200937093 . 鏡頭移位機構3 制動部（actuating part ) 30 徑向活動體31 斜面32 八、 本案若有化學式時，請揭示最能顯示發明特徵的化 學式：（無） 九、 發明說明： 【發明所屬之技術領域】 ❹ 本發明係有關一種鏡頭移位機構，係應用於一自動對 焦或變焦之鏡頭組，尤指一種在鏡頭套筒之底緣或外緣上 上設置一徑向傾斜之斜面，並使其對應抵接於一對應徑向 活動體之對應斜面上，使徑向活動體因受制動器之制動力 驅動而向内/向外徑向移動時，可藉二相互對應抵接之斜 面之間的推抵作用，相對地使鏡頭在中心軸上產生向前/ 向後之轴向移動者。 【先前技術】 目前使用之數位相機、具拍攝功能的手機、筆記型電 ❹ 腦等手持式電子裝置上，常設有一可自動對焦 (auto-focusing，簡稱AF )或變焦（zooming )之微型鏡 頭模組（compact camera module，簡稱CCM )，而該鏡頭 模組基本上包含：一由上蓋及底蓋所形成的容腔；一鏡頭 由鏡片群（lensgroup)及一鏡頭套筒（iensh〇lder)組成，其 套設在容腔内並可在中心轴方向上前後滑動移位；及一鏡 頭移位機構（lens displacement/driving mechanism )，其主要 目的是利用制動器（actuator )來提供制動力（actuating force )以驅動該鏡頭在容腔内之中心軸上產生軸向移位動 作，藉以達成自動對焦或變焦之功效。 3 200937093 習知鏡頭移位機構所使用的制動器（actuator)包含多 種不同模式，如一種稱為壓電馬達（piezoelectric motor )， 其係利用壓電（piezoelectric )材料形成，如US7,212,358、 US2003/0227560、US2006/0044455A1、JP2006-293083、 JP2006-101611等，利用對壓電馬達施予一電壓以產生制動 力（actuating force );又一種稱為音圈馬達（voice coil motor，簡稱VCM )者，其係利用線圈、磁鐵與彈性件 (如彈簧或彈片）配合形成，如US7,262,927、 US7，196,978、US7,002,879、US6,961，090、US6,687,062、 US20070133110 > JP2005037865 ' JP2005258355 ' ® W02007026830等，該等習知技術大部分係利用線圈與永夂 磁鐵（permanentmagnet)配組使用，如在鏡頭之外圍上固設 一線圈成一同步連動體，再於線圈之外圍環狀排列設置一 個或數個永久磁鐵並係持固定不動，使線圈通電後可在永 久磁鐵所建立之磁場中產生向上或向下之電磁力以驅動鏡 頭移動；再者’有一種是利用形狀記憶合金（shaped memoryalloy ’簡稱SMA)之鏡頭移位機構，其係利用SMA 之熱縮冷涨之特性以作為制動器（actuator )之驅動力源， WUS6,307,678B2、US6,449,434B1、US2007058070、 ❹ US2007047938、JP2005275270、JP2005195998 等，然而， SMA熱縮冷漲的動作較慢，而且再經制動器（actuat〇r)與 鏡頭之間的連動結構傳動，無法簡易達成即時自動對焦或 變焦之功效。 然，習知鏡頭移位機構中，其使用的制動器雖包含多 種不同模式可供選擇’但該制動器（aetuat〇r) 一般係與鏡 頭模組的其他構件如其中最主要的鏡頭成一體式配合設 計’也就是當決定所使用制動器之模式時，該制動器與鏡 頭（包含鏡片群及一鏡頭套筒）之間的連動結構也是同時 設定完成如US2006/0044455A1所揭示者，藉以使制動器所 4 200937093 ❹ Ο 產生之制動力（actuatingforce )可直接藉該連動結構以驅 動鏡頭在容腔内之中心轴上產生軸向移位動作，故不同模 式之制動器無法藉相同之連動結構來傳達制動力，致無法 更換使用；尤其，習知鏡頭移位機構之制動器，其制動力 之作用方向大部分係與光轴（即鏡頭中心軸）同方向，致 其移動量為1:1 ’較耗費制動力，若要增加鏡頭之相對 移動量，則須增加其他連動結構，致使整體結構複雜化而 不利於量產化反降低成本；另，先前技術中雖有利用斜面 作用以驅動鏡頭移位之驅動方式如US5,930,544，其係藉一 第一活動件（firstmovementmember )以驅動鏡頭左、右向 移位’且同時再藉一第二活動件（second movement member)及一槓桿支軸以驅動鏡頭上、下向移位，而使鏡 頭之中心軸呈現一橢圓形軌跡之移位效果，致其結構較複 雜，且其引用之斜面作用並非用來驅動鏡頭作軸向運動， 也就是其並非是利用一制動器之徑向運動而經由斜面作用 而轉換鏡頭之軸向運動；因此發展有放高倍解析度且增加 鏡頭相對移動量之新技術以解決鏡頭移位機構中移動量為 1·1及制動器與鏡頭之間的連動結構須同時設定的問 題’將有迫切需要。 【發明内容】 明主要目的在於提供一種鏡頭移位機構，供應用 或變焦之鏡頭模組，其主要包含：在鏡頭套 徑向傾以::軸f稱之位置處設置至少-個 底緣或外緣：外：：夂ίί—個徑向活動體設於鏡頭套筒 對應抵接外？各'又有，徑向傾斜之第二斜面以分別 少-制叙j頭套筒之底緣或外緣上之第—斜面上；及至 精制動器產生制動力以驅動各徑向活動體同步向 5 200937093 内/向外徑向移動時，藉二相互對應抵接之第一、二斜面 之間的推抵作用，可驅使鏡頭套筒底緣或外緣上之第一斜 面由徑向活動體之第二斜面之一低點/高點位置移位至一 高點/低點位置，相對地使鏡頭在中心軸（光軸）上產生 向前/向後之軸向移動，達成自動對焦或變焦之功能。 本發明再一目的在於提供一種鏡頭移位機構，其中該 制動部所使用之制動器進一步可隨鏡頭模組之設計需要而 選擇音圈馬達（VCM)、壓電馬達（piezoelectric motor )、利 用形狀記憶合金（SMA)形成之制動器、或利用線圈與電磁 鐵（electromagnet)形成之制動器之組群（获0叩）中一種制 動器’藉由控制以產生制動力（actuating force )以驅動鏡 頭在鏡頭模組之容腔内之中心軸（光轴）上產生軸向移位 動作。 本發明另一目的在於提供一種鏡頭移位機構，其進一 步可在鏡頭（或鏡頭套筒）上配置一彈簧，當制動器之制 動力（actuatingforce )或徑向活動體的驅動力消失或不產 生作用時，該彈簧可對鏡頭提供一相對之回復力，以使鏡 頭達到動態平衡或回復原位，而達成自動對焦或變焦效 果。 G 本發明之鏡頭移位機構主要係利用一可徑向移動之第 二斜面及一可軸向移動之第一斜面相互對應抵接構成，其 中可軸向移動之第一斜面係設於鏡頭套筒之底緣或外緣上 上，而可徑向移動之第二斜面係設於一可徑向移動之徑向 活動體上，並使鏡頭套筒底緣或外緣上之第一斜面對應抵 接在徑向活動體之第二斜面上；其中，當徑向活動體被驅 動進行向内或向外之徑向移動時，藉二相互對應抵接之第 一、二斜面之間的推抵作用，可驅使鏡頭在中心軸上產生 相對之向前或向後之軸向移動，如徑向活動體向中心轴靠 近移動（即向内移動）時，其斜面即可迫使鏡頭套筒之底 6 200937093 緣或外緣上第一斜面向上爬升移位，. 上向前移位；而如經向活動體齙pq +在中〜 動）時，其第二斜面由移動（即向外移 移動，使鏡頭相對在中心第=向下滑降 目的。再者，本發明之鏡頭移位棬 達成鏡頭移位之 二斜面及可軸向移動之第—斜面 ^藉由徑向移動之第 的選擇設計，以提供鏡頭在容腔内^互=之不同角度 生轴向快速移位動作或精密移位動作。#(光軸）上產 【實施方式】 Ο 下列ί使本明確詳實’兹列舉較佳實施例並配合 下列圖不，將本發明之結構及其技術特徵詳述如後： 本發明以下所揭示之實施例，主 構:ϊΐ:明’並不用來限制鏡頭模組之其他： 變的;Hi其:構改 d 片群及—鏡頭套筒）的形狀或結構不 ，如鏡片群了包含單—鏡片或數個鏡片，且鏡片群可 Ο ，各設在-固定件内而再與鏡頭套筒結合形成一鏡頭 t般熟悉此項技藝之人士瞭解，本發明所揭示自動對： :變焦鏡頭模組之構件並不限制於以下所揭示之實施例钟 才冓0 ' ° 參考圖1、2、3所示’其分別係本發明鏡頭移 冓一實施例之上視、剖視及局部立體之示意圖。