Tunable RF probe for use in NMR spectroscopy experiments and method of tuning

Abstract: A tunable element of an RF resonant circuit in an NMR RF probe including: an inner conductor having a variable length and a first and second end; a movable contact strip at the second end; and the inner conductor electrically connected to an outer grounded conductor via the contact strip. A tunable element, which has an electrical length with a first and second end, including: components for varying the electrical length; the second end connected to near ground; and a matching element electrically connected to the tunable element between the first and second ends. An NMR RF probe having: an RF terminal, a sample coil, and an RF resonant circuit with a matching element electrically connected to a tunable element between a top and bottom end of the tunable element. The tunable element's electrical length can be varied. Furthermore, a method for tuning and matching an RF resonant circuit of an NMR RF probe is described.

Description: BACKGROUND OF THE INVENTION The present invention relates generally to single-, double-, triple-, or quadruple-tuned Nuclear Magnetic Resonance (NMR) probes. And more particularly, this invention relates to single radio-frequency (RF) coil NMR probes, which are tunable by changing the geometry of a single-port tunable element, for use in single-, double-, triple-, or quadruple-resonance spectroscopy experiments. Samples studied using NMR spectroscopy equipment can be irradiated with up to four RF signals (each having a different frequency) generated by, typically, one or more RF coils. A "single-coil" NMR probe uses one RF coil capable of generating the desired RF signal(s) as well as receiving/detecting resultant signals radiated from a sample. In operation, the RF coil of a single-coil NMR probe transmits RF energy at the desired frequency(ies) to excite nuclear spins (a nuclear spin is the total angular momentum of an atomic nucleus) in a sample. When an RF excitation ceases, the excited nuclei of the sample radiate energy that is detected by the RF coil. Most NMR systems irradiate samples with RF energy at multiple frequencies. For example, double-resonance NMR experiments performed on solid samples utilize NMR probes capable of transmitting RF signals at two frequencies: a low RF frequency and a high RF frequency. Probes used in double-resonance NMR experiments are commonly referred to as "double-tuned" since the high-frequency and the low-frequency resonant circuits must both be tuned. Likewise, triple-resonance NMR experiments utilize "triple-tuned" NMR probes capable of transmitting RF signals at three frequencies: a low, middle, and high RF frequency. Probes used in triple-resonance NMR-experiments are commonly referred to as "triple-tuned". Although not as commonly used today, one can use separate RF coils for transmitting and receiving rather than a single RF coil capable of doing both. One known NMR probe for use in double-resonance NMR experiments uses two separate orthogonal coils for transmitting RF signals--one coil is capable of transmitting the high-frequency RF signal and the other capable of transmitting the low-frequency RF signal. An advantage of these dual-coil probes is that the low- and high-frequency circuits are physically isolated. One problem with these dual-coil probes is that they promote inhomogeneities in the two RF frequency fields produced. RF field inhomogeneities lead to a degradation of the quality of experimental results. Another problem with the dual-coil probes is that they have an inner and an outer coil. The outer coil operates less efficiently since it has greater spatial separation from the sample. Additionally, a problem of arcing between the two coils usually limits this type of known probe to low power experiments. A typical double-resonance experiment involves irradiating a sample with a high-frequency RF signal while a lower frequency radiation from the sample is observed. For experiments using solid-state samples, the high-frequency power level is generally 70-600 watts whereas the low frequency radiation from the sample may be less than a nanowatt. Regardless of the number of RF signal transmit coils used in an NMR probe, it is desirable to isolate the high-frequency circuit from the low-frequency circuit in double-tuned NMR probes. Similarly, it is desirable to isolate all three frequencies from each other in a triple-tuned NMR probe. One type of conventional single-coil double-resonance NMR probe is discussed in an article titled "Single-coil Probe With Transmission-Line Tuning for Nuclear Magnetic Double Resonance" written by V.R. Cross, R. K. Hester, and J. S. Waugh. The article appears in the Review of Scientific Instrumentation, Vol. 47, No. 12, December 1976. The Cross probe uses variable length transmission lines to tune the circuits. The tuning range of the high-frequency (HF) circuit is limited since most of the voltage in the high-frequency circuit is across this fixed capacitor. Also, if only a moderate voltage drop is placed across the fixed capacitor, then the variable transmission line will have the effect of