TWI451633B - Antenna - Google Patents
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- TWI451633B TWI451633B TW097136896A TW97136896A TWI451633B TW I451633 B TWI451633 B TW I451633B TW 097136896 A TW097136896 A TW 097136896A TW 97136896 A TW97136896 A TW 97136896A TW I451633 B TWI451633 B TW I451633B
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Description
本發明涉及通信終端的天線技術,特別是一種天線。The present invention relates to antenna technology for communication terminals, and more particularly to an antenna.
在筆記型電腦上使用多天線系統需要同時安裝多個天線單元,但可以安裝天線單元的空間位置有限,而且天線單元之間必須保持足夠的間距以減小耦合,因此每個天線單元可以佔據的空間不得不縮小。一般而言,筆記型電腦天線都安裝在機器邊緣,呈長條狀。通常要求天線單元尺寸約為四分之一波長,這樣,在900 MHz的GSM頻段,天線單元要約80~90 mm。天線單元間隔要大於三分之一波長,即110 mm,要安裝兩個天線單元需要約270 mm。而考慮到還要加裝其他頻帶、如2.4 GHz的WLAN天線,則筆記型電腦邊長需要超過300 mm,這一尺寸要求和筆記型電腦小型化設計的趨勢形成矛盾。The use of multiple antenna systems on a notebook computer requires the installation of multiple antenna units at the same time, but the spatial position at which the antenna units can be mounted is limited, and there must be sufficient spacing between the antenna elements to reduce coupling, so each antenna unit can occupy The space has to shrink. In general, notebook antennas are mounted on the edge of the machine and are elongated. The antenna unit size is usually required to be about a quarter of a wavelength, so that in the 900 MHz GSM band, the antenna unit is about 80 to 90 mm. The antenna unit spacing is greater than one-third of the wavelength, or 110 mm, and it takes about 270 mm to install two antenna elements. Considering that other frequency bands, such as 2.4 GHz WLAN antennas, are required, the notebook computer needs more than 300 mm of side length, which is in contradiction with the trend of miniaturization of notebook computers.
目前,採用集總參數載入減小天線尺寸,或者用摺疊偶極減小天線尺寸,或者在輻射體上開槽、割縫的方法減小天線尺寸。然而,現有技術中至少存在如下問題:At present, the lumped parameter loading is used to reduce the antenna size, or the antenna size is reduced by folding the dipole, or the antenna size is reduced by slotting and slitting the radiator. However, at least the following problems exist in the prior art:
採用電容或者電感做載入,雖然可以減小天線尺寸,但在行動通信頻率(800 MHz以上)器件損耗比較大,造成天線實際增益較低;摺疊偶極可以減小天線尺寸,但是在筆記型電腦的邊緣使用摺疊偶極,由於輻射體離筆記型電腦金屬框架很近,輻射空間很有限,輻射阻抗很低,不容易阻抗匹配,天線頻寬窄;開槽割縫雖然可以減小天線尺寸,但是在筆記型電腦上天線需要安裝在螢幕邊緣,經常沒有足夠的空間去開槽割縫。Capacitance or inductance is used for loading. Although the antenna size can be reduced, the loss of the device at the mobile communication frequency (above 800 MHz) is relatively large, resulting in a lower actual antenna gain. The folded dipole can reduce the antenna size, but in the notebook type. The edge of the computer uses a folded dipole. Because the radiator is close to the metal frame of the notebook computer, the radiation space is very limited, the radiation impedance is very low, the impedance matching is not easy, and the antenna bandwidth is narrow. Although the slotted slit can reduce the antenna size, But on the notebook computer, the antenna needs to be installed on the edge of the screen, and often there is not enough space to slot the slit.
有鑒於此,本發明提供了一種天線,能降低天線諧振頻率,減小天線尺寸。In view of this, the present invention provides an antenna capable of reducing the antenna resonance frequency and reducing the antenna size.
為達到上述目的,本發明一種技術方案是這樣實現的:一種天線,包括參考地面、第一輻射枝和第二輻射枝; 所述參考地面,包括有第一接地點和第二接地點;所述第一輻射枝,通過所述第一接地點與所述參考地面連接;所述第二輻射枝,通過所述第二接地點與所述參考地面連接;其中,所述第一輻射枝與第二輻射枝之間形成有縫隙,通過所述縫隙耦合形成分佈電容,用於耦合信號;所述第二輻射枝用於耦合信號的一端與射頻饋線的連接點為饋電點,所述饋電點位於第一接地點與第二接地點之間。In order to achieve the above object, a technical solution of the present invention is implemented as follows: an antenna including a reference ground, a first radiating branch, and a second radiating branch; The reference ground includes a first grounding point and a second grounding point; the first radiating branch is connected to the reference ground through the first grounding point; and the second radiating branch passes the second ground a grounding point is connected to the reference ground; wherein a gap is formed between the first radiant branch and the second radiant branch, and a distributed capacitance is formed through the slot coupling for coupling a signal; the second radiant branch is used for A connection point of one end of the coupled signal and the RF feed line is a feed point, and the feed point is located between the first ground point and the second ground point.