本發明 頭移位機構3係供應用於一自動對焦或變焦之鏡頭模組 1 ，本實施例之鏡頭模組1為一方形鏡頭模組，至少包 3 · —谷腔10，一鏡頭組20由鏡片群（iens识〇叩)21及一鏡 碩套筒22組成；及鏡頭移位機構3用以驅動鏡頭組2〇在鏡 頭模組1之容腔10内的中心軸（光轴）z上滑動移位；本 7 200937093 實施例設具兩個鏡頭移位機構3，其係分別設於方形鏡頭 模組1内部之中心軸對稱之角端位置處，即對角位置處。 本發明鏡頭移位機構3主要包含：鏡頭套筒22之底緣 上（如圖1-7所示）或外緣上（如圖8-10所示）之第一斜 面23、徑向活動體31及制動部（actuating part) 30 ;其中該 第一斜面23為一徑向傾斜之斜面，圖1、7、8分別所示 實施例1、2、4，其第一斜面23為兩個相同斜度之斜 面，分別設在鏡頭套筒22之底緣上（如圖1-7所示）或外 緣上（如圖8-10所示）以中心轴Z對稱之二對稱位置處； 其中圖8-10所示之實施例4，其第一斜面23係設在鏡頭套 0 筒22之外緣上兩個相同凸緣體24之底面上。 該徑向活動體31係對應鏡頭套筒22底緣或外緣上之第 一斜面23而設置於鏡頭套筒22之底緣或外緣的外圍，上述 各實施例係設有兩個徑向活動體31且分別對應鏡頭套筒22 之底緣或外緣上兩個第一斜面23 ;又各徑向活動體31上設 有一徑向傾斜且斜度與第一斜面23相同之第二斜面32，以 分別對應抵接於鏡頭套筒22之底緣或外緣之第一斜面23 亡，其中該徑向活動體31之第二斜面32的長度大於鏡頭套 筒22之底緣上第一斜面23的長度，使的長度斜面23可在第 ❹ 二斜面32的長度範圍中滑動移位》 該制動部（actuatingpart) 30包含一制動器，供可藉由 相機控制器（圖未示）以控制制動部3〇中之制動器以產生 制動力，用以驅動徑向活動體31同步向内或向外徑向移 動。 藉上述結構’當制動部30利用其制動器而產生一向内 (向中心軸Z)之徑向制動力（如圖4之箭頭A所示）以 驅動各徑向活動體31同步向内徑向移動時，此時藉由二相 互對應抵接之第一、二斜面23、32之間的推抵作用，可驅 使鏡頭套筒22之第一斜面23由徑向活動體31之第二斜面32 8 200937093 上-低點位：上爬升而移位至第 二斜面32 上一高點位襄H =上套筒22 (即鏡頭20)相 對地在令心(无㈤上向_向移動（如圖4之箭頭 B1i制動部=制”不作用或所產生之徑向制動力 (如圖4之箭病念：不^肖失時或產生反向（向外）之徑 向制;力，此: = 2接之第-、二斜㈣ 32之間的推柢作ά Λ7< —= 涛22之第一斜面23失去向 前之支撐力’而1)仫二‘芨=31之苐二斜面32上-高點 位置（如圖5所不)一、向下落降移位至第二斜面32上-低 ❹‘點位置（如C 鏡頭套筒。（即鏡頭20)相對 地在中心軸Ζ (光？）士向後軸向移動而回復至原位。 再參考圖6所其係本發明鏡頭20之軸向移位量 (h )與據向Ϊ二移位量（d )的相對關係說 明圖。當二相矣對應抵f之第一、二斜面23、32之斜面斜 度為Θ。時，則匕二，恤θ ’其中”為抽向移動效 率，U 1，77可依據第一、二斜面23、32之摩擦力不 同，對於不同财質或，面今小、方式，可由實際實驗可 得。假設當f1 ’ =45。時，tan Θ=1 ’因此h 〇 =d;而當Θ ^ 時，則h^d，如㊀ 。=53。時 Ρ 1,33(1，如㊀=63.43。時 h=2d，故只要 將使二相互對爲柢接之第一、一斜面U、32之斜面斜度㊀ 設計為^45 15，即可^加鏡頭相對移動量，藉以解決習知 鏡頭移^機構之制動器的制動力之作用方向大部分與光轴 = i且其移動量為1 : 1而較耗費制 沿釉向快迷移勒问的鏡碩20設計，在希望使鏡頭2〇能 Θ。245。，例如，可將第一、二斜面23、32之斜面斜度 活動體31之褪向，㊀。=60。，h=1.73d，此時，徑向 仅量（d )僅移動imm時時，軸向移位 9 200937093 量（h )則移動1.73mm，同樣，對於不同的鏡頭2q設計， 在希望使鏡頭20沿軸向較為精密移動時，可將第一、二斜 面23、32之斜面斜度㊀。$45。，例如，㊀。=30。， h=0.577d，此時，徑向活動體31之徑向移位量（d )移動 1mm時，軸向移位量（h )則移動〇577mm。惟，為能使 鏡頭20移動穩定順暢，在施以適當潤滑且無外加其他機 情形下，斜面斜度Θ不應小於22.3。、不應大於71 5。。 再參考圖1、7、8所示，本發明之鏡頭移機 的設置數目及位置並不限制，以兩個或以上 四個等，惟須考慮鏡頭移位機構3之成本及組裝作;之方 機構3以等‘角度環 ff 底緣（如圖1-7所示）或外緣（如圖8-10所 =沉外圍為佳，以圖1所示實施例方形鏡頭模組J而 二Iff兩個鏡頭移位機構3在鏡頭模組1内部之中心 播構3 位置處即對角位置處，或設置四個鏡頭移位 ? 内部之四個角端位置處；而以圖7所 ^構組2而言’可設置兩個鏡頭移位 處；以圖部之中心軸對稱之短邊内端位置 ❹ 短邊内端位晉虚機構3在鏡頭模組1内部以中心軸對稱之 =:¾筒位機構3以等間隔角度環 生制動力均勾施作動動部3〇之制動器所產 提供均勻之軸向體31上’進而對鏡頭套筒22 上穩定地軸向移動。，有利於鏡碩20在中心軸Ζ (光轴） 制，=使用制動 器的制動模式並不限 移動即可，且不活動體31同步向内或向外徑向 -斜面23 致影響二相互對應抵接之 200937093 32之間的推抵作用；因此製作時，可隨鏡頭模組之設計需 要而選擇音圈馬達（VCM)、壓電馬達（piezoelectric motor )、利用形狀記憶合金（SMA)形成之制動器、或利 用線圈與電磁鐵（electromagnet)形成之制動器之組群 (group )中一種制動器，相對增加制動部30所使用制動 器之選擇性。 參考圖1、7所示，制動部30上進一步可包含一導執 裝置33，如圖1所示，使徑向活動體31可藉該導轨裝置33 而穩定地徑向滑動。 本發明之鏡頭移位機構3進一步可在鏡頭20或其鏡頭 ❹ 套筒22上配置一彈簧40，當制動部30之制動器的制動力 (actuatingforce )或徑向活動體31的驅動力消失或不產生 作用時’該彈簧40可對鏡頭20提供一相對之回復力，以使 鏡頭20達到動態平衡或回復原位，而達成自動對焦或變焦 效果。至於該彈簧40之彈性型態如壓縮式 (compression ) 彈簧或伸張式（extension )彈簧、結構型態如線圈彈簧或 非線圈彈簧、數目或設立位置等並不限制，可隨鏡頭模組 之設計需要或鏡頭的運動方向而改變。 以上所述僅為本發明的較佳實施例，對本發明而言僅 © 是說明性的，而非限制性的；本專業技術人員理解，在本 發明權利要求所限定的精神和範圍内可對其進行許多改 變，修改，甚至等效變更，但都將落入本發明的係護範圍 内。 【圖式簡單說明】 圖1係本發明鏡頭移位機構一實施例之上視示意圖。 圖2係圖1中剖面線2-2之剖視示意圖。 圖3係本發明鏡頭移位機構之局部立體示意圖。 圖4係圖2中鏡頭套筒之底緣斜面對應抵接於徑向活動體 200937093 之對應斜面上低點位置之局部放大示意圖。 圖5係圖4中鏡頭套筒之底緣斜面移位至徑向活動體之對 應斜面上高點位置之局部放大示意圖。 圖6係本發明鏡頭之軸向移位量與徑向活動體之徑向移位 量的相對關係說明圖。 圖7係本發明鏡頭移位機構另一實施例之上視示意圖。 圖8係本創作鏡頭移位機構又另一實施例之上視示意圖。 圖9係圖8之一側面剖視示意圖。 圖10係圖8鏡頭移位機構之局部立體示意圖。 ❹ 【主要元件符號說明】 鏡頭模組1、2、4 容腔10 鏡頭組20 鏡片群（lensgroup)21 鏡頭套筒22 斜面23 凸緣體24 鏡頭移位機構3 ◎ 制動部（actuating part ) 30 徑向活動體31 斜面32 導軌裝置33 彈簧40 12200937093 . Lens shifting mechanism 3 Actuating part 30 Radial moving body 31 Inclined surface 32 8. If there is a chemical formula in this case, please disclose the chemical formula that best shows the characteristics of the invention: (none) IX. Description of invention: TECHNICAL FIELD The present invention relates to a lens shifting mechanism, which is applied to an autofocus or zoom lens group, and more particularly to a radial inclined bevel on a bottom edge or an outer edge of a lens sleeve. And correspondingly abutting on a corresponding inclined surface of a corresponding radial movable body, so that when the radial movable body is driven to move radially inward/outward due to the braking force of the brake, the inclined surface corresponding to each other can be used The push between them relatively causes the lens to produce a forward/backward axial movement on the central axis. [Prior Art] On the handheld electronic devices currently used, such as digital cameras, mobile phones with shooting functions, and notebook-type electronic devices, there is a miniature lens module with auto-focusing (AF) or zooming. A compact camera module (CCM), the lens module basically comprises: a cavity formed by the upper cover and the bottom cover; a lens consisting of a lens group and a lens sleeve (iensh〇lder) The sleeve is disposed in the cavity and can be slidably displaced back and forth in the direction of the central axis; and a lens displacement/driving mechanism whose main purpose is to provide an braking force by using an actuator (actuating force) ) to drive the lens to produce an axial shifting action on the central axis in the cavity to achieve autofocus or zoom. 3 200937093 The actuator used in conventional lens shifting mechanisms contains a number of different modes, such as a piezoelectric motor, which is formed using piezoelectric materials such as US 7,212,358, US 2003/ 0227560, US2006/0044455A1, JP2006-293083, JP2006-101611, etc., using a voltage applied to a piezoelectric motor to generate an actuating force; another type called a voice coil motor (VCM), It is formed by a coil, a magnet and an elastic member such as a spring or a spring. For example, US 7,262,927, US 7,196,978, US 7,002,879, US 6,961,090, US 6,687,062, US20070133110 > JP2005037865 ' JP2005258355 ' ® W02007026830 Etc., most of these conventional techniques use a coil and a permanent magnet to be used in combination, such as fixing a coil on the periphery of the lens to form a synchronous linkage, and then arranging one or several rings in the outer circumference of the coil. A permanent magnet is held stationary, so that when the coil is energized, it can generate upward or downward electromagnetic force in the magnetic field established by the permanent magnet. The lens is driven to move; in addition, there is a lens shifting mechanism using a shape memory alloy (SMA), which utilizes the heat-shrinking property of the SMA to serve as a driving force source for the actuator, WUS6. , 307, 678B2, US6, 449, 434B1, US2007058070, ❹ US2007047938, JP2005275270, JP2005195998, etc. However, the SMA heat shrinking cold movement is slower, and it can not be driven by the interlocking structure between the brake (actuat〇r) and the lens. Easy to achieve instant autofocus or zoom. However, in the conventional lens shifting mechanism, the brake used includes a plurality of different modes to choose from, but the brake is generally integrated with other components of the lens module such as the most important lens. The design 'that is, when determining the mode of the brake used, the interlocking structure between the brake and the lens (including the lens group and a lens sleeve) is also set at the same time as disclosed in US 2006/0044455 A1, whereby the brake device 4 200937093 ❹ Ο The generated braking force (actuatingforce) can directly drive the lens to generate an axial displacement action on the central axis of the cavity. Therefore, the brakes of different modes cannot communicate the braking force by the same linkage structure. Can not be replaced; in particular, the brake of the conventional lens shifting mechanism, the direction of the braking force is mostly in the same direction as the optical axis (ie, the central axis of the lens), so that the amount of movement is 1:1 'more braking power, In order to increase the relative movement of the lens, other interlocking structures must be added, which complicates the overall structure and is not conducive to mass production. Reducing the cost; in addition, in the prior art, there is a driving method that uses a bevel to drive the lens shift, such as US 5,930,544, which uses a first movable member (firstmovement member to drive the lens to the left and right shifts) and at the same time By using a second movement member and a lever fulcrum to drive the upper and lower displacement of the lens, the central axis of the lens exhibits an elliptical trajectory displacement effect, resulting in a complicated structure, and The referenced beveling effect is not used to drive the lens for axial movement, that is, it does not use the radial motion of a brake to convert the axial movement of the lens via the bevel action; therefore, the development has a high resolution and increases the relative movement of the lens. The new technology to solve the problem that the amount of movement in the lens shifting mechanism is 1.1 and the interlocking structure between the brake and the lens must be set at the same time will be urgently needed. SUMMARY OF THE INVENTION The main objective of the present invention is to provide a lens shifting mechanism, a lens module for supplying or zooming, which mainly comprises: at least a bottom edge or at a position where the lens sleeve is radially inclined to: the axis f Outer edge: Outer::夂ίί—A radial moving body is placed on the lens sleeve corresponding to the outside? Each of the 'reversely inclined second inclined faces to respectively reduce the bottom edge of the j-head sleeve or the first inclined surface on the outer edge; and the fine brake generates a braking force to drive the radial moving bodies to synchronize 5 200937093 When the inner/outward radial movement, the first inclined surface on the bottom edge or the outer edge of the lens sleeve can be driven by the radial movable body by the pushing action between the first and second inclined surfaces corresponding to each other. The low/high position of one of the second slopes is shifted to a high/low position, and the lens is relatively moved forward/backward on the central axis (optical axis) to achieve autofocus or zoom The function. Another object of the present invention is to provide a lens shifting mechanism, wherein the brake used in the braking portion can further select a voice coil motor (VCM), a piezoelectric motor (piezoelectric motor), and shape memory according to the design requirements of the lens module. A brake formed by an alloy (SMA) or a group of brakes formed by a coil and an electromagnet (a 0) is controlled by an actuating force to drive a lens in a lens module. An axial displacement action