CN1794003A - Strong magnetic impedance magnetic field sensor - Google Patents
Strong magnetic impedance magnetic field sensor Download PDFInfo
- Publication number
- CN1794003A CN1794003A CN 200510017257 CN200510017257A CN1794003A CN 1794003 A CN1794003 A CN 1794003A CN 200510017257 CN200510017257 CN 200510017257 CN 200510017257 A CN200510017257 A CN 200510017257A CN 1794003 A CN1794003 A CN 1794003A
- Authority
- CN
- China
- Prior art keywords
- frequency
- magnetic field
- amorphous ribbon
- signal
- crystal oscillator
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Images
Landscapes
- Measuring Magnetic Variables (AREA)
Abstract
A transducer of giant magnetic impedance field is prepared as applying transistor with cut-off frequency of 3-60 MH2 as kerr magnetic oscillation circuit, applying the same resistance value on two voltage-dividing resistances between base electrode and ground as well as between base electrode and DC power supply, series-connecting crystal oscillator with frequency of 1-20 MH2 with vibration starting capacity between base electrode and ground, existing noncrystalling belt as part of radio electrode load.
Description
Technical field
The invention belongs to weak magnetic measurement device technique field, particularly a kind of giant magnetic impedance (GMI) magnetic field probe.
Background technology
Magnetic-field measurement is a major issue in each field of production scientific research, has a lot of new technologies and new material all to be applied on the device of magnetic-field measurement now.The most frequently used magnetic field sensor has Hall (Hell) sensor, fluxgate sensor, and vibration or rotating coil etc., but these sensors all have certain defective.The hall device output signal changes little, also has certain magnetic direction anisotropy when measuring magnetic field, is applicable to the medium-high magnetic field measurement; Fluxgate and magnetic test coil measuring magnetic field, accurate especially to coil winding, signal processing requirement is higher; And the circuit too complex of the sensor, cost is higher.
The prior art close with the present invention is the article of the exercise question of publication on " Sensors and Actuators A 59 (1997) 1-8 " for " Recent advances of micro magnetic sensors and sensing application ".Disclosed sensor is the formations such as Bryant thatch (Colpitts) oscillatory circuit, rectification circuit, amplifying circuit of sectional pressure element by the CoFeSiB of annealing or the amorphous wire of CoSiB or CoFeMoSiB material or amorphous ribbon, with this amorphous wire (band).
The Bryant thatch oscillatory circuit of background technology as shown in fig. 1.V represents direct supply among Fig. 1, R
mBe amorphous wire, H
ExBe externally-applied magnetic field, C
1, C
2Be feedback capacity, E
OutBe output voltage.When the circuit starting of oscillation, there is high frequency ac signal to pass through R
m, the voltage signal on it is E
f, oscillation frequency f;
Wherein, R
0Be the intrinsic input resistance of circuit; L is R
mInductance value, r is R
mDirect current resistance, R
mResistance value Z=r+2 π jfL, amorphous wire R in circuit
mBe connected between transistorized base stage and the collector, make sectional pressure element and exist.As external magnetic field H
ExAct on R
mThe time, R
mResistance value Z will change, wherein, r and L will change, oscillation frequency f also can change like this, but the resistance value Z of non-crystalline material changes, that is, giant magnetic impedance rate of change (being abbreviated as GMI leads) is outfield H
ExWith the function of drive current frequency f, when the two all changes, can't guarantee that the resistance value Z variation (GMI leads) of non-crystalline material is clocklike.
The circuit of carrying in the background technology, R (30 Ω～300 Ω), Re (3 Ω～30 Ω), the drive current frequency f is that (15MHz～400MHz), be coupled with other element produces bigger noise to high frequency.Background technology has higher sensitivity, reaches 10～100%/Oe, and minimum resolution magnetic field is 10
-6Oe, but measurement range is below 5Oe.
Summary of the invention
The present invention is based on giant magnetic impedance (GMI) effect that the amorphous soft magnet band is had, the magnetic field sensor of design has well solved the giant magnetic impedance rate of change and detected magnetic field is corresponding one by one, noise is low, the problem of expansion measurement range; And make structure of the present invention small and exquisite, convenient and practical.
