The present invention relates to a method of viewing nuclear magnetic resonance (NMR) and, in particular, to a method of providing high-resolution NMR spectra of solids. The invention can be used in various fields of physics, chemistry and biology to provide information on the intrinsic properties of substance, such as characteristics of chemical bonds, magnitude of electron-nuclear interactions, composition and structure of molecules, etc., which manifest themselves in small shifts of the NMR resonance frequency.

In many cases, particularly, in solids, these shifts which carry valuable information are obscured by dipolar spin-spin interactions between the gyromagnetic nuclei of the test material. In typical solids these interactions cause broadening of the NMR lines to 10⁴ Hz, thus appreciably limiting the resolution of conventional NMR spectrometers. The currently available methods for reducing the effects of nuclear dipolar interactions in solids require complex and costly equipment and also special interpretation of the measurement results with the aid of Fourier transformation.

The conventional well-known method of viewing NMR consists in immersing a test sample containing gyromagnetic nuclei in to a unidirectional polarizing magnetic field H₀, subjecting this test sample to the effect of a radio-frequency magnetic field with a frequency ω perpendicular to the sense of H₀, and displaying the component of magnetization of the test sample perpendicular to H₀ at a frequency of nuclear magnetic resonance in the field H₀ in accordance with the relationship ω₀ = γH₀, where γ is a nuclear gyromagnetic ratio. For obtaining the NMR spectrum, one of the parameters H₀ or ω is swept within the range where the NMR condition is satisfied.

In accordance with the method described above, a conventional NMR spectrometer comprises a magnet which provides a polarizing magnetic field H₀ ; an inductance coil which contains a test sample and is located in the field H₀ so that the coil axis is perpendicular to this field; a source of radio-frequency oscillations at a frequency ω, and a receiver tuned to a frequency ω₀, the source of radio-frequency oscillations and the receiver being connected to the inductance coil.

The reduction of the effects of nuclear dipolar spin-spin interactions in solids has untill now been achieved by the following method.

A known method consists in mechanical rotation of a test sample about an axis which lies at a so-called "magic angle" of 54°44' to the direction of the field H₀. To achieve the reduction of dipolar interactions in typical solids, the rotation speed must be 10⁶ revolutions per minute which renders this method impractical for extensive use.

Another known method consists in applying to a test sample placed in a polarizing magnetic field H₀ a continuous radio-frequency pulse of an exciting magnetic field directed perpendicularly to H₀ and having an amplitude 2H₁, the frequency ω of the exciting radio-frequency field being selected such that the relationship γH₁ /(ω - γH₀) = ±√2 is fulfilled, and the value H₁ exceeds the average value of the local field produced by the gyromagnetic nuclei of the test sample. After the exciting radio-frequency pulse has been terminated, the NMR signal is detected by registering the component of magnetization of the sample perpendicular to H₀ at a frequency ω₀ = γH₀. The required information can be obtained only after repeating the experiment many times at different lengths of the exciting radio-frequency pulse which requires a considerable observation period. Besides, additional complex processing of the output signal (Fourier analysis) is needed to obtain a required NMR spectrum.

Another known method consists in that a test sample is placed in a polarizing field H₀ and is subjected to the effect of an exciting magnetic field in the form of definite sequences of short radio-frequency pulses, the time intervals between the pulses, the length, amplitude and phases of the radio-frequency oscillations in the pulses being specially programmed. The NMR signal is registered in time intervals between the pulses which makes it possible to reduce the observation time as compared with the method described above. However, the output signal obtained by this means also requires interpretation using Fourier transformation, and the realization of this method needs a highly complicated pulsed apparatus.

Known in the art are also method and devices for viewing NMR in which the component of magnetization of the test sample parallel to the field H₀ is registered. Thus, a known method consists in placing a test sample in a polarizing magnetic field H₀, subjecting this sample to the effect of a magnetic radio-frequency field which causes saturation of nuclear magnetic resonance, and after switching off this saturating field, registering the change in the component of magnetization of the sample parallel to H₀ which is due to nuclear spin-lattice relaxation. A respective apparatus comprises a pick-up coil which has its axis parallel to H₀ and is connected to a receiver tuned to a frequency of the order of T₁ ^-1, where T₁ is the time of nuclear spin-lattice relaxation (usually T₁ ≧ 10^-3 sec). This method, however, fails to provide the reduction of the effect of nuclear dipolar interactions in solids.