is generated on the central axis (optical axis) in the cavity. Another object of the present invention is to provide a lens shifting mechanism, which can further configure a spring on the lens (or the lens sleeve), when the brake force (actuating force) or the driving force of the radial movable body disappears or does not function. The spring provides a relative restoring force to the lens to achieve dynamic balance or return to the original position for autofocus or zoom. The lens shifting mechanism of the present invention is mainly configured by a second inclined surface that can be moved radially and an axially movable first inclined surface, wherein the first inclined surface that is axially movable is attached to the lens cover. The bottom edge or the outer edge of the cylinder is upper, and the radially movable second slope is disposed on a radially movable radial movable body, and corresponds to the first slope on the bottom edge or the outer edge of the lens sleeve Abutting on a second inclined surface of the radially movable body; wherein, when the radially movable body is driven to move radially inward or outward, the push between the first and second inclined surfaces corresponding to each other is abutted The abutting action can drive the lens to move axially forward or backward relative to the central axis. For example, when the radial moving body moves toward the central axis (ie, moves inward), the inclined surface can force the bottom of the lens sleeve. 6 200937093 The first slope on the edge or the outer edge is up and down, and the upper slope is shifted forward; and if the moving body is pq + in the middle, the second slope is moved (ie, moved outward) , so that the lens is relatively down in the center = down direction. Again, this hair The shifting lens of the lens achieves the two bevels of the lens shift and the elliptical surface that can be moved axially. The first choice of the radial movement is to provide the lens with a different axial angle in the cavity. Shift action or precision shift action. #(光轴)上出 [Embodiment] 下列 The following is a clear and detailed description. The preferred embodiment is illustrated and the following figures are omitted. The structure and technical features of the present invention are detailed. As described in the following: The embodiments disclosed in the following description of the present invention, the main structure: ϊΐ: 明' is not used to limit the other of the lens module: variable; Hi: the shape or structure of the d-group and the lens sleeve No, if the lens group includes a single lens or a plurality of lenses, and the lens group is sturdy, each is disposed in the fixing member and then combined with the lens sleeve to form a lens. The person familiar with the art understands that the present invention The disclosed automatic pair: The components of the zoom lens module are not limited to the embodiment disclosed below. The clock is shown in FIGS. 1, 2, and 3, which are respectively the lens of the present invention. Schematic diagram of top view, cross-section and partial solid. The lens shifting mechanism 3 of the present invention is provided with a lens module 1 for autofocusing or zooming. The lens module 1 of the present embodiment is a square lens module, which includes at least 3, a valley chamber 10, and a lens group 20. It is composed of a lens group 21 and a mirror sleeve 22; and the lens shifting mechanism 3 is used to drive the central axis (optical