TW200841010A - Multi-wavelength fluorescence detecting method of a microchip system - Google Patents

Multi-wavelength fluorescence detecting method of a microchip system Download PDF

Info

Publication number
TW200841010A
TW200841010A TW96111791A TW96111791A TW200841010A TW 200841010 A TW200841010 A TW 200841010A TW 96111791 A TW96111791 A TW 96111791A TW 96111791 A TW96111791 A TW 96111791A TW 200841010 A TW200841010 A TW 200841010A
Authority
TW
Taiwan
Prior art keywords
sample
wavelength
channel
microfluidic wafer
receiving unit
Prior art date
Application number
TW96111791A
Other languages
Chinese (zh)
Other versions
TWI336399B (en
Inventor
Che-Hsin Lin
Shih-Wey Lin
Guan-Liang Chang
Original Assignee
Univ Nat Sun Yat Sen
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Univ Nat Sun Yat Sen filed Critical Univ Nat Sun Yat Sen
Priority to TW96111791A priority Critical patent/TWI336399B/en
Publication of TW200841010A publication Critical patent/TW200841010A/en
Application granted granted Critical
Publication of TWI336399B publication Critical patent/TWI336399B/en

Links

Abstract

A multi-wavelength fluorescence detecting method of a microchip system comprising following steps: providing a microchip comprising a board, an injection channel, a separation channel and a reference channel, and injecting a sample into the injection channel connecting with the separation channel; providing a potential in the microchip to drive the sample to move to a detecting position on the separation channel; providing an optical apparatus with a continuous light source and a receiving unit to excite the sample to emit a fluorescence via an exciting light emitted by the continuous light source and receiving the fluorescence by the receiving unit, wherein the exciting light doesn't beam the receiving unit; and transmitting the fluorescent signal received by the receiving unit to an optical analyzing unit to analyze; wherein the reference channel is provided to measure the data of the background to correct the data of the sample.

Description

200841010 九、發明說明: 【發明所屬之技術領威】 本發明係關於/種微流體晶片系統之多波長螢光偵 測方法,特別是關於利用一光學儀器之一連續光源激發一 微流體晶片系統發出螢光,並對該螢光進行偵測,以提升 偵測效率、準確度、簡化設備及降低成本之微流體晶片系 統之多波長螢光偵测方法。 【先前技術】 習用微流體晶片系統之螢光偵測方法,如中華民國公 告第490558號「具有晶片式電泳裝置之樣品分析系統」^200841010 IX. INSTRUCTIONS: [Technical Leadership of the Invention] The present invention relates to a multi-wavelength fluorescence detection method for a microfluidic wafer system, and more particularly to exciting a microfluidic wafer system using a continuous light source of an optical instrument. Fluorescent detection and detection of the fluorescence to improve detection efficiency, accuracy, simplification of equipment and cost reduction of multi-wavelength fluorescence detection methods for microfluidic wafer systems. [Prior Art] A fluorescent detection method for a conventional microfluidic wafer system, such as the Republic of China Bulletin No. 490558 "Sample analysis system with a wafer type electrophoresis device" ^

明專利,其包含一自動進樣裝置、一晶片、一雷、、盾你;! X 曰曰々 包源供應器 、一偵測單元、一訊號擷取單元及一訊號處理單元。該自 動進樣裝置係用以將一樣品填充或導入該晶月中。曰 s 1 綠曰曰月 係設置有數個槽道,且其係供該自動進樣裝置將樣品進樣 並對該樣品進行分離。該電源供應器係用以提供一電壓於 該晶片中,進而利用該電壓使該樣品於該晶片中進行分離 u測單元係選擇t螢光偵測單元,其係用以债測該 木Xtm所產生之汛號。該訊號操取單元係用以擷取該彳貞測單 元所測得之樣品的訊號。該訊號處理單元係將訊號輪出。 其中,該榮光偵測單元係包含一光源、—透鏡、一激發渡 片、一分光鏡、一放射濾片、一針孔及—光電倍增管。 當利用該習用微流體晶片系統之榮光偵;;亀 樣品進行侧時,首先,經由該自動進樣裝置將該樣品導 入該晶片中°接著,顧該電源供絲施加—電壓於該晶The patent includes an automatic sample introduction device, a wafer, a mine, a shield, a X 曰曰々 package source supply, a detection unit, a signal acquisition unit and a signal processing unit. The autosampler is used to fill or introduce a sample into the crystal.曰 s 1 Green Moon is equipped with several channels, which are used by the autosampler to sample and separate the sample. The power supply is configured to provide a voltage in the wafer, and the voltage is used to separate the sample in the wafer. The unit is configured to select a fluorescent detection unit, which is used to measure the wood Xtm. The nickname produced. The signal operation unit is configured to capture the signal of the sample measured by the test unit. The signal processing unit rotates the signal. The glory detecting unit comprises a light source, a lens, an excitation ferrite, a beam splitter, a radiation filter, a pinhole and a photomultiplier tube. When utilizing the conventional microfluidic wafer system, the sample is introduced into the wafer via the autosampler, and then the voltage is applied to the crystal.

