Source: https://patents.google.com/patent/JP2008283404A/en
Timestamp: 2020-02-18 23:46:48
Document Index: 405356903

Matched Legal Cases: ['art 3', 'arts 4', 'art 3', 'arts 4', 'art 4', 'art 4', 'art 4', 'art 4', 'art)\n4', 'art 5', 'art 7', 'art 8']

JP2008283404A - Cross double tag, and rfid system using the same - Google Patents
Cross double tag, and rfid system using the same Download PDF
JP2008283404A
JP2008283404A JP2007125055A JP2007125055A JP2008283404A JP 2008283404 A JP2008283404 A JP 2008283404A JP 2007125055 A JP2007125055 A JP 2007125055A JP 2007125055 A JP2007125055 A JP 2007125055A JP 2008283404 A JP2008283404 A JP 2008283404A
JP2007125055A
JP4806373B2 (en
2007-05-09 Application filed by Fujitsu Ltd, 富士通株式会社 filed Critical Fujitsu Ltd
2008-11-20 Publication of JP2008283404A publication Critical patent/JP2008283404A/en
2011-11-02 Publication of JP4806373B2 publication Critical patent/JP4806373B2/en
<P>PROBLEM TO BE SOLVED: To provide a tag for generating a circularly polarized waves with an extended distance of communication with a reader-writer by using the tag of linearly polarized waves as it is without using a special circuit or the like, and to provide an RFID system using the same. <P>SOLUTION: Two tags 1 (1a, 1b) respectively provided with a dipole antenna 2 formed of a conductor, a power supply part 3 connected with an IC chip 5 at the center of the dipole antenna 2 and loop-shaped inductance parts 4 (4a, 4b) formed in the middle of the dipole of the dipole antenna 2 and connected to the power supply part 3 in parallel with the dipole of the dipole antenna 2 in same plane are prepared. They are crossed and tightly attached and piled up so that the loop shapes of the respective inductance parts 4 overlap in a range as wide as possible and so as to eliminate a gap at a crossing part. <P>COPYRIGHT: (C)2009,JPO&INPIT
The present invention relates to a crossed double tag in which two linear polarization tags are crossed and stacked to extend a communication distance with a reader / writer, and an RFID (radio frequency identification) system.
2. Description of the Related Art Conventionally, an RFID system has been put to practical use as a contactless authentication technique in which various information about people and things are recorded in an RFID IC (integrated circuit) chip and read out wirelessly. Although there are various names for the above-mentioned RFID, it is generally called a wireless tag or simply a tag.
The tag includes a metal antenna formed on a plane such as a sheet or film having a thickness of about 0.1 mm, and an IC chip connected to a feeding point of the antenna.
Usually, an IC chip is extremely small, and its size is about 0.2 mm in thickness and about 1 mm square in area. The antenna connected to the IC chip is formed as a dipole antenna pattern, and the communication radio wave due to the resonance current is linearly polarized.
The RFID system transmits a radio wave signal of about 1 W from the reader / writer, receives the signal on the tag side, and sends back the information in the IC chip as a response signal from the tag to the reader / writer side. It is a system that reads with a writer.
There is no battery in the tag, and when the reader / writer approaches the reader / writer, the antenna resonates with the radio wave transmitted from the reader / writer, producing a current. It has become a mechanism.
The antenna on the reader / writer side is formed so as to transmit a circularly polarized radio wave so that it can communicate with the tag regardless of the direction of the tag communicating with the linearly polarized wave. The radio wave used for this transmission is UHF (Ultra High Frequency) in the range of 860 to 960 MHz, but in Japan, 952 MHz to 954 MHz is used.
The communication distance between the reader / writer and the tag is approximately 3 m to 5 m in an ideal state, although it depends on the gain of the tag antenna, the operating voltage of the IC chip, the surrounding environment, and the like.
The reader / writer antenna communicates with circularly polarized radio waves, whereas the tag antenna communicates with linearly polarized waves. Therefore, power generated by resonance with radio waves received from the reader / writer, that is, power received from the reader / writer. Can receive only half of the assumption that the tag is a circularly polarized tag.
Since the transmission power attenuates in inverse proportion to the square of the distance, the actual communication distance 3 m to 5 m described above is 1 / √2 = 1 when the tag is assumed to be circularly polarized. /1.41.
