201232919 六、發明說明： 【發明所屬之技術領域】 本發明係關於一種整合式號角天線裝置，尤指一種可 改善輻射場型且增加指向性的天線。 【先前技術】 近年來工業發展科技化，為即時監控儲存槽内的料位而 於槽頂架設雷達天線裝置，該雷達天線裝置可發射一微波訊 ® 號，當此訊號接觸到物料會產生一反射訊號，藉由發射訊號 與接收訊號兩者的頻率差與時間差，進而算出至待測物間的 距離。 既有的雷達天線裝置中的天線結構如圖]5的美國專利 US 6353418所示，其係在一導波管91的輸入端設有一訊 號輸入接頭92’該導波管91的輸出端設有一漏斗狀號角天 線93,又導波管91的内部形成有—腔體，該腔體内係㈣ 柱介質94所填滿’該圓柱介質94表面從導波管91輸出端 •向漏斗狀號角天線93 &伸形成有—線性圓錐介質轉換器 95(如圖16所示），且該圓柱介質94可由鐵氟龍2F(pTFE) 構成。 唯，此種天線結構因為該線性圓錐介質轉換$ 95的頂 點951係為尖角，故該線性圓錐介質轉換器95之輕射場型 在主波束峰端易造成尖端場型影響天線輕射效率；且因導波 管91内的腔體係為圓柱介質94所填滿，故訊號從訊號輸 入接頭92輸人導波管91時’該訊號會直接進人圓柱介質 94内’並由圓柱介質94輸入至線性圓錐介質發射錐體95， 201232919 但因訊號輸入接頭92阻抗（50歐姆）通常遠較在號角形天線 93内的空氣介質阻抗（377歐姆）小，要直接從訊號輸入接頭 92的小阻抗轉換成號角形天線93内空氣介質的大阻抗實屬 不易’且阻抗過於大幅轉換會降低天線頻寬。以上所述皆為 既有技術未臻理想之處’實有待進一步檢討，並謀求可行 的解決方案。 【發明内容】 為此，本發明的主要目的在於提供一種整合式號角天 線裝置’主要係改良天線中的導波管及介質發射錐體，使 該整合式號角天線裝置可達成良好的阻抗轉換，並具有更 好的指向性’進而提高輻射的效率。 為達成前述目的採取的主要技術手段係令前述整合式 號角天線裝置包括有： 一導波管，其具有一輸入端與一輸出端，該導波管内 係形成有一空氣共振腔體，且該空氣共振腔體與導波管的 輪入端與輸出端連通； -號角天線，其具有一輸入端與一輸出端，其輸入端 與該導波管的輸出端連接’且該號角天線的内徑從其輸入 端至其輸出端漸增； 一介質導波管，係設於該導波管的輸出端上，該介f 導灰s具有-第一端與一第二端’且該介質導波管第一端 的外徑係與空氣共振腔體的内徑對應； 一介質發射錐體，其係形成於該介質導波管上的第二 端’該介質發射錐體係位於該號角天線内，且該介質發射 錐體的頂點為一非尖角； 201232919 一訊號輸入接頭，係設於該導波管的輸入端，用以饋 入訊號，且不與介質導波管接觸； 一天線罩透鏡，係設於該號角天線之輸出端。 藉由前述的技術手段本發明可達到以下的優點及功 效： 因為該介質發射錐體的頂點為一非尖角，可避免主波 束頂端具有突出場型’故可有效的改善其輻射場型；且因 訊號先經過空氣共振腔體再經過介質發射錐體，故阻抗可 經兩次較小幅度的轉換’較易保持天線頻寬；又因為本發 明的天線罩透鏡可將圓錐天線輻射的平面波聚焦，故可有 效提升指向性，使半波束寬度更窄，增加對量測環境的抗 干擾性。 【實施方式】 以下配合圖式與本發明之較佳實施例，進一步闌述本 鲁發明為達成預疋發明目的所採取的技術手段。 請參閱圖1所示，本發明第一較佳實施例包括有一導 波管10、一訊號輸入接頭20、一號角天線3〇、—介質導 波官40、一介質發射錐體5〇、一天線罩透鏡6〇 ;其中： 該導波f 10具有_輸入端與一輸出端，又導波管扨 内係形成有-空氣共振腔體H，且該空氣共振腔體W與該 導波管1G的輸人端與輸出端連通，該導波f 1()可 構成； 該號角天線3G具有_輸人端與—輸出端，其輸入端與 邊導波f 1 〇的輸出端連接，且該號角天線3〇係呈錐筒狀， 201232919 其内徑從其輸入端至其輸出端漸增，在此較佳實施例中， 該號角天線30可用螺絲、法蘭與導波管1 〇鎖合； 該介質導波管40係設於該導波管1〇的輸出端上，又 介質導波管40具有一第一端及一第二端，其第一端的外徑 係與空氣共振腔體11的内徑對應； 請參閱圖1與圖3所示，該介質發射錐體50其係形成 於該介質導波管40上的第二端，該介質發射錐體5〇係位 於該號角天線30内，且該介質發射錐體具有一頂點51與 一周壁53，該周壁53具有一頂端及一底端，其周壁53外 徑由底端向頂端遞減’該介質發射錐體50的較佳實施例示 意圖請參閱圖3至圖5所示，圖3的介質發射錐體50形狀 係為一段線性頂點51純化圓錐形，其中一段係指該介質發 射錐體50具有一段周壁53 ’線性係指周壁53外徑由底端 向頂端遞減的幅度係為線性，頂點51鈍化係指頂點非為尖 角，又稱鈍化頂點’其可為平角的頂點也可為圓角的頂點； 圖11與圖12係為介質發射錐體5〇的E平面（E平面）與Η 平面（H-plane)的輻射場型，其中實線為同極化場型，虛線 為交又極化場型。 圖4的介質發射錐體50B係為一段曲線頂點51B鈍化 圓錐形’ 一段曲線頂點51 B鈍化圓錐形的一段係指該介質 發射錐體50B具有一段周壁53B，其周壁53B外徑由底端 向頂端遞減’而一段曲線頂點51 B鈍化圓錐形的曲線係指 周壁53B壁面由頂端至底端形成一内凹弧面，頂點5彳B鈍 化係指頂點51 B為鈍化頂點。 圖5的介質發射錐體50C係為二段曲線頂點51C純化 201232919 圓錐形，其中二段曲線頂點51 C鈍化圓錐形的二段係指該 介質發射錐體50C具有上周壁53C與下周壁54C，今上 下周壁53C、54C分別具有一頂端及一底端， 丄 F周 壁53C、54C的壁面分別由其頂端至底端形成一内凹弧面， 頂點51 C鈍化係指頂點51 C為鈍化頂點；圖1 3與圖】4為 該介質發射錐體50C的E平面與Η平面的輻射場型，圖内 實線為同極化場型’虛線為交叉極化場型；在其他實施例 中，該介質發射錐體也可形成有三段、四段或更多段周壁， ® 且頂點可為尖角頂點也可為純化頂點。 該介質導波管40與該介質發射錐體50可由高分子聚 合物、陶瓷或玻璃常用的材質，如氣乙烯（PVC)、氣化聚氣 乙稀（CPVC)、聚乙烯（HDPE)、乙烯鋼（UPE)、鐵氟龍 2F(PVDF)、鐵氟龍 4F(PTFE)、聚脂膠（PET)、聚丙烯（pp)、 尼龍 6(N-6)、尼龍 66(N-66)、MC 尼龍（MC)、塑膠鋼（POM)、 ABS樹脂（ABS)、聚笨乙烯（ps)、壓克力（PMMA)、聚碳酸 醋（pc)、聚醚醚酮（PEEK)、電木（Bake丨jte)、玻璃纖維 • (FRP)……等構成。 在其他實施例中，請參閱圖2所示，並令前述整合式 號角天線裝置進一步包括一内介質發射錐體70’其係形成 於該介質導波管4〇上的第一端，其設於該空氣共振腔體11 内’且該内介質發射錐體70也具有一頂點與一周壁’該周 壁具有一頂端與一底端，且該内介質發射錐體70的形狀可 與該介質發射錐體50相同，且其頂點係遠離該介質導波管 40的第一端。 