CN104749511B - The description method of trap resistance - Google Patents

The description method of trap resistance Download PDF

Info

Publication number
CN104749511B
CN104749511B CN201310752999.0A CN201310752999A CN104749511B CN 104749511 B CN104749511 B CN 104749511B CN 201310752999 A CN201310752999 A CN 201310752999A CN 104749511 B CN104749511 B CN 104749511B
Authority
CN
China
Prior art keywords
mrow
trap
resistance
resistor
buried layer
Prior art date
Legal status (The legal status 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 status listed.)
Active
Application number
CN201310752999.0A
Other languages
Chinese (zh)
Other versions
CN104749511A (en
Inventor
武洁
徐萍
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanghai Huahong Grace Semiconductor Manufacturing Corp
Original Assignee
Shanghai Huahong Grace Semiconductor Manufacturing Corp
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 Shanghai Huahong Grace Semiconductor Manufacturing Corp filed Critical Shanghai Huahong Grace Semiconductor Manufacturing Corp
Priority to CN201310752999.0A priority Critical patent/CN104749511B/en
Publication of CN104749511A publication Critical patent/CN104749511A/en
Application granted granted Critical
Publication of CN104749511B publication Critical patent/CN104749511B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Semiconductor Integrated Circuits (AREA)

Abstract

Method is described the invention discloses a kind of trap resistance, on the basis of conventional trap resistance is evaluated, the buried regions current potential of trap resistance is raised, trap resistance is changed, in the evaluation procedure that buried regions current potential is included in trap resistance to the influence factor of trap resistance, trap resistance can more accurately be described.