However, as a tag simply for transmitting circularly polarized waves, two dipole antennas are orthogonally crossed, and one of the dipole antennas and one of the other dipole antennas and the other of the one dipole antenna and the other dipole. There has been proposed a configuration in which two feeding terminals that electrically connect the other of the antennas are formed, and an IC tag and a circuit having a phase difference of π / 2 are connected between the two feeding terminals. (For example, refer to Patent Document 1.)
JP 2003-249820 A
By the way, as described above, if the tag is a circularly polarized tag, two orthogonal linearly polarized dipole antennas are connected by a circuit having a phase difference of π / 2, that is, a 90 ° phase shifter. There must be.
Usually, as described above, since the tag has a simple structure in which the dipole antenna pattern is directly connected to a small IC having an area of about 1 mm × 1 mm, a 90 ° phase shifter as in Patent Document 1 is used separately from the IC. The structure of attaching is not desirable because the whole structure becomes expensive.
The technology of Patent Document 1 is a dedicated tag for circularly polarized wave generation in which a dipole antenna crosses in a cross shape so that it cannot be separated and is connected to an IC tag and a 90 ° phase shifter. There is a problem that a process is required and design flexibility is lacking.
SUMMARY OF THE INVENTION In view of the above-described conventional situation, an object of the present invention is to use a linearly polarized wave tag as it is without using a special circuit or the like, and a tag for generating a circularly polarized wave having an extended communication distance with a reader / writer, and the tag It is to provide an RFID system using the.
First, the intersecting double tag according to the first invention is formed between a dipole antenna formed of a conductor in the same plane, a feeding portion to which an IC is connected at the center of the dipole antenna, and a dipole of the dipole antenna. The first and second tags each having a loop-shaped inductance portion connected in parallel with the dipole antenna bipolar to the power feeding portion, and the loop shapes of the respective inductance portions overlap each other. The first and second tags are configured to intersect each other.
In this intersecting double tag, the inductance portion is formed, for example, in a square shape, a circular shape, or a loop shape approximate thereto.
Further, the first and second tags are configured, for example, such that the loop shapes of the inductance portions are crossed so as to overlap as wide as possible and are stacked with no gap as much as possible. For example, the first and second tags generate circularly polarized waves at an intersection angle of 90 °.
Further, the cross double tag includes a holding member having a depression corresponding to a shape in which the first and second tags intersect, and the first and second tags are formed by the depression of the holding member. It is configured to be held by the holding member in a crossed shape.
Next, an RFID (radio frequency identification) system according to a second aspect of the present invention is a dipole antenna formed of a conductor in the same plane, a power supply unit to which an IC chip is connected at the center of the dipole antenna, and the dipole antenna. A loop-shaped inductance portion formed in the middle of the bipolar and having a loop-shaped inductance portion connected in parallel to the bipolar pole of the dipole antenna with respect to the power feeding portion, and the loop shape of each of the inductance portions A cross-polarized tag formed by crossing the first and second tags so that they overlap each other, and a circularly polarized radio signal is transmitted to read out the information of the first tag or the information of the second tag And a reader / writer.
In this RFID (radio frequency identification) system, for example, the reader / writer sets the first tag as a read tag, sets the second tag as a non-read tag, and only the information of the first tag. Is always read.
In addition, for example, the first and second tags each include a user memory area in which the same information is written, and the reader / writer is configured so that the circularly polarized wave plane of the circularly polarized radio signal is in either forward or reverse direction. The information in the user memory area may be read from the first or second tag that responds more strongly to the switched circularly polarized wave.
Further, for example, the first and second tags each include a user memory area in which different information is written, and the reader / writer sequentially switches the circular polarization plane of the circularly polarized radio signal in both forward and reverse directions. By reading the information in the user memory area from the first or second tag that responds more strongly to circularly polarized waves in response to the switching, the user memory can be read from either the first or second tag. It may be configured to read the information of the area.
According to the present invention, a circularly polarized wave is generated by using two linearly polarized waves as they are crossed and overlapped without using a special circuit or the like. A circularly polarized wave generating tag in which the communication distance with the reader / writer extends approximately 1.41 times as compared with the case of one tag and an RFID system using the same can be provided at low cost.