優選地,所述第一輻射枝為共面波導耦合輻射枝。Preferably, the first radiant branch is a coplanar waveguide coupled radiant branch.
所述第二輻射枝為平面倒F型天線輻射枝。The second radiating branch is a planar inverted-F antenna radiating branch.
所述第一輻射枝、第二輻射枝的非接地端向同側或異側伸展。The non-ground ends of the first radiant branch and the second radiant branch extend toward the same side or the opposite side.
所述射頻饋線是同軸線、微帶線、帶狀線或波導中任一種。The RF feed line is any one of a coaxial line, a microstrip line, a strip line, or a waveguide.
所述共面波導耦合輻射枝是折線形金屬片或由平面金屬片折疊形成的立體結構。The coplanar waveguide coupling radiation branch is a polygonal metal sheet or a three-dimensional structure formed by folding a planar metal sheet.
所述平面倒F型天線輻射枝是T形金屬片或由平面金屬片折疊形成的立體結構。The planar inverted-F antenna radiating branch is a T-shaped metal piece or a three-dimensional structure formed by folding a planar metal piece.
所述參考地面為平面金屬片或由平面金屬片折疊形成的立體結構。The reference ground is a planar metal sheet or a three-dimensional structure formed by folding a flat metal sheet.
本發明所提供的天線,具有如下優點:因為天線諧振枝之間採用了共面波導耦合結構,等效於電容載入,而且分佈電容載入的場主要集中在空氣中,所以克服了集總參數電容器載入後器件內電阻造成的功率損耗,進而達到了降低天線諧振頻率,減小了天線尺寸。The antenna provided by the invention has the following advantages: since the co-planar waveguide coupling structure is adopted between the antenna resonance branches, equivalent to the capacitive loading, and the field of the distributed capacitance is mainly concentrated in the air, the lumping is overcome. The power loss caused by the resistance of the device after the parameter capacitor is loaded, thereby reducing the antenna resonance frequency and reducing the antenna size.
本發明採用天線輻射枝之間的耦合形成電容,從而減少了元件及隔離空間,縮小了天線尺寸,使天線更符合便攜設備對尺寸的需求。The invention adopts the coupling between the antenna radiation branches to form a capacitor, thereby reducing the components and the isolation space, reducing the size of the antenna, and making the antenna more suitable for the size requirements of the portable device.
圖1是本發明第一實施例的結構示意圖,如圖1所示,共面波導耦合雙頻天線由參考地面1、共面波導耦合輻射枝2和平面倒F型天線(PIFA,Planar Inverted F Antenna)輻射枝3構成。其中,參考地面1為窄長條結構的平面金屬;共面波導耦合輻射枝2為折線形窄長條金屬片,一端與參考地面1平行,另一端與參考地面1連接點為接地點A;PIFA輻射枝3是T 形金屬片,與參考地面1連接點為接地點B,一個分枝末端為饋電點C,另一分枝為輻射枝且末端懸空。共面波導耦合輻射枝2和PIFA輻射枝3無直接電連接,而是依靠縫隙4耦合來饋電,形成分佈電容。1 is a schematic structural view of a first embodiment of the present invention. As shown in FIG. 1, a coplanar waveguide coupled dual-frequency antenna is coupled with a ground plane 1, a coplanar waveguide, a radiating branch 2, and a planar inverted-F antenna (PIFA, Planar Inverted F Antenna). ) radiant branches 3 constitute. Wherein, the reference ground 1 is a plane metal of a narrow strip structure; the coplanar waveguide coupling radiant branch 2 is a strip-shaped narrow strip of metal strip, one end is parallel to the reference ground 1, and the other end is connected to the reference ground 1 as a ground point A; PIFA Radiation Branch 3 is T The metal piece is connected to the reference ground 1 as the grounding point B, one branch end is the feeding point C, and the other branch is the radiating branch and the end is suspended. The coplanar waveguide coupled radiation branch 2 and the PIFA radiation branch 3 have no direct electrical connection, but are fed by the slot 4 coupling to form a distributed capacitance.