increasing the voltage across the variable capacitor. In addition to the variable-length transmission lines, an open transmission-line segment and a shorted transmission-line segment are still required for frequency isolation. The losses in these transmission lines make the Cross probe impractical for use with today's high-frequency spectrometers. Turning to the known probe at 100 in Figure 1, variable tuning capacitors 108A, 108B replace the variable length transmission lines of the Cross probe. Furthermore, no fixed capacitor has been included in probe 100. RF sample coil 102 is used to generate the dual-frequency radiation and detect the radiation from the excited sample nuclei. Shorted transmission line segment 104 (its center conductor has been grounded) has a high input impedance at the high frequency, but passes the low frequencies to ground to isolate the low-frequency power from the high-frequency side 116 of the probe 100. Open transmission line segment 106 passes the high-frequency to ground to isolate the high frequency from the low-frequency side 114 of the probe 100. One disadvantage of the single-coil double-resonance NMR probe 100 is that it requires four high voltage, high current variable capacitors 108A, 108B, 108C, 108D. Not only do these capacitors consume space, but the operating power level of the probe 100 is limited as a result of including these capacitors. Other disadvantages of probe 100 include: the finite impedance presented by the shorted transmission line segment 104 results in a dramatic loss in high-frequency efficiency; and the low-frequency side 114 is difficult to tune at the frequencies on the high end of the low-frequency range. In "A Multinuclear Double-Tuned Probe for Applications with Solids or Liquids Utilizing Lumped Tuning Elements" by F. David Doty, Ruth R. Inners, and Paul D. Ellis, appearing in the Journal of Magnetic Resonance 43, pp. 399-416 (1981), another single-coil double-resonance NMR probe is disclosed. The Doty probe uses lumped element equivalents (combinations of capacitors and inductors) in place of the transmission line segments 104, 106 of probe 100 in Figure 1. A primary disadvantage of this design is that the variable inductor used in the high-voltage region of the probe (see pages 412-413 of the Doty article) introduces significant low-frequency losses and limits the range of high-frequency applications. US -A-4,446,431 issued to Robert A. McKay describes yet another single-coil double-resonance NMR probe. The McKay probe uses a tapped transmission line having. two segments and a Junction Point B where the low frequency input and detection circuit connects to the transmission line. Disadvantages of the McKay probe are as follows: the length of the tapped transmission line results in losses at both frequencies (which is a problem, in particular, for probes operating at a high-frequency above 300MHz); the probe does not isolate the low-frequency energy from the high-frequency circuit; both the high-frequency and low-frequency portions of the probe are at high voltage on the same side of the sample coil which increases the possibility of arcing; and, each time a different high-frequency is chosen, Junction Point B must be changed which limits the high-frequency tuning range of the McKay probe. Another use of the variable length transmission line in an NMR probe is described in US-A-5055792. This Patent discloses the use of a two-port two wire transmission line segment to replace variable inductors in a multi-frequency circuit in which a cascade of tank circuits is used to combine several frequencies to operate from a single RF port. In accordance with a first aspect of the present invention, there is provided an NMR probe for transmitting RF energy between a source and a sample coil, as defined by Claim 1. In accordance with a second aspect of the present invention, there is provided a method for tuning and matching an RF resonant circuit of an NMR RF probe, as defined by Claim 17. BRIEF DESCRIPTION OF THE DRAWINGS The present invention will be described with reference to the accompanying drawings, wherein: Fig. 1 is a schematic illustrating a known single-coil double-tuned NMR probe 100 using transmission line segments 104, 106 for frequency isolation and capacitors for circuit tuning. Fig. 2 is a schematic of a single-coil double-tuned NMR probe 500 of the present invention. Fig. 3 is a schematic of a single-coil triple-resonance NMR probe 600 of the present invention. Fig. 4 is an exploded-assembly illustrating one set of preferred mechanical components which can be assembled to form a single-port tunable element such as that shown in Figure 2. Fig. 5 is a schematic incorporating certain mechanical features of the Fig. 4 tunable element with the electrical schematic of Fig. 2. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS To perform NMR spectroscopy, an NMR probe is used to generate and detect RF signals which are processed by the spectrometer to produce a spectrum. The tunable element NMR probe of the present invention can be used with most existing standard NMR spectrometers without any modifications to the spectrometers. An example of a spectrometer to which this probe may be interfaced is the CMX-II Spectrometer available from Chemagnetics in Fort Collins, Colorado. Figure 2 illustrates a single-port tunable element NMR probe 500 for use in double-resonance spectroscopy experiments. The tunable element NMR probe 500 includes off-the-shelf components as well as a custom fabricated single-port tunable element 556. Sample coil 552 is used to irradiate a sample (not shown, but is positioned within the windings of the sample coil) to be analyzed with high- and low-frequency RF energy. Sample coils are typically made out of silver-plated copper wire into a helix. High-frequency RF energy is input to the probe via high-frequency terminal 554 from a spectrometer (not shown). Low-frequency RF energy is input to the probe from the spectrometer at a low-frequency terminal 562. These inputs are located at either end of sample coil 552. The sample coil 552 irradiates the sample being analyzed with these RF frequencies. The sample coil 552 also receives low- and high-frequency RF radiation from the sample. This detected radiation resonates in the sample coil as well as tuned circuits 560, 570 of the NMR probe 500 (discussed in greater detail below). Low-frequency detected radiation is sent to the spectrometer through low-frequency terminal 562. High-frequency detected radiation is sent to the spectrometer through the high-frequency terminal 554. Low-frequency RF energy detected by the sample coil resonates in the sample coil 552 and the low-frequency resonant circuit 570 of the probe. As illustrated, the low-frequency resonant circuit 570 comprises a tuning capacitor 566, for tuning circuit 570, and a matching capacitor 568. The tuning capacitor 566 also isolates the high-frequencies from the low-frequency portion of the probe 500 by shorting the high frequencies to ground through variable capacitor 566. The low-frequency circuit 570 must be impedance matched, using suitable means such as a matching capacitor 568, to the impedance of the spectrometer channel (not shown) used and the impedance of the preamplifier used (not shown). High frequencies transmitted to, or detected from, the sample by the sample coil 552 resonate in the sample coil 552 and high-frequency circuit 560. The unique design of high-frequency resonant circuit 560 includes a tunable element 556 and a matching capacitor 558 located between high-frequency terminal 554 and the inner conductor of tunable element 556 at point B. The physical location of the electrical connecting point of matching capacitor 558 and the inner conductor of tunable element 556 is not critical. Not only is the tunable element 556 used to tune the high-frequency resonant circuit 560, but it operates to isolate the low-frequency energy from high-frequency circuit 560 and it allows for positioning of high-frequency matching capacitor 558 away from the high voltage region (near point C) of the probe. Tuning of the high-frequency resonant circuit 560 at a desired frequency is accomplished by changing the conductor length ℓ A of the tunable element. This changes the impedance seen by the sample coil 552. Changing the length of the tunable element 556 illustrated in Figure 2 is accomplished by sliding a contact strip 564 along a portion of the length of the tunable element 556. The contact strip 564 shorts the inner conductor of the tunable element 556 to its grounded housing (not labeled) at a point A. The tunable element 556 is tuned so that, at grounded point A, the high-frequency voltage level is zero and the high-frequency current is high. As already mentioned briefly, tunable element 556 can isolate the low-frequencies from the high-frequency terminal 554 to minimize interference with the high-frequency signals sent to the spectrometer. The low-frequency voltage is grounded at point A via the inner conductor and contact strip 564. Since the length of the tunable element 556 is short compared to the wavelength of the low frequencies, the low-frequency voltage is fairly constant along the entire length of the tunable element 556. Therefore, the low-frequency voltage is no more than a few volts at point B, where it would most interfere with the high-frequency signal if the voltage was high. Furthermore, the reactance of high-frequency matching capacitor 558 is high for the low-frequencies used. The design of present invention allows one to position matching capacitor 558 in a low-voltage region of the probe 500. Grounded point A is the point where the high-frequency voltage is minimum; zero for a properly tuned circuit. A point C near the coil 552 is the point at which the high-frequency voltage is maximum. The matching capacitor 558 is electrically connected to the inner conductor at point B. The closer point B is to point A, the lower the voltage at point B. In the preferred embodiments of Figures 2-5, there is a tradeoff to moving point B closer to point A: as point B is moved closer to point A, the tuning range of the tunable element RF probe 500 is diminished. If, for example, point B is positioned at a point 52% of the distance from point A to point C, the tuning range is 40% of the