請重新參閱圖1所示，該訊號輸入接頭20係設於導波 201232919 管10的輸入端’且不與介質導波管40接觸’該訊號輸入 接頭20用以饋入訊號至導波管10内的空氣共振腔體11 ’ 且該訊號輸入接頭20可為SMA接頭； 該天線罩透鏡60係設於該號角天線30之輸出端’該 天線罩透鏡60可由高分子聚合物、陶瓷或玻璃常用的材 質，如氣乙烯（PVC)、氣化聚氣乙烯（CPVC)、聚乙烯 (HDPE)、乙烯鋼（UPE)、鐵氟龍2F(PVDF)、鐵氟黃I 4F(PTFE)、聚脂膠（PET)、聚丙烯（PP)、尼龍6(N-6)、尼 龍 66(N-66)、MC 尼龍（MC)、塑膠鋼（POM)、ABS 樹脂 (ABS)、聚苯乙烯（PS)、壓克力（PMMA)、聚碳酸酯（PC)、 聚醚醚酮（PEEK)、電木（Bake丨ite)、玻璃纖維（FRP)......等 構成；該天線罩透鏡60的中心轴可與介質發射錐體5〇的 中心轴相同或不同；該天線罩透鏡6〇可為雙凸透鏡、平凸 透鏡、凹凸透鏡，凸凹透鏡、平凹透鏡或雙凹透鏡，如在 天線罩透鏡60的中心軸與號角天線3〇的中心軸不同的狀 態下，該天線罩透鏡60也可為環型的結構；請參閱圖7所 不，在此較佳實施例中，該天線罩透鏡6〇的中心軸與介質 發射錐體5G的中心軸相同，且該天線罩透鏡6Q係為凸透 鏡，其可為雙凸透鏡、平凸透鏡、凹凸透鏡，無論是何種 凸透鏡，請參閱圖6 ^ m 所不，其透鏡中央的厚度hi皆需大於 透鏡兩端的厚度^ * h3才為凸透鏡。圖7與圖8係分別為 使用平凸透鏡虫平叫泳拉+ 兄/、十凹透鏡時訊號的行進圖，當訊號從介質 错fin Γ 〇發射時，其係為平面波，待訊號通過天線罩透 無，疋圖7的平凸透鏡60與圖8的平凹透鏡 60A，訊號皆會集 达鏡 取焦在一點上；請參閱圖9與圖1 〇所 201232919 示’且天線罩透鏡60的中心軸也可與號角天線30的中心 轴不同’即天線罩透鏡60相對於號角天線30的中心軸係 為偏心’當訊號從介質發射錐體50發射時，其係為平面波， 待訊號通過偏心的天線罩透鏡60後，無論是圖9的平凸透 鏡60與圖1〇的平凹透鏡60A，訊號皆會偏向而集中聚焦 在一點上》 當訊號從訊號輸入接頭20(阻抗50歐姆）輸入導波管1〇 時，該訊號會先進入空氣共振腔體11(阻抗1〇〇~15〇歐姆） 内’再從空氣共振腔體11進入介質導波管40,並由介質導 波官40傳輸至介質發射錐體50發射至空氣介質（阻抗377 歐姆），故訊號的阻抗可經兩次較小幅度的轉換，較易保持 天線頻寬。 因為該介質發射錐體的頂點不為一尖角，避免主波束 頂端有突出場型’故可有效的改善其輻射場型；且因訊號 先經過空氣共振腔體再經過介質發射錐體，故阻抗可經兩 次較小幅度的轉換’較易保持天線頻寬；又因為本發明的 天線罩透鏡可將可將圓錐天線輻射的平面波聚焦，故可有 效提升指向性，使半波束寬度更窄，增加對量測環境的抗 干擾性。 且相較於周壁外徑由底端向頂端遞減的幅度係為線性 的介質發射錐體，周壁壁面由頂端至底端形成一内凹弧面 的介質發射錐體可使1、天線頻寬較線性介質發射錐體的天 線頻寬寬，2、天線的輻射場型旁波瓣與主波瓣的比值會提 高’故旁波束可壓低，故信號集中在主波束，可進一步提 高指向性’更進一步提高輻射的效率。 201232919 以上所述僅為本發明之較佳實施例，並非對本發明作 可：弋t限制’雖然本發明已以較佳實施例揭露如 公然而並非用以限定本發明，任何熟悉本專業的技術人 _ 2不脱離本發明技術方案的範圍内，#可利用上述揭 二曰：：：作出些許更動或修飾為等同變化的等效實施 技術實質：t:r發明技術方案的内容，依據本發明的 修飾，I 所作的任何簡單修改、等同變化與 二仍屬於本發明技術方案的範圍内。 、 【圖式簡單說明】 示意：1係為該整合式號角天線裝置-較佳實施例的剖面 意圖圖2係為該整合式號角天線裝置另-實施例的剖面示 錐體示意圖係杨狀H線性頂點鈍化圓錐形的介質發射 圖4係為形狀為一 錐體示意圖。 ’曲線頂點鈍化圓錐形的介質發射 圖5係為形狀為二段曲線頂點鈍化jg 錐體示意圖。 化圓錐形的介質發射 圖6係為透鏡比例的示意圖。 二至至圖1〇係為訊號穿越透鏡的行進示意圖。 圖14係為不同介質發射錐體 圖15係為既有天線結構的剖面;^的㈣場型圖。 6係為既有介質發射錐體的示意圖。 201232919 【主要元件符號說明】 10導波管 20訊號輸入接頭 30號角天線 40介質導波管 50、 50B、50C介質發射錐體 51、 51 B、51 C 頂點 53、53B周壁 • 53C上周壁 54C下周壁 60、60A天線罩透鏡 70内介質發射錐體 91導波管 92訊號輸入接頭 93漏斗狀號角天線 94圓柱介質 • 95線性圓錐介質轉換器201232919 VI. Description of the Invention: [Technical Field] The present invention relates to an integrated horn antenna device, and more particularly to an antenna which can improve the radiation pattern and increase directivity. [Prior Art] In recent years, the industrial development has been scientific and technological. In order to monitor the material level in the storage tank in real time, a radar antenna device is installed on the top of the tank. The radar antenna device can emit a microwave signal meter number. When the signal contacts the material, a The reflected signal is calculated by the frequency difference between the transmitted signal and the received signal and the time difference, thereby calculating the distance to the object to be tested. The antenna structure of the existing radar antenna device is shown in US Pat. No. 6,335,418, which is shown in Fig. 5, which is provided with a signal input connector 92' at the input end of a waveguide 91. The output end of the waveguide 91 is provided with a The funnel-shaped horn antenna 93, and the inside of the waveguide 91 is formed with a cavity in which the column medium 94 is filled. The surface of the cylindrical medium 94 is output