Known in the art is also a method of viewing nuclear magnetic resonance which consists in placing a sample material containing gyromagnetic nuclei into a unidirectional polarizing magnetic field H₀ set up by a magnetic system; applying to this sample a radio-frequency magnetic field directed perpendicularly to the unidirectional polarizing magnetic field and set up by an exciting coil which is electrically coupled with a generator of radio-frequency oscillations; viewing the component of magnetization of the test sample longitudinal to the unidirectional polarizing magnetic field with the aid of a pick-up coil which is electrically coupled with a receiver; and viewing magnetic resonance by viewing changes in said longitudinal component of magnetization.

In the above method the frequency of the radio-frequency magnetic field is swept through the NMR region at such a rate as to meet the fast adiabatic passage condition, and said longitudinal component of magnetization is viewed by detecting its changes at a frequency determined by the rate of the fast adiabatic passage. In this method, a receiver used is a sensitive magnetometer.

The above method fails to provide the reduction of the effects of nuclear dipolar interactions which imposes restrictions on the resolution of the NMR spectrometer used for testing solids.

It is an object of the present invention to provide a method of viewing nuclear magnetic resonance which makes it possible to view nuclear magnetic resonance at a NMR frequency in the frame of reference rotating about the direction of a polarizing magnetic field at a frequency of a radio-frequency magnetic field which acts on the test sample.

It is another object of the invention to reduce the effects of nuclear dipolar spin-spin interactions and, as a result, to raise the resolution of NMR in solids.

Still another object of the invention is viewing of NMR directly in the form of a frequency spectrum.

To achieve the foregoing objects, a method of viewing nuclear magnetic resonance, comprising the steps of: immersing a test sample of material containing gyromagnetic nuclei into a unidirectional polarizing magnetic field set up by a magnetic system; subjecting this test sample to the effect of a radio-frequency magnetic field directed perpendicularly to the unidirectional polarizing magnetic field and set up by an exciting coil which is electrically coupled with a generator of radio-frequency oscillations; selecting an amplitude of said radio-frequency magnetic field so as to exceed the average local magnetic field set up by the gyromagnetic nuclei in the test sample, viewing the component of magnetization of the test sample longitudinal towards the unidirectional polarizing magnetic field with the aid of a pick-up coil which is electrically coupled with a receiver; according to the invention, comprises also the steps of viewing changes in said longitudinal component of magnetization at a frequency of nuclear magnetic resonance in an effective magnetic field H_ef, the magnitude whereof is calculated from the relationship: ##EQU1## where H₀ = intensity of the unidirectional polarizing magnetic field, H₁ = half amplitude of the radio-frequency magnetic field,

ω = frequency of the radio-frequency magnetic field,

γ = gyromagnetic ratio of nuclei in the test sample,

and viewing nuclear magnetic resonance by changes in said longitudinal component of magnetization, said longitudinal component of magnetization being viewed with a receiver tuned to the frequency of nuclear magnetic resonance in said effective magnetic field.

It is expedient that the frequency of the radio-frequency magnetic field be selected so as to meet the condition: ##EQU2##

It is advantageous that said longitudinal component of magnetization of the test sample be viewed by additionally subjecting this test sample to the effect of an alternating magnetic field at a frequency Ω which is directed in parallel to the unidirectional polarizing magnetic field and set up by said pick-up coil electrically coupled with a generator of electrical oscillations at a frequency Ω, and by sweeping at least one of the parameters H₀, H₁, ω, Ω within the range where the resonance condition:

Ω = γHef 

is satisfied.

It is advisable that the parameters H₀, H₁, ω, Ω be selected so as to simultaneously satisfy the relationships:

Ω = γHef, ##EQU3##

It is also expedient that said longitudinal component of magnetization of the test sample be viewed through modulating the frequency or the amplitude of said radio-frequency magnetic field at a frequency Ω_m by a modulator electrically connected to said generator of electrical oscillations, and through sweeping at least one of the parameters H₀, H₁, ω, Ω_m within the range where the resonance condition

Ωm = γHef 

is satisfied.

It is advisable that the parameters H₀, H₁, ω, Ω_m be selected so as to simultaneously the relationships:

Ωm = γHef, ##EQU4##

The preferred method of viewing nuclear magnetic resonance makes it possible, using simple means and within a short time, to appreciably increase the resolution of NMR in solids and, as a result, to provide valuable information on chemical bonds, electron-nuclear interactions and other internal properties of substances. The preferred method makes it also possible to provide new effective methods for physical investigation of dynamic and relaxation processes in nuclear spin systems.