high-frequency. In Figure 2, point B is positioned at a point approximately 30% of the distance from point A to point C. This provides a tuning range of 25% of the high-frequency value chosen and positions the matching capacitor 558 at a low enough voltage level to satisfy safety concerns. A tuning range of 25% of the high-frequency is a substantial improvement over conventional single-coil double-tuned NMR probes, which typically have tuning ranges of about 2%. Component values for the embodiment are illustrated by the following example. For a probe operating at a high-frequency of 400 Mhz and a low-frequency from 40-160 Mhz, typical component values are as follows. The high-frequency matching capacitor 558 is a 0.3-3.0 picofarads (pf) variable capacitor; the sample coil is 200 nanohenrys (nH); the low-frequency tuning capacitor is 1-80 pf; and the low-frequency matching capacitor is 1-7 pf. For operation at different frequencies, one with ordinary skill in the art can easily determine new component values. The length of the tapped tunable element 556 is chosen to be slightly longer than λ√4 where λ is the wavelength of the high-frequency. Figure 3 illustrates a second embodiment of the invention. In this second embodiment a single-port tunable element NMR probe 600 is provided for applications requiring three RF frequencies, a high-, a middle-, and a low-frequency. Tunable element 656 is utilized to: tune a high-frequency circuit 694, isolate the low-frequency energy from the high-frequency circuit 694, and remove the matching capacitor 658 from the high voltage region of the probe 600. A tuning capacitor 672 and a matching capacitor 674 are housed within the tunable element 656. These capacitors are provided to tune the low-frequency portion of the probe. The tuning capacitor 672 functions as a near short circuit at the high-frequency. Therefore, for high frequencies the function of the contact strip 664 of Figure 3 is equivalent to the function of the contact strip 564 in the embodiment represented in Fig. 2. Electrical length ℓ B is selected so that at point D the voltage of the high-frequency is zero and the current is high. The high-frequency signal is tapped, at point E, into the tunable element 656. This point is chosen to optimize the tuning range of the circuit while removing the matching capacitor from the high voltage region of the probe 600. The middle-frequency is introduced to the probe 600 at a middle-frequency input terminal 676. A matching capacitor 678 matches the impedance of the middle-frequency circuit 690 to the impedance of the spectrometer channel (not shown) used and the impedance of the preamplifier used (not shown). A tuning capacitor 680 tunes the middle-frequency resonant circuit 690. The tuning capacitor 680 also isolates the high-frequency from the middle-frequency circuit 690 by grounding the high-frequency. A stop coil 682 forms part of the middle-frequency and low-frequency resonant circuits 690, 692. The stop coil 682 isolates the low frequencies from the middle-frequency resonant circuit 690 by sending the low frequencies to ground. An important consideration in the design of the stop coil 682 is to control the fraction of the available middle-frequency and low-frequency energy that dissipated across the sample coil 652. For example, if the middle-frequency coil 682 is much larger than the sample coil 652, the middle-frequency current follows the sample coil 652 path. As a result, most of the middle-frequency energy is applied to the sample coil 652 and probe 600 performance is optimized for the middle-frequency-but the low-frequency performance will be poor. If the middle-frequency coil 682 is selected to be small in relation to the sample coil 652, the middle-frequency performance will be poor and low-frequency performance will be optimized. It is therefore necessary to find a compromise when selecting the sample coil 652 and middle-frequency coil 682. Coil 652, 682 sizes may be selected to optimize performance for the middle or low-frequency depending on the application. In this second embodiment, the probe 600 can be designed to operate at many different sets of frequencies. As an example, a high-frequency of 300 Mhz, a middle-frequency of 75 Mhz and a low-frequency of 30 Mhz, may be chosen. Typically, at these frequencies the low-frequency tuning capacitor 672 is selected at 100 to 120 picofarads, and the matching capacitor 674 is selected at 8 picofarads. The tunable element 656 length is 26 centimeters (slightly longer than λ/4 of the high-frequency). The high-frequency matching capacitor 658 value is 0.3- 3.0 pf. The middle-frequency coil 682 is 300 nH and the middle-frequency tuning capacitor 680 is 45pf. The middle-frequency matching capacitor 678 is 4pf. The sample coil is 350nH. Operation at this set of frequencies has been provided by way of example only. It will be obvious to one of ordinary skill in the art how to build a probe operating at other sets of frequencies. The electrical length ℓ A in Figure 2 or ℓ B in Figure 3 can be varied using means other than that illustrated in Figures 2-5, such as: positioning a dielectric material inbetween