FIG. 1 is a perspective view showing the configuration of an extremely small tag and its antenna in the first embodiment. The overall size of the tag 1 shown in the figure is 53 mm wide × 7 mm long.
The tag 1 includes a dipole antenna 2, a power feeding unit 3, and an inductance unit 4 that are formed of a conductor in the same plane. In addition, it is preferable to use Cu, Ag, or Al for said conductor.
The power feeding unit 3 constitutes a chip mounting portion at the center of the dipole antenna 2 and has an IC chip 5 mounted thereon. A diball portion 6 having a line width of 1 mm is formed on both sides of the feeding portion 3 as a center, and the dipole antenna 2 is formed as a whole.
The dipole antenna 2 composed of the diball portions 6 on both sides is bent from both sides by bending portions 7 (7-1, 7-7, 7-3, 7-4) that bend the dipoles at least at four locations inside, respectively. It is formed in a square spiral shape. That is, in this example, each die ball portion 6 has four bent portions.
The total length of the dipole antenna 2 when the four bent portions 7 are straightened is formed so as to be shorter than ½ of the antenna resonance wavelength.
Further, in the vicinity of the center of the dipole antenna 2, the above-described inductance portion 4 is disposed in the middle of both the dipole portions 6 and 6 formed in the shape of the square spiral.
The inductance section 4 is connected in parallel to both the dipole sections 6 and 6 with respect to the power feeding section 3 of the dipole antenna 2, that is, the IC chip 5.
The IC chip 5 mounted on the power supply unit 3 is, for example, a chip with Rc = 500Ω and Cc = 1.4 pF. The inductance part 4 is arranged on the antenna side, and the inductance part 4 is configured to cancel the capacitance component of 1.4 pF of the IC chip 5.
In the example shown in FIG. 1, the inductance portion 4 is formed in a substantially rectangular one-round loop shape. However, the one-round loop shape of the inductance portion 4 is not limited to this, and is square. , A circle, or a loop shape approximate to them.
Both surfaces (upper and lower surfaces in the figure) of the tag 1 are covered so as to be sandwiched between resin protective films 8 having a dielectric constant εr = 3 and a thickness t = 0.75 mm.
For the resin protective film 8, for example, ethylene terephthalate film or the like is used. Further, instead of the resin protective film 8, it may be coated from both sides with appropriate paper.
FIG. 2 is a diagram showing the frequency characteristics of reflection of the dipole antenna 2 of the tag 1 calculated by the electromagnetic field simulator. In the figure, the horizontal axis indicates the frequency (800 MHz to 1100 MHz), and the vertical axis indicates the reflection (−5 dB to 0 dB). As can be seen from the figure, the reflection is the smallest in the vicinity of 975 MHz.
FIG. 3 is a diagram showing the antenna gain calculation value of the dipole antenna 2 of the tag 1 calculated by the electromagnetic field simulator. In the figure, the horizontal axis indicates the frequency (800 MHz to 1100 MHz), and the vertical axis indicates the antenna gain (-4 dBi to 2 dBi). The antenna gain shown in the figure is the maximum near 1050 MHz.
That is, although there is a defect that the reflection becomes large in the vicinity of 1050 MHz, the antenna gain is large in the vicinity of 1050 MHz as shown in FIG. 3, so that the large antenna gain compensates for the large reflection.
FIG. 4 is a communication distance characteristic diagram obtained by combining the reflection characteristics and gain characteristics of the dipole antenna 2 of the tag 1 on Excel. In the figure, the horizontal axis indicates the frequency (800 MHz to 1100 MHz), and the vertical axis indicates the relative communication distance normalized by the maximum distance.
Thus, the communication distance characteristic of the dipole antenna 2 of the tag 1 is asymmetrical with respect to the reader / writer operating frequency 953 MHz, but the change is gentle on the frequency side higher than the reader / writer operating frequency 953 MHz. The communication distance is relatively stable.
In the above calculation by the electromagnetic field simulator, since the upper and lower sides of the resin protective film 8 shown in FIG. 1 are set as air, the communication distance at the reader / writer operating frequency 953 MHz is that the tag 1, that is, the dipole antenna 2 is in the air. Is the distance when
The communication distance in the air is 0.95 with respect to the standardized maximum distance as shown in FIG. That is, 95% of the maximum distance is secured.
