TWI394965B - Method for determining diode parameters by using a diode forward i-v characteristic - Google Patents

Method for determining diode parameters by using a diode forward i-v characteristic Download PDF

Info

Publication number
TWI394965B
TWI394965B TW97150004A TW97150004A TWI394965B TW I394965 B TWI394965 B TW I394965B TW 97150004 A TW97150004 A TW 97150004A TW 97150004 A TW97150004 A TW 97150004A TW I394965 B TWI394965 B TW I394965B
Authority
TW
Taiwan
Prior art keywords
diode
parameters
obtaining
characteristic curve
forward bias
Prior art date
Application number
TW97150004A
Other languages
Chinese (zh)
Other versions
TW201024764A (en
Inventor
Chin Min Hsiung
Original Assignee
Univ Nat Pingtung Sci & Tech
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 Pingtung Sci & Tech filed Critical Univ Nat Pingtung Sci & Tech
Priority to TW97150004A priority Critical patent/TWI394965B/en
Publication of TW201024764A publication Critical patent/TW201024764A/en
Application granted granted Critical
Publication of TWI394965B publication Critical patent/TWI394965B/en

Links

Landscapes

  • Testing Of Individual Semiconductor Devices (AREA)

Description

利用二極體之順向偏壓 I - V 特性曲線取得其參數之方法Method for obtaining parameters by using the forward bias I - V characteristic curve of a diode

本發明係關於一種利用二極體之順向偏壓I-V 特性曲線取得二極體參數之方法,本發明特別是關於利用二極體之順向偏壓I-V 特性曲線之新曲線函數,以圖示法〔graphical method〕直接取得其參數之方法。The present invention relates to a method for obtaining a diode parameter by using a forward bias IV characteristic curve of a diode. The present invention particularly relates to a new curve function using a forward bias IV characteristic curve of a diode to illustrate The method of obtaining the parameters directly from the graphical method.

利用二極體之電壓及電流間I-V 特性曲線可取得二極體之參數。The parameters of the diode can be obtained by using the voltage and current IV characteristic curves of the diode.

例如,根據熱電子發散理論〔thermionic emission theory〕,蕭基二極體〔Schottky diode〕之I-V 理想曲線為 For example, according to the thermionic emission theory, the IV ideal curve of the Schottky diode is

其中q 為電荷量,V 為二極體電壓,k 為Boltzmann常數,T 為絕對溫度。Where q is the amount of charge, V is the diode voltage, k is the Boltzmann constant, and T is the absolute temperature.

蕭基二極體之飽和電流I s The saturation current I s of the Xiaoji diode is

其中A 為接觸面積,S 為Richardson常數,為能障,β =q/kTI 0 =AST 2Where A is the contact area and S is the Richardson constant. For energy barrier, β = q/kT , I 0 = AST 2 .

利用二極體之順向偏壓特性擷取能障時,傳統方法需將方程式(1)取半對數對電壓作圖〔semi-logarithmic(Eq.(1)) vs.V plot〕即〔半對數電流-電壓圖〕〔ln I vs .V plot〕。在電壓略大於1/β 後,方程式(1)簡化為I =I s exp(βV ) (2)Capturing the energy barrier by using the forward bias characteristic of the diode In the traditional method, the equation (1) is to be taken as a semi-logarithmic pair voltage [semi-logarithmic (Eq. (1)) vs. V plot] that is [semi-logarithmic current-voltage diagram] [ ln I vs. V plot] . After the voltage is slightly larger than 1/ β , the equation (1) is reduced to I = I s exp( βV ) (2)

在半對數電流-電壓圖中為具有斜率β 的直線,且在零電壓之 截距為I s 。然後,利用簡單運算即可取得能障In the semi-logarithmic current-voltage diagram is a straight line with a slope of β , and the intercept at zero voltage is I s . Then, using simple calculations, you can get energy barriers. .

一般而言,方程式(1)之理想二極體I-V 曲線並未符合實際特性。另一較普遍接受的二極體I-V 曲線之方程式為 In general, the ideal diode IV curve of equation (1) does not meet the actual characteristics. Another more commonly accepted equation for the diode IV curve is

其中R 為內部串聯電阻,n 為理想因子。Where R is the internal series resistance and n is the ideal factor.