from the waveguide 91. To the funnel-shaped horn antenna 93 & is formed with a linear conical medium converter 95 (shown in Figure 16), and the cylindrical medium 94 can be composed of Teflon 2F (pTFE). However, since the antenna structure has a sharp angle of 951 vertices of the linear conical medium conversion, the light-shooting field type of the linear conical medium converter 95 tends to cause the tip field type to affect the antenna light-emission efficiency at the peak end of the main beam; And because the cavity system in the waveguide 91 is filled with the cylindrical medium 94, when the signal is input from the signal input connector 92 to the waveguide 91, the signal will enter the cylindrical medium 94 directly and input by the cylindrical medium 94. To linear cone dielectric launch cones 95, 201232919, however, the impedance of the signal input connector 92 (50 ohms) is typically much smaller than the air dielectric impedance (377 ohms) in the horn antenna 93, with a small impedance directly from the signal input connector 92. It is not easy to convert the large impedance of the air medium into the horn antenna 93 and the impedance is too large to reduce the antenna bandwidth. All of the above are the ideals of the existing technology. It needs to be further reviewed and a feasible solution is sought. SUMMARY OF THE INVENTION Accordingly, it is a primary object of the present invention to provide an integrated horn antenna device that is mainly used to improve a waveguide and a medium emission cone in an antenna, so that the integrated horn antenna device can achieve good impedance conversion. And has better directivity' and thus improve the efficiency of radiation. The main technical means for achieving the foregoing objective is that the integrated horn antenna device includes: a waveguide having an input end and an output end, the air duct is formed with an air resonance cavity, and the air is formed The resonant cavity and the leading end of the waveguide are connected to the output end; the horn antenna has an input end and an output end, and the input end thereof is connected to the output end of the waveguide tube and the inner diameter of the horn antenna From the input end to the output thereof, a dielectric waveguide is disposed at the output end of the waveguide, the ash s has a first end and a second end and the medium guide The outer diameter of the first end of the wave tube corresponds to the inner diameter of the air resonance cavity; a medium emission cone is formed at the second end of the dielectric waveguide; the medium emission cone system is located in the horn antenna And the apex of the medium emission cone is a non-sharp angle; 201232919 a signal input connector is disposed at the input end of the waveguide for feeding the signal and not contacting the dielectric waveguide; Lens, which is located in the horn antenna End. The present invention can achieve the following advantages and effects by the foregoing technical means: Since the apex of the medium transmitting cone is a non-sharp angle, the