The strong magnetic impedance magnetic field sensor principle is that in the AC signal of amorphous ribbon loading high frequency, the amorphous ribbon two ends have corresponding high-frequency voltage signal in the circuit; When externally-applied magnetic field acted on the amorphous ribbon, the AC impedance of amorphous ribbon can change, and the voltage of respective ends also can change, and available this high-frequency voltage signal changes and reflects changes of magnetic field.
The present invention is by amorphous ribbon, Bryant thatch oscillatory circuit, and prime amplifier, rectification circuit and zeroing output amplifier constitute; Prime amplifier input termination amorphous ribbon two ends, prime amplifier amplifying signal are by output termination rectification circuit, and rectification circuit is converted into the direct current signal of two times of AC signal peak values with high frequency ac signal, connects the zeroing output amplifier again; Whole sensor shields with the non-ferromagnetic metal shell; Said Bryant thatch oscillatory circuit is to be that the transistor of 3～60MHz constitutes base stage and direct supply V by cutoff frequency
CcBetween and base stage equate with two divider resistance resistances between ground; Frequency is that the crystal oscillator (crystal oscillator) of 1～20MHz and starting of oscillation capacitance series are between base stage and ground; Said amorphous ribbon is to contain the iron-based of zirconium or/and contain the cobalt-based material of zirconium, one end ground connection, and the other end is connected transistorized emitter with pull-up resistor series connection back, and amorphous ribbon is done the part existence of emitter-base bandgap grading load.
Amorphous ribbon of the present invention has unimodal giant magnetic impedance rate of change (GMI leads) with the changes of magnetic field curve without annealing in process, and sensitivity is more preferably greater than 1%/Oe.Such as the amorphous ribbon that adopts materials such as CoZrB, FeZrB, FeCoZrB.
The frequency range of crystal oscillator (crystal oscillator) is preferably in 1～12MHz, and the optimum frequency scope is 2～5MHz.Can use quartz crystal oscillator.
The present invention makes circuit frequency stabilization vibration owing to introduced crystal oscillator (crystal oscillator) in Bryant thatch circuit; Owing to take the design of stable transistor base stage quiescent point, two divider resistances equate that transistor emitter-base bandgap grading DC voltage amount is stable during work; Owing to adopt and contain the iron-based of zirconium or/and contain the unannealed amorphous ribbon of the cobalt-based material of zirconium, and as the part of emitter-base bandgap grading load, have unimodal giant magnetic impedance rate of change (GMI leads) with the changes of magnetic field curve, make the measurement device scope become big, can measure the low-intensity magnetic field of 2～50Oe.Electronic circuit of the present invention is simple, compact conformation is small and exquisite, economy is convenient and practical, can be widely used in each field magnetic-field measurement of production scientific research.
Description of drawings
The GMI magnetic field sensor circuit figure of Fig. 1 background technology.
Fig. 2 GMI magnetic field sensor circuit of the present invention figure.
Fig. 3 Co of the present invention
72Zr
8B
20The GMI of amorphous ribbon leads with the changes of magnetic field curve.
Voltage signal (a) on Fig. 4 amorphous ribbon of the present invention and through prime amplifier amplifying signal (b).
Fig. 5 voltage of the present invention is with the changes of magnetic field curve of output.
Embodiment
Below in conjunction with description of drawings concrete structure of the present invention and working method
Embodiment 1
Among Fig. 2,1 is Bryant thatch (Colpitts) oscillatory circuit, and 2 is prime amplifier, and 3 is rectification circuit, and 4 are the zeroing output amplifier, and 5 is amorphous ribbon, and 6 is crystal oscillator, and 7 is feedback capacity C
1, 8 is feedback capacity C
2, 9 is transistor, 10 are the starting of oscillation capacitor C
3, 11 is high-frequency operational amplifier, and 12 is two commutation diodes, and 14 is operational amplifier, and 16 is the divider resistance that two resistances equate, and 17 is variohm, and 18 is the emitter-base bandgap grading current-limiting resistance, and 19 is filter capacitor, 20 is electric capacity of voltage regulation.