在電壓略大於1/β 後,上述方程式簡化為 After the voltage is slightly greater than 1/ β , the above equation is simplified to

然而,利用傳統圖示法由方程式(3)取得參數n 〔理想因子〕、R 〔電阻〕及〔能障〕具有兩個技術困難。第一困難為對於未知參數nR 另需兩個額外方程式;而第二困難為R/n 必須呈常數、I 函數或V 函數。若前述兩個技術困難得到解決時,方程式(3)變為 However, the parameters n (ideal factor), R [resistance], and the equation (3) are obtained by the conventional graphic method. [Energy barrier] has two technical difficulties. The first difficulty is that two additional equations are needed for the unknown parameters n and R ; the second difficulty is that R/n must be a constant, an I function or a V function. If the above two technical difficulties are solved, equation (3) becomes

方程式(4)與方程式(2)相似。因此,其參數〔能障〕可由傳統圖示法取得。Equation (4) is similar to equation (2). Therefore, its parameters [Energy barrier] can be obtained by the traditional graphic method.

為了取得參數nR ,學者Norde假設n =1,並建議一個輔助函數 In order to get the parameters , n and R , the scholar Norde assumes that n =1, and suggests a helper function

上述函數F 對電壓具有極小值,因此在極小值處存在dF/dV =0之關係。利用此關係式可導出 The above function F has a minimum value for the voltage, so there is a relationship of dF/dV =0 at the minimum value. Use this relationship to export

其中I min 為電流在極小值之電流值。結合方程式(4)及(5)時獲得 Where I min is the current value at which the current is at a minimum value. Obtained when combining equations (4) and (5)

上述方程式具有方程式(2)及(4)之形式。因此,其參數〔能障〕可由傳統圖示法取得。The above equation has the form of equations (2) and (4). Therefore, its parameters [Energy barrier] can be obtained by the traditional graphic method.

對於n >1的情形,許多學者提出各種不同的取出參數方法。For the case of n > 1, many scholars propose various different extraction parameters. method.

學者Bohlin修改Norde的輔助函數提出另一輔助函數 Scholar Bohlin modifies Norde's helper function to propose another helper function

其中r 為大於n 之任意常數。顯然,在函數F 對電壓圖〔F (V ) vs.V plot〕對於每個r 具有一個對應之函數F 曲線。由函數F 曲線的最小值獲得類似於方程式(5)的方程式為 Where r is any constant greater than n . Obviously, the function F vs. voltage map [ F ( V ) vs. V plot] has a corresponding function F curve for each r . The equation similar to equation (5) is obtained from the minimum value of the function F curve.

利用兩個不同的r 值可獲得一組方程式,在解聯立方程式後,可產生參數Rn 。然後,參數〔能障〕可由傳統圖示法取得。A set of equations can be obtained using two different r values, and the parameters R and n can be generated after the unjoined cubic equation. Then, the parameters [Energy barrier] can be obtained by the traditional graphic method.

學者Sato及Yasumura利用Norde的方法但在兩個不同溫度下量測兩組I-V 資料而獲得兩個函數F 曲線。其它所有類似Norde的方法也都利用函數F 對電壓圖〔F (V ) vs.V plot〕的存在及dF/dV =0而獲得必要的方程式,因而歸類為Norde方法家族。Scholars Sato and Yasumura used the Norde method to measure two sets of IV data at two different temperatures to obtain two function F curves. All other Norde-like methods also use the function F to obtain the necessary equations for the existence of the voltage graph [ F ( V ) vs. V plot] and dF/dV =0, and are therefore classified as the Norde method family.

學者Cheung及Cheung及學者Werner則提出利用不同於Norde方法家族的另一方法,以解決前述問題。他們對求得參數Rn 並未使用輔助函數F 。Cheung及Cheung發現半對數電流-電壓圖〔V vs. the semi-logarithmicI plot〕為具有斜率RY 軸截距n/β 的直線,其為 Scholars Cheung and Cheung and scholar Werner proposed another method different from the Norde method family to solve the aforementioned problems. They did not use the auxiliary function F for the parameters R and n . Cheung and Cheung found semi-logarithmic current - voltage plots [V vs. the semi-logarithmic I plot and R] is a straight line having a slope of the Y intercept n / β, which is

一旦參數Rn 由上述圖取得時,其參數由傳統圖示法取得。Once the parameters R and n are obtained from the above graph, their parameters Obtained by the traditional graphic method.

