WO2006050704A1 - Spectrum analyzer and frequency level measurement method - Google Patents
Spectrum analyzer and frequency level measurement method Download PDFInfo
- Publication number
- WO2006050704A1 WO2006050704A1 PCT/DE2005/002010 DE2005002010W WO2006050704A1 WO 2006050704 A1 WO2006050704 A1 WO 2006050704A1 DE 2005002010 W DE2005002010 W DE 2005002010W WO 2006050704 A1 WO2006050704 A1 WO 2006050704A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- spectrum analyzer
- frequency
- yig
- coil
- analyzer according
- Prior art date
Links
- 238000001228 spectrum Methods 0.000 title claims abstract description 31
- 238000000691 measurement method Methods 0.000 title 1
- 230000001105 regulatory effect Effects 0.000 claims abstract description 5
- 230000004044 response Effects 0.000 claims abstract description 3
- 230000008859 change Effects 0.000 claims description 3
- 238000000034 method Methods 0.000 claims description 3
- 238000006243 chemical reaction Methods 0.000 claims description 2
- 239000011162 core material Substances 0.000 claims description 2
- 238000012423 maintenance Methods 0.000 claims description 2
- 229910000859 α-Fe Inorganic materials 0.000 claims description 2
- NEEKVKZFYBQFGT-BTJKTKAUSA-N 9-amino-1,2,3,4-tetrahydroacridin-1-ol;(z)-but-2-enedioic acid Chemical compound OC(=O)\C=C/C(O)=O.C1=CC=C2C(N)=C(C(O)CCC3)C3=NC2=C1 NEEKVKZFYBQFGT-BTJKTKAUSA-N 0.000 claims 1
- 238000012544 monitoring process Methods 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 4
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 230000001419 dependent effect Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 238000007792 addition Methods 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000001914 filtration Methods 0.000 description 1
- 239000002223 garnet Substances 0.000 description 1
- MTRJKZUDDJZTLA-UHFFFAOYSA-N iron yttrium Chemical compound [Fe].[Y] MTRJKZUDDJZTLA-UHFFFAOYSA-N 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 230000002277 temperature effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- 238000011144 upstream manufacturing Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/08—Details of the phase-locked loop
- H03L7/099—Details of the phase-locked loop concerning mainly the controlled oscillator of the loop
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R23/00—Arrangements for measuring frequencies; Arrangements for analysing frequency spectra
- G01R23/16—Spectrum analysis; Fourier analysis
- G01R23/173—Wobbulating devices similar to swept panoramic receivers
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/08—Details of the phase-locked loop
- H03L7/085—Details of the phase-locked loop concerning mainly the frequency- or phase-detection arrangement including the filtering or amplification of its output signal
- H03L7/093—Details of the phase-locked loop concerning mainly the frequency- or phase-detection arrangement including the filtering or amplification of its output signal using special filtering or amplification characteristics in the loop
Definitions
- the invention relates to a spectrum analyzer, comprising a YIG oscillator whose output frequency is to be determined in response to a nominal frequency requirement by means of a magnetic field acting on a YIG sphere, and to a method for measuring frequency levels.
- Spectrum analyzers generally have an oscillator whose output frequency signal is mixed into a mixing stage to form a previously filtered measurement signal.
- the mixing stage transforms the signal component at the currently measured frequency to a fixed intermediate frequency at which filtering takes place.
- the oscillator frequency of the mixer is varied over time so that the entire frequency range to be examined is traversed.
- the filtered signal is amplified and its amplitude is measured.
- the spectrum analyzer thus measures the signal level over the frequency.
- the high input sensitivity and the wide dynamic range of spectrum analyzers enable the analysis of signals that can not be displayed with an oscilloscope.
- the oscillator used is a YIG oscillator (YTO-YIG Tuned Oscillator for short), which can be tuned exactly over a wide frequency range.
- the YIG oscillator consists essentially of two blocks, a high-frequency oscillator circuit and a tuning unit, a coil system.
- the high-frequency Oszil ⁇ lator circuit is an LC generator whose frequency-determining component is a YIG ball (yttrium iron garnet).
- the gain element in this circuit is a transistor, wherein the YIG ball is seated within a conductor loop inserted in the emitter circuit of the transistor. It has special magnetic properties. By means of an external magnetic field, which flows through the ball, the resonance frequency of the high-frequency oscillator circuit can be tuned without, for example, to generate phase noise.
- the disadvantage is that to generate the exact magnetic field to be set either a permanent magnet or a large coil and at least one other coil must be used.
- the YTOs are also heated to a constant temperature, preferably between 8O 0 C and 125 0 C. This can cause temperature problems in the circuit and there are consuming circuits for the required elements to make.
- the object of the present invention is to provide a simple control of the magnetic field, whereby the disadvantages of the prior art are avoided.