The supply voltage V of Bryant thatch oscillatory circuit 1
CcCan be 12V, take the design of stable transistor 9 base stage quiescent points, because two divider resistance 16 resistances equate that then the extremely basic quiescent operation voltage of transistor 9 is 6V, transistor 9 emitter-base bandgap grading quiescent operation voltages are stabilized in about 5.3V; Amorphous ribbon 5 adopts CoZrB or FeZrB or FeCoZrB material, as a part and emitter-base bandgap grading current-limiting resistance 18 places in circuit of emitter-base bandgap grading load, and about 3 Ω of amorphous ribbon 5 direct current resistances, emitter-base bandgap grading current-limiting resistance 18 is 390 Ω; Bryant thatch oscillatory circuit 1 frequency stabilization vibration, oscillation frequency is the frequency 3.5795MHz of crystal oscillator 6; Regulate feedback capacity C
1With feedback capacity C
2, make the stable sinusoidal signal of emitter-base bandgap grading output; Two ends produce certain ac voltage signal to amorphous ribbon 5 because bigger AC impedance is arranged, referring to Fig. 4 (a); This signal amplifies at the prime amplifier 2 through mainly being made of high-frequency operational amplifier 11, referring to Fig. 4 (b), AC signal after the amplification is connected to the rectification circuit 3 that mainly is made of two commutation diodes 12, high frequency ac signal is converted into the direct current signal of two times of AC signal peak values; This d. c. voltage signal inserts zeroing output amplifier 4 input ends that mainly are made of operational amplifier 14 again, under the situation of no external magnetic field, variohm 17 is regulated in stable back makes the positive input terminal voltage of operational amplifier 14 equate with negative input end voltage, and the magnitude of voltage of output amplifier 4 outputs of then returning to zero is 0.
When externally-applied magnetic field acted on the amorphous ribbon 5, the AC impedance value of amorphous ribbon 5 can change, and referring to Fig. 3, Δ Z/Z is giant magnetic impedance rate of change (GMI leads) among Fig. 3, Δ Z/Z=(Z (H)-Z (H
Sat))/Z (H
Sat) * 100%, wherein, Z (H) is the AC impedance value of amorphous ribbon 5 under any magnetic field, Z (H
Sat) be that amorphous ribbon 5 magnetization are to saturated back AC impedance value.Ac voltage signal amplitude on the amorphous ribbon 5 also can change (frequency of ac voltage signal does not change) with the variation of AC impedance, so, this signal is outputing to zeroing output amplifier 4 through prime amplifier 2 and rectification circuit 3, the difference of the signal of input end and original signal just can be amplified output, the external magnetic field size that this signal difference and amorphous ribbon 5 accepted has corresponding relation, thereby the stool and urine that has recorded signal difference has recorded the size of external magnetic field.
The difference of the signal of output amplifier 4 input ends and original signal will connect the numeral that A/D conversion and microprocessor carry out magnetic field value again and show if will return to zero, and can reach the function of direct demonstration magnetic-field measurement data.
Embodiment 2
Provide an embodiment of each several part circuit component data.
Bryant thatch oscillatory circuit 1 among Fig. 2, amorphous ribbon 5 is thick 10um～40um, wide 1mm～2mm, long 60mm～200mm have giant magnetic impedance (GMI) effect, and sensitivity can be adopted Co greater than 1%/Oe
72Zr
8B
20Amorphous ribbon; Transistor 9 uses the high frequency transistor of 2SC1815 model, its cutoff frequency f
rGreater than 5 times of crystal oscillator 6 frequencies.The frequency of crystal oscillator 6 is more than the 1MHz, the starting of oscillation capacitor C
3But be all starting of oscillations of 15pF～10nF.Two divider resistances 16 can be selected 10k Ω for use; Emitter-base bandgap grading current-limiting resistance 18 is 390 Ω; Feedback capacity C
1Be 1000pF～2200pF, feedback capacity C
2Be 60pF～200pF, and feedback capacity C
1With feedback capacity C
2Ratio between 2 to 25.The oscillation frequency of Bryant thatch oscillatory circuit promptly is the frequency of crystal oscillator 6.