the inner conductor and outer grounded housing; terminate the lower end of the inner conductor with a very small variable reactance (by connecting a variable inductance of value much smaller than the sample coil 652); or any means of altering the characteristic impedance of the tunable elements 556 or 656. Each time a tube-shaped component (not shown) made of a different dielectric material is positioned between the inner and outer grounded housings, the effective electrical length of the tunable element will change. Variable matching capacitors 558, 658 can be replaced with other impedance matching means such as an antenna. For very high frequencies a waveguide having no inner conductor (not shown) may be substituted for tunable elements 556, 656--its effective electrical length can be varied by the same means as set forth above. Turning to Figure 4, an inner conductor rod 707 slides up and down within a hollow conductor tube 713 through a guide disk 708. The guide disk 708 guides inner conductor rod 707 into and through contact ring 712. The bottom of inner conductor rod 707 is electrically shorted to a grounded, conductive proton tuning tube 710 via conductive contact fingers 705a of a conductive contact ring 705 which has been secured onto a conductive slider plate 706. As shown, inner conductor rod 707 has a threaded portion 707a which can be screwed into slider plate 706. An RF tap point 716 has been provided through which a high-frequency generator and receiver may be connected via a high-frequency matching capacitor such as that shown at 558, 658 in Figures 2, 3. The end 703a of slider rod 703 is press-fit, or secured by other means, into slider-plate spacer 704 (which can be made of a nylon such as DELRIN® manufactured by E.I du Pont). Spacer 704 is fit into slider plate 706. A bottom nut 702 screws onto the slider rod 703, which has a threaded portion 703b. Slider rod 703 can be made of any suitable rigid insulative material such as plastic with sufficient mechanical integrity. The bottom nut 702 is threaded on the outside so that it may be secured into a threaded sleeve 709. The assembly consisting of the inner conductor rod 707, contact ring 705, slider rod 703, slider-plate spacer 704, and slider plate 706 are positioned within the proton tuning tube 710 by screwing threaded sleeve 709 onto the proton tuning tube. Conductor tube 713 is fitted with a conductive contact ring 712, which has conductive cantilever contact fingers 712a, and two TEFLON® centering spacers 711, 714. The conductor tube assembly, shown at 720, fits inside the proton tuning tube 710. It is necessary that conductor tube 713 be centered within proton tuning tube 710--centering spacers 711, 714 aid in accomplishing this. A conductor tube plug 715 fits onto the top end of the conductor tube 713. A knob 701, the outside of which has been knurled, is secured onto the end of slider rod 703 so that it may be used to turn slider rod 703. When knob 701 is turned (see, also, the arrow 800 in Figure 5) the threaded slider rod 703 turns within the internal threads of bottom nut 702. This causes the threaded slider rod 703 to move up or down within the proton tuning tube 710 depending upon the direction in which the knob 701 is turned. The movement of slider rod 703 causes inner conductor rod 707 to, correspondingly, slide up or down within conductor tube 713. See, also, Figure 5. As inner conductor 707 slides up into conductor tube 713, the wavelength to which tunable element 556 is tuned is shortened. Similarly, as the inner conductor 707 is retracted from within the conductor tube 713, the wavelength to which tunable element 556 is tuned, lengthens. Note also that contact fingers 705a of contact ring 705, which are electrically connected to inner conductor rod 707, move as inner conductor rod 707 slides within conductor tube 713. Thus, in operation, the tunable element 556 is an adjustable-length waveguide that can be used to tune the high-frequency resonant circuit 560 of NMR probe 500. Mechanical components 705, 705a, 706 may be used to perform the function of the contact strip 564. There are a number of suitable means for fastening high-frequency matching capacitor 558 to tunable element 556. In the preferred embodiment, high-frequency tuning capacitor 558 is mounted to a brass ring called a deck (not shown) located nearby RF tap point 716. This deck is, in turn, mounted to the proton tuning tube 710. Although not shown, tunable element 556 of Figure 4 has been modified to house the low-frequency circuit 692 and low-frequency input terminal 684 of the embodiment illustrated in Figure 3. A proton tuning tube 710 for the Figure 3 triple-tuned embodiment has a larger diameter than that necessary for the Figure 2 double-tuned embodiment so that tuning capacitor 672 and matching capacitor 674 may be mounted to or nearby slider plate 706. While various embodiments of the present invention have been described above, it should be understood that they have been presented by way of example only, and not limitation. Thus, the breadth and scope of the present invention should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.