- a spectrum analyzer according to the preamble of claim 1, wherein only one, the magnetic field generating tuning coil is provided, the output frequency signal of the YIG oscillator as the actual value and the instantaneous frequency requirement of the spectrum analyzer is supplied as the setpoint of a PLL control circuit by which the coil current of the tuning coil is to be regulated by means of a downstream voltage / current converter.
- the coil current of the tuning coil is adjusted so that a minimum field strength is achieved to achieve saturation of the sphere, for example 500 Gauss, because the oscillator is operated in saturation.
- the fine adjustment of the magnetic field to achieve the desired frequency in accordance with the frequency requirement of the spectrum analyzer is then achieved loop loop by means of a single coil and a single coil. This simplification of the circuit simplifies the Circuit design and makes the control safer and faster.
- the control has a high frequency stability.
- the PLL control thus provides a control to a reference frequency, preferably according to the reference of a DDS, a high-precision quartz oscillator, for example in a frequency range of 10-20 MHz.
- a possibly existing delay is canceled because of the phase specification by the reference frequency.
- Frequencies in a wide frequency range may be generated based on the supplied reference frequency if the output frequency signal of the YIG oscillator is to be passed through a frequency divider before being applied to the PLL control circuit.
- the signal of the YIG oscillator which is in the Ghz range, can be controlled by a signal of a DDS in the range of 10-20 MHz.
- the frequencies can thus have very different sizes by a respective upstream frequency divider.
- a doubling of the frequency of the reference signal is achieved if the output frequency signal of the YIG oscillator is to be passed through a frequency bisector before being fed to the PLL control circuit.
- High-frequency additions in the signal can easily be filtered out if the output signal is to be fed to a low-pass filter.
- a filter which can be set to different frequency modes is present if the output signal of the PLL is to be fed to a loop filter.
- a heater holding the YIG in a certain temperature range can be dispensed with if the PLL control circuit also detects a frequency deviation of the YIG oscillator due to temperature fluctuations by means of a change in the YIG oscillator
- Coil current of the tuning coil is to be corrected.
- a changed frequency on Temperature changes can be reset by the PLL circuit.
- the range is bandwidth to about 3 GHz, in particular for measurements on satellite-TV systems, it is advantageous if the YIG oscillator to an output frequency of approximately 8 GHz 1 in particular zwi ⁇ rule about 3.5 GHz and about 6.5 GHz is planted vetn is.
- the core material of the tuning coil is ferrite. As a result, eddy current losses are avoided with advantageous material properties.
- the output signal of the PLL control circuit is to be supplied to a YIG driver circuit for voltage / current conversion and / or constant maintenance of the power supply of the spectrum analyzer in the case of the alternating coil currents.
- An easily transportable spectrum analyzer is present when the energy supply of the spectrum analyzer is a battery. By eliminating a heater and the use of only one coil, the power consumption of the device is greatly reduced and can be sufficiently ensured by a battery.
- FIG. 1 shows a schematic circuit diagram of a YIG oscillator with a tuning coil
- FIG. 2 shows a circuit diagram of a YIG oscillator with a tuning coil with functional elements
- 1 shows a schematic circuit diagram of a YIG oscillator 3 with a tuning coil 2 to be controlled according to the invention.
- the arrangement of the YIG sphere 1 is set to an external magnetic field which is built up by the tuning coil 2, then magnetic dipoles caused in the YIG sphere 1 due to electron spin are aligned parallel to the external magnetic field.
- a small alternating magnetic field is irradiated orthogonally thereto, so that the dipoles precess around the magnetic field generated by the tuning coil 2.
- the YIG order absorbs a majority of the injected coupling field. This resonant frequency is almost linearly dependent on the magnetic field of the tuning coil 2, which in turn is almost linearly dependent on the coil current, so that a very precise regulation of the frequency of the YIG oscillator 3 can take place.
- the frequency of the YIG oscillator 3 is achieved according to the invention via the control of an output signal coupled out of the YIG oscillator 3 with a réellesig ⁇ nalfrequenz to a predetermined frequency.
- the regulation takes place via the regulation of the magnetic field of the tuning coil 2 by means of a PLL control circuit 4. There, it is used to tune an oscillator so that it exactly follows the reference frequency, in particular the phase of the signal.
- the output frequency signal of the YIG oscillator 3, in particular after passing through a frequency divider 6, is compared in the PLL control circuit 4 with a reference frequency signal 11 of the spectrum analyzer.
- a reference frequency signal 11 of the spectrum analyzer For this purpose, only one tuning coil 2 is provided, the output frequency signal of the YIG oscillator 3 being supplied as the actual value and the instantaneous frequency requirement of the spectrum analyzer as the desired value of a PLL control circuit 4, which uses a nachge switched voltage / current transformer 5, the coil current of the tuning coil. 2 ruled.
- the output frequency signal of the YIG oscillator is regularly a Hochfrequenz ⁇ signal, about 3.5 to 6.5 GHz.