Prime amplifier 2 among Fig. 2, should select gain bandwidth product GBP for use is crystal oscillator (6) frequency more than 5 times, the high frequency amplifier that offset voltage 4mV is following.High-frequency operational amplifier 11 can be selected LM318 for use
In the rectification circuit 3 among Fig. 2, commutation diode 12 is selected schottky diode for use.
In the zeroing output amplifier 4 among Fig. 2, operational amplifier 14 can be selected op-07 for use.
The relation curve by measuring magnetic field that applies on output voltage that detects with the device of present embodiment and the amorphous ribbon 5 is seen Fig. 5.With the changes of magnetic field curve of output, magnetic field overlaps in the scope of 2～50Oe along amorphous ribbon positive dirction and reciprocal voltage curve of output by voltage shown in Figure 5, illustrate the present invention can be in range indifference accurately measure the magnetic field of both forward and reverse directions.
Claims (3)
1, a kind of strong magnetic impedance magnetic field sensor, by amorphous ribbon (5), Bryant thatch oscillatory circuit (1), prime amplifier (2), rectification circuit (3) and zeroing output amplifier (4) constitute; Prime amplifier (2) input termination amorphous ribbon two ends, prime amplifier (2) amplifying signal is by output termination rectification circuit (3), rectification circuit (3) is converted into the direct current signal of two times of AC signal peak values with high frequency ac signal, connects zeroing output amplifier (4) again; Whole sensor shields with the non-ferromagnetic metal shell; It is characterized in that said Bryant thatch oscillatory circuit (1) is to be that the transistor of 3～60MHz constitutes by cutoff frequency, between base stage and direct supply Vcc and base stage equate with two divider resistances (16) resistance between ground; Frequency is that crystal oscillator (6) and the starting of oscillation electric capacity (10) of 1～20MHz is serially connected between base stage and the ground; Said amorphous ribbon (5) is to contain the iron-based of zirconium or/and contain the cobalt-based material of zirconium, one end ground connection, and the other end and pull-up resistor (18) series connection back are connected the emitter of transistor (9).
According to the described strong magnetic impedance magnetic field sensor of claim 1, it is characterized in that 2, said amorphous ribbon (5) is CoZrB or FeZrB or FeCoZrB material; The frequency range of said crystal oscillator (6) is 2～5MHz.
According to claim 1 or 2 described strong magnetic impedance magnetic field sensors, it is characterized in that 3, said amorphous ribbon (5) is Co
72Zr
8B
20Material; The frequency of said crystal oscillator (6) is 3.5795MHz.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CNB2005100172579A CN100403050C (en) | 2005-11-02 | 2005-11-02 | Strong magnetic impedance magnetic field sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CNB2005100172579A CN100403050C (en) | 2005-11-02 | 2005-11-02 | Strong magnetic impedance magnetic field sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN1794003A true CN1794003A (en) | 2006-06-28 |
| CN100403050C CN100403050C (en) | 2008-07-16 |
Family
ID=36805561
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CNB2005100172579A Expired - Fee Related CN100403050C (en) | 2005-11-02 | 2005-11-02 | Strong magnetic impedance magnetic field sensor |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN100403050C (en) |
Cited By (12)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101038305B (en) * | 2007-03-06 | 2010-05-19 | 吉林大学 | Array giant magnetic impedance effects current sensor |