Linda\PKHat\PU03ll.doc f* 200841010 片上並產生電滲透流〔electr〇〇sm〇sis n〇w〕,以影響該樣 口口中各成分於各槽道中之流動速率,進而產生分離。接著 於該槽道中預設一偵測位置。待樣品流至該偵測位置後, 利用該光源發丨-激發光通過該激發濾丨,以過濾並得到 特疋波長之激發光,再以該分光鏡反射該激發光,並經 由該透鏡將該激發光聚焦至該_位置,關用該聚焦後 之激發光照射位於該制位置之樣品。經該激發光照射後 之樣品將產生螢光放射。接著將婦品所產生之螢光由該 透鏡收集後依序經該分光鏡、放射濾片及―針孔至該光電 倍增管,以利用該光電倍增管放大該#品所產生之榮光訊 號’之後域訊賴取單元將類比訊賴紐位訊號後, 由該訊號處理單元輸出樣品分析後之數據。如此便完成該 樣品之彳貞測。 m 一般而言,上述習用微流體晶片系統之螢光偵測方法 具^下列缺點’例如:該激發光通常係直接射入該訊號榻 取單元I’又該激發光之強度大於該樣品所發出之榮光甚 多,使得該螢光之訊號相對較不明顯,如此將降低量測準 確度。因此’該習用個方法需另設置該激發渡片,以過 滤出特定波長之激發光,造成其具有成本昂貴及設 之缺點:再者,該習用债測方法受限於單一波長的激發與 债測’热法同時制多波長之螢光放射,使得其 ς 樣品之螢光激發波長調整該激發光之波長並重複二 制,除增加樣品損耗量外亦增加檢測時間 侧效率低落之缺點。同時,因該習用_‘33 P:\01-l LindaNPK Pat\PKI03ll.doc 一 7 一 200841010 長激發與偵測的限制,使得所偵測之數據範圍較小,後續 所求得之量化數據準確性不足。基於上述原因,有必要進 一步改良上述習用微流體晶片系統之多波長螢光债測方法 〇 有鑑於此,本發明改良上述之缺點,其係利用一光學 儀器之連績光源激發一微流體晶片糸統發出螢光,並利用 一光學分析單元對該螢光進行偵測。藉此,本發明確實能 提升偵測效率、準確度、降低成本及簡化設備之微流體晶 片系統之多波長螢光偵測方法。 【發明内容】 本發明主要目的係提供一種微流體晶片系統之多波 長螢光偵測方法,其係利用一光學儀器之連續光源激發一 微流體晶片系統發出螢光,並利用一光學分析單元進行偵 測,使得本發明具有提升偵測效率之功效。Linda\PKHat\PU03ll.doc f* 200841010 An electroosmotic flow [electr〇〇sm〇sis n〇w] is generated on-chip to influence the flow rate of each component in the channel in each port, thereby generating separation. A detection position is then preset in the channel. After the sample flows to the detecting position, the light source generates excitation-excitation light through the excitation filter to filter and obtain excitation light of a special wavelength, and then reflects the excitation light by the beam splitter, and the lens is reflected through the lens The excitation light is focused to the _ position, and the focused excitation light is used to illuminate the sample at the position. The sample irradiated with the excitation light will generate fluorescence emission. Then, the fluorescent light generated by the feminine product is collected by the lens, and then sequentially passed through the spectroscope, the radiation filter and the “pinhole” to the photomultiplier tube to enlarge the glory signal generated by the # product by using the photomultiplier tube. After the domain information acquisition unit compares the analog signal, the signal processing unit outputs the sample analysis data. This completes the speculation of the sample. In general, the fluorescent detection method of the conventional microfluidic wafer system has the following disadvantages: for example, the excitation light is directly incident on the signal receiving unit I', and the intensity of the excitation light is greater than that emitted by the sample. The glory of the glory makes the fluorescent signal relatively insignificant, which will reduce the measurement accuracy. Therefore, the conventional method needs to set the excitation wave to filter out the excitation light of a specific wavelength, which causes it to be expensive and has disadvantages: in addition, the conventional debt measurement method is limited by the excitation and debt of a single wavelength. The 'thermal method simultaneously produces multi-wavelength fluorescence emission, so that the fluorescence excitation wavelength of the ς sample adjusts the wavelength of the excitation light and repeats the two systems. In addition to increasing the sample loss, it also increases the disadvantage of low efficiency on the detection time side. At the same time, due to the long-term excitation and detection limitation of the _'33 P:\01-l LindaNPK Pat\PKI03ll.doc one 7-200841010, the detected data range is small, and the quantified data obtained subsequently is accurate. Insufficient. For the above reasons, it is necessary to further improve the multi-wavelength fluorescence fingerprinting method of the conventional microfluidic wafer system. In view of the above, the present invention improves the above-mentioned disadvantages by exciting a microfluidic wafer using a continuous light source of an optical instrument. Fluorescence is emitted and the fluorescence is detected using an optical analysis unit. Thereby, the present invention can indeed improve the detection efficiency, accuracy, cost reduction and simplification of the multi-wavelength fluorescence detection method of the microfluidic wafer system of the device. SUMMARY OF THE INVENTION The present invention is directed to a multi-wavelength fluorescence detection method for a microfluidic wafer system that utilizes a continuous light source of an optical instrument to excite a microfluidic wafer system to emit fluorescence and utilize an optical analysis unit. The detection makes the invention have the effect of improving the detection efficiency.

---- I * W i 本發明次要目的係提供一種微流體晶片系統之多波 長螢光偵測方法,其中該光學儀器係為一暗視野光學組, 使得本發明具有降低成本及簡化設備之功效。 本發明另一目的係提供一種微流體晶片系統之多波 長螢光偵測方法,其中該微流體晶片系統之微流體晶片上 係η又置荟考槽道,以求得一背景值,進而使得本發明具 有提升偵測準確性之功效。 八 4據本毛月之微流體晶片系統之多波長螢光偵測方 ^其包含步驟:提供-微流體晶片具有-基板、二進樣 W、—分離槽道及—參考槽道,並將-樣品導入與該分 D:\ni-1 LindaNPl; Pat\PKI03H.doc η7/η«!/η3/ιι:ηι aji —8 — 200841010 上曰通之進樣槽道中;提供一電壓於該微流體晶片 二二吏該樣品移動至該分離槽道上之-娜置,·經 碎光提供—連續光毅—接收單元,關用該連 、、Ά原發it{之—激發光激發祕品 =__光,其中’該激發光並未直接照射: 4 一、,及將該光學儀$所接收之螢光訊號傳至該光學分---- I * W i A secondary object of the present invention is to provide a multi-wavelength fluorescence detection method for a microfluidic wafer system, wherein the optical instrument is a dark field optical group, so that the invention has the advantages of reducing cost and simplifying equipment The effect. Another object of the present invention is to provide a multi-wavelength fluorescence detecting method for a microfluidic wafer system, wherein a microfluidic wafer on the microfluidic wafer system is further provided with a reference channel to obtain a background value, thereby The invention has the effect of improving the detection accuracy. VIII. According to the multi-wavelength fluorescence detection method of the Maoyue microfluidic wafer system, the method comprises the steps of: providing - the microfluidic wafer has a substrate, a two-injection W, a separation channel, and a reference channel, and - sample introduction and the division D: \ ni-1 LindaNPl; Pat \ PKI03H.doc η7 / η « ! / η3 / ιι: ηι aji — 8 — 200841010 in the injection channel of Shangyutong; provide a voltage in the micro The fluid wafer is moved to the separation channel, and the sample is moved to the separation channel, and the continuous light-receiving unit is provided by the broken light, and the connection is used, and the original light is activated. __Light, where 'the excitation light is not directly illuminated: 4, and the fluorescent signal received by the optical instrument $ is transmitted to the optical sub