Description

Description method of trap resistance
Technical Field
The invention relates to the field of semiconductor integrated circuit design, in particular to a well resistor description method.
Background
Analog circuit design requires not only high resistance accuracy, but also accurate resistance parameters to correctly describe resistance performance. At present, the evaluation of the trap resistance adopts a conventional resistance evaluation method, namely a two-end resistance method, the influence on a buried layer is neglected, and the resistance parameter extraction characterization formula is as follows:
R(V)=R0*(1+VC1*(n1n2)+VC2*(n1n2)2)
however, in practical circuit applications, a high potential is often required to be added to the buried layer, and different potentials loaded on the buried layer greatly affect the resistance of the well resistor. The buried layer potential is particularly important for extracting the voltage parameter of the conventional well resistor, and the accurate voltage dependency coefficient provides a more accurate well resistor for circuit application. Therefore, the introduction of the buried layer voltage dependency coefficient in the well resistance evaluation is the key point.
Disclosure of Invention
The invention aims to provide a well resistance description method, which can accurately calculate the well resistance.
In order to solve the above problems, the well resistor according to the present invention is described by the following formula:
wherein,
F1(V(n1,n2))=1+VC1*V(n1,n2)+VC2*V(n1,n2)2
F2(V(n2,n3))=1+VC3*V(n2,n3)+VC4*V(n2,n3)2
F3(V(n2,n3))=1+VC5*V(n2,n3)+VC6*V(n2,n3)2
F4(V(n2,n3))=1+VC7*V(n2,n3)+VC8*V(n2,n3)2
in the formula, V (n1, n2) represents the voltage between two nodes of n1 and n2, V (n2, n3) represents the voltage between two nodes of n2 and n3, L represents the resistance length, W represents the resistance width, dl represents the deviation of the resistance length caused by process errors, dw represents the deviation of the resistance width caused by process errors, R0 represents the resistance of a well resistor square, VC1 and VC2 are first-order and second-order voltage coefficients of a conventional well resistor, VC3 and VC4 are first-order and second-order voltage coefficients extracted by a buried layer voltage influencing the well resistor, VC5 and VC6 are first-order and second-order voltage coefficients influencing the well resistor length by the buried layer voltage raising, and VC7 and VC8 are first-order and second-order voltage coefficients influencing the well resistor width by the buried layer voltage raising; VC 1-VC 8 are trap resistance coefficients.
The trap resistivity extraction method comprises the following steps:
a) when the potential of the buried layer under the trap is 0 potential, extracting trap resistance coefficients dl, dw, VC1, VC2 and R0 through an R (V) calculation formula;
b) when the potential of a buried layer under a trap is raised, selecting trap resistance test values under 3-5 different buried layer voltages, selecting a trap resistor with the length and width both larger than 10 mu m, and removing the influence of 2dw and 2dl in an R (V) calculation formula through an R (V) calculation formula because the resistor width and the resistor length are large, and extracting trap resistance coefficients VC3 and VC 4;
c) selecting trap resistance test values of 3-5 different buried layer voltages, selecting a group of trap resistances with the same length and the width of more than 10 mu m and different widths through an R (V) calculation formula, and extracting trap resistance coefficients VC7 and VC 8;
d) selecting trap resistance test values of 3-5 different buried layer voltages, selecting a group of trap resistances with the same width and the length of more than 10 mu m and extracting trap resistance coefficients VC5 and VC6 through an R (V) calculation formula.
On the basis of conventional well resistance evaluation, the invention arranges the influence factors of the potential of the buried layer under the well on the well resistance into an evaluation system of the well resistance, so that the influence of the potential of the buried layer on the well resistance can be accurately calculated, and more accurate well resistance value is provided for circuit application.
Drawings
Fig. 1 is a schematic diagram of a P-well structure.
Detailed Description
The trap resistor is described by the following formula:
wherein,
F1(V(n1,n2))=1+VC1*V(n1,n2)+VC2*V(n1,n2)2
F2(V(n2,n3))=1+VC3*V(n2,n3)+VC4*V(n2,n3)2
F3(V(n2,n3))=1+VC5*V(n2,n3)+VC6*V(n2,n3)2
F4(V(n2,n3))=1+VC7*V(n2,n3)+VC8*V(n2,n3)2
in the formula, V (n1, n2) represents the voltage between two nodes of n1 and n2, V (n2, n3) represents the voltage between two nodes of n2 and n3, L represents the resistance length, W represents the resistance width, dl represents the deviation of the resistance length caused by process errors, dw represents the deviation of the resistance width caused by process errors, R0 represents the resistance of a well resistor square, VC1 and VC2 are first-order and second-order voltage coefficients of a conventional well resistor, VC3 and VC4 are first-order and second-order voltage coefficients extracted by a buried layer voltage influencing the well resistor, VC5 and VC6 are first-order and second-order voltage coefficients influencing the well resistor length by the buried layer voltage raising, and VC7 and VC8 are first-order and second-order voltage coefficients influencing the well resistor width by the buried layer voltage raising; VC 1-VC 8 are trap resistivity. The trap resistivity extraction method comprises the following steps:
a) when the potential of the buried layer under the trap is 0 potential, extracting trap resistance coefficients dl, dw, VC1, VC2 and R0 through an R (V) calculation formula;