- the output frequency signal is supplied to the PLL control IC.
- the output frequency signal, the actual signal is divided down into the range of the DDS reference frequency, the desired signal, by the frequency divider 6 within the PLL control IC. There, the setpoint is compared with the actual value.
- the phase-frequency discriminator 9 is the actual regulating element of the PLL control IC. It compares two alternating voltages with each other and generates a DC voltage at the output, which is a measure of the softening of the two frequencies or of the phase positions in front of each other. It behaves as a frequency comparator that automatically transitions to phase comparison as it approaches the synchronicity of the two signals.
- the control deviation of the two signals is fed as an output signal to the Schleifenfil ⁇ ter 7.
- the filter constants can be switched over between two values in accordance with the use of the YIG high-frequency signal as a sweep sweep of a wide frequency range or as a fixed frequency setting.
- the filter constants influence the control speed and the phase noise of the PLL control loop.
- the output signal of the loop filter 7 (Utun-OUT) is supplied to the YIG driver circuit 10. This converts the voltage of the output signal of the loop filter 7 in the time required for the tuning coil 2 regulated coil current.
- the YIG driver circuit 10 keeps the load on the power supply of the entire device constant with the changing YIG control currents. According to the change of the coil current of the tuning coil 2, the YIG oscillator output frequency changes.
- the YIG PLL control loop consists of several modules, the YIG oscillator, a PLL module, a loop filter and a YIG driver circuit 10. LIST OF REFERENCE NUMBERS
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- Physics & Mathematics (AREA)
- Mathematical Physics (AREA)
- General Physics & Mathematics (AREA)
- Inductance-Capacitance Distribution Constants And Capacitance-Resistance Oscillators (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Abstract
Description
Claims
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE112005003392T DE112005003392A5 (en) | 2004-11-09 | 2005-11-09 | Spectrum analyzer and method for measuring frequency levels |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102004054261.9 | 2004-11-09 | ||
DE200410054261 DE102004054261A1 (en) | 2004-11-09 | 2004-11-09 | Spectrum analyzer and method for measuring frequency levels |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2006050704A1 true WO2006050704A1 (en) | 2006-05-18 |
Family
ID=35825347
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/DE2005/002010 WO2006050704A1 (en) | 2004-11-09 | 2005-11-09 | Spectrum analyzer and frequency level measurement method |
Country Status (2)
Country | Link |
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DE (2) | DE102004054261A1 (en) |
WO (1) | WO2006050704A1 (en) |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4581594A (en) * | 1984-03-27 | 1986-04-08 | Systron Donner Corporation | Drive circuit for YIG tuned devices |
DE19680092C2 (en) * | 1995-01-27 | 2000-10-26 | Advantest Corp | Spectrum analyzer |
US6201449B1 (en) * | 1999-07-24 | 2001-03-13 | Stellex Microwave Systems, Inc. | Ferromagnetic tuning ring for YIG oscillators |
US6233288B1 (en) * | 1995-01-24 | 2001-05-15 | Advantest Corp. | Spectrum analyzer |
US20050104667A1 (en) * | 2003-11-14 | 2005-05-19 | Williams Anthony D. | Frequency synthesizer having PLL with an analog phase detector |
-
2004
- 2004-11-09 DE DE200410054261 patent/DE102004054261A1/en not_active Withdrawn
-
2005
- 2005-11-09 DE DE112005003392T patent/DE112005003392A5/en not_active Withdrawn
- 2005-11-09 WO PCT/DE2005/002010 patent/WO2006050704A1/en active Application Filing
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4581594A (en) * | 1984-03-27 | 1986-04-08 | Systron Donner Corporation | Drive circuit for YIG tuned devices |
US6233288B1 (en) * | 1995-01-24 | 2001-05-15 | Advantest Corp. | Spectrum analyzer |
DE19680092C2 (en) * | 1995-01-27 | 2000-10-26 | Advantest Corp | Spectrum analyzer |
US6201449B1 (en) * | 1999-07-24 | 2001-03-13 | Stellex Microwave Systems, Inc. | Ferromagnetic tuning ring for YIG oscillators |
US20050104667A1 (en) * | 2003-11-14 | 2005-05-19 | Williams Anthony D. | Frequency synthesizer having PLL with an analog phase detector |
Non-Patent Citations (1)
Title |
---|
ANONYMUS: "Kommunikationselektronik", 23 March 2001 (2001-03-23), pages INHALTSVERZEICHNIS, 1.1 - 2.11, XP002369477, Retrieved from the Internet <URL:http://www.e-technik.fh-kiel.de/regiue/dldaten/k1-kt.pdf> [retrieved on 20060222] * |
Also Published As
Publication number | Publication date |
---|---|
DE102004054261A1 (en) | 2006-05-11 |
DE112005003392A5 (en) | 2007-10-25 |
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