths distribution of neutrons at sample position measured before and after new neutron guide installation. In small window you see normalized to 1 the same spectra. One can see that new effective spectrum of neutrons is shifter to short wavelengths to high energies of neutrons. Distribution of neutrons at exit of neutron guide is symetric which was shown by measuremnt of beam by PSD detector

Modernization of HRFD By activation method: Before ~6·106 n/cm2/s On this slide you see the same graphs. And Ratio of some diffraction peaks of corundum measured before and after neutron guide installation. You can see that average effect is about 2.5 that is in agreement with our expectation. Activation method on golden foils has shown also that neutron flux was increased more than in two times. By activation method: Before ~6·106 n/cm2/s After ~1.37·107 n/cm2/s

Modernization of HRFD Old New Rotation 0 → 4000 → 0 rmp Contrast TF: from ~ 25 → 100 Low level of vibration Max velocity: 4000 → 6000 rpm Better quality of rotation signal (PICK-UP) In this summer new Fourier chopper was also installed. This chopper was ordered at Mirratron company in 2014. And in 2016 they finished this project. In contrast to old chopper where disk was rotated in air, disk of new chopper rotates in vacuum. It significantly deacreased level of vibration. New chopper has better in 4 times contrast of transmission function of neutrons. Due to setup more precise rotation encoder quality of rotation signal was also improved. It helped us to increase ratio effect/background in obtained high resolution patterns in 1.5 times. On top figures you see comparison of signal of chopper rotation from old device and from new one. Lower dispersion is better.

+ Modernization of HRFD My next slide shows results of new chopper and neuton guide installation on High resolution mode of HRFD. Diffraction peaks have become more intensive particulary at short wavelengths. But resolution degraded on 21%. But it is still very high resolution. We connect this degradation with increasing of angular divergence of neutrons at neutron guide exit. We hope we decide this problem by soller collimator.

New possibilities for High Intensity experiments HR – High Resolution HR High Intensity High Intensity HR High Intensity HR HR Because of our station works not only in high resolution mode but also in high intensity mode we purchased and installed precise linear translator for the chopper. After installation of new neutron guide Due to full removing of the chopper from the neutron beam we have in 5 times more neutrons at sample position in High intensity mode if we compare to situation before when we could not move the chopper remotely and needed to find manualy the maximum of transmission function. Possibility of remote control of chopper placement helps very well in combine experiment then we study some transition process by high intensities and in some crucial points to do high resolution experiment to analyze crystal and microcrystal parameters. For example It could be some processes in power cells or more standard experiment with temperature depended phase-transitions. Example is shown on this graph. During heating or annealing high intensity experiment is applied to study phase transitions but in some key points high resolution applied. High Intensity High Resolution HI Flux: in ~5 times more! Time economy!

New sight at Fe-Al phase diagram These kind of experiments we made to study phase transition in some functional alloys. For example here phase content and type of phases during temperature changes was studied in high intensity mode but at room temperature before and after heating and at highest temperature point microstructure of alloy was studied by high resolution. It was obtained that earlier considered single phase condition has evidenses of second phase and phase diagram can should be reviewed. JETP Letters, 104 (2016)

Comparative study of structural phase transitions in bulk and powdered Fe-27Ga alloy by real-time neutron thermo-diffractometry In this work compare phase transitions and bulk and powder sample. Phase content and temperature of transitions were studied by high intensity mode. But microstructure details were studied by high resolution mode. It was obtained that there is visible (noticible) difference between powder and bulk sample as in phase content as well in microstructure parameters. J. Appl. Cryst., 50 (2017)

Recent problems ServoDrive UPS Vibration sensor Servo Drive Warranty case! From bad news unfortunately in this month new chopper does not work due to problems with several important components. The chopper is quite complicate device and have many electronics details. Now we have broken Power Supply, Vibration sensor and servo-drive computer which control directly the chopper motor. All happened problems in the chopper control system are warranty case we hope it will be solved soon. UPS

Suggestion for modernization - detectors 25 years old. Aperture of the main detectors based on 6Li scintillators: 0.16 sr. Very long time for data acquisition! High gamma sensitivity. Now I can go to next suggestion for modernization: The main detectors. The current detectors life-time is expired. They are 25 years old! But it is not all. Its have very small aperture (area) – 0.16 steradians! Which drammaticaly influence at general efficiency (luminosity) of diffractometer.

New Back Scattering Detector ZnS(Ag)/6LiF V.A.Kudryashev, ICANS-XIX  Ω = 1.5 Sr S = 13.5 m2 ≈190 elements Rg: from 0.0004 to 0.0009 1.813  0.221 8 0.202 7 0.252 6 0.237 5 0.225 4 0.216 3 0.208 2 1 0.050 W, str Ring Installing of new detector with large square and based on ZnS-scintillator improves efficiency of neutron detection in 10 times! And considerably decrease gamma-background. (Zink sulphide) . Here you see draft and some calculations for possible new detector. Total price of this detector is about 600 kDollars Based on last news. Spectrometers Department of our Lab can made this type of detector. Geometrical contribution to the resolution function for sample of 5x5x5 mm3 1 2 3 4 5 6 7 8 3.7E-4 5.4E-4 6.1E-4 6.7E-4 7.3E-4 7.8E-4 8.3E-4 8.8E-4 Efficiency of neutron detection will be increased in 10 times!

Conclusions T H A N K Y O U ! Technical and software support of HRFD: In 2016 new neutron guide was purchased and installed. As result HRFD has a new neutron guide and neutron flux at sample position was increased more than 2 times. In 2016 new Fourier chopper (made by Mirratron) was installed. It has shown many advantages over old one and many warranty cases. Totally in High resolution we increase efficiency of the diffractometer in approximately 3 times. In High Intensity mode in 5 times. - The main proposed modernization for next period: New ZnS backscattering detector (~ 600 k$) . It may be made by Spectrometers Department of FLNP. Technical and software support of HRFD: N.D. Zernin, A.P. Sirotin and V.V. Zhuravlev T.B. Petukhova, S.M. Murashkevich and D.A. Balagurov And at the end I would like to express thanks