—並進行”析,其巾,該參考槽道係用以測^一背景 值,以進一步校正該樣品所測得之數據。 ’、 【實施方式】 目的、特徵、優點能更明顯 實施例,並配合所附圖式, 為讓本發明之上述及其他 易懂,下文特舉本發明之較佳 作洋細說明如下: 杯照第1及2圖所示’本發明較佳實施例之微流體 晶#彡、统之乡波錢光制方法的第-步驟S1係··提供— 微流體晶片1具有一基板η、_進樣槽道12、一分離槽道 • 13及$考槽3^ 14 ’並將一樣品〔未緣示〕導入與該分離 槽運13相連通之進樣槽道12.中。更詳言之,該樣本係選 擇由至^-待測物與一背景溶液混合配製而成。該待測物 〔未繪不〕係預先以—螢光染劑〔未纟會示〕對該待測物進 行標定,以利後續螢光激發之進行。該基板u係選擇為一 - 玻璃基板。該進樣槽道12係供該樣品導入,且長度係選擇 , 為0.8cm。該分離槽道13係用以分離該樣品,且^係=該 進樣槽道12相連通並相交形成一十字形。該分離槽道u 上係預設一偵測位置a,且該分離槽道13之長度係^擇為- and performing "analysis, the towel, the reference channel is used to measure a background value to further correct the data measured by the sample. ', [Embodiment] The purpose, features, advantages can be more obvious embodiments, BRIEF DESCRIPTION OF THE DRAWINGS In order to make the above and other aspects of the present invention readily apparent, the following detailed description of the present invention will be described as follows: Cup-like photographs 1 and 2 show a microfluid of the preferred embodiment of the present invention. The first step S1 of the method of making crystals of the crystals and the method of the method of the invention is provided. The microfluidic wafer 1 has a substrate η, a sample injection channel 12, a separation channel, and a test slot. 14 ' and a sample (not shown) is introduced into the injection channel 12 which is in communication with the separation tank 13. In more detail, the sample is selected from the mixture of the analyte and the background solution. The test object (not shown) is pre-calibrated with a fluorescent dye (not shown) to facilitate subsequent fluorescence excitation. The substrate u is selected as A - glass substrate. The sample channel 12 is for the sample to be introduced, and the length is selected to be 0.8 cm. 13 is used to separate the sample, and the system is connected to and intersects to form a cross shape. The separation channel u is preset with a detection position a, and the length of the separation channel 13 Choose ^ as