The invention will be made clear by the following description of preferred embodiments thereof when read in conjunction with the accompanying drawings, in which:

FIG. 1 is a vector representation of magnetic fields and magnetization of the test sample in a rotating frame of reference, according to the invention;

FIG. 2 is a block diagram of an apparatus for carrying into effect the proposed method of viewing NMR, according to the invention;

FIG. 3 is a block diagram of another embodiment of the apparatus for carrying into effect the proposed method, according to the invention;

FIG. 4 is a block diagram of a third embodiment of the apparatus for carrying into effect the proposed method, according to the invention.

Consider a material containing gyromagnetic nuclei which is placed in a static magnetic field H₀ directed along the Z-axis of the Cartesian coordinate system. The movement of the magnetic moments in this field is Larmor precession about the Z-axis at an angular frequency ω₀ = γH₀, where γ is a nuclear gyromagnetic ratio. Assume that the strength of the field H₀ is sufficiently large to provide noticable magnetization of the magnetic moments, i.e. the orientation of their Z-components in the direction of H₀ (typical values of H₀ are 10³ to 10^-4 oerst).

Further, apply to this material a radio-frequency magnetic field with a frequency ω close to ω₀, and an amplitude 2H₁ is directed perpendicular to the Z-axis. In order to describe the movement of the magnetic moments in these conditions, it is convenient to change to a frame of reference which rotates about the Z-axis in the direction of the Larmor precession of the nuclei at a frequency ω.

The vector representation of magnetic fields in the rotating frame of reference is illustrated in FIG. 1.

In FIG. 1, the Z-axis indicates the sense of a polarizing magnetic field H₀ ; vectors H₁ and H₀ - (ω/γ) denote, respectively, the transverse and longitudinal (relative to the Z-axis) components of the magnetic field in the rotation frame of reference; vector H_ef is an effective magnetic field in this frame of reference; θ is an angle between H_ef and the Z-axis; M is nuclear magnetization of a test sample which precesses about H_ef ; M.sub.⊥^r is a component of the vector M in the sense perpendicular to H_ef ; M_z ^r is a projection of the vector M.sub.⊥^r onto the Z-axis; vector H.sub.⊥^ef is a component of an additional alternating magnetic field at a frequency Ω perpendicular to the sense of H_ef.

In such a rotating frame, said radio-frequency field becomes a static magnetic field with strength H₁, and the magnetic field H₀ is reduced to the value H₀ - (ω/γ) (FIG. 1). The resulting effective magnetic field H_ef in the rotating frame is, consequently, equal to ##EQU5## and is inclined to the Z-axis at an angle θ equal to: ##EQU6##

In the rotating frame of reference, nuclear magnetic moments undergo Larmor precession about the direction H_ef (FIG. 1) at an angular frequency

Ω0 = γHef.

At this frequency the well-known nuclear magnetic resonance must occur in the rotating frame, the viewing of this phenomenon being the object of the present invention.

For viewing NMR in the rotating frame, it is necessary to register the component M.sub.⊥^r of magnetization M of the sample which is perpendicular to the direction of H_ef (FIG. 1).

In FIG. 1 it can be seen that rotation of the vector M.sub.⊥^r about H_ef at the angular frequency Ω₀ causes the appearance of the component M_z ^r of magnetization which is longitudinal relative to the Z-axis and oscillates at the same frequency Ω₀. The viewing of this longitudinal component at the frequency Ω₀ is the subject of the invention.

If a radio-frequency magnetic field is applied to a sample abruptly, this causes the damped precession of the equilibrium magnetization of the sample around the sense of H_ef which induces in the above-mentioned pick-up coil damped oscillations at a frequency Ω₀. The waveform of these oscillations is the Fourier transform of the NMR frequency spectrum.

For viewing NMR in the rotating frame using stationary means, it is necessary to apply to the test sample a weak (non-saturating) alternating magnetic field with a frequency Ω equal or close to Ω₀ which has the non-zero component H.sub.⊥^ef perpendicular to the sense of H_ef (FIG. 1). Such a field can be induced by a coil the axis of which is parallel to Z, or through modulating the frequency ω of the radio-frequency magnetic field at a frequency Ω_m ≃ Ω₀ which will result in a respective modulation of the value H₀ - (ω/γ) of the Z-component of the field H_ef and in the appearance of the required variable component H.sub.⊥^ef. The same result can also be obtained, as can be seen from FIG. 1, by modulating the value of H₁, i.e. the amplitude of the radio-frequency magnetic field, if θ ≠ (π/2).