main beam tip can be prevented from having a prominent field type, so that the radiation field pattern can be effectively improved; And because the signal first passes through the air resonance cavity and then passes through the medium emission cone, the impedance can be relatively easy to maintain the antenna bandwidth through two smaller amplitude conversions; and because the radome lens of the present invention can radiate the plane wave of the cone antenna Focusing, it can effectively improve the directivity, make the half beam width narrower, and increase the anti-interference to the measurement environment. [Embodiment] Hereinafter, the technical means adopted by the present invention for achieving the objective of the invention will be further described in conjunction with the preferred embodiments of the present invention. Referring to FIG. 1, a first preferred embodiment of the present invention includes a waveguide 10, a signal input connector 20, a horn antenna 3A, a dielectric guide 40, a medium emission cone 5, one day. a wire cover lens 6〇; wherein: the guided wave f 10 has an _ input end and an output end, and a waveguide air 扨 is formed with an air resonance cavity H, and the air resonance cavity W and the waveguide tube The input end of the 1G is connected to the output end, and the guided wave f 1() can be configured; the horn antenna 3G has an _ input end and an output end, and an input end thereof is connected to an output end of the side guide wave f 1 ,, and The horn antenna 3 has a tapered cylindrical shape, and its inner diameter gradually increases from its input end to its output end in 201232919. In the preferred embodiment, the horn antenna 30 can be locked by a screw, a flange and a waveguide 1 The dielectric waveguide 40 is disposed at the output end of the waveguide 1 , and the dielectric waveguide 40 has a first end and a second end, and the outer diameter of the first end is resonant with the air. The inner diameter of the cavity 11 corresponds to; as shown in FIG. 1 and FIG. 3, the medium emission cone 50 is formed on the dielectric waveguide 40. The medium emitting cone 5 is located in the horn antenna 30, and the medium emitting cone has a vertex 51 and a peripheral wall 53. The peripheral wall 53 has a top end and a bottom end, and the outer wall of the peripheral wall 53 has a bottom outer diameter. Referring to FIG. 3 to FIG. 5, the shape of the medium emission cone 50 of FIG. 3 is a linear apex 51 purified conical shape, wherein a segment refers to a preferred embodiment of the medium emission cone 50. The medium-emitting cone 50 has a section of peripheral wall 53' linear. The peripheral wall 53 has an outer diameter which decreases linearly from the bottom end to the top end. The vertex 51 is a passivated finger whose vertex is not a sharp corner, which is also called a passivation vertex, which can be a flat angle. The vertices can also be the vertices of the rounded corners; Figure 11 and Figure 12 are the E-plane (E-plane) and the H-plane radiation field of the medium-emitting