| CN101363903B (en) * | 2008-09-16 | 2011-05-18 | 北京科技大学 | Magnetic field sensor utilizing ferromagnetic nanometer ring strong magnetic resistance effect |
| CN102356545A (en) * | 2009-03-19 | 2012-02-15 | Lg伊诺特有限公司 | Amplifying driving unit using giant magneto resistance sensor and diagnosis device using the same |
| CN102478646A (en) * | 2010-11-29 | 2012-05-30 | 中国科学院合肥物质科学研究院 | Magnetic sensor based on amorphous magnetic core coil and working method thereof |
| CN103777151A (en) * | 2014-02-11 | 2014-05-07 | 中国科学院电子学研究所 | Magnetic field sensor |
| CN103885006A (en) * | 2014-03-31 | 2014-06-25 | 哈尔滨工业大学深圳研究生院 | Alternating current magnetic field sensor with measuring frequency scanning function |
| CN103885001A (en) * | 2014-03-31 | 2014-06-25 | 哈尔滨工业大学深圳研究生院 | Series array type alternating current magnetic field sensing device |
| CN103885000A (en) * | 2014-03-31 | 2014-06-25 | 哈尔滨工业大学深圳研究生院 | Alternating current induced magnetic field sensor with measuring frequency scanning function |
| CN104280698A (en) * | 2013-07-09 | 2015-01-14 | 北京嘉岳同乐极电子有限公司 | Magnetic field measurement device |
| CN107247125A (en) * | 2017-06-14 | 2017-10-13 | 中北大学 | Metal enclosed internal test instrument triggering method based on giant magnetoresistance effect |
| CN108983123A (en) * | 2018-07-20 | 2018-12-11 | 常州微磁非晶丝传感器有限公司 | A kind of high-resolution amorphous wire orthogonal fluxgate sensor and its manufacturing technology |
| CN110907867A (en) * | 2019-12-13 | 2020-03-24 | 中国人民解放军国防科技大学 | Magnetic focusing device for giant magneto-impedance sensor and giant magneto-impedance sensor |
Family Cites Families (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE59812241D1 (en) * | 1997-09-24 | 2004-12-16 | Infineon Technologies Ag | Sensor device for detecting the direction of an external magnetic field by means of a magnetoresistive sensor element |
| JPH11112055A (en) * | 1997-10-01 | 1999-04-23 | Fujitsu Ltd | Magnetic sensor |
| JPH11287668A (en) * | 1998-02-04 | 1999-10-19 | Denso Corp | Amplification circuit and position detection device using the same |
| JP2000055999A (en) * | 1998-08-11 | 2000-02-25 | Tdk Corp | Magnetic sensor device and current sensor device |
| US6657476B1 (en) * | 2002-07-09 | 2003-12-02 | Honeywell International Inc. | AC-coupled sensor signal conditioning circuit |
| CN2906638Y (en) * | 2005-11-02 | 2007-05-30 | 吉林大学珠海学院 | Giant magneto-impedance magnetic field sensor |
-
2005
- 2005-11-02 CN CNB2005100172579A patent/CN100403050C/en not_active Expired - Fee Related
Cited By (17)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101038305B (en) * | 2007-03-06 | 2010-05-19 | 吉林大学 | Array giant magnetic impedance effects current sensor |
| CN101363903B (en) * | 2008-09-16 | 2011-05-18 | 北京科技大学 | Magnetic field sensor utilizing ferromagnetic nanometer ring strong magnetic resistance effect |
| CN102356545A (en) * | 2009-03-19 | 2012-02-15 | Lg伊诺特有限公司 | Amplifying driving unit using giant magneto resistance sensor and diagnosis device using the same |
| CN102478646A (en) * | 2010-11-29 | 2012-05-30 | 中国科学院合肥物质科学研究院 | Magnetic sensor based on amorphous magnetic core coil and working method thereof |
| CN104280698B (en) * | 2013-07-09 | 2018-09-28 | 北京嘉岳同乐极电子有限公司 | Magnetic field measuring device |
| CN104280698A (en) * | 2013-07-09 | 2015-01-14 | 北京嘉岳同乐极电子有限公司 | Magnetic field measurement device |
| CN103777151B (en) * | 2014-02-11 | 2016-03-23 | 中国科学院电子学研究所 | Magnetic field sensor |
| CN103777151A (en) * | 2014-02-11 | 2014-05-07 | 中国科学院电子学研究所 | Magnetic field sensor |
| CN103885006A (en) * | 2014-03-31 | 2014-06-25 | 哈尔滨工业大学深圳研究生院 | Alternating current magnetic field sensor with measuring frequency scanning function |
| CN103885001A (en) * | 2014-03-31 | 2014-06-25 | 哈尔滨工业大学深圳研究生院 | Series array type alternating current magnetic field sensing device |