In all these cases direct viewing of the required NMR spectrum can be accomplished through sweeping at least one of the parameters H₀, ω, H₁, Ω, Ω_m within the range where the resonance condition

Ω = γHef or Ωm = γHef 

in the rotating frame is satisfied.

It is well known that in the rotating frame nuclear dipolar spin-spin interactions are partially damped (see, for instance, A. G. Redfied, Physical Review, 98, 1787 /1955/). Therefore, viewing of NMR with the aid of the proposed method causes narrowing of the NMR spectrum lines in solids and, consequently, increases the resolution of an NMR spectrometer. The maximum reduction of nuclear dipolar interactions occurs on the condition that:

θ = θm = arc cos 1/√3,

where θ_m = 54°44', i.e. the so-called "magic angle". Here, the value of H₁ must exceed the average strength of the local magnetic field H_L set up by the gyromagnetic nuclei of the test sample.

It follows from FIG. 1 that for the condition θ = θ_m to be satisfied, the parameters of the polarizing and radio-frequency magnetic fields must be selected according to the relationship: ##EQU7## which must be satisfied simultaneously with the above resonance condition in the rotating frame of reference.

In order to have the maximum amplitude of the viewed NMR signal in the rotating frame, the maximum nuclear magnetization of the test sample must be maintained during the experiment. For this purpose, it is recommended that the duration of the experiment should be shorter than the nuclear spin-lattice relaxation time.

Below are given typical values of the parameters used. For an ordinary solid containing hydrogen or fluorine nuclei, γ/2π ≈ 4.10³ Hz/Oe, H_L ≈ 1 Oe. In the field H₀ = 10⁴ Oe the frequency ω₀ /2π ≈ 40 MHz which corresponds to the range of a typical conventional NMR spectrometer. Selecting H₁ = 20-100 Oe and using the condition θ = θ_m, we obtain H_ef ≈ 25-125 Oe and Ω₀ = γH_ef ≈ 100-500 kHz. At these levels of the parameters, the effect of nuclear dipolar interactions is reduced 100 to 1000 times.

A test sample 1 (FIG. 2) of a material containing gyromagnetic nuclei (a CaF₂ crystal in the embodiment being described) is immersed into a unidirectional polarizing magnetic field H₀ shown in the drawing by an arrow, which is set up by a magnetic system 2 of an apparatus for carrying into effect the method of NMR viewing. The sample 1 is inside an exciting coil 3 and a pick-up coil 4 of the above apparatus.

The axis of the exciting coil 3 is oriented perpendicular to the field H₀, and the coil 3 itself is electrically connected to a generator 5 of radio-frequency oscillations at a frequency ω. The axis of the pick-up coil 4 is oriented parallel to the field H₀, and the coil 4 itself is connected to an input of a receiver 6 tuned to a frequency Ω₀ of nuclear magnetic resonance in the effective magnetic field H_ef (FIG. 1) in a frame of reference rotating around H₀ with the frequency ω in the direction of the Larmor precession of the nuclei in the sample I, where H_ef is found from the relationship: ##EQU8##

In the second embodiment of the apparatus, electrical coupling of the generator 5 (FIG. 2) with the coil 3 is through a power amplifier 7 (FIG. 3) tuned to the frequency ω of the generator 5, and through a switch 8 which connects the output of generator 5 to the input of the amplifier 7. The power amplifier 7 is of well-known design, for example, of the type described by Jones, Donglass and McCall, Review of Scientific Instruments, 36, 1460/1975.

In the described embodiment, the receiver 6 comprises a variable capacitor 9 which is connected in parallel with the coil 4 and forms with the coil a resonance circuit tuned to a frequency Ω₀. The coil 4 and the capacitor 9 are connected to the input of a low-pass LC-filter 10 which provides undistorted passage of signals at the frequency Ω₀ and suppression of signals at the frequency ω. The output of the LC-filter 10 is connected to the input of a resonance amplifier II tuned to the frequency Ω₀. The output of the amplifier II is connected to the input of an amplitude detector 12 the output of which is connected to the Y-input of a display device 13 (an oscilloscope in the preferred embodiment of the invention).