Werner獨立提出三個方法,其中之一與Cheung及Cheung發展者相同。Werner的第一個方法採用在小訊號下傳導率G 〔small signal conductance〕的概念,以避免需要繪製類Norde圖。在小訊號下傳導率定義為G =dI/dV 。由G 的定義及方程式(3)的結合而獲得 Werner independently proposed three methods, one of which is the same as the Cheung and Cheung developers. Werner's first method uses the concept of G (small signal conductance) under small signals to avoid the need to draw a class-like Norde diagram. Conductivity is defined as G = dI/dV under small signals. Obtained by the definition of G and the combination of equation (3)

上述方程式顯示G/IG 圖為直線,其具有Y軸截距為β/n 、X軸截距為R 及斜率為-βR/n 。一旦參數nR 由上述圖取得時,其參數由傳統圖示法取得。The above equation shows that the G/I versus G graph is a straight line with a Y-intercept of β/n , an X-axis intercept of R, and a slope of -βR/n . Once the parameters n and R are obtained from the above graph, their parameters Obtained by the traditional graphic method.

Werner的另兩個方法亦採用在小訊號下傳導率的概念,但其可靠度及準確度稍差。Werner's other two methods also use the concept of conductivity under small signals, but their reliability and accuracy are slightly worse.

在理論上,為了取出三個參數nR,Cheung及Cheung的方法及Werner的方法皆需兩個圖,一個圖為取出參數nR ,另一個圖為取出參數In theory, in order to take out three parameters n , R and The Cheung and Cheung methods and the Werner method require two diagrams, one for taking out the parameters n and R and the other for taking the parameters. .

學者MeLean表示在考量其它較複雜的電流傳輸機制時,不易由簡單的圖示法取得參數nR,所以就發展數值曲線撮合法〔numerical curve fitting method〕,於此不予贅述。Scholar MeLean said that it is not easy to obtain the parameters n , R and the simple graphical method when considering other complicated current transmission mechanisms. Therefore, the numerical curve fitting method is developed, and will not be described here.

然而,利用圖示法取得參數nR係屬最容易使用及瞭解的方法。前述Norde的方法係雖然利用圖示法取得參數,但其僅適用於n =1的案例。另外,前述Bohlin或Sato及Yasumura的方法係並非完全的利用圖示法取得參數,而另需解一組方程式方能取得參數。無論Norde或Bohlin的方法都忽略多數的I-V 資料 ,其僅適用在最小值附近的幾組資料而已。因此,其取得參數值可靠度不佳。此外,前述各學者採用的方法僅為說明本發明技術背景及過去技術發展狀態而已,其並非用以限制本發明之範圍,合先敘明。However, using the graphical method to obtain the parameters n , R and It is the easiest way to use and understand. Although the aforementioned Norde method uses the graphical method to obtain parameters, it is only applicable to the case of n =1. In addition, the aforementioned methods of Bohlin or Sato and Yasumura do not completely take the parameters to obtain the parameters, but also need to solve a set of equations to obtain the parameters. Neither Nord nor Bohlin's method ignores most of the IV data, which applies only to groups of data near the minimum. Therefore, the reliability of the obtained parameter values is not good. In addition, the methods used by the above-mentioned various scholars are merely illustrative of the technical background of the present invention and the state of the art in the past, and are not intended to limit the scope of the present invention.

有鑑於此,本發明為了改良上述缺點,而提供一種利用二極體之順向偏壓IV 特性曲線取得其參數之方法,該方法為全新的技術方法。In view of the above, in order to improve the above disadvantages, the present invention provides a method for obtaining parameters by using a forward bias I - V characteristic curve of a diode, which is a completely new technical method.