Linda\PK Pat\PKI03H.doc —9 — 200841010 5cm。該參考槽道M解行設置於該分離槽道u之一側 ’讀2景溶液導人並_其勞光訊號作為後續數據分 析之一背景值’進而減少偵測誤差並提升偵測準確性。該 :考心運U距該分離槽道13之距離係選擇為5麵。該微 Γ體Γ片1較佳係另設置—刻度線15,且該刻度線15係 平仃叹置於該分離槽道13之一側,以利判斷該樣品之移動 位置。其中’各槽道之寬度係選擇為_,深度係選擇 為 36 // m 〇 .明再荟照第1及2圖所示,本發明較佳實施例中,該 進本;》^a道12之相對兩端係分別形成一第一通孔I〕〗、ι21, 與該,樣槽道12相通’該第—通孔121係供該樣品導入, 另一第-通孔121,係用以排除多餘樣品。該分離槽道13 ^相對兩端係分卿成—第二通孔131、131,與該分離槽 逼13相通。該參考槽道14之相對兩端係分別形成一第三 通孔⑷、⑷,與該參考槽道14相通,該第三通孔i4i係 供該背景溶液導入以測定該背景值,另一第三通孔141,係 用以排除多餘之背景溶液。 ^ 凊再麥照第1及2圖所示,本發明較佳實施例之微流 體晶片系統之多波長螢光偵測方法的第二步驟S2係:提供 一電壓於該微流體晶片1上,以驅使該樣品移動至該分離 槽道13上之-偵測位s a。更詳言之,該電塵係施加於該 分離槽道13之兩端以形成一電場〔未繪示〕並產生一電滲 透流〔electroosmosis flow〕。由/於該樣品中之各成分受該 電滲透流之影響各不相同’因此可經由該電滲透流驅動該 B:\0I-I Linda\PK Pat\PK103ll.doc ——10—— 200841010 樣ncr中之各成分,使得該樣品可沿著該分離槽道Η進行分 離並移動至該偵測位置a。 請再參照第1至3圖所示,本發明較佳實施例之微流 體曰曰片系統之多波長螢光偵測方法的第三步驟S3係··經由 一光學儀器2提供一連續光源21及一接收單元22,以利 用該連續光源21發出之一激發光211激發該樣品發射一螢 光,亚經由該接收單元22接收該螢光,其中,該激發光 211並未直接照射該接收單元22。更詳言之,本實施例之 光學儀斋2係選擇但不受限於一暗視野光學組。該光學儀 器2係包含一連續光源21、一接收單元22、一擋板、 一聚光單元24及一針孔25。該樣品較佳係介於該連續光 源21及接收單元22之間。該連續光源21係可發出一多波 長fe圍之激發光211,以激發位於該偵測位置a之樣品發 螢光〔未繪示〕。藉由該連續光源21可同時激發多種不 同之螢光染劑,進而增進偵測效率。該連續光源21係選擇 但不X限為一鎢燈。該接收單元22係用以接收該樣品所發 出之螢光。該激發光211之強度大於該樣品所發出之螢光 甚多,若該接收單元22同時接收該激發光211與螢光之訊 號,則該螢光之訊號則相對較不明顯。因此該連續光源21 所發出之激發光2Π並未直接照射該接收單元22,以避免 該接收單元22接收該強度過強之激發光211,而影響該樣 口口所發出之螢光的相對訊號強度。該接收單元22係選擇為 一物鏡。 、 4再苓照第1至3圖所示,本發明較佳實施例中,該 200841010 連續光源21係選擇設置於該接收單元22之下方。為避免 該連續光源21直接照射該接收單元22,因此於該連續光 源21與該接收單元22之間的水平方向設置該擋板23阻擋 .該連續光源21所發出之激發光211。於該擋板23阻擋後 ,該連續光源21所發出之光係形成一中空管狀之激發光 211。該擋板23係選擇為圓形。該擋板23與接收單元u 之二係設置-聚光單元24,以利用該聚光單元%將該中 二官狀之激發光211聚焦,進而激發該樣品發出螢光。該 聚$單元24係選擇為一暗視野聚光鏡。該樣品係位於該接 收單元22與聚光單元24之間。該針孔25是設置於該接收 單元22之上方,以於該接收單元22接收該樣品之榮光訊 號後,經由該針孔25並傳送至後續之光學分析單元3以進 JJ行訊號之分析。如此,該連續光源21所發出之激發光2ιι 經由該檔板23阻擋後形成一中空管狀之激發光2ιι。接著 再經過該聚光單元24使該激發光211形成一中空錐形之激 鲁 1光211’亚聚焦於該微流體晶片i之偵測位置經由該 激發光211使得位於該偵測位置&之樣品發出螢光’且該 螢光係由該接收單元22接收。由於該激發光2ιι係形成該 中空錐形之激發光211,且該錐形頂點係位於該微流體晶 片1上’因此可避免該激發光211直接進域接收單元^ - ^且僅有少數糾娜狀射之激發光211可進入該接 . 收单:22中。該中空錐形之激發光211較佳係聚焦於該偵 請再參照第1至3圖所示, 本發明較佳實施例之微流 i»:\0l-l LindaNPK Pat\Pi;l〇3l 1. doc η7/η4/ίχνπ:〇ί —12 — 200841010 妝曰日片系統之多波長螢光偵測方法的第四步驟S4係:將該 光子儀為2所接收之螢光訊號傳至該光學分析單元3並進 行刀析。更詳言之,該光學儀器2所接收之螢光訊號係選 擇,由一光纖〔〇ptical fiber〕將該螢光訊號傳至該光學分 析,tl 3以進行分析。該螢光訊號亦可選擇經由一光電倍 〔未繪示〕放大後,再傳至該光學分析單元3。該光 :刀析單元3較佳係選擇為一紫外_可見_近紅外光之光譜 分析儀,以便同時彻彳各種不同波圍之螢光。該營光 訊號經由該光學分析單幻分析後,可得到時間〔秒〕、波 ,〔nm〕及穿透率〔%〕之相對變化義,亦可進一步求 得更加精準之量化數據。另外,請參照第〗圖所示,為使 所測得之數據更域準,較佳係於上述步驟完成後,另進 ^下列步驟以取得該背景值:將該背景溶液導人該參考槽 :二之本第三通孔141中,並施加電壓驅使該背景溶液移動 、。茶考槽道U上之-參考位置b;利用該激發光2 杯考位置b之背景光,並經由該接收單元22接收 W光’將景錢之光喊傳至該光學分析單元3 取得該f景值。其中該參考位置W位於該參考 心迢14上’聪對應該_位置a。最後再將該樣品 所得之螢紐據扣輯背景值之麟,如此便可校正鮮 品所測得之螢光數據’亦可進—步得到更精準之量化妻= 請再參照1至3圖所示,當實行本發明較佳實施例時 ,首先進龍[倾S1 :將經由螢光軸標定後之^ D:\ni-* Lirwln\PK Pat\PKI03H.doc η7/η·ι/η3/ιι;〇,,,, 13 200841010 〔未繪不〕注入該微流體晶片i之進樣槽道12中。待兮 品逐漸流動至該進樣槽道12與分離槽道13之交點後' = 著進行該第二㈣S2 :提供—電壓於該微流體晶片i ; 驅使該樣品沿著齡離槽道13軸至_測位置& ;再進 行該第三步驟S3 :利用該連續光源21發射出多波長 發光211,再依序經由該擋板23及聚光單元%使該激笋 光211形成一中空錐形之激發光211,並聚焦於該偵^ 置a,以激發位於該偵測位置a之樣品發出螢光。該樣品 1 所發出之螢光將被該接收單元22接收,且該激發光2lj": 未直接照射該接收單元22,以避免影響該榮光訊號之相對 —強度;最後進行該第四步驟料:將該光學儀器2所接收之 _螢光訊號經由該光纖傳至該光學分析單元3並進行分析, 以得到時間、波長及穿透率之相對變化關係。如此,便完 成本發明較佳實施例之微流體晶片系統之多波長偵測方= 。藉此’本發明確實具有提升債測效率、準確度、降低成 本及簡化設備之功效。 凊參照第4圖所示,本發明實施例中,係選擇以fitc 、RhB及Atto610作為該樣品之螢光染劑。第4圖係為各 該螢光染劑經由本發明之多波長螢光偵測方法所測得之吸 收及發射光譜圖形。圖中虛線係指各該螢光染劑之吸收光 波長’而實線係指各該螢光染劑之發射光波長。可得知 FITC、RhB及Atto610之最大吸收光波長係分別為49〇nm 〔奈米〕、553nm及614nm,而最大放射光波長係分別為 514nm、578nm及633nm。各該螢光染劑之最大放射光波 D:\01-I LindaSPK Pat\PKI0311.doc - - ητ/ηΊ/η-νιι;^ ^ 200841010 長係為後績螢光分析之重要指標。 5 f 5 ㈤相對穿透率之分析&果。^ 射波長強度所得到的時 扣除該背景值之_後所彳^ 品之營光數據 * ’該3D電泳圖形係可明 二圖可 營光於時間、波長及穿透率之相對^,射之 用以判斷該榮光之強度。第5及6圖=;_係 1胃用螢光偵測方法需對應各該螢辭=二弟5圖之 長強度分別進行多次债測,益法同時對^大貧光放射波 &長之螢光染劑進行偵測。而第6圖之^日不同螢^放射 由於該激發光211並未直接進入該接收:明較佳實施例 須裝設任= ^此無 订夂债測,即可同時進;m丄 而進 ,請再參照第5=種=;:_測: !光進行定量分析時,係將第5圖中之:峰==對該 取得量化數據,但由於其所测得之數據僅,以 =放射波長強度下之偵測結果,使 !1=積=,電泳圖形可將㈣平面1 料作體積刀,如此所取得之量化 低:::=*有_測效率、準確度= 如上所述,相較於習用微流體晶片系統之多波長螢光 D:\0I-1 LindaNPJ: Pal\PXl〇3U. dix 15 200841010 ==有出特定波長之激發 用崎法受 圖 體晶片 多波長之螢n 7放考偵都,热法同時偵測 時,因_具有制效率低落之缺點。同 得其且之單—波絲發雜_限制,使 之置化數據準確性不足等缺點。反觀第1 晶片i $_ 先學儀器2之連續光源21激發該微流Linda\PK Pat\PKI03H.doc —9 — 200841010 5cm. The reference channel M is disposed on one side of the separation channel u. 'Reading the 2 scene solution guide and _ its work light signal as a background value of subsequent data analysis' further reduces detection error and improves detection accuracy . The distance between the test core U and the separation channel 13 is selected to be five sides. The micro-cylinder blade 1 is preferably provided with a scale line 15 and the scale line 15 is placed on one side of the separation channel 13 to facilitate the determination of the moving position of the sample. Wherein, the width of each channel is selected to be _, and the depth system is selected to be 36 // m 明. As shown in Figures 1 and 2, in the preferred embodiment of the present invention, the input is; The opposite ends of the 12 are respectively formed with a first through hole I], ι21, and the sample channel 12 is in communication with the sample channel 12, the first through hole 121 is for introducing the sample, and the other first through hole 121 is used for To exclude excess samples. The separation channel 13 ^ is divided into two ends - a second through hole 131, 131, which communicates with the separation groove 13. The opposite ends of the reference channel 14 respectively form a third through hole (4), (4), and communicate with the reference channel 14, the third through hole i4i is used for introducing the background solution to determine the background value, and another A three-way aperture 141 is provided to remove excess background solution. The second step S2 of the multi-wavelength fluorescence detecting method of the microfluidic wafer system of the preferred embodiment of the present invention is to provide a voltage on the microfluidic wafer 1 as shown in FIGS. 1 and 2, To detect the movement of the sample to the detection channel sa on the separation channel 13. More specifically, the electric dust is applied to both ends of the separation channel 13 to form an electric field (not shown) and to generate an electroosmosis flow. The components in/from the sample are affected by the electroosmotic flow. Thus, the B:\0I-I Linda\PK Pat\PK103ll.doc ——10——200841010 can be driven via the electroosmotic flow. The components of the ncr are such that the sample can be separated along the separation channel and moved to the detection position a. Referring again to FIGS. 1 to 3, a third step S3 of the multi-wavelength fluorescence detecting method of the microfluidic chip system of the preferred embodiment of the present invention provides a continuous light source 21 via an optical instrument 2. And a receiving unit 22, wherein the excitation light 211 is emitted by the continuous light source 21 to excite the sample to emit a fluorescent light, and the fluorescent light is received through the receiving unit 22, wherein the excitation light 211 does not directly illuminate the receiving unit twenty two. More specifically, the optical instrument 2 of the present embodiment is selected but not limited to a dark field optical group. The optical instrument 2 comprises a continuous light source 21, a receiving unit 22, a baffle, a concentrating unit 24 and a pinhole 25. Preferably, the sample is between the continuous light source 21 and the receiving unit 22. The continuous light source 21 emits a plurality of wavelengths of excitation light 211 to excite the sample at the detection position a to emit fluorescence (not shown). The continuous light source 21 can simultaneously excite a plurality of different fluorescent dyes, thereby improving detection efficiency. The continuous light source 21 is selected but not limited to a tungsten lamp. The receiving unit 22 is configured to receive the fluorescent light emitted by the sample. The intensity of the excitation light 211 is greater than the amount of fluorescence emitted by the sample. If the receiving unit 22 simultaneously receives the signal of the excitation light 211 and the fluorescent light, the signal of the fluorescent light is relatively insignificant. Therefore, the excitation light 2 emitted by the continuous light source 21 is not directly irradiated to the receiving unit 22, so as to prevent the receiving unit 22 from receiving the excessively intense excitation light 211, and affecting the relative signal of the fluorescent light emitted by the sample port. strength. The receiving unit 22 is selected as an objective lens. 4, in the preferred embodiment of the present invention, the 200841010 continuous light source 21 is selectively disposed below the receiving unit 22. In order to prevent the continuous light source 21 from directly