When this tag 1 is attached to a plastic having, for example, εr = 3 and a thickness of 2 mm, the effective dielectric constant around the antenna increases and the band shifts by about 10%. That is, the waveform of FIG. 4 is shifted by about 100 MHz to the low frequency side.
In other words, in the waveform of FIG. 4, the value of the relative communication distance at a frequency of 1050 MHz, which is about 10% higher than 953 MHz, is the communication distance when the tag 1 is attached to a plastic with a thickness of 2 mm.
The communication distance at this time is 0.8 distance with respect to the standardized maximum distance as shown in FIG. 4, and 80% of the maximum distance is secured.
Thus, as can be seen from FIG. 4, the tag 1 of this example is a distance within 80% of the maximum communication distance, whether in the air, affixed to foamed polystyrene, or affixed to a plastic with a thickness of 2 mm. Can be secured at all times, and it has extremely high distance stability.
The feature of the tag 1 of this example is that the antenna pattern consisting of a dipole part and an inductance part is adjusted so as to be as close as possible to the optimum antenna value near the reader / writer operating frequency of 953 MHz. The reflection increases with distance from the value, but the communication distance is not greatly deteriorated by the increase of the antenna gain.
In order to increase the antenna gain at a frequency higher than 953 MHz, the total length of the antenna is made to approach ½ of the antenna resonance wavelength with good gain efficiency.
The feature of the antenna pattern of the dipole antenna 2 of the tag 1 of this example is that the total length of the antenna when the bent portion 7 is straightened is slightly shorter than 1/2 of the antenna resonance wavelength λ.
In the example shown in FIG. 1, the total length of the antenna when the bent portion 7 is straightened is about 120 mm, and ½ of the antenna resonance wavelength λ is about 130 to 140 mm. The allowable width of the antenna resonance wavelength λ of 10 mm is based on the upper and lower resin protective films 8.
Further, the dipole portion 6 is bent inward from the end side so as to be as close to a straight line as possible. Further, since it is preferable that the two dipole portions 6 and 6 are not close to each other, it is desirable to form the inductance portion 4 between the two dipole portions 6 and 6.
With this configuration, the impedance at 953 MHz is set to be close to the optimum antenna value, and the antenna gain is set to be the maximum in the vicinity of 1050 MHz.
As a result, the tag 1 having extremely high distance stability that can always secure a distance within 80% of the maximum communication distance is realized even in the air, on foamed polystyrene, or on a plastic with a thickness of 2 mm.
As shown in FIG. 1, the tag 1 in this example has a size of 53 mm in width and 7 mm in length and is formed with four bent portions 7 on one side of both dipole portions 6 and 6. What is necessary is just to increase the number of bending parts, such as 5 times or 6 times on one side.
By the way, the tag 1 described above is a tag that outputs linearly polarized waves. In the second embodiment, the above-described linearly polarized wave tag 1 is used as it is without using a special circuit or the like, thereby realizing a tag that generates circularly polarized waves having an extended communication distance with the reader / writer.
In FIG. 5, the upper diagram is a perspective view showing the configuration of the circularly polarized wave generating tag in the second embodiment, and the lower diagram is a plan view with the resin removed.
By the way, the tag 1 shown in FIG. 1 in the first embodiment has the same longitudinal shape in the left and right directions (plus X direction and minus X direction), but the short direction is centered. On the other hand, the front and rear (plus Y direction and minus Y direction) are not the same shape.
The intersecting double tag 10 shown in FIG. 5 is configured such that two tags 1 (1a, 1b) similar to those shown in FIG. 1 intersect and overlap each other at an angle of 90 °. The configuration of the tag 1a and the tag 1b is as described with reference to FIG.
In addition, in the upper part of FIG. 5, X, Y, and Z arrows indicating directions indicate the orientation with respect to the tag 1 a. The tag 1b has the same orientation as shown in the lower part of FIG.
In this example, a tag in which the positive Y direction of the tag is directed to the positive X direction of the other tag is defined as the first tag 1a, and a tag in which the positive Y direction of the tag is directed to the negative X direction of the other tag is defined as the first tag 1a. 2 tag 1b.