The magnetic system 2 comprises a power supply unit 14 of well-known design, for example, of the type V-FR 2503 Fieldial Mark I, produced by Varian in the USA, connected to the winding of a conventional electromagnet 15.

For obtaining a nuclear magnetic resonance spectrum on the screen of the display device 13, the above circuit comprises additionally a conventional A.C. voltage generator 16 operating at a frequency Ω which is connected through a resistor 17 to the coil 4. The resistance of the resistor 17 exceeds the active equivalent resistance of the resonance circuit formed by the coil 4 and the variable capacitor 9, at the frequency Ω₀.

The circuit also comprises a sweeping unit 18 which is basically a conventional infrasonic-frequency A.C. generator. The unit 18 is connected via a switch 19 to an input of the external control device of the power supply unit 14, via switches 20 and 21 to control inputs regulating, respectively, the oscillation frequency and amplitude of the generator 5, and via a switch 22 to the frequency control input of the generator 16. Besides, the output of the sweeping unit 18 is connected to the X-input of the display device 13.

The third embodiment of the apparatus for viewing nuclear magnetic resonance employs a circuit similar to that described above.

Its difference is that it comprises a modulator 23 (FIG. 4) which is basically a conventional A.C. voltage generator operating at a frequency Ω_m. For modulating the frequency or the amplitude of the radio-frequency magnetic field, the output of the modulator 23 is connected via a switch 24, respectively, to the frequency or amplitude modulation inputs of the generator 5. Besides, the output of the modulator 23 is connected via a conventional phase shifter 25 to the control input of a phase detector 26 which is used in this embodiment of the apparatus instead of the amplitude detector 12 (FIG. 3).

For sweeping the modulation frequency Ω_m the output of the sweeping unit 18 is connected via a switch 27 to a frequency control input of the modulator 23.

According to the invention, nuclear magnetic resonance is viewed as follows.

The test sample 1 (FIG. 2) is immersed into a unidirectional polarizing magnetic field H₀ set up by the magnetic system 2. The purpose of the magnetic field H₀ is to cause polarization of nuclear magnetic moments in the sample 1. Radio-frequency voltage is applied at a frequency ω from the generator 5 to the exciting coil 3, thereby inducing at the sample 1 a radio-frequency magnetic field at the frequency ω oriented perpendicularly to the field H₀, the amplitude of this radio-frequency magnetic field being selected so as to exceed the average magnitude of a local magnetic field caused by the gyromagnetic nuclei of the sample 1. The precession of nuclear magnetization of the sample 1 in the effective magnetic field H_ef (FIG. 1) in the rotating frame of reference causes the appearance of the component of magnetization of the sample 1 longitudinal to the field H₀ (FIG. 2). The component of magnetization oscillates at a frequency Ω₀ = γH_ef of nuclear magnetic resonance in the effective field H_ef. Nuclear magnetic resonance is viewed by detecting this longitudinal component with the aid of the pick-up coil 4 in which the NMR signal at a frequency Ω₀ is induced. This signal goes to the receiver 6 tuned to the frequency Ω₀ where it is amplified, detected and observed or recorded.

The NMR signal at the frequency Ω₀ can be registered by any known means used in NMR spectroscopy, for instance, by the free induction, spin echo, fast adiabatic passage, steady-state absorption or dispersion methods. Certain versions of registrating are illustrated in FIGS. 3, 4.

The free induction method consists in closing a switch 8 (FIG. 3) to apply radio-frequency voltage at a frequency ω from the generator 5 through the power amplifier 7 to the exciting coil 3. Immediately following this delivery of voltage, damped oscillations of the frequency Ω₀ are induced in the pick-up coil 4 and are sent to the receiver 6. In this case additional processing of the output signal by Fourier transformation is required to obtain a desired NMR spectrum.

The same means may be used for viewing NMR during pulsed operation of the generator 5 according to any preset program.

Steady-state methods are recommended for direct viewing of a required NMR spectrum. One of such methods, a so-called method of a "Q-meter" (see, for example, E. Andrew, Nuclear Magnetic Resonance, Cambridge, 1955) is illustrated in FIG. 3.

Alternating voltage of a frequency generated by the generator 16 is delivered through the resistor 17 to the pick-up coil 4. The resistor 17 is intended to prevent shunting of the resonance circuit formed by the coil 4 and the capacitor 9 by the internal resistance of the generator 16. The above voltage induces at the sample 1 an alternating magnetic field of a frequency Ω oriented parallel to the polarizing magnetic field H₀.