illuminating the receiving unit 22, the baffle 23 is disposed in the horizontal direction between the continuous light source 21 and the receiving unit 22 to block the excitation light 211 emitted by the continuous light source 21. After the baffle 23 is blocked, the light emitted by the continuous light source 21 forms a hollow tubular excitation light 211. The baffle 23 is selected to be circular. The baffle 23 and the receiving unit u are provided with a concentrating unit 24 for focusing the intermediate-second excitation light 211 by the concentrating unit %, thereby exciting the sample to emit fluorescence. The poly unit 24 is selected as a dark field concentrating mirror. The sample is located between the receiving unit 22 and the concentrating unit 24. The pinhole 25 is disposed above the receiving unit 22, and after receiving the glory signal of the sample, the receiving unit 22 transmits the signal to the subsequent optical analysis unit 3 via the pinhole 25 for analysis of the JJ signal. In this way, the excitation light 2 ιι emitted by the continuous light source 21 is blocked by the baffle 23 to form a hollow tubular excitation light 2 ιι. Then, the illuminating unit 211 is configured to form a hollow cone-shaped luminaire 1 211 ′ to focus on the detection position of the microfluidic chip i via the excitation light 211 to be located at the detection position & The sample emits fluorescence 'and the fluorescence is received by the receiving unit 22. Since the excitation light 2 ιι forms the hollow cone excitation light 211, and the cone apex is located on the microfluidic wafer 1 'the excitation light 211 can be prevented from directly entering the receiving unit ^ ^ ^ and only a few corrections The excitation light 211 of the Na-shaped shot can enter the connection. The acquirer: 22. The hollow cone-shaped excitation light 211 is preferably focused on the detection. Referring again to Figures 1 to 3, the microflow i»:\0l-l LindaNPK Pat\Pi;l〇3l of the preferred embodiment of the present invention 1. doc η7/η4/ίχνπ:〇ί —12 — 200841010 The fourth step of the multi-wavelength fluorescence detection method of the makeup system is S4: the photon is transmitted to the received fluorescent signal The optical analysis unit 3 performs knife analysis. More specifically, the fluorescent signal received by the optical device 2 is selected, and the fluorescent signal is transmitted from the optical fiber to the optical analysis, t13 for analysis. The fluorescent signal can also be selected to be amplified by a photomultiplier (not shown) and then transmitted to the optical analysis unit 3. The light: the knife unit 3 is preferably selected as a UV-visible_near-infrared light spectrum analyzer to simultaneously illuminate the fluorescent light of various wavelengths. After the optical analysis of the camping light signal, the relative change of time [second], wave, [nm] and transmittance [%] can be obtained, and more accurate quantitative data can be further obtained. In addition, please refer to the figure, in order to make the measured data more accurate, preferably after the above steps are completed, another step is taken to obtain the background value: the background solution is guided to the reference slot : In the third through hole 141, a voltage is applied to drive the background solution to move. The tea test channel U is on the reference position b; the background light of the position b is measured by the excitation light 2, and the W light is received via the receiving unit 22, and the light of the Jing Qianguang is transmitted to the optical analysis unit 3 to obtain the f view value. Wherein the reference position W is located on the reference palpe 14 and corresponds to the position a. Finally, the sample obtained from the sample is deducted from the background value of the lining, so that the fluorescent data measured by the fresh product can be corrected, and the fluorescence data measured by the fresh product can be further improved to obtain a more accurate quantified wife = please refer to the 1 to 3 figure. As shown, when implementing the preferred embodiment of the present invention, the first step is to enter the dragon [pour S1: to be calibrated via the fluorescent axis ^ D:\ni-* Lirwln\PK Pat\PKI03H.doc η7/η·ι/η3 / ιι; 〇,,,, 13 200841010 [not depicted] injected into the injection channel 12 of the microfluidic wafer i. After the product is gradually flowing to the intersection of the sampling channel 12 and the separation channel 13, the second (four) S2 is supplied: voltage is supplied to the microfluidic wafer i; the sample is driven along the axis of the channel 13 And performing the third step S3: using the continuous light source 21 to emit the multi-wavelength light-emitting 211, and sequentially forming the bamboo shoot light 211 into a hollow cone via the baffle 23 and the concentrating unit %. The excitation light 211 is shaped and focused on the detector a to excite the sample located at the detection position a to emit fluorescence. The fluorescent light emitted by the sample 1 will be received by the receiving unit 22, and the excitation light 2lj": is not directly irradiated to the receiving unit 22 to avoid affecting the relative intensity of the glory signal; finally, the fourth step is performed: The _fluorescent signal received by the optical device 2 is transmitted to the optical analysis unit 3 via the optical fiber and analyzed to obtain a relative change in time, wavelength, and transmittance. Thus, the multi-wavelength detection side of the microfluidic wafer system of the preferred embodiment of the invention is completed. Thus, the present invention does improve the efficiency, accuracy, cost, and simplification of equipment. Referring to Fig. 4, in the examples of the present invention, fitc, RhB and Atto610 were selected as the fluorescent dyes of the sample. Figure 4 is a graph of the absorption and emission spectra of each of the phosphor dyes measured by the multi-wavelength fluorescence detection method of the present invention. In the figure, the dotted line means the wavelength of the absorption light of each of the fluorescent dyes, and the solid line means the wavelength of the emitted light of each of the fluorescent dyes. It can be seen that the maximum absorption wavelengths of FITC, RhB and Atto610 are 49 〇 nm [nano], 553 nm and 614 nm, respectively, and the maximum emission wavelengths are 514 nm, 578 nm and 633 nm, respectively. The maximum emission light of each of the fluorescent dyes D:\01-I LindaSPK Pat\PKI0311.doc - - ητ/ηΊ/η-νιι;^ ^ 200841010 The long-term is an important indicator for the subsequent analysis of fluorescence. 5 f 5 (5) Analysis of relative transmittance & ^ When the wavelength intensity is obtained, the background data is subtracted from the background data of the product. 'The 3D electrophoresis pattern can be used to compare the time, wavelength and transmittance. It is used to judge the intensity of the glory. Figures 5 and 6 =; _ system 1 stomach fluorescence detection method needs to correspond to the long intensity of each of the above-mentioned syllabary = second brother 5 maps to conduct multiple debt tests, and the beneficial method simultaneously pairs the large poor light radiation & Long fluorescent dyes are detected. In the sixth picture, the different radiations are not directly entered into the reception due to the excitation light 211: the preferred embodiment must be installed with any = ^ this unsubscribed debt test, which can be simultaneously entered; , please refer to the 5th ==::_ test: ! When the light is quantitatively analyzed, it will be in the 5th picture: the peak == the obtained quantitative data, but because of the measured data only, to = The detection result under the radiation wavelength intensity is such that !1=product=, the electrophoresis pattern can use (4) plane 1 as the volumetric knife, so that the obtained quantization is low:::=* has _ measurement efficiency, accuracy = as described above Compared with the conventional multi-fluidic wafer system, multi-wavelength fluorescence D:\0I-1 LindaNPJ: Pal\PXl〇3U. dix 15 200841010 == There is a specific wavelength excitation for the multi-wavelength of the image-bearing wafer n 7 test the detective, when the thermal method is detected at the same time, because of the shortcomings of low efficiency. The same is true - the wave is miscellaneous _ limit, so that the accuracy of the data is insufficient. In contrast, the first wafer i $_ learns the continuous light source 21 of the instrument 2 to excite the microfluid