That is, the crossed double tag 10 of the present example includes the first tag 1a and the second tag 1b, and the loop shapes of the respective inductance portions 4 (4a, 4b) are overlapped as wide as possible. One tag 1a and the second tag 1b intersect at an angle of 90 °, that is, in a cross shape. Further, the intersections are overlapped so that there is no gap as much as possible.
In FIG. 6, the upper figure schematically shows the first tag 1a and the second tag 1b stacked in a cross shape, and the middle figure shows the holder 11 made of, for example, resin, The lower figure shows the first tag 1 a and the second tag 1 b held by the holder 11.
As shown in the center of FIG. 6, a cross groove 12 is formed in the holder 11, and the first tag 1 a and the second tag 1 b are fitted into the cross groove 12. Is fixed by being pressed from above with an appropriate member not shown.
In the cross double tag 10, the configuration in which the first tag 1a and the second tag 1b are stacked in a cross shape is not limited to the configuration in which the cross tag 12 is held by the holder 11 in which the cross groove 12 is formed. You may make it seal between these resin sheets.
In FIG. 7, the upper diagram shows the direction of polarization of the antenna of the reader / writer (RW), and the middle diagram shows two crossings when the polarization plane of the first tag 1a faces the direction of the reader / writer. The figure explaining operation | movement of the heavy tag 10 is a figure explaining the operation | movement of the crossing double tag 10 in case the polarization plane of the 2nd tag 1b has faced the direction of the reader / writer.
As shown in the center of FIG. 7, when the polarization plane of the first tag 1a faces the reader / writer, the first tag 1a operates.
As described above, when the first tag 1a is first operated, a current flows through the loop of the inductance portion 4a of the first tag 1a, and the high frequency coupling with the loop of the inductance portion 4b of the second tag 1b is performed. Accordingly, the second tag 1b operates with a phase delay of 90 ° as will be described later.
Further, as shown in the lower part of FIG. 7, when the polarization plane of the second tag 1b faces the reader / writer, the second tag 1b operates.
As described above, when the second tag 1b is first operated, a current flows through the loop of the inductance portion 4b of the second tag 1b, and the high-frequency coupling is performed with the loop of the inductance portion 4a of the first tag 1a. Accordingly, the first tag 1a operates with a phase delay of 90 ° as will be described later.
FIG. 8 shows a calculation model for calculating the operation of the above-described intersecting double tag 10 with an electromagnetic field simulator.
Both the IC chip 5 of the first tag 1a and the IC chip 5 of the second tag 1b have a capacitance component of Ccp = 1.43 pF. Although not specifically shown, each has an internal impedance of Rcp = 420Ω.
FIG. 9 is a diagram showing the results calculated by the electromagnetic field simulator, and the upper diagram is a diagram showing the relationship between the voltage generated in the IC chip 5 of the first tag 1a and the second tag 1b and its cycle, The lower diagram is also a diagram showing the relationship between the period and phase of the voltage generated in each IC chip 5.
In the upper diagram of FIG. 9, the horizontal axis indicates the voltage cycle from 0.7 GHz to 1.2 GHz, and the vertical axis indicates the voltage from 0V to 1.2V. As shown in the upper figure, the voltage V2 (0.8 V) which is about the same voltage V1 (0.88 V) as the voltage V1 generated in the IC chip of the tag 1 a at the period of 0.953 GHz is the IC chip of the tag 1 b. Has occurred.
In the lower part of FIG. 9, the horizontal axis indicates the voltage period from 0.7 GHz to 1.2 GHz, and the vertical axis indicates the phase of the period from minus 180 ° to plus 180 °.
Looking at the period / phase relationship diagram shown in the lower part of FIG. 9, in the upper figure, the voltage V2 of the tag 1b is generated in the period 0 · 953 GHz in which the tag 1b generates the same voltage V2 as the voltage V1 of the tag 1a. It can be seen that the phase of is delayed by 90 ° with respect to the phase of the voltage V1 of the tag 1a.
That is, as shown in FIG. 9, at an operating frequency of 953 MHz, a voltage of 0.8V is generated in the tag 1b with respect to a generated voltage of 0.88V in the tag 1a, and the phase of the tag 1b with respect to the phase of the tag 1a. It can be seen that is operating 90 ° behind.
