The home-built pulse nuclear magnetic resonance spectrometer with digital quadrature detection for 3He research at low temperatures Текст научной статьи по специальности «Физика»

ISSN 2072-5981

Volume 15, 2013 No. 1, 13104 - 6 pages

http://mrsej.ksu.ru

Established and published by Kazan University Sponsored by International Society of Magnetic

Resonance (ISMAR) Registered by Russian Federation Committee on Press,

August 2, 1996 First Issue was appeared at July 25, 1997

© Kazan Federal University (KFU)

"Magnetic Resonance in Solids. Electronic Journal" (MRSey) is a

peer-reviewed, all electronic journal, publishing articles which meet the highest standards of scientific quality in the field of basic research of a magnetic resonance in solids and related phenomena. MRSey is free for the authors (no page charges) as well as for the readers (no subscription fee). The language of MRSey is English. All exchanges of information will take place via Internet. Articles are submitted in electronic form and the refereeing process uses electronic mail. All accepted articles are immediately published by being made publicly available by Internet (http://MRSey.ksu.ru).

Editors-in-Chief Jean Jeener (Universite Libre de Bruxelles, Brussels) Boris Kochelaev (KFU, Kazan) Raymond Orbach (University of California, Riverside)

Executive Editor

Yurii Proshin (KFU, Kazan) Editor@ksu.ru

Editors

Vadim Atsarkin (Institute of Radio Engineering and Electronics, Moscow) Detlef Brinkmann (University of Zürich,

Zürich)

Yurij Bunkov (CNRS, Grenoble) John Drumheller (Montana State University, Bozeman) Mikhail Eremin (KFU, Kazan) David Fushman (University of Maryland,

College Park)

Yoshio Kitaoka (Osaka University, Osaka) Boris Malkin (KFU, Kazan) Haruhiko Suzuki (Kanazawa University,

Kanazava) Murat Tagirov (KFU, Kazan)

In Kazan University the Electron Paramagnetic Resonance (EPR) was discovered by Zavoisky E.K. in 1944.

The home-built pulse nuclear magnetic resonance spectrometer with

3

digital quadrature detection for He research at low temperatures

E.M. Alakshin *, R.R. Gazizulin, A.V. Klochkov, V.V. Kuzmin, A.M. Sabitova, T.R. Safin,

M.S. Tagirov

Kazan Federal University, Kremlevskaya, 18, Kazan 420008, Russia

*E-mail: alakshin@gmail.com

(Received April 5, 2013; revised May 6, 2013; accepted May 10, 2013)

The home-built pulse nuclear magnetic resonance spectrometer for 3He research is described. The temperature range is 1.5 - 4.2 K, the frequency range is 3 - 20 MHz, the dead time is 10 (s at 10 MHz. The spectrometer software is based on programming language LabVIEW. The advantages of digital technique are described; particularly the implementation of digital quadrature detector.

PACS: 75.10.Dg, 76.30.-v, 75.20.

Keywords: 3He, nuclear magnetic resonance, spectrometer, low temperature, digital detection 1. Introduction

The nuclear magnetic resonance (NMR) of 3He in contact with porous media could give an unique information about structure, porosity and pore-size distribution of the media [1-4]. It was found [5] that the magnetic relaxation of liquid 3He in confined geometry acquires new features compared with the relaxation in bulk liquid, and a new mechanism of magnetic relaxation has been proposed. Thus, the longitudinal relaxation time, the transverse relaxation time and the spectral line width strongly depend on the size of the volume filled by liquid 3He.

As it is well known, there are two types of the NMR spectrometers for condensed matter: the devices for liquids and ones for solids. In liquids due to molecular motion there is effective averaging of the local magnetic fields produced by neighbor nuclei, that is why NMR lines are narrow. This type of resonance is also known as High Resolution NMR (HR NMR) [6]. As a rule, components of the spectrum have narrow width and their form is not interesting for researchers. In HR NMR the spin-spin relaxation time T2 is comparable with the spin-lattice relaxation time T and is about seconds. It is much longer than the dead time of the standard NMR spectrometer (~10 (is). In solids nuclear moments are localized in the crystal structure. For nuclei with spin I = 1/2 the line width of the NMR spectrum is due to dipole-dipole interaction with neighbor electron and nuclear spins. The NMR line width can vary from few Gauss (local field produced by nearest nucleus) to thousands of Gauss (165Ho NMR, I = 7/2, in Rb2NaHoF6 [7]). In Wide Line NMR (WL NMR) the spin-spin relaxation time T2 is shorter than the spin-lattice relaxation time T and can be even shorter than the dead time of the Pulse NMR spectrometer.