目前有關二極體IV 特性曲線技術僅提及於少數美國專利而已。例如:美國專利US5406217之〝Method of measuring the current-voltage characteristics of a DUT〞;美國專利US4902912之〝Apparatus including resonant-tunneling device having multiple-peak current-voltage characteristics〞;美國專利US4456880之〝IV curve tracer employing parametric sampling〞;美國專利US4129823之〝System for determining the current-voltage characteristics of a photovoltaic array〞;美國專利US4080571之〝Apparatus for measuring the current-voltage characteristics of a TRAPATT diode〞,且前述諸美國專利無關於利用二極體之IV 特性曲線取得其參數。前述諸美國專利僅為用以說明目前技術發展狀態而已,其並非用以限制本發明之範圍。At present, the technology related to the diode I - V characteristic curve is only mentioned in a few US patents. For example, US Patent No. 5,406,217, Method of measuring the current-voltage characteristics of a DUT〞; US Patent No. 4,902,912, Appartus including resonant-tunneling device having multiple-peak current-voltage characteristics; US Patent No. 4,456,880 I - V curve Tracer employing parametric sampling; US Patent No. 4,129,823, System for determining the current-voltage characteristics of a photovoltaic array; US Patent No. 4,085,571, Apparatus for measuring the current-voltage characteristics of a TRAPATT diode, and the aforementioned US patents are not The parameters are obtained by using the I - V characteristic curve of the diode. The foregoing U.S. patents are merely illustrative of the state of the art and are not intended to limit the scope of the invention.

以下說明僅針對本發明目的及本發明較佳實施例予以概要方式說明,做為本發明之概要說明。至於本發明較佳實施例採用的二極體IV 模型函數之推導部分及利用圖示法之取得參數部份,另於【實施方式】中予以詳細說明。The following description is merely illustrative of the preferred embodiments of the invention and the preferred embodiments of the invention. The derivation portion of the diode I - V model function used in the preferred embodiment of the present invention and the parameter acquisition portion using the pictorial method are also described in detail in the [Embodiment].

本發明之主要目的係提供一種利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其提出二極體順向偏壓I-V 特性曲線之數學模型函數F (n, ,R ),並完全以圖示法取得其參數,本發明達成簡化取得參數操作之目的。The main object of the present invention to provide a system using the cis-biased diode IV characteristic curve acquisition parameters of its methods, which proposes a mathematical model function F (n forward bias IV characteristic curve of the diode cis, , R ), and its parameters are obtained completely by the method of illustration, and the present invention achieves the purpose of simplifying the operation of obtaining parameters.

為了達成上述目的,本發明較佳實施例之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法包含:量測二極體之順向偏壓I-V 特性曲線; 利用模型函數獲得模型函數,以提供F (I )-I 圖,以便由該F (I )-I 圖取得二極體參數之Rn ;其中r 為可調變數,且將r 調整至等於n ,即n =r ,並獲得方程式;當I =0時,取得RF (I )之斜率〔R/n 〕取得。In order to achieve the above object, a method for obtaining a parameter by using a forward bias IV characteristic curve of a diode according to a preferred embodiment of the present invention includes: measuring a forward bias IV characteristic curve of the diode; Model function acquisition a model function to provide an F ( I ) -I map to obtain a diode parameter from the F ( I ) -I map , R , n ; where r is a tunable variable and r is adjusted to be equal to n , ie n = r and obtained Equation; when I =0, get ; R is obtained from the slope [ R / n ] of F ( I ).

因此,其僅需單一次量測F-I 關係,而不需要使用dF/dV =0關係式或額外解一組方程式。Therefore, it only needs to measure the FI relationship in a single pass, without using the dF/dV =0 relationship or an additional solution to a set of equations.

本發明另一較佳實施例之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法包含: 建立模型函數; 在建立模型函數時,進一步獲得模型函數,以提供F (I )-I 圖; 將r 調整至等於二極體參數之n ,以取得方程式 ;其中n 等於r ;當I =0時,取得RFI 〕之斜率〔R/n 〕取得。A method for obtaining a parameter by using a forward bias IV characteristic curve of a diode according to another preferred embodiment of the present invention includes: Model function; When the model function is further obtained Model function to provide F ( I ) -I graph; adjust r to equal to the diode parameter n to obtain Equation; where n is equal to r ; when I =0, obtain R is obtained from the slope [ R/n ] of F [ I ].

為了充分瞭解本發明,於下文將舉例較佳實施例並配合所附圖式作詳細說明,且其並非用以限定本發明。In order to fully understand the present invention, the preferred embodiments of the present invention are described in detail below, and are not intended to limit the invention.