cone 5〇, where the solid line is co-polarized Field type, the dotted line is the intersection and polarization field type. The medium emission cone 50B of Fig. 4 is a curved apex 51B passivated conical 'a curved apex 51 B. The passivated conical section means that the medium emission cone 50B has a peripheral wall 53B whose outer diameter of the peripheral wall 53B is from the bottom end The apex decrement' and the curve apex 51 B passivate the conical curve means that the wall of the peripheral wall 53B forms a concave curved surface from the top end to the bottom end, and the apex 5 彳 B passivation means that the apex 51 B is a passivation apex. The medium emission cone 50C of FIG. 5 is a two-segment curve apex 51C purification 201232919 conical shape, wherein the two-segment curve apex 51 C passivation conical two-stage means that the medium emission cone 50C has an upper peripheral wall 53C and a lower peripheral wall 54C The upper and lower peripheral walls 53C, 54C respectively have a top end and a bottom end, and the wall surfaces of the 周F peripheral walls 53C, 54C respectively form a concave curved surface from the top end to the bottom end thereof, and the apex 51 C passivation means that the apex 51 C is a passivation apex. Fig. 13 and Fig. 4 are the radiation patterns of the E plane and the Η plane of the medium emission cone 50C, and the solid line in the figure is the same polarization field type 'the dotted line is the cross polarization field type; in other embodiments The medium emission cone can also be formed with three, four or more segments, and the apex can be a sharp apex or a purified apex. The dielectric waveguide 40 and the medium emission cone 50 may be commonly used in high molecular polymers, ceramics or glass, such as ethylene (PVC), gasified polyethylene (CPVC), polyethylene (HDPE), ethylene. Steel (UPE), Teflon 2F (PVDF), Teflon 4F (PTFE), Polyester (PET), Polypropylene (pp), Nylon 6 (N-6), Nylon 66 (N-66), MC nylon (MC), plastic steel (POM), ABS resin (ABS), polystyrene (ps), acrylic (PMMA), polycarbonate (PC), polyetheretherketone (PEEK), bakelite ( Bake丨jte), fiberglass • (FRP)...etc. In other embodiments, please refer to FIG. 2, and the integrated horn antenna device further includes an inner medium emission cone 70' formed on the first end of the dielectric waveguide 4? In the air resonance cavity 11 'and the inner medium emission cone 70 also has a vertex and a peripheral wall 'the peripheral wall has a top end and a bottom end, and the shape of the inner medium emission cone 70 can be emitted with the medium The cone 50 is identical and has its apex away from the first end of the dielectric waveguide 40. Referring back to FIG. 1 , the signal input connector 20 is disposed at the input end of the guide wave 201232919 tube 10 and is not in contact with the dielectric waveguide 40. The signal input connector 20 is used to feed the signal to the waveguide 10 . The inner air cavity 11' and the signal input connector 20 can be an SMA connector; the radome lens 60 is disposed at the output end of