In these conditions at least one of the parameters H₀, ω, H₁, Ω is swept within the range where the resonance condition in the rotating frame:

Ω = γHef 

is satisfied.

According to the means shown in FIG. 3, the parameter H₀ is swept. For this purpose, infrasonic frequency voltage at a frequency of, for example, 0.5 Hz, is applied from the sweeping unit 18 through a closed switch 19 to the power supply unit 14 of the electromagnet 15 causing periodic changes in the value of the magnetic field H₀ in the above range. When the field H₀ passes through the resonance condition, the energy of the alternating magnetic field with a frequency Ω = Ω₀ is absorbed in the sample 1. The resulting voltage change at the resonance circuit formed by the coil 4 and the capacitor 9 passes through the low-pass filter 10 which suppresses leakage of the radio-frequency signal at a frequency ω, is amplified in the amplifier 11 and detected by the amplitude detector 12. From the output of the detector 12, the signal is applied to the Y-input of the display device 13.

At the same time, a sweep voltage is applied from the sweeping unit 18. As a result, a required NMR spectrum can be viewed directly on the display device 13.

For sweeping other said parameters ω, H₁, Ω or for simultaneous sweeping of several parameters, the switches 20, 21, 22, respectively, are closed. In this case, the NMR spectrum is viewed in the same way as when sweeping the parameter H₀.

Another version of the proposed method is illustrated in FIG. 4. In this version, the frequency or the amplitude of the radio-frequency magnetic field of a frequency ω is modulated at a frequency Ω_m for viewing a NMR spectrum. Voltage at a frequency Ω_m is applied from the modulator 23 through the switch 24 to the frequency or amplitude modulation inputs of the generator 5. In this version, the position of the switch 24 corresponds to frequency modulation.

Frequency-modulated radio-frequency oscillations from the generator 5 are amplified, after closure of the switch 8, in the power amplifier 7 and applied to the exciting coil 3. If the resonance condition Ω_m = γH_ef is satisfied which is made possible through the above sweeping of H₀, a NMR signal is induced in the coil 4 at a frequency Ω_m = Ω₀, applied to the receiver 6 and registered in the way described above. In contrast to the circuit of FIG. 3, in FIG. 4 the amplitude detector 12 is replaced by the phase discriminator 26 which is controlled by Ω_m -frequency reference voltage fed from the modulator 23 through the phase shifter 25. The phase of the reference voltage is selected so as to enable display of a signal propertional either to the real part of the resonant magnetic susceptibility at a frequency Ω_m (a dispersion signal) or to the imaginary part of this susceptibility (an absorption signal).

The NMR spectrum is viewed in the same way when sweeping the modulation frequency Ω_m, for which purpose voltage from the output of the sweeping unit 18 is applied to the frequency control input of the modulator 23 by closing the switch 27.

When viewing NMR using any of the described method, in order to achieve maximum reduction of the effects of nuclear dipolar interactions and maximum resolution of the NMR spectrometer, the parameters of the polarizing and alternating magnetic fields must be selected so as to satisfy at the same time the "magic angle" condition: ω = γ(H₀ ± H₁ /√2), and the condition of resonance in the rotating frame of reference:

Ω = γHef or Ωm = γHef.

For meeting both conditions simultaneously, it is necessary to preselect appropriate relationships between the parameters which do not change during the experiment. Thus, if the frequency Ω is swept, the parameters ω, H₀ and H₁ are preselected in accordance with the above "magic angle" condition; if the value of H₀ or frequency ω is swept, the parameters H₁ and Ω must be preadjusted to satisfy the relationship

Ω √2 = γH1 √3

which follows directly from simultaneous satisfaction of the two above conditions.

Simultaneous sweeping of several parameters is also possible, for example, sweeping of the parameters H₀ and H₁ in such as way as to meet the above "magic angle" condition throughout the experiment.

The entire experiment must be completed within the time shorter than the time of spin-lattice relaxation of the gyromagnetic nuclei in the test sample.

Thus, the method of viewing NMR according to the invention makes it possible to increase the resolution of NMR spectra, particularly in solids without using complex and costly pulsed apparatus and the Fourier transformation of the output signal. High-resolution NMR spectra are provided using traditional well-designed steady state methods noted for simplicity, reliability and low costs.