士 i b光’並利用該光學分析單元3進行制, ===參考槽道14求得該背景值以校正該樣品之螢 ::及=設 雖然本發明已利用上述較佳實施例揭示,然其並非用 錄定本發明,任何熟習此技藝者在不脫離本發明之精神 和範圍之内,相對上述實關猜各種更動歸改仍屬本 發明所保護之技術範,,因此本發明之保護範圍當視後附 之申請專利範圍所界定者為準。 16 — D:\OI-i Linda\PK Pat\PK103n.doc 07/0^1/03/11: 200841010 【圖式簡單說明】 蒂去第心圖/發日倾佳實施例之微流體晶片系、统之多波長 螢^偵測方法的流程方塊圖。 f圖·本發明較佳實施例之微流體晶片之立體圖。 慈=圖·本發明較佳實施例之微流體晶片減之多波長 金先偵測方法的示意圖。 射:Γ。·本發明較佳實施例之各該螢光染劑之吸收及放 第5圖·本發明較佳實施例之微流體晶片系統 螢光偵測方法的3D電泳圖。 4 ' 涵 第6圖·習用微流體晶片系統之榮光镇測方法 時間相對穿透率〔%〕之分析結果。 ’、亍之</ RTI> </ RTI> and using the optical analysis unit 3, === the reference channel 14 to determine the background value to correct the sample of the fire:: and = set although the invention has been disclosed using the preferred embodiment described above, The present invention is not intended to be used in the present invention, and it is still within the spirit and scope of the present invention. This is subject to the definition of the scope of the patent application. 16 — D:\OI-i Linda\PK Pat\PK103n.doc 07/0^1/03/11: 200841010 [Simple description of the diagram] The microfluidic chip system of the first embodiment And the flow block diagram of the multi-wavelength detection method. Figure 3 is a perspective view of a microfluidic wafer in accordance with a preferred embodiment of the present invention. BRIEF DESCRIPTION OF THE DRAWINGS A schematic diagram of a multi-wavelength gold first detection method for a microfluidic wafer according to a preferred embodiment of the present invention. Shoot: Hey. Absorbing and Discharging of Each of the Fluorescent Dyeing Agents in a Preferred Embodiment of the Invention FIG. 5 is a 3D electropherogram of a microfluidic wafer system fluorescent detection method according to a preferred embodiment of the present invention. 4 ' 第 Figure 6 · The glory of the conventional microfluidic wafer system method The analysis of the time relative transmittance [%]. ‘,亍之