the horn antenna 30. The radome lens 60 can be commonly used in high molecular polymers, ceramics or glass. Materials such as ethylene (PVC), gasified polystyrene (CPVC), polyethylene (HDPE), ethylene steel (UPE), Teflon 2F (PVDF), iron fluoride yellow I 4F (PTFE), polyester Glue (PET), polypropylene (PP), nylon 6 (N-6), nylon 66 (N-66), MC nylon (MC), plastic steel (POM), ABS resin (ABS), polystyrene (PS) ), acrylic (PMMA), polycarbonate (PC), polyetheretherketone (PEEK), bakelite (Bake丨ite), glass fiber (FRP), etc.; the radome lens The central axis of 60 may be the same as or different from the central axis of the medium emission cone 5〇; the radome lens 6〇 may be a lenticular lens, a plano-convex lens, a meniscus lens, a convex-concave lens, a flat concave The lenticular lens or the biconcave lens may have a ring-shaped structure in a state in which the central axis of the radome lens 60 is different from the central axis of the horn antenna 3A; please refer to FIG. In a preferred embodiment, the central axis of the radome lens 6 is the same as the central axis of the medium emission cone 5G, and the radome lens 6Q is a convex lens, which may be a lenticular lens, a plano-convex lens, a meniscus lens, no matter what For a convex lens, please refer to Figure 6 ^ m, the thickness of the center of the lens must be greater than the thickness of the two ends of the lens ^ * h3 is a convex lens. Fig. 7 and Fig. 8 are respectively a traveling diagram of a signal when a plano-convex lens is used to pull a kick + a brother/deep concave lens. When the signal is emitted from a medium error fin Γ ,, it is a plane wave, and the signal is transmitted through the radome. No, the plano-convex lens 60 of FIG. 7 and the plano-concave lens 60A of FIG. 8 are all collected by the mirror at a point; please refer to FIG. 9 and FIG. 1 2012201232,129 shown and the central axis of the radome lens 60 is also It may be different from the central axis of the horn antenna 30. That is, the radome lens 60 is eccentric with respect to the central axis of the horn antenna 30. When the signal is emitted from the medium emission cone 50, it is a plane wave, and the signal passes through the eccentric radome. After the lens 60, both the plano-convex lens 60 of FIG. 9 and the plano-concave lens 60A of FIG. 1 will be biased and focused on one point. When the signal is input from the signal input connector 20 (impedance 50 ohms) to the waveguide 1〇 When the signal enters the air resonance cavity 11 (impedance 1〇〇~15〇 ohms), it enters the dielectric waveguide 40 from the air resonance cavity 11 and is transmitted by the dielectric guide 40 to the medium emission cone. Body 50 is emitted to the air medium (resistance 377 ohms), so that the impedance of the signal may be converted by the two smaller amplitude, easier to maintain the antenna bandwidth. Because the apex of the medium emission cone is not a sharp angle, and the protruding end field of the main beam is prevented from being prominent, the radiation pattern can be effectively improved; and since the signal