3He monatomic molecules at low temperatures in porous media can be found in three different aggregate states: solid (adsorbed layer), liquid and gaseous. The structure of the porous samples leads to the transformation of the diffusion motion spectrum and, as a result, 3He NMR takes the intermediate position between HR NMR and WL NMR. So it requires the specific equipment. Firstly, the dead time should be the same order of magnitude as in the standard HR NMR spectrometer. Secondly, the homogeneity of the magnetic field should be higher than in the standard WL NMR spectrometer. Thirdly, the magnetic field stability should be quite good. Such investigations require high time resolution of Analog-to-Digital Converter (ADC) because the 3He spin echo signal in porous media can be quite sharp (about 5 ( s) in time dimension. The implementation of digital technique gives the following advantages: a simple realization of various pulse sequences, phase inversion, absence of additional noise in digital schemes using of digital filters with sharp characteristics, flexible realization of the spectrometer operation schemes.

The home-built pulse nuclear magnetic resonance spectrometer with digital quadrature detection...

In recent years several implementations of digital techniques for NMR spectrometers have been developed [8-10]. The major differences of the described NMR spectrometer are: LabVIEW platform usage, software realization of quadrature detector and filters. The usage of LabVIEW platform makes the modifications of spectrometer's abilities easy and flexible, including pulse sequences and signal processing algorithms. In particular, the software realization of quadrature detector avoids problems with synchronization [9].

2. Spectrometer block diagram

It was suggested to use the BORDO-221 ADC (Auris Inc) with time resolution down to 10 ns. For synchronization of the spectrometer digital part and for the pulse sequences generation the Pulse Blaster PB16-32k, SpinCore Technologies Inc., was used. The spectrometer digital part is controlled by LabVIEW software.

Figure 1. Block diagram of the pulse NMR spectrometer.

The block diagram of the spectrometer is shown in fig. 1. Reference radiofrequency (RF) signal from the Rohde&Schwarz SML01 generator is applied to the input A of the multiplier AD835. Programmed on LabVIEW, the Pulse Blaster is connected to the input B. As a result, at the output C of the multiplier, we obtain the RF pulses with the frequency equal to the Rohde&Schwarz SML01 generator frequency. After the Rohde&Schwarz BBA100-C125 amplifier, the video pulses are applied to the NMR coil and excite a spin system. The response of a spin system after pre-amplifier proceeds to ADC.

The vacuum system for 3He research in contact with porous samples was used. To control the volume of 3He which is condensed in the sample the calibration volume (8 cm3) was designed. The amount of 3He is controlled by pressure gauge Piza 111. The helium leak detector Pfeiffer Vacuum Inc has been used for system leakage testing. The temperature of the sample 1.5 - 4.2 K is achieved by 4He bath pumping and measured by calibrated Allen-Bradley carbon resistor.

3. Analog-to-digital converter and pulse generator

The digital part of the NMR spectrometer consists of the pulse generator (Pulse Blaster PB16-32k, SpinCore Technologies Inc.) and the analog-to-digital converter (ADC BORDO 221, Auris Inc.).

PB and ADC, made as a PCI board, are connected to PCI bus. The LabVIEW program was written for controlling them (fig. 2). The abilities of this program are: the generation of the pulse sequences and data acquisition.

Figure 2. Interface of pulse NMR spectrometer.

The home-built pulse nuclear magnetic resonance spectrometer with digital quadrature detection... Main features of PB and ADC are shown in the table 1.

For testing of the program the carbonate geological sample was used. The method of sample preparation is described in [1]. The free induction decay of 3He is presented in fig. 3.

Table 1. Main features of PB and ADC.