共面波導耦合結構5由共面波導耦合輻射枝2的折回部分和PIFA輻射枝3的非輻射端共面耦合構成,共面波導耦合結構5與參考地面1通過同軸線連接,饋電點C接同軸線內導體,參考地面1的連接點D接同軸線外導體,該結構等效於電容載入,可以降低天線諧振頻率。共面波導耦合輻射枝2在低頻段(GSM 960 MHz)諧振PIFA輻射枝3在高頻段(DCS/PCS 1800 MHz)諧振。整個天線為窄長條結構,圖2是第一實施例的效果圖,該天線可以貼合在筆記型電腦機殼或者液晶螢幕6的邊緣,並具有接近全向的方向圖和增益。The coplanar waveguide coupling structure 5 is formed by coplanar coupling of the folded portion of the coplanar waveguide coupling radiation branch 2 and the non-radiative end of the PIFA radiation branch 3, and the coplanar waveguide coupling structure 5 is connected to the reference ground 1 through a coaxial line, and the feeding point C Connect the inner conductor of the coaxial line, and connect the connection point D of the ground 1 to the outer conductor of the coaxial line. This structure is equivalent to the loading of the capacitor and can reduce the resonance frequency of the antenna. The coplanar waveguide couples the radiating branch 2 in the low frequency band (GSM 960 MHz) to resonate the PIFA radiating branch 3 in the high frequency band (DCS/PCS 1800 MHz). The entire antenna has a narrow strip structure. FIG. 2 is an effect diagram of the first embodiment. The antenna can be attached to the edge of the notebook computer case or the liquid crystal screen 6 and has a nearly omnidirectional pattern and gain.
圖3是本發明第二實施例的示意圖,將PIFA輻射枝3的輻射端改為與共面波導耦合輻射枝2同向共面波導耦合輻射枝2側伸展,PIFA輻射枝3和共面波導耦合輻射枝2均為平面金屬片折疊的立體結構。這樣,增加了縫隙4的長度,使得諧振頻率有所下降,以適應不同需求。圖4是該實施例的效果圖,從圖4中可以看出,與第一實施例相比,天線的外形尺寸也有所不同,能夠更佳地滿足需求。3 is a schematic view showing a second embodiment of the present invention, in which the radiant end of the PIFA radiant branch 3 is changed to be coplanar with the coplanar waveguide coupling radiant branch 2 co-planar waveguide waveguide radiant branch 2, PIFA radiant branch 3 and coplanar waveguide The coupled radiant branches 2 are three-dimensional structures in which the planar metal sheets are folded. Thus, the length of the slit 4 is increased, so that the resonance frequency is lowered to suit different needs. Fig. 4 is an effect diagram of the embodiment. As can be seen from Fig. 4, the outer dimensions of the antenna are different as compared with the first embodiment, and the demand can be more satisfactorily satisfied.
圖5是本發明的第三實施例示意圖,將共面波導耦合輻射枝2的輻射端與PIFA輻射枝3的輻射端同向PIFA輻射枝3側伸展,同樣增加了縫隙4的長度,此外還可以將參考地面1設計為平面金屬片所折疊成的立體結構,以適應不同的空間需求。Figure 5 is a schematic view of a third embodiment of the present invention, in which the radiating end of the coplanar waveguide coupled radiating branch 2 and the radiating end of the PIFA radiating branch 3 are extended toward the side of the PIFA radiating branch 3, which also increases the length of the slit 4, in addition The reference ground 1 can be designed as a three-dimensional structure in which flat metal sheets are folded to suit different space requirements.
圖6是本發明第四實施例示意圖,將共面波導耦合輻射枝2的輻射端與PIFA輻射枝3的輻射端相向,即向異側伸展,更進一步減小天線的尺寸,此時縫隙4的長度增加,可以通過調整縫隙4的寬度,使諧振頻率增加,從而滿足需求。連接饋電點C與參考地面1的連接點D之間的射頻饋線還可以是微帶線、帶狀線或波導等。6 is a schematic view of a fourth embodiment of the present invention, in which the radiating end of the coplanar waveguide coupling radiation branch 2 faces the radiating end of the PIFA radiation branch 3, that is, extends to the opposite side, further reducing the size of the antenna, and the gap 4 at this time The length is increased, and the resonance frequency can be increased by adjusting the width of the slit 4 to satisfy the demand. The RF feed line connecting the connection point C of the feed point C and the reference ground 1 may also be a microstrip line, a strip line or a waveguide or the like.