本發明較佳實施例之利用二極體之順向偏壓IV 特性曲線取得其參數之方法可應用於各種二極體,例如:pn二極體或蕭基〔Schottky〕二極體,但其並非用以限制本發明之範圍。本發明整個說明書中採用「二極體」之定義並非限定於任何特定一種二極體,於此不予詳細贅述。The method for obtaining the parameters by using the forward bias I - V characteristic curve of the diode of the preferred embodiment of the present invention can be applied to various diodes such as a pn diode or a Schottky diode. However, it is not intended to limit the scope of the invention. The definition of "diode" used throughout the specification of the present invention is not limited to any particular one of the diodes, and will not be described in detail herein.

本發明較佳實施例之利用二極體之順向偏壓IV 特性曲線取得其參數之方法適當採用二極體IV 模型函數之數學推導,該數學推導方式僅為用以說明本發明可行性,其並非用以限制本發明之範圍。The method for obtaining the parameters by using the forward bias I - V characteristic curve of the diode in the preferred embodiment of the present invention suitably adopts the mathematical derivation of the diode I - V model function, and the mathematical derivation is only for explaining the present The invention is not intended to limit the scope of the invention.

本發明之二極體之順向偏壓IV 特性曲線取得其參數之方法係屬可利用電腦執行之程序〔computer-executable process〕,其可執行於各種電腦設備〔computer equipment〕,如桌上型電腦〔desktop computer〕、筆記型電腦〔notebook〕、工作站電腦〔workstation computer〕等,但其並非用以限制本發明之範圍。The method for obtaining the parameters of the forward bias I - V characteristic curve of the diode of the present invention is a computer-executable process, which can be executed on various computer equipment, such as a table. A desktop computer, a notebook, a workstation computer, etc., but are not intended to limit the scope of the present invention.

以下說明為本發明較佳實施例採用的二極體IV 模型函數之簡單數學推導:首先,本發明較佳實施例採用二極體順向偏壓IV 曲線函數為 The following is a brief mathematical derivation of the diode I - V model function used in the preferred embodiment of the present invention. First, the preferred embodiment of the present invention uses a diode forward bias I - V curve function as

其中r 為可調變數。將方程式(3)及(6)結合而獲得 Where r is a tunable variable. Combine equations (3) and (6) to obtain

由於r 為可調變數,因而可依需求予以調整。當rn 時,方 程式(7)右邊第1項為零,而方程式(7)變為 Since r is an adjustable variable, it can be adjusted as needed. When r = n , the first term on the right side of equation (7) is zero, and equation (7) becomes

方程式(8)為具有斜率R/n 之直線方程式。因此,直接量測F (I )-I 圖〔F (I ) vs.I plot〕即可獲得斜率R/n 。一旦取得斜率R/n 時,可藉由傳統圖示法取得參數。或者,亦可由F (I )-I 圖之電流〔I 〕軸之截距量取參數。因此,本發明較佳實施例利用二極體之順向偏壓I-V 特性曲線取得其參數之方法係由單一次量測F-I 關係即可取得參數nR,而不像習用方法需要使用dF/dV =0關係式或額外解一組方程式。Equation (8) is a straight line equation having a slope R/n . Therefore, the slope R/n can be obtained by directly measuring the F ( I ) -I map [ F ( I ) vs. I plot]. Once the slope R/n is obtained, the parameters can be obtained by conventional graphical methods. . Alternatively, the parameter of the interception of the current [ I ] axis of the F ( I ) -I diagram can also be used. . Therefore, in the preferred embodiment of the present invention, the method for obtaining the parameters by using the forward bias IV characteristic curve of the diode is to obtain the parameters n , R by a single measurement of the FI relationship. Instead of using a dF/dV =0 relationship or an additional solution to a set of equations, as in the conventional method.