Parameter BORDO 221 Parameter PB16-32k

Bit depth 10 bit Number of channels 16

Input voltage 0-8 V Pulse duration 50 ns - 2 year

Band 0-150 MHz The time between pulses 10 ns

100 200 300 400 500 Time, |is

Figure 3. FID of liquid 3He in geological sample (4 scans). 4. Digital quadrature detector

A signal, the spectrum of which does not contain frequencies above fe (Hz), can be recovered if the reference values of the signal, taken at regular intervals of time At = 1/2fe (s), is known. In the spectrometer the ADC with sampling period At = 10 (ns) is used, so we can correctly digitize the signal the spectrum of which does not contain frequencies above 50 MHz. The block diagram of the digital quadrature detector is shown in fig. 4.

The signal from the harmonic reference generator Rohde&Schwarz SML01 is applied to the input A of the double channel ADC. The obtained array is supplied to the 900 phase shift unit and to the multiplier C. The signal from the pre-amplifier is applied to the input B of the ADC. This array of data is supplied to the two multipliers, C and D. After multipliers data sets arrive to the low-pass filters (LPF) from LabVIEW library.

Figure 4. The block diagram of a digital quadrature detector.

Let us describe the operation of the 900 phase shift unit. If we have the signal sin cot as the digitized array then we need to have array C with the signal cos ct. Let us create an additional array B which is obtained from the array A by shifting its elements into two index up, i.e. B[i] = A[i + 2]. Obviously, the array B can be written as sin(ct + p), where p = 2cAt is the phase shift, At is the sampling period. Using the following trigonometric equations:

sin(ct + p) = sin ct cosp + cos ct sinp, (1)

cosc = —

sin ct + sin(ct + p) tan p sin p

(2)

we can conclude that any element of the array C can be obtained as the sum of the corresponding element of the array A and the corresponding element of the array B with the following coefficients:

1

a = —

tanp

(3)

P = ~

sinp

(4)

i.e. C[i] = cA[i] + Mi].

As a result, the output of the quadrature detector has the following signals - channel "A" and "B" (the results of the two synchronous detectors, the reference signals are out of phase), and the channel "C" which is called quadrature (or C 2 = A2 + B2).

5. Conclusion

We have developed and described here the experimental setup of home-build pulse NMR spectrometer. The digital spectrometer gives the following advantages: absence of additional noise in a quadrature detection and low frequency amplifiers, using of digital filters with sharp characteristics, flexible realization of the spectrometer operation scheme.

Acknowledgments

This work is partly supported by the Ministry of Education and Science of the Russian Federation (project no. 02.G25.31.0029). We wish to acknowledge professor D.K. Nourgaliev for providing the geological samples.

The home-built pulse nuclear magnetic resonance spectrometer with digital quadrature detection...

References

1. Gazizulin R.R., Klochkov A.V., Kuzmin V.V. Safiullin K.R., Tagirov M.S., Yudin A.N., Izotov V.G., Sitdikova L.M. Appl. Magn. Resonance 38, 271 (2010)

2. Gazizulin R.R., Klochkov A.V., Kuzmin V.V., Safiullin K.R., Tagirov M.S., Yudin A.N. Magn. Reson. Solids 11, 33 (2009)

3. Tagirov M.S., Alakshin E.M., Gazizulin R.R., Egorov A.V., Klochkov A.V., Korableva S.L., Kuzmin V.V., Nizamutdinov A.S., Kono K., Nakao A., Gubaidullin A.T. J. Low Temp. Phys. 162, 645 (2011)

4. Alakshin E.M., Gazizulin R.R., Klochkov A.V., Kuzmin V.V., Mulders N., Tagirov M.S., Tayurskii D A. JETP Letters 93, 223 (2011)

5. Naletov V.V., Tagirov M.S., Tayurskii D.A., Teplov M.A. JETP 81, 311 (1995)

6. Fukushima E., Roeder S.B.W. Experimental Pulse NMR: A Nuts and Bolts Approach, Addison-Wesley Publishing Company, Inc (1981)

7. Egorov A.V., Livanova L.D., Tagirov M.S., Teplov M.A. Sov. Phys. Solid. State 22, 1655 (1980)

8. Gengying L., Yu J., Xiaolong Y., Yun J., Rev. Sci. Instrum. 72, 4460 (2001)

9. Michal C.A., Broughton K., Hansen E. Rev. Sci. Instrum. 73, 453 (2002)

10. Tang W., Wang W., Meas. Sci. Technol. 22, 015902 (2011)