通過仿真試驗從饋電點C測得回波損耗值如圖7所示,在頻率為980 MHz和1780 Mhz附近,回波損耗值分別只有-10 dB、-20 dB左右,而這正是GSM頻段與DCS/PCS頻段,從而說明本發明性能滿足需求。The return loss value measured from the feed point C by simulation test is shown in Fig. 7. At frequencies around 980 MHz and 1780 Mhz, the return loss values are only -10 dB and -20 dB, respectively, and this is GSM. The frequency band and the DCS/PCS band indicate that the performance of the present invention satisfies the requirements.
仿真試驗還檢測了天線增益。所謂天線增益是在輸入功率相等的條件下,實際天線與理想的輻射單元在空間同一點處所產生的信號的功率密度之比,天線增益定量地描述一個天線把輸入功率集中輻射的程度。圖8是仿真實驗中天線輻射方向的坐標系建立的視圖,根據圖8中的坐標系,圖9是在GSM頻段天線增益的三維視圖。天線具有接近全向的方向圖和增益,輻射方向圖坐標系如圖8中所示,偶極軸沿Y方向,參考地和大地在坐標系中央,天線單元在坐標系左側,平均增益約為0 dBi。The simulation test also detected the antenna gain. The so-called antenna gain is the ratio of the power density of the signal generated by the actual antenna to the ideal radiating element at the same point in space under the condition of equal input power. The antenna gain quantitatively describes the degree to which an antenna concentrates the input power. Fig. 8 is a view showing the establishment of a coordinate system of the radiation direction of the antenna in the simulation experiment. According to the coordinate system in Fig. 8, Fig. 9 is a three-dimensional view of the antenna gain in the GSM band. The antenna has a nearly omnidirectional pattern and gain. The radiation pattern coordinate system is shown in Figure 8. The dipole axis is in the Y direction, the reference ground and the earth are in the center of the coordinate system, and the antenna unit is on the left side of the coordinate system. The average gain is about 0 dBi.
圖10、圖11、圖12分別為GSM頻段天線增益的X-Y、X-Z、Y-Z平面視圖,頻率為980 MHz。圖13是在DCS/PCS頻段天線增益的三維視圖,平均增益約為0 dBi。圖14、圖15、圖16分別為GSM頻段天線增益的X-Y、X-Z、Y-Z平面視圖,頻率為1780 MHz。仿真試驗表明,該天線增益在0 dBi以上,具有很好的實用性。Figure 10, Figure 11, and Figure 12 show the X-Y, X-Z, and Y-Z plane views of the GSM band antenna gain, respectively, at a frequency of 980 MHz. Figure 13 is a three-dimensional view of the antenna gain in the DCS/PCS band with an average gain of approximately 0 dBi. Figure 14, Figure 15, and Figure 16 show the X-Y, X-Z, and Y-Z plane views of the GSM band antenna gain, respectively, at a frequency of 1780 MHz. Simulation experiments show that the antenna gain is above 0 dBi and has good practicability.
前文係針對本發明之較佳實施例為本發明之技術特徵進行具體之說明,唯熟悉此項技術之人士當可在不脫離本發明之精神與原則下對本發明進行變更與修改,而該等變更與修改,皆應涵蓋於如下申請專利範圍所界定之範疇中。The foregoing is a description of the preferred embodiments of the present invention, and the present invention may be modified and modified without departing from the spirit and scope of the invention. Changes and modifications are to be covered in the scope defined by the scope of the patent application below.