first passes through the air resonance cavity and then passes through the medium emission cone, The impedance can be easily maintained by two smaller amplitude conversions; and because the radome lens of the present invention can focus the plane wave radiated by the cone antenna, the directivity can be improved and the half beam width can be narrowed. Increase the immunity to the measurement environment. And compared with the outer diameter of the peripheral wall from the bottom end to the top of the decreasing amplitude is a linear medium emission cone, the peripheral wall wall surface from the top to the bottom end forming a concave arc surface of the medium emission cone can be 1, the antenna bandwidth The antenna of the linear medium emission cone has a wide bandwidth. 2. The ratio of the radiation field type side lobes of the antenna to the main lobes is increased. Therefore, the side beam can be depressed, so the signal is concentrated in the main beam, which can further improve the directivity. Further improve the efficiency of radiation. The above description is only the preferred embodiment of the present invention, and is not intended to limit the invention. Although the invention has been disclosed in the preferred embodiments, it is not intended to limit the invention. The person _ 2 does not depart from the scope of the technical solution of the present invention, and may use the above-mentioned disclosure::: make a slight change or modify the equivalent implementation technology essence: t: r content of the technical solution of the invention, according to the present Modifications of the invention, any simple modifications, equivalent variations and modifications made by I, are still within the scope of the technical solution of the invention. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a cross-sectional view of the integrated horn antenna device - a preferred embodiment. FIG. 2 is a cross-sectional view of the integrated horn antenna device. Linear Vertex Passivation Conical Media Emission Figure 4 is a schematic view of a cone shape. 'Transition of the Curve Vertex Passive Conical Media Figure 5 is a schematic diagram of the shape of the two-segment curve vertex passivation jg cone. Conical Cone Medium Emission Figure 6 is a schematic representation of the lens ratio. 2 to Figure 1 is a schematic diagram of the travel of the signal through the lens. Figure 14 is a different medium emission cone. Figure 15 is a cross section of the existing antenna structure; (4) field pattern. The 6 series is a schematic diagram of an existing medium emission cone. 201232919 [Description of main components] 10 waveguide 20 signal input connector 30 horn antenna 40 dielectric waveguide 50, 50B, 50C medium emission cone 51, 51 B, 51 C apex 53, 53B peripheral wall • 53C upper peripheral wall 54C Lower wall 60, 60A radome lens 70 medium emission cone 91 waveguide tube 92 signal input connector 93 funnel horn antenna 94 cylindrical medium • 95 linear cone media converter
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