axis) of the lens group 2 in the cavity 10 of the lens module 1 The upper slide shifting; the present embodiment is provided with two lens shifting mechanisms 3, which are respectively disposed at the angular end positions of the central axis symmetry inside the square lens module 1, that is, at diagonal positions. The lens shifting mechanism 3 of the present invention mainly comprises: a first inclined surface 23 on the bottom edge of the lens sleeve 22 (as shown in FIG. 1-7) or an outer edge (as shown in FIG. 8-10), and a radial movable body. 31 and an actuating part 30; wherein the first inclined surface 23 is a radially inclined inclined surface, and the first, second, and fourth embodiments shown in Figs. 1, 7, and 8, respectively, the first inclined surface 23 is the same The inclined slopes are respectively disposed on the bottom edge of the lens sleeve 22 (as shown in FIG. 1-7) or on the outer edge (as shown in FIG. 8-10) at the symmetrical position of the central axis Z; In the embodiment 4 shown in Figs. 8-10, the first inclined surface 23 is provided on the bottom surface of the two identical flange bodies 24 on the outer edge of the lens sleeve 0 barrel 22. The radial movable body 31 is disposed on the outer edge of the bottom edge or the outer edge of the lens sleeve 22 corresponding to the first inclined surface 23 on the bottom edge or the outer edge of the lens sleeve 22. The above embodiments are provided with two radial directions. The movable body 31 respectively corresponds to two first inclined surfaces 23 on the bottom edge or the outer edge of the lens sleeve 22; and each of the radial movable bodies 31 is provided with a second inclined surface which is inclined obliquely and has the same inclination as the first inclined surface 23. 32, the first inclined surface 23 corresponding to the bottom edge or the outer edge of the lens sleeve 22 respectively is dead, wherein the length of the second inclined surface 32 of the radial movable body 31 is greater than the first edge of the lens sleeve 22 The length of the ramp 23 is such that the length ramp 23 is slidably displaceable over the length of the second ramp 32. The braking portion 30 includes a brake for control by a camera controller (not shown) The brake in the brake portion 3 is configured to generate a braking force for driving the radially movable body 31 to move radially inward or outward. By the above structure 'When the braking portion 30 utilizes its brake, a radial braking force (shown by an arrow A in FIG. 4) is generated inward (toward the central axis Z) to drive the radially inwardly moving bodies 31 to move radially inwardly. At this time, the first inclined surface 23 of the lens sleeve 22 can be driven by the second inclined surface 32 of the radial movable body 31 by the pushing action between the first and second inclined surfaces 23 and 32 which are mutually abutted. 200937093 Upper-lower position: Upper climb and shift to second slope 32 Upper high position 襄H = Upper sleeve 22 (ie lens 20) is relatively moving in the center of the heart (none (five)) 4 arrow B1i braking part = system "no effect or generated radial braking force (as shown in Figure 4 arrow disease: not ^ Xiao lost or reversed (outward) radial system; force, this: = 2 followed by the first - and second oblique (four) 32 between the push 柢 Λ 7 < — = the first slope 23 of the Tao 22 lost the forward support force 'and 1) 仫 two '芨 = 31 苐 two slopes 32 The upper-high position (as shown in Fig. 5) is shifted downward to the second slope 32-lower than the 'point position (such as the C lens sleeve. (ie, the lens 20) is relatively at the central axis ( Light?) The rear axial movement returns to the original position. Referring again to Fig. 6, the relative displacement relationship between the axial displacement amount (h) and the second displacement amount (d) of the lens 20 of the present invention is illustrated.