That is, since the above 90 ° phase delay operation is repeated at a period of 0.995 GHz, it can be seen that when the tag 1a and the tag 1b are considered as one set, the operation is close to circular polarization.
However, ideally, the same voltage is generated in both the tag 1a and the tag 1b, and a phase shift of 90 ° is desirable for an operation closer to circular polarization.
At this time, as shown in the center of FIG. 7, the direction of circular polarization of the reader / writer (the counterclockwise direction in the figure shown in the upper part of FIG. 7) coincides with the rotation direction of the crossed double tag 10. Communication distance will increase. That is, the information held by the tag 1a can be read even at a distance of √2 times, that is, 1.41 times the maximum communication distance between the circularly polarized reader / writer and the linearly polarized tag.
On the other hand, as shown in the lower diagram of FIG. 7, when the tag 1b is operated, the tag 1a operates with a phase delay of 90 °. Therefore, the circular polarization operation described above is performed in the rotational direction of the circular polarization of the reader / writer. Is the opposite. For this reason, the communication distance of the tag 1b becomes short contrary to the case of the tag 1a.
However, when the reader / writer can switch the rotation direction of the circularly polarized wave in both forward and reverse directions at a constant cycle, both the tag 1a and the tag 1b are 1.41 times as long as the tag alone. You can communicate.
FIG. 10 is a diagram illustrating a result calculated by an electromagnetic field simulator when a space of a distance h = 1 mm is opened without closely contacting the overlapping portion (intersection portion) of the tag 1a and the tag 1b.
The upper diagram in FIG. 10 shows a cross double tag 15 in which a tag 1a and a tag 1b are crossed with a space of a distance h = 1 mm, and the middle diagram shows voltages generated in the tag 1a and the tag 1b, respectively. The figure which shows the relationship between the period and the lower figure is a figure which similarly shows the relationship between the period and phase of the voltage which generate | occur | produces, respectively.
Comparing the middle diagram of FIG. 10 and the upper diagram of FIG. 9, it can be seen that the generated voltage V2 of the tag 1b is slightly weaker than the generated voltage V1 of the tag 1a.
Further, comparing the lower diagram of FIG. 10 with the lower diagram of FIG. 9, it can be seen that the phase difference of the generated voltage V2 of the tag 1b with respect to the generated voltage V1 of the tag 1a is 75 °. That is, it can be seen that the degree of circular polarization is slightly weakened.
From these facts, it can be seen that in order to generate a circularly polarized wave in the intersecting double tag, it is better to make the intersecting part as close as possible.
It can also be seen that elliptical polarized waves are generated when the intersections of the intersecting double tags are crossed with a certain space left in close contact.
FIG. 11 is a diagram illustrating a result calculated by the electromagnetic field simulator when the loops are completely unsuperposed without overlapping the loops of the inductance part 4a of the tag 1a and the inductance part 4b of the tag 1b.
The upper diagram in FIG. 11 shows a crossed double tag 16 in which the loops of the inductance portions of the tag 1a and the tag 1b are completely removed and crossed, and the middle diagram shows the tag 1a and the tag 1b, respectively. The figure which shows the relationship between the voltage which generate | occur | produces, and its period, and a lower figure are figures which show the relationship between the period and voltage of the voltage which generate | occur | produce each similarly.
11 shows that the voltage V2 of the tag 1b is hardly generated with respect to the generated voltage V1 of the tag 1a, that is, the tags are not resonance-coupled.
From these, it can be seen that it is desirable that the loops of the inductance portions of the tag 1a and the tag 1b overlap as much as possible. Therefore, it can be said that the loop shape of the inductance portion is desirably a square, a circle, or a shape similar to them.
In the above-described embodiment, the UHF band RFID has been described, but it goes without saying that the present invention can also be applied to a 2.45 GHz RFID.
Further, the case where the reader / writer side is circularly polarized has been described. However, when the reader / writer side is an elliptically polarized wave between the linearly polarized wave and the circularly polarized wave, the two tags are not 90 °, for example, 60 °. By overlapping, the cross double tag side can also be operated with elliptical polarization.
Alternatively, even if the overlapping state of the loop of the inductance portion is shifted, the operation can be performed with elliptically polarized waves.