1‧‧‧參考地面1‧‧‧ reference ground
2‧‧‧共面波導耦合輻射枝2‧‧‧coplanar waveguide coupled radiation branch
3‧‧‧PLFA輻射枝3‧‧‧PLFA radiation branch
4‧‧‧縫隙4‧‧‧ gap
5‧‧‧共面波導耦合結構5‧‧‧Coplanar waveguide coupling structure
6‧‧‧液晶螢幕6‧‧‧ LCD screen
A‧‧‧接地點A‧‧‧ Grounding point
B‧‧‧接地點B‧‧‧ Grounding point
C‧‧‧饋電點C‧‧‧Feeding point
D‧‧‧連接點D‧‧‧ connection point
圖1為本發明第一實施例的結構示意圖;圖2為本發明第一實施例的效果圖;圖3為本發明第二實施例的結構示意圖;圖4為本發明第二實施例的效果圖;圖5為本發明第三實施例的結構示意圖;圖6為本發明第四實施例的結構示意圖;圖7為本發明一個實施例仿真參數示意圖;圖8為本發明一個實施例輻射方向坐標系視圖;圖9為本發明一個實施例GSM頻段天線增益三維視圖;圖10為本發明一個實施例GSM頻段天線增益X-Y平面投影視圖;圖11為本發明一個實施例GSM頻段天線增益X-Z平面投影視圖; 圖12為本發明一個實施例GSM頻段天線增益Y-Z平面投影視圖;圖13為本發明一個實施例DCS/PCS頻段天線增益三維視圖;圖14為本發明一個實施例DCS/PCS頻段天線增益X-Y平面投影視圖;圖15為本發明一個實施例DCS/PCS頻段天線增益X-Z平面投影視圖;圖16為本發明一個實施例DCS/PCS頻段天線增益Y-Z平面投影視圖。1 is a schematic structural view of a first embodiment of the present invention; FIG. 2 is a schematic view of a first embodiment of the present invention; FIG. 3 is a schematic structural view of a second embodiment of the present invention; Figure 5 is a schematic structural view of a third embodiment of the present invention; Figure 6 is a schematic structural view of a fourth embodiment of the present invention; Figure 7 is a schematic diagram of simulation parameters of an embodiment of the present invention; Figure 9 is a three-dimensional view of the gain of the GSM band antenna according to an embodiment of the present invention; Figure 10 is an XY plane projection view of the GSM band antenna gain according to an embodiment of the present invention; Figure 11 is an XZ plane of the GSM band antenna gain according to an embodiment of the present invention. Projection view 12 is a JPEG plane antenna gain YZ plane projection view according to an embodiment of the present invention; FIG. 13 is a three-dimensional view of a DCS/PCS band antenna gain according to an embodiment of the present invention; FIG. 14 is a DCS/PCS band antenna gain XY plane according to an embodiment of the present invention; FIG. 15 is a view showing a DCS/PCS band antenna gain XZ plane projection view according to an embodiment of the present invention; FIG. 16 is a DCS/PCS band antenna gain YZ plane projection view according to an embodiment of the present invention.
1‧‧‧參考地面1‧‧‧ reference ground
2‧‧‧共面波導耦合輻射枝2‧‧‧coplanar waveguide coupled radiation branch
3‧‧‧PIFA輻射枝3‧‧‧PIFA radiation branch
4‧‧‧縫隙4‧‧‧ gap
5‧‧‧共面波導耦合結構5‧‧‧Coplanar waveguide coupling structure
A‧‧‧接地點A‧‧‧ Grounding point
B‧‧‧接地點B‧‧‧ Grounding point
C‧‧‧饋電點C‧‧‧Feeding point
D‧‧‧連接點D‧‧‧ connection point
Claims (6)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| TW097136896A TWI451633B (en) | 2008-09-25 | 2008-09-25 | Antenna |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| TW097136896A TWI451633B (en) | 2008-09-25 | 2008-09-25 | Antenna |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| TW201014044A TW201014044A (en) | 2010-04-01 |
| TWI451633B true TWI451633B (en) | 2014-09-01 |
Family
ID=44829525
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| TW097136896A TWI451633B (en) | 2008-09-25 | 2008-09-25 | Antenna |
Country Status (1)
| Country | Link |
|---|---|
| TW (1) | TWI451633B (en) |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI227576B (en) * | 2004-03-30 | 2005-02-01 | Kin-Lu Wong | Dual-band inverted-F antenna with a shorted parasitic element |
| US7081854B2 (en) * | 2002-05-02 | 2006-07-25 | Sony Ericsson Mobile Communications Ab | Printed built-in antenna for use in a portable electronic communication apparatus |
| TWM321153U (en) * | 2007-01-25 | 2007-10-21 | Wistron Neweb Corp | Multi-band antenna |
-
2008
- 2008-09-25 TW TW097136896A patent/TWI451633B/en active
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7081854B2 (en) * | 2002-05-02 | 2006-07-25 | Sony Ericsson Mobile Communications Ab | Printed built-in antenna for use in a portable electronic communication apparatus |
| TWI227576B (en) * | 2004-03-30 | 2005-02-01 | Kin-Lu Wong | Dual-band inverted-F antenna with a shorted parasitic element |
| TWM321153U (en) * | 2007-01-25 | 2007-10-21 | Wistron Neweb Corp | Multi-band antenna |
Also Published As
| Publication number | Publication date |
|---|---|
| TW201014044A (en) | 2010-04-01 |
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