為了利用二極體之順向偏壓I-V 特性曲線取出二極體參數,本發明藉由前述二極體I-V 模型函數界定兩個本發明較佳實施例,並予以說明如下:本發明第一較佳實施例之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法包含:直接量測二極體之順向偏壓I-V 特性曲線; 利用模型函數獲得模型函數,以提供F (I )-I 圖,以便由該取得F (I )-I 圖取得二極體參數之Rn ;其中r 為可調變數,且將r 調整至等於n ,例如:手動方式 或由電腦程式自動調整r ,即n =r ,並獲得方程式;當I =0時,取得RFI 〕之斜率〔R/n 〕取得。In order to extract the diode parameters by using the forward bias IV characteristic curve of the diode, the present invention defines two preferred embodiments of the present invention by the aforementioned diode IV model function, and is described as follows: The method for obtaining the parameters of the forward bias IV characteristic curve of the diode using the preferred embodiment includes: directly measuring the forward bias IV characteristic curve of the diode; Model function acquisition a model function to provide an F ( I ) -I map to obtain a diode parameter from the F ( I ) -I map , R , n ; where r is a tunable variable and r is adjusted to be equal to n , for example: manual mode or automatically adjusted by computer program r , ie n = r , and obtained Equation; when I =0, get R is obtained from the slope [ R/n ] of F [ I ].

另外,本發明第二較佳實施例之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法包含: 建立模型函數; 在建立模型函數時,進一步獲得模型函數,以提供F (I )-I 圖; 將r 調整至等於二極體參數之n ,例如:手動方式或由電腦 程式自動調整r ,以取得方程式; 其中n 等於r ;當I =0時,取得RF (I )之斜率〔R/n 〕取得。In addition, the method for obtaining the parameters by using the forward bias IV characteristic curve of the diode according to the second preferred embodiment of the present invention includes: Model function; When the model function is further obtained Model function to provide F ( I ) -I diagram; adjust r to equal to the dipole parameter n , for example: manual mode or automatically adjust r by computer program to get Equation; where n is equal to r ; when I =0, obtain ; R is obtained from the slope [ R / n ] of F ( I ).

顯然,本發明之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法只需一次量測I-V ,藉由圖示法取得其特性參數:電阻R 、能障及理想因子n 。再者,本發明第一及第二較佳實施例之方法係適用具有符合I-V 特性曲線方程式為之 二極體。Obviously, the method for obtaining the parameters by using the forward bias IV characteristic curve of the diode of the present invention only needs to measure IV once, and obtains its characteristic parameters by the following method: resistance R , energy barrier And the ideal factor n . Furthermore, the methods of the first and second preferred embodiments of the present invention are applicable to equations having an IV characteristic curve. The two poles.

請參照第1圖所示,其揭示本發明較佳實施例之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法顯示函數模型-電流之關係曲線圖,其係屬蕭基二極體之函數模型-電流之曲線圖。在第1圖中,蕭基二極體之電阻R =101Ω,能障為=0.861eV及理想因子n =1.049。前述各項數據僅用以說明實驗結果,其並非用以限制本發明之範圍。Please refer to FIG. 1 , which discloses a method for displaying a function model-current relationship by using a forward bias IV characteristic curve of a diode according to a preferred embodiment of the present invention, which belongs to Xiao Jier. The function model of the polar body - the graph of the current. In Figure 1, the resistance of the Xiaoji diode is R = 101Ω, and the energy barrier is =0.861 eV and ideal factor n = 1.049. The foregoing data is only used to illustrate the experimental results and is not intended to limit the scope of the invention.

請再參照第1圖所示,其顯示:當n =1.047及n =1.048時,曲線往上彎曲;當n =1.050及n =1.051時,曲線往下彎曲;當n =1.049時,呈斜線,具有斜率。是以,本發明只需一次量測I-V ,藉由圖示法取得其特性參數之電阻R ,能障為及理想因子nReferring again to Figure 1, it shows that when n = 1.047 and n = 1.048, the curve is curved upwards; when n = 1.050 and n = 1.051, the curve is bent downward; when n = 1.049, it is oblique With a slope. Therefore, the present invention only needs to measure IV once, and obtains the resistance R of its characteristic parameter by the graphic method, and the energy barrier is And the ideal factor n .

前述較佳實施例僅舉例說明本發明及其技術特徵,該實施例之技術仍可適當進行各種實質等效修飾及/或替換方式予以實施;因此,本發明之權利範圍須視後附申請專利範圍所界定之範圍為準。The foregoing preferred embodiments are merely illustrative of the invention and the technical features thereof, and the techniques of the embodiments can be carried out with various substantial equivalent modifications and/or alternatives; therefore, the scope of the invention is subject to the appended claims. The scope defined by the scope shall prevail.