In addition, the loop shape of the inductance part is desirably a square, a circle, or a shape similar to them, but even if the loop shape is a rectangular shape as in the embodiment, the operation can be sufficiently close to a circularly polarized wave. Therefore, it goes without saying that the cross double tag of the present invention and the RFID system using the same can be applied to two tags each having a loop.
Here, the actual use environment of the intersection double tag will be described.
Usually, when mass-producing tags, different IDs are written to the respective tags. Therefore, with the structure of the cross double tag as in the present invention, when communicating with the reader / writer at a short distance, the two IDs of the tag 1a and the tag 1b are read on the reader / writer side.
Therefore, the tag to be read on the reader / writer side is, for example, the tag 1a, the tag 1b is considered as a dummy, the ID of the tag 1b is designated as “kill” in the reader / writer, and only the information on the tag 1a is always read. It is good to do so.
Note that the above matters are based on the premise that different IDs are written to all tags at the time of factory shipment. However, users who can freely write information into the area in the IC chip later can be included in the tags. Some have memory.
In such a case, if the same information is written in both the user areas of the tag 1a and the tag 1b, no trouble occurs even if the reader / writer reads the tag 1b at a short distance.
Further, as apparent from FIG. 7, if the circular polarization plane of the reader / writer is switched in the reverse direction, the communication distance of the tag 1b can be extended and the communication distance of the tag 1a can be reduced.
As described above, by switching the circular polarization plane of the reader / writer in both forward and reverse directions, it is possible to read any information of the tag 1a or the tag 1b in a state where the communication distance is extended. That is, different information can be written in the two user memories, and the different information can be read by the reader / writer, so that the user memory is not wasted.
As described above, conventionally, in order to make the tag circularly polarized, it has been necessary to provide a complicated circuit such as a 90 ° phase shifter by crossing two linearly polarized tags. According to this crossed double tag, it is possible to extend the communication distance with the reader / writer simply by overlapping the existing linearly polarized wave tag having the loop of the inductance portion in a cross shape.
It is a perspective view which shows the structure of the very small tag antenna in 1st Embodiment. It is a figure which shows the frequency characteristic of the reflection calculated with the electromagnetic field simulator of the antenna for tags in 1st Embodiment. It is a figure which shows the antenna gain calculation value calculated with the electromagnetic field simulator of the antenna for tags in 1st Embodiment. It is a communication distance characteristic view obtained by combining the reflection characteristics and gain characteristics of the tag antenna in the first embodiment on Excel. It is the perspective view which shows the structure of the crossing double tag in 2nd Embodiment, and the top view which removed the resin protective film. It is a figure which shows the state which hold | maintains and comprises the 1st tag and 2nd tag which were piled up on the cross of the cross double tag in 2nd Embodiment in a holder. It is a figure explaining operation | movement of the intersection double tag in 2nd Embodiment with respect to a reader / writer (RW). It is a figure which shows the calculation model for calculating operation | movement of the intersection double tag in 2nd Embodiment with an electromagnetic field simulator. It is a figure which shows the relationship between the voltage computed with the electromagnetic simulator of the crossing double tag in 2nd Embodiment, and its period, and the figure which shows the relationship between a period and a phase. It is a figure which shows the result calculated with the electromagnetic field simulator when the space | interval of distance h = 1mm is made open without making the cross | intersection part of a 1st tag and a 2nd tag contact | adhered as a trial. It is a figure which shows the result calculated with the electromagnetic field simulator at the time of making the trial and the overlap of the loop of the inductance part of a 1st tag and the loop of the inductance part of a 2nd tag completely remove as a trial.
1 (1a, 1b) tag (linear polarization tag)
2 Dipole antenna 3 Feeder (chip mounting part)
4 (4a, 4b) Inductance part 5 IC chip 6 Dipole part 7 (7-1, 7-7, 7-3, 7-4) Bending part 8 Resin 10 Crossing double tag 11 Holder 12 Cross groove 15, 16 crossing double tag
A dipole antenna formed of a conductor in the same plane, a feeding part connected with an IC chip at the center of the dipole antenna, and a dipole of the dipole antenna formed in the middle of the dipole of the dipole antenna. Loop-shaped inductance parts connected in parallel to each other, and the first and second tags are crossed so that the loop shapes of the inductance parts overlap each other. A crossing double tag characterized by consisting of:
The crossed double tag according to claim 1, wherein each of the inductance portions is formed in a square shape, a circular shape, or a loop shape approximate thereto.