Claims: An NMR probe (500;600) for transmitting RF energy between a source and a sample coil (552;652) by means of a tunable element (556;656), the tunable element comprising: an inner conductor; a grounded outer conductor; an electrical path between a first end of the inner conductor and the sample coil (552;652); a connection between the second end of the inner conductor and the grounded outer conductor; and means for varying the effective electrical length of the tunable element (556;656); said probe further comprising: an RF energy terminal (554;654); and means electrically connected to the inner conductor at a position between the first and the second ends for matching the probe to an impedance value corresponding to an external transmitter/receiver connected, in use, to said RF energy terminal (554;654). A probe as claimed in Claim 1, wherein said means for varying the effective electrical length comprises said inner conductor, having a variable length, electrically connected to said outer grounded conductor via a movable contact strip (564;664). A probe as claimed in Claim 2, further comprising: a slider rod (703) positioned coaxially within said outer grounded conductor and in contact with said movable contact strip (564;664) and being capable of moving said movable contact strip (564;664) to change said variable length. A probe as claimed in any preceding Claim, wherein said means for varying said electrical length comprises a dielectric material positioned between said inner and outer grounded conductors. A probe as claimed in any preceding Claim, wherein said means for varying said electrical length comprises an electrical component, having a reactance, positioned at said second end. A probe as claimed in any preceding Claim, wherein said means for matching is a variable capacitor (558;658). A probe as claimed in any one of Claims 1 to 6, wherein said means for matching is an antenna having an end inserted into said tunable element (556;656). A probe as claimed in any preceding Claim, wherein said inner conductor comprises: an inner conductor rod (707) inserted at least partially into a conductor tube (713); and a conductive first contact ring (712) secured to said conductor tube (713) at an end thereof such that said rod (707) and said tube (713) are in sliding contact. A probe as claimed in Claim 8, further comprising a plug located at said first end. A probe as claimed in Claim 8 or Claim 9, when dependent on Claim 2, wherein said movable contact strip (564;664) comprises a slider plate secured to said inner conductor rod (707), and a second contact ring (705) secured to said slider plate (706). A probe as claimed in any preceding claim, wherein said sample coil (552;652) is capable of transmitting and receiving RF signals at a low-frequency and a high-frequency. A probe as claimed in Claim 11, wherein said sample coil (652) is capable of transmitting and receiving RF signals at a low frequency, a medium frequency, and a high frequency. A probe as claimed in any preceding claim, further comprising: a second RF resonant circuit (570;690) comprising means for matching said second RF resonant circuit to a second impedance value; said second RF resonant circuit (570;690) being connected between said sample coil (552;652) and a second RF energy terminal (562;676); and the first-mentioned RF energy terminal (554;654) being used for inputting said high-frequency RF signal and said second RF energy terminal (562;676) used for inputting said low-frequency RF signal. A probe as claimed in Claim 13, when dependent on Claim 13, further comprising: a third RF resonant circuit comprising means for impedance matching to a third impedance value and being connected to said inner conductor and a third RF energy terminal (684). A probe as claimed in Claim 15, wherein the first-mentioned RF energy terminal (654) is used for inputting said high-frequency RF signal, said second RF energy terminal (676) is used for inputting said middle-frequency RF signal, and said third RF energy terminal (684) is used for inputting said low-frequency RF signal. A probe as claimed in Claim 15, wherein said first, second and third RF energy terminals (654,676,684) are used for sending RF signals received by said sample coil (652). A method for tuning and matching an RF resonant circuit of an NMR RF probe, comprising the steps of: transmitting at least one RF signal to a sample coil (552;652) via a tunable element (556;656) comprising an inner conductor and a grounded outer conductor, a first end of the inner conductor being electrically connected to the sample coil (552;652) and the second end being connected to near ground by virtue of an electrical connection between the second end of the inner conductor and the grounded outer conductor; varying the electrical length of said tunable element (556;656) ; and matching, at a position between said first and second ends, the RF resonant circuit to a first impedance value. A method as claimed in Claim 17, wherein: said step of transmitting comprises transmitting said RF signal via an inner conductor of said tunable element (556;656) ; and said step of varying comprises moving a conductive contact strip (564;664) along an inner wall of an outer grounded conductor surrounding said inner conductor, said contact strip being electrically connected to said inner conductor. A method as claimed in Claim 17, wherein: said step of transmitting comprises transmitting said RF signal via an inner conductor of said tunable element (556;656) ; and said step of varying comprises positioning a dielectric material between said inner conductor and an outer grounded conductor surrounding said inner conductor.

Inventors: PALMER ALLEN R, PALMER, ALLEN R.
Applicants: VARIAN ASSOCIATES, VARIAN ASSOCIATES, INC.
Application year: 1993
Main classification: G01R33
IPC codes: G01R33