〔無元件符號〕[No component symbol]

第1圖:本發明較佳實施例之利用二極體之順向偏壓IV 特性曲線取得其參數之方法顯示函數模型-電流之關係曲線圖。Fig. 1 is a graph showing a function model-current relationship using a method for obtaining a parameter of a forward bias I - V characteristic curve of a diode according to a preferred embodiment of the present invention.

〔無元件符號〕[No component symbol]

Claims (10)

一種利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其包含:量測二極體之順向偏壓I-V 特性曲線; 利用模型函數獲得模 型函數,以提供F (I )-I 圖,以便由該F (I )-I 圖取得二極體參數之Rn ,其中為能障,R 為電阻,n 為理想因子;其中r 為可調變數,且將r 調整至等於n ,即n =r ,並獲得方程式;當I =0時,取得RF (I )之斜率〔R/n 〕取得。A method for obtaining a parameter by using a forward bias IV characteristic curve of a diode, comprising: measuring a forward bias IV characteristic curve of the diode; Model function acquisition a model function to provide an F ( I ) -I map to obtain a diode parameter from the F ( I ) -I map , R , n , where For energy barrier, R is the resistance and n is the ideal factor; where r is the tunable variable and r is adjusted to be equal to n , ie n = r and obtained Equation; when I =0, get ; R is obtained from the slope [ R / n ] of F ( I ). 依申請專利範圍第1項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其應用於pn二極體或蕭基二極體。A method for obtaining a parameter using a forward bias IV characteristic curve of a diode according to the first aspect of the patent application, which is applied to a pn diode or a Schottky diode. 依申請專利範圍第1項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,利用圖示法取得其參數RnThe method for obtaining the parameters by using the forward bias IV characteristic curve of the diode according to the first item of the patent application scope, and obtaining the parameters by the graphic method , R , n . 依申請專利範圍第1項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其中n 由手動調整r 的方式取得。A method for obtaining a parameter using a forward bias IV characteristic curve of a diode according to the first aspect of the patent application, wherein n is obtained by manually adjusting r . 依申請專利範圍第1項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其中n 由電腦程式自動調整r 的方式取得。A method for obtaining a parameter using a forward bias IV characteristic curve of a diode according to the first aspect of the patent application, wherein n is obtained by automatically adjusting r by a computer program. 一種利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其包含: 建立模型函數; 在建立模型函數時,進一步獲得模型函數,以提供F (I )-I 圖; 將r 調整至等於二極體參數之n ,以取得方程式; 其中n 等於r ;當I =0時,取得RF (I )之斜率〔R/n 〕取得,其中為能障,R 為電阻,n 為理想因子。A method for obtaining a parameter by using a forward bias IV characteristic curve of a diode, comprising: establishing Model function; When the model function is further obtained Model function to provide F ( I ) -I graph; adjust r to equal to the diode parameter n to obtain Equation; where n is equal to r ; when I =0, obtain ; R is obtained from the slope [ R / n ] of F ( I ), where For energy barrier, R is the resistance and n is the ideal factor. 依申請專利範圍第6項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其應用於pn二極體或蕭基二極體。A method for obtaining a parameter using a forward bias IV characteristic curve of a diode according to item 6 of the patent application, which is applied to a pn diode or a Schottky diode. 依申請專利範圍第6項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,利用圖示法取得其參數RnThe method for obtaining the parameters by using the forward bias IV characteristic curve of the diode according to item 6 of the patent application scope, and obtaining the parameters by the graphic method , R , n . 依申請專利範圍第6項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其中n 由手動調整r 的方式取得。A method for obtaining a parameter using a forward bias IV characteristic curve of a diode according to item 6 of the patent application scope, wherein n is obtained by manually adjusting r . 依申請專利範圍第6項所述之利用二極體之順向偏壓I-V 特性曲線取得其參數之方法,其中n 由電腦程式自動調整r 的方式取得。A method for obtaining a parameter using a forward bias IV characteristic curve of a diode according to item 6 of the patent application scope, wherein n is obtained by automatically adjusting r by a computer program.
TW97150004A 2008-12-22 2008-12-22 Method for determining diode parameters by using a diode forward i-v characteristic TWI394965B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW97150004A TWI394965B (en) 2008-12-22 2008-12-22 Method for determining diode parameters by using a diode forward i-v characteristic