矣 Corresponding to the slope of the first and second slopes 23, 32 corresponding to f is Θ. When the second, the shirt θ 'where" is the pumping movement efficiency, U 1,77 can be based on the first and second slopes 23, The frictional force of 32 is different. For different financial qualities, the face is small and the mode can be obtained by actual experiments. Assume that when f1 '=45, tan Θ=1 'so h 〇=d; and when Θ ^, Then h^d, such as a ==53. When Ρ 1,33 (1, such as a = 63.43. When h = 2d, so as long as the two pairs of the first pair, the slope of the first slope, U, 32 The slope 1 is designed as ^45 15, which can be used to increase the relative movement of the lens, so as to solve the problem that the braking force of the brake of the conventional lens shifting mechanism is mostly with the optical axis = i and the movement amount is 1:1. It is more expensive to use the Mirror 20 design that moves along the glaze to the fascinating fascination. It is hoped that the lens can be smashed. 245. For example, the slanting movable body 31 of the first and second slanting faces 23 and 32 can be faded. to One.=60., h=1.73d. At this time, the radial amount only (d) only moves the imm, the axial shift 9 200937093, the quantity (h) moves 1.73mm, and the same, for different lens 2q design When it is desired to relatively precisely move the lens 20 in the axial direction, the slopes of the first and second slopes 23, 32 can be inclined by one. $45. For example, one = 30., h = 0.577d, at this time, the diameter When the radial displacement amount (d) of the movable body 31 is moved by 1 mm, the axial displacement amount (h) is shifted by 577 mm. However, in order to make the lens 20 move smoothly and smoothly, the inclined slope Θ should not be less than 22.3 when proper lubrication is applied and no other machine is applied. Should not be greater than 71 5 . . Referring again to FIGS. 1, 7, and 8, the number and position of the lens shifting machine of the present invention are not limited to two or more, etc., but the cost and assembly of the lens shifting mechanism 3 must be considered; The square mechanism 3 is equal to the 'angle ring ff bottom edge (as shown in Figure 1-7) or the outer edge (as shown in Figure 8-10 = sinking peripheral, preferably the square lens module J shown in Figure 1 and two Iff two lens shifting mechanisms 3 are located at the center of the lens module 1 at the position of the diagonal position 3, that is, at the diagonal position, or four lens shifts are provided at the four corner positions of the interior; In the case of the framing 2, two lens shifting positions can be set; the short-side inner end position symmetrical with the central axis of the figure ❹ the short-side inner end position imaginary mechanism 3 is symmetric with the central axis inside the lens module 1 = : 3⁄4 the cylinder mechanism 3 is equally angularly generated, and the braking force is applied to the axial body 31 provided by the brake of the moving portion 3', thereby stably moving axially