| CN103885000A (en) * | 2014-03-31 | 2014-06-25 | 哈尔滨工业大学深圳研究生院 | Alternating current induced magnetic field sensor with measuring frequency scanning function |
| CN103885001B (en) * | 2014-03-31 | 2016-08-17 | 哈尔滨工业大学深圳研究生院 | Serial array formula AC magnetic field sensing device |
| CN107247125A (en) * | 2017-06-14 | 2017-10-13 | 中北大学 | Metal enclosed internal test instrument triggering method based on giant magnetoresistance effect |
| CN107247125B (en) * | 2017-06-14 | 2019-05-17 | 中北大学 | Metal enclosed internal test instrument triggering method based on giant magnetoresistance effect |
| CN108983123A (en) * | 2018-07-20 | 2018-12-11 | 常州微磁非晶丝传感器有限公司 | A kind of high-resolution amorphous wire orthogonal fluxgate sensor and its manufacturing technology |
| CN110907867A (en) * | 2019-12-13 | 2020-03-24 | 中国人民解放军国防科技大学 | Magnetic focusing device for giant magneto-impedance sensor and giant magneto-impedance sensor |
| CN110907867B (en) * | 2019-12-13 | 2022-03-22 | 中国人民解放军国防科技大学 | Magnetic focusing device for giant magneto-impedance sensor and giant magneto-impedance sensor |
Also Published As
| Publication number | Publication date |
|---|---|
| CN100403050C (en) | 2008-07-16 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN1794003A (en) | Strong magnetic impedance magnetic field sensor | |
| Mohri et al. | Sensitive and quick response micro magnetic sensor utilizing magneto-impedance in Co-rich amorphous wires | |
| CN101038305B (en) | Array giant magnetic impedance effects current sensor | |
| US6698299B2 (en) | Magnetoelastic torque sensor | |
| CN2906638Y (en) | Giant magneto-impedance magnetic field sensor | |
| WO2000060369A1 (en) | Passive solid-state magnetic field sensors and applications therefor | |
| JP4731087B2 (en) | Position and electromagnetic field sensors | |
| US9018887B2 (en) | Ultrasonic system controls, tool recognition means and feedback methods | |
| Bushida et al. | Sensitive and quick response micro magnetic sensor using amorphous wire MI element Colpitts oscillator | |
| US10613159B2 (en) | Magnetoelectric magnetic field measurement with frequency conversion | |
| CN101915900A (en) | Amorphous wire magneto-impedance transducer and magnetic field detection method based on amorphous wire magneto-impedance effect | |
| JP4007464B2 (en) | Magnetic detector | |
| KR920704150A (en) | Self-detection device | |
| CN101915898A (en) | Amorphous wire magneto-impedance sensor and amorphous wire magneto-impedance effect-based magnetic field detection method | |
| CN108241130A (en) | A kind of fluxgate magnetic field sensor based on magnetoelectric effect | |
| JP5711368B2 (en) | Magnetic field detection method and magnetic field detection circuit | |
| CN101604966B (en) | Exciting circuit of flux gate sensor | |
| Li et al. | AC/DC dual-mode magnetoelectric sensor with high magnetic field resolution and broad operating bandwidth | |
| CN201435719Y (en) | Fluxgate sensor excitation circuit of single operational amplifier | |
| CN100489471C (en) | Sensor | |
| CN201876534U (en) | Amorphous-wire magneto-impedance sensor | |
| WO2014113694A1 (en) | Magnetoelectric pickup element for detecting oscillating magnetic fields | |
| Kikuchi et al. | Considerations of output voltage waveform on magnetic linear encoder for artificial heart using linear pulse motor | |
| EP0204928A2 (en) | Exciting of magnetic field for amorphous-alloy sensor | |
| CN221039215U (en) | Single power supply current detection circuit based on fluxgate principle |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| C17 | Cessation of patent right | ||
| CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20080716 Termination date: 20091202 |