【主要元件符號說明】 1 微流體晶片 12 進樣槽道 121 ’第一通孔 131第二通孔 14 參考槽道 14Γ第三通孔 2 光學儀器 211激發光 23擋板 25 針孔 11 基板 121第一通孔 13 分離槽道 131 ’第二通孔 141第三通孔 15刻度線 21 ’連續光源 22接收單元 24 聚光單元 3 光學分析單元 D:\OM LindaXPK Pat\PKin3H.doc —17 200841010 a 偵測位置 b 參考位置 SI 第一步驟 S2 第二步驟 S3 第三步驟 S4 第四步驟[Main component symbol description] 1 microfluidic wafer 12 injection channel 121 'first through hole 131 second through hole 14 reference channel 14 Γ third through hole 2 optical instrument 211 excitation light 23 baffle 25 pinhole 11 substrate 121 First through hole 13 separation channel 131 'second through hole 141 third through hole 15 tick mark 21 'continuous light source 22 receiving unit 24 concentrating unit 3 optical analysis unit D: \OM LindaXPK Pat\PKin3H.doc — 17 200841010 a Detection position b Reference position SI First step S2 Second step S3 Third step S4 Fourth step

Claims (1)

200841010 十、申請專利範圍: 1、一種微流體晶片系統之多波長螢光偵測方法,其包含步 驟: 提供一微流體晶片具有一基板、一進樣槽道、一分離槽 道及一參考槽道,並將一樣品導入與該分離槽道相連通 之進樣槽道中;200841010 X. Patent Application Range: 1. A multi-wavelength fluorescence detection method for a microfluidic wafer system, comprising the steps of: providing a microfluidic wafer having a substrate, a sampling channel, a separation channel and a reference slot a channel and introducing a sample into the injection channel in communication with the separation channel; 提供一電壓於該微流體晶片上,以驅使該樣品移動至該 分離槽道上之一偵測位置; 經由一光學儀器提供一連續光源及一接收單元,以利用 該連續光源發出之一激發光激發該樣品發射一螢光,並 經由該接收單元接收該螢光,其中,該激發光並未直接 照射該接收單元;及 將該光學儀器所接收之螢光訊號傳至該光學分析單元 並進行分析; 其中,該參考槽道係用以測定一背景值,以進一步校正 該樣品所測得之數據。 2、 依申請專利範圍第1項所述之微流體晶片系統之多波長 螢光偵測方法,其中該光學儀器係為一暗視野光學組。 3、 依申請專利範圍第1項所述之微流體晶片系統之多波長 螢光偵測方法,其中該樣品係由一待测物及一背景溶液 配製而成。 4、 依申請專利範圍第3項所述之微流體晶片系統之多波長 螢光偵測方法,其中該背景值係經由下列步驟取得:將 該背景溶液導入該茶考槽道中’並施加電壓驅使該背景 D:\0i-! LindaXPK Pat\PKi03H.doc —19 — 200841010 洛液移動至該參考槽道上之一參考值置;利用該激發光 激,攸於該參考位置之背景溶液發射榮光,並經由該接 ^単^接收$七㈣背景雜之螢输賴至該光學 分析單元,以分析並取得該背景值。 5、 依Λ請專利範圍第1項所述之微流體晶片系統之多波長 邊光偵測方法,其中係經由將樣品分析所得之螢光數據 扣除該背景值,以校正該樣品之螢光分析數據。 6、 =請專利範圍第4項所述之微流體晶片系統之多波長 a光偵測方法,其中該參考位置係對應該偵測位置。 7、 依^請專利範圍第i項所述之微流體晶片系統之多波長 1制方法,其巾該光學儀器係包含軸續光源、接 收單元、一擋板、一聚光單元及一針孔。 8、 依★申請專利範圍第7項所述之微流體晶片系統之多波長 gm:螢光制方法,其中該連續光_發出之》光係被胃 擂板阻擋並形成一中空管狀之激發光。 9、 依t請專魏隨8韻狀微趙晶統之多波長 營光侧方法’其巾該巾空管狀之激發光經職聚光單 元聚焦後形成-中空錐形之激發光,且該激發光並未直 接照射該接收單元。 10、 依申請專利範圍第9項所述之微流體晶片㈣之多波長 螢光_方法,其巾該巾蜂形讀發絲聚焦於贿 流體晶月上之一偵測位置。 11、 依申請專利關第7項所述之微流體晶片系、统之多波長 螢光福測方法’其中該樣品所放射之螢光進人該接收^ D:\0M Linda\PJ; Pat\PKI03n.(foc —20 — 07/04/03/11:0.} A.V 200841010 元後,接著通過該針孔並傳至該光學分析單元。 12、 依申請專利範圍第1項所述之微流體晶片系統之多波長 螢光偵測方法,其中該連續燈源係為一鎢燈。 13、 依申請專利範圍第1項所述之微流體晶片系統之多波長 螢光偵測方法,其中該光學儀器係經由一光纖將該螢光 訊號傳至該光學分析單元。Providing a voltage on the microfluidic wafer to drive the sample to move to a detection position on the separation channel; providing a continuous light source and a receiving unit via an optical instrument to emit excitation light by using the continuous light source The sample emits a fluorescent light, and receives the fluorescent light through the receiving unit, wherein the excitation light does not directly illuminate the receiving unit; and transmits the fluorescent signal received by the optical instrument to the optical analysis unit for analysis Wherein the reference channel is used to determine a background value to further correct the data measured by the sample. 2. A multi-wavelength fluorescence detection method for a microfluidic wafer system according to claim 1, wherein the optical instrument is a dark field optical group. 3. The multi-wavelength fluorescence detecting method of the microfluidic wafer system according to claim 1, wherein the sample is prepared from a sample to be tested and a background solution. 4. The multi-wavelength fluorescence detection method of the microfluidic wafer system according to claim 3, wherein the background value is obtained by: introducing the background solution into the tea-chamber channel and applying a voltage to drive The background D:\0i-! LindaXPK Pat\PKi03H.doc — 19 — 200841010 Loose liquid moves to a reference value on the reference channel; with the excitation light, the background solution at the reference position emits glory, and The $7 (four) background is transmitted to the optical analysis unit via the interface to analyze and obtain the background value. 5. The multi-wavelength edge light detecting method of the microfluidic chip system according to claim 1, wherein the fluorescence value of the sample is subtracted from the background value to correct the fluorescence analysis of the sample. data. 6. A multi-wavelength a-light detection method for a microfluidic wafer system as described in claim 4, wherein the reference position corresponds to a position to be detected. 7. The multi-wavelength 1 method of the microfluidic wafer system according to the scope of the invention, wherein the optical device comprises a shaft continuous light source, a receiving unit, a baffle, a concentrating unit and a pinhole. . 8. The multi-wavelength gm:fluorescent method of the microfluidic wafer system according to item 7 of the patent application scope, wherein the continuous light-emitting light system is blocked by the gastric raft and forms a hollow tubular excitation light. . 9. According to t, please use the multi-wavelength camp side method of Wei Wei 8 韵 微 微 微 微 微 微 ' 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其 其The receiving unit is not directly illuminated. 10. The multi-wavelength fluorescent method of the microfluidic wafer (4) according to claim 9 of the patent application, wherein the bee-shaped hair reading of the towel is focused on a detection position on the brittle fluid crystal moon. 11. According to the patent application, the microfluidic wafer system and the multi-wavelength fluorescence measurement method described in the seventh paragraph of the patent application, wherein the fluorescent light emitted by the sample enters the reception ^ D:\0M Linda\PJ; Pat\PKI03n (foc — 20 — 07/04/03/11:0.} AV 200841010 yuan, then passed through the pinhole and passed to the optical analysis unit. 12. Microfluidic wafer according to claim 1 The multi-wavelength fluorescence detecting method of the system, wherein the continuous light source is a tungsten lamp. 13. The multi-wavelength fluorescence detecting method of the microfluidic chip system according to claim 1, wherein the optical instrument The fluorescent signal is transmitted to the optical analysis unit via an optical fiber. D:\0t-l LindaXPK Pat\PKl03H.doc —21 —D:\0t-l LindaXPK Pat\PKl03H.doc —21 —
TW96111791A 2007-04-03 2007-04-03 Multi-wavelength fluorescence detecting method of a microchip system TWI336399B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW96111791A TWI336399B (en) 2007-04-03 2007-04-03 Multi-wavelength fluorescence detecting method of a microchip system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW96111791A TWI336399B (en) 2007-04-03 2007-04-03 Multi-wavelength fluorescence detecting method of a microchip system