on the lens sleeve 22. Mirror 20 is made in the center axis 光 (optical axis), = the brake mode of the brake is used, and it is not allowed to move, and the inactive body 31 is synchronized. Or the outward radial-bevel 23 affects the pushing between the two mutually corresponding abutting 200937093 32; therefore, the voice coil motor (VCM) and the piezoelectric motor can be selected according to the design requirements of the lens module. A piezoelectric motor, a brake formed using a shape memory alloy (SMA), or a brake in a group of brakes formed by a coil and an electromagnet, relatively increases the selectivity of the brake used in the braking portion 30. As shown in FIG. 1 and 7, the braking portion 30 further includes a guiding device 33. As shown in FIG. 1, the radial movable body 31 can be stably slid radially by the rail device 33. The lens of the present invention The shifting mechanism 3 can further be provided with a spring 40 on the lens 20 or its lens cymbal sleeve 22, when the braking force of the brake of the braking portion 30 or the driving force of the radial movable body 31 disappears or does not act. The spring 40 can provide a relative restoring force to the lens 20 to achieve dynamic balance or return to the original position of the lens 20 to achieve an autofocus or zoom effect. As for the elastic type of the spring 40, such as pressure Compression Springs or extension springs, structural types such as coil springs or non-coil springs, number or set position are not limited and may vary depending on the design of the lens module or the direction of motion of the lens. The above description is only the preferred embodiment of the present invention, and the present invention is only for the purpose of illustration and not limitation; those skilled in the art understand that the scope of the invention Many changes, modifications, and even equivalents are made, but all fall within the scope of the present invention. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a top plan view of an embodiment of a lens shifting mechanism of the present invention. Figure 2 is a cross-sectional view of the section line 2-2 of Figure 1. 3 is a partial perspective view of the lens shifting mechanism of the present invention. 4 is a partially enlarged schematic view showing the bottom edge of the lens sleeve of FIG. 2 corresponding to the low point of the corresponding inclined surface of the radial movable body 200937093. Fig. 5 is a partially enlarged schematic view showing the shifting of the bottom edge of the lens sleeve of Fig. 4 to the position of the high point on the corresponding inclined surface of the radially movable body. Fig. 6 is an explanatory view showing the relative relationship between the axial displacement amount of the lens of the present invention and the radial displacement amount of the radially movable body. Figure 7 is a top plan view of another embodiment of the lens shifting mechanism of the present invention. Fig. 8 is a top plan view showing still another embodiment of the present lens shifting mechanism. Figure 9 is a side cross-sectional view of Figure 8. Figure 10 is a partial perspective view of the lens shifting mechanism of Figure 8. ❹ [Main component symbol description] Lens module 1, 2, 4 cavity 10 Lens group 20 Lens group 21 Lens sleeve 22 Bevel 23 Flange body 24 Lens shift mechanism 3 ◎ Brake (actuating part) 30 Radial movable body 31 inclined surface 32 rail device 33 spring 40 12