The first and second tags are configured such that the loop shapes of the inductance portions are crossed so as to overlap as wide as possible and are overlapped with no gap as much as possible. The intersecting double tag according to claim 1 or 2.
4. The cross double tag according to claim 1, wherein the first and second tags generate circularly polarized waves at a cross angle of 90 °.
A holding member having a recess corresponding to a shape in which the first and second tags intersect with each other, and the recess in the holding member causes the first and second tags to intersect with the holding member. The cross double tag according to claim 1, 2, 3, or 4, wherein the cross double tag is held.
A dipole antenna formed of a conductor in the same plane, a feeding part connected with an IC chip at the center of the dipole antenna, and a dipole of the dipole antenna formed in the middle of the dipole of the dipole antenna. The first and second tags each have a loop-shaped inductance portion connected in parallel, and the first and second tags intersect so that the loop shapes of the respective inductance portions overlap each other. Intersecting double tag,
A reader / writer for transmitting a circularly polarized radio signal to read out the information of the first tag or the information of the second tag;
An RFID (radio frequency identification) system comprising:
The reader / writer is configured such that the first tag is set as a read tag, the second tag is set as a non-read tag, and only the information of the first tag is always read. RFID (radio frequency identification) system as described.
Each of the first and second tags includes a user memory area in which the same information is written,
The reader / writer switches the circular polarization plane of the circularly polarized radio signal in either the forward or reverse direction and responds more strongly to the switched circular polarization from the first or second tag to the user. Read memory area information,
The RFID (radio frequency identification) system according to claim 5.
Each of the first and second tags includes a user memory area in which different information is written.
The reader / writer sequentially switches the circular polarization plane of the circularly polarized radio signal in both forward and reverse directions, and responds more strongly to circular polarization in response to the switching from the first or second tag to the user memory area. 6. The RFID (radio frequency identification) system according to claim 5, wherein the information in the user memory area is read from both of the first and second tags by reading the information.
JP2007125055A 2007-05-09 2007-05-09 Tag device and RFID system using the same Expired - Fee Related JP4806373B2 (en)
TW097112843A TWI350613B (en) 2007-05-09 2008-04-09 Crossed dual tag and rfid system using the crossed dual tag
US12/081,344 US8022886B2 (en) 2007-05-09 2008-04-15 Crossed dual tag apparatus and system using crossed dual tag apparatus
EP20080103626 EP1993168B1 (en) 2007-05-09 2008-04-21 Crossed dual tag and RFID system using the crossed dual tag
CN 200810096423 CN101303747B (en) 2007-05-09 2008-05-09 Cross double tag and RFID system using the same
JP2008283404A true JP2008283404A (en) 2008-11-20
JP4806373B2 JP4806373B2 (en) 2011-11-02
JP2007125055A Expired - Fee Related JP4806373B2 (en) 2007-05-09 2007-05-09 Tag device and RFID system using the same
JP2010161959A (en) * 2009-01-14 2010-07-29 Mitsubishi Electric Corp Earmark rfid tag for animal
JP2013090633A (en) * 2012-12-10 2013-05-16 Mitsubishi Electric Corp Rfid animal ear tag
JP2016051432A (en) * 2014-09-02 2016-04-11 東芝テック株式会社 Radio frequency detector
WO2017006752A1 (en) * 2015-07-09 2017-01-12 株式会社オートネットワーク技術研究所 Clamp and electrical wire with clamp
CN106816697A (en) * 2016-12-26 2017-06-09 上海交通大学 The broadband circle polarized handheld terminal antennas of UHF of low section
WO2006011187A1 (en) * 2004-07-23 2006-02-02 Mitsubishi Denki Kabushiki Kaisha Radio tag communication system
KR100641636B1 (en) * 2004-12-08 2006-11-02 한국전자통신연구원 Dual Polarization Antenna and Radio Frequency Identification Reader
2008-05-09 CN CN 200810096423 patent/CN101303747B/en not_active IP Right Cessation
KR100984429B1 (en) 2010-09-30
JP2005218021A (en) 2005-08-11 Small loop antenna for inductive reader/writer