Publications (2)

Publication Number Publication Date
TW200841010A true TW200841010A (en) 2008-10-16
TWI336399B TWI336399B (en) 2011-01-21

Family

ID=44821395

Family Applications (1)

Application Number Title Priority Date Filing Date
TW96111791A TWI336399B (en) 2007-04-03 2007-04-03 Multi-wavelength fluorescence detecting method of a microchip system

Country Status (1)

Country Link
TW (1) TWI336399B (en)

Also Published As

Publication number Publication date
TWI336399B (en) 2011-01-21

Similar Documents

Publication Publication Date Title
Galievsky et al. “Getting the best sensitivity from on-capillary fluorescence detection in capillary electrophoresis”–A tutorial
JP2005500513A (en) Scanning spectrophotometer for high-throughput fluorescence detection
JP2008530554A (en) Apparatus and measurement method for measuring signal from fluorescent nanodrop held at surface tension
US9494779B2 (en) Optical analysis device, optical analysis method and computer program for optical analysis using single particle detection
RU2593623C2 (en) Device for photometric or spectrometric analysis of liquid sample
EP2620762A1 (en) Photometric analysis method using single light-emitting particle detection
CN101551345B (en) Spectrometer based on X ray inspired light source
Ryder et al. Time-domain measurement of fluorescence lifetime variation with pH
Peng et al. Handheld laser-induced fluorescence detection systems with different optical configurations
CN108106994A (en) A kind of scan-type local enhances biochemical sensitive device
US9134177B2 (en) Self-referencing fiber-optic Raman probe
JP2000283960A (en) Micro-chip electrophoretic device
TW200841010A (en) Multi-wavelength fluorescence detecting method of a microchip system
JP5447172B2 (en) Surface plasmon resonance fluorescence analyzer and surface plasmon resonance fluorescence analysis method
WO2005080945A9 (en) Method for avoiding bleaching when using fluorescence correlation spectroscopy
CN204514810U (en) A kind of laser-induced fluorescence detection system
JP2003130795A (en) Method for calibrating sample analyzer
RU200181U1 (en) Device for rapid analysis of molecular structures
CN115607110B (en) Mammary gland tumor detection system based on autofluorescence
CN111826422B (en) Optical system for detecting fluorescence polarization and polarization degree measuring unit
CN217586919U (en) A microchip detection device for high flux liquid phase biomolecule detects
JP3042487B2 (en) Electrophoresis device
JP2024513950A (en) Natural fluorescence detection for protein analysis in capillary electrophoresis
JP3296351B2 (en) Electrophoresis device
KR20160092085A (en) Proactive portable algae detecting method and apparatus

Legal Events

Date Code Title Description
GD4A Issue of patent certificate for granted invention patent
MM4A Annulment or lapse of patent due to non-payment of fees