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW97150004A TWI394965B (en) 2008-12-22 2008-12-22 Method for determining diode parameters by using a diode forward i-v characteristic

Publications (2)

Publication Number Publication Date
TW201024764A TW201024764A (en) 2010-07-01
TWI394965B true TWI394965B (en) 2013-05-01

Family

ID=44852287

Family Applications (1)

Application Number Title Priority Date Filing Date
TW97150004A TWI394965B (en) 2008-12-22 2008-12-22 Method for determining diode parameters by using a diode forward i-v characteristic

Country Status (1)

Country Link
TW (1) TWI394965B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI415203B (en) * 2009-10-16 2013-11-11 Univ Nat Pingtung Sci & Tech Method for obtaining parameters by using reverse iv characteristic of diodes

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5285151A (en) * 1991-03-22 1994-02-08 Hewlett-Packard Company Method and apparatus for measuring the breakdown voltage of semiconductor devices
TWM277928U (en) * 2005-05-18 2005-10-11 Union Optronics Corp A parameter testing device for dual-wavelength laser diode
TWI250707B (en) * 2005-05-18 2006-03-01 Union Optronics Corp Method for testing electrical parameters, light form and angle of divergence of laser diode

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5285151A (en) * 1991-03-22 1994-02-08 Hewlett-Packard Company Method and apparatus for measuring the breakdown voltage of semiconductor devices
TWM277928U (en) * 2005-05-18 2005-10-11 Union Optronics Corp A parameter testing device for dual-wavelength laser diode
TWI250707B (en) * 2005-05-18 2006-03-01 Union Optronics Corp Method for testing electrical parameters, light form and angle of divergence of laser diode

Also Published As

Publication number Publication date
TW201024764A (en) 2010-07-01

Similar Documents

Publication Publication Date Title
Römer et al. Recombination behavior and contact resistance of n+ and p+ poly-crystalline Si/mono-crystalline Si junctions
Chegaar et al. Extracting dc parameters of solar cells under illumination
Ouennoughi et al. A simpler method for extracting solar cell parameters using the conductance method
CN107248496B (en) The modification method of ohmic contact regions square resistance
Kale et al. Effect of Crystallographic Orientation and Nanoscale Surface Morphology on Poly-Si/SiO x Contacts for Silicon Solar Cells
Yordanov et al. Series resistance determination and further characterization of c-Si PV modules
Reichel et al. Influence of the transition region between p-and n-type polycrystalline silicon passivating contacts on the performance of interdigitated back contact silicon solar cells
TWI394965B (en) Method for determining diode parameters by using a diode forward i-v characteristic
CN106646174B (en) A kind of high speed three-dimensional electrology characteristic test system applied to transistor
Ocaya A current–voltage–temperature method for fast extraction of schottky diode static parameters
Chibbaro et al. A general and precise method to evaluate the series resistance of photovoltaic cells from IV characteristics
Wang et al. High fill factors of Si solar cells achieved by using an inverse connection between MOS and PN Junctions
TWI414033B (en) Method for determining diode parameters by using a diode forward i-v characteristic with noises
Hallam et al. Method of extracting solar cell parameters from derivatives of dark I–V curves
CN105140277A (en) Terahertz sensor based on tunneling transistor structure
Jiang et al. Real-space microscopic electrical imaging of n+-p junction beneath front-side Ag contact of multicrystalline Si solar cells
TWI394964B (en) Method for determining diode parameters by using a diode reverse i-v characteristic
CN104316771B (en) The Ohmic contact method of testing of silicon carbide device
CN106684011A (en) Method for testing square resistance of ohmic contact region
Khalis et al. Extraction of equivalent circuit parameters of solar cell: influence of temperature
CN107153157A (en) Dipulse Sofe Switch method of testing distinguishes GaN HEMT surfaces and cushion current collapse
Müller et al. Modelling of photo‐and electroluminescence of hydrogenated microcrystalline silicon solar cells
de Vries et al. Measuring the concentration and energy distribution of interface states using a non-contact corona oxide semiconductor method
Ling et al. Three-dimensional numerical analysis of hybrid heterojunction silicon wafer solar cells with heterojunction rear point contacts
Fink Capacitance-based characterization of PIN devices

Legal Events

Date Code Title Description
MM4A Annulment or lapse of patent due to non-payment of fees