b) when the potential of a buried layer under a trap is raised, selecting trap resistance test values under 3-5 different buried layer voltages, selecting trap resistances with the resistance length and width larger than 10 microns, such as trap resistances with W/L =20/20, and removing the influences of 2dw and 2dl in the R (V) calculation formula through an R (V) calculation formula due to the fact that the resistance width and length are large, and extracting trap resistance coefficients VC3 and VC 4;
c) selecting well resistance test values of 3-5 different buried layer voltages, selecting a group of well resistances with the same length and more than 10 μm and different widths, such as well resistances of W/L =0.2/20, W/L =1/20, W/L =2/20, W/L =5/20, W/L =10/20 and W/L =20/20, and extracting well resistance coefficients VC7 and VC8 by an R (V) calculation formula;
d) selecting well resistance test values of 3-5 different buried layer voltages, selecting a group of well resistances with the same width and larger than 10 mu m and different lengths, such as W/L =20/5, W/L =20/10 and W/L =20/20, and extracting well resistance coefficients VC5 and VC6 by an R (V) calculation formula.
The above description is a well resistance description method of the present invention, and is specifically described as follows with reference to an embodiment:
taking a P-type well resistor as an example, the structure of the P-type well resistor is shown in fig. 1, the P-type well and a P-type substrate are separated by an N-type epitaxial layer (N-EPI) and an N-type buried layer (NBL), two ends of the well resistor are respectively connected to two contact PADs (N1, N2), and simultaneously, the leading-out 1 end of the N-type buried layer is connected to 1 contact PAD (N3).
In the application of the analog circuit, different potentials are required to be applied to the buried layer end according to different application requirements. With the rising of the potential of the buried layer, a PN junction formed by the P well and the N type epitaxy enters a reverse bias state, a depletion region is formed at the PN junction, and the current path of the P well resistor is narrowed due to the widening of the depletion region at the side of the P well, so that the resistance value of the P well resistor is increased. The invention takes the influence factor of the buried layer potential on the trap resistance into consideration, and extracts the resistance parameters R0, VC 1-VC 8, dL and dW through the formula 1. The invention considers the influence of the potential of the buried layer on the voltage coefficient of the well resistor and the length and width dimensions of the well resistor.
In equation 1 above:
f1(V (n1, n2)) describes the well resistance voltage coefficient itself:
F1(V(n1,n2))=1+VC1*V(n1,n2)+VC2*V(n1,n2)2
f2(V (n2, n3)) describes the well voltage resistance coefficient introduced by the buried layer potential:
F2(V(n2,n3))=1+VC3*V(n2,n3)+VC4*V(n2,n3)2
f3(V (N2, N3)) describes the depletion of the PN junction of the P-well/N-type epitaxy due to the potential difference between the buried layer and the P-well, causing the variation of the well resistance length:
F3(V(n2,n3))=1+VC5*V(n2,n3)+VC6*V(n2,n3)2
f4(V (N2, N3)) describes the depletion of the PN junction of the P-well/N-type epitaxy due to the potential difference between the buried layer and the P-well, causing the variation of the well resistance width:
F4(V(n2,n3))=1+VC7*V(n2,n3)+VC8*V(n2,n3)2
the main extraction steps of the parameters of the trap resistance are as follows:
designing a set of well resistor structure arrays of different widths and lengths, as listed in the following table: (unit: μm)
W 20 10 5 2 1 0.5 20 20
L 20 20 20 20 20 20 10 5
When the N-type buried layer is at 0 potential, the well resistivity can be extracted by equation 1: dL, dW, VC1, VC2 and R0.
When the potential of the N-type buried layer is raised, well resistance test values when 3-5 different N-type buried layer voltages are selected, well resistance with a large size (W/L = 20/20) is selected and substituted into formula 1, and because the resistance width and the length are large, 2dW and 2dL influences can be removed at the moment, so that the well resistance coefficient can be extracted: VC3 and VC 4.
Selecting well resistance test values of 3-5 different N-type buried layer voltages, and extracting well resistance coefficients by using well resistances of a group of sizes of W/L =0.5/20, W/L =1/20, W/L =2/20, W/L =5/20, W/L =10/20 and W/L =20/20 according to formula 1: VC7 and VC 8.
Selecting trap resistance test values of 3-5 different NBL voltages, and extracting a trap resistance coefficient by using trap resistances of a group of sizes such as W/L =20/5, W/L =20/10 and W/L =20/20 according to formula 1: VC5 and VC 6.
In equation 1 above, in conjunction with FIG. 1:
n 1: a high potential end of a finger well resistor;
n 2: a low potential end of a finger well resistor;
n 3: a buried layer potential terminal;
l indicates the length of the resistor, W indicates the width of the resistor, and the unit is mum;
dl refers to the deviation of the resistance length caused by process errors, and dw refers to the deviation of the resistance width caused by process errors, and the unit is mum;
r0, which is the resistance of the trap resistor square with the unit of omega/□;
VC1, VC 2: the first-order and second-order voltage coefficients of the conventional trap resistor;
VC3, VC 4: the voltage of the buried layer influences the first-order and second-order voltage coefficients extracted by the well resistor;
VC5, VC 6: the first-order and second-order voltage coefficients which influence the length of the well resistor are raised by the voltage of the buried layer;
VC7, VC 8: the first order and second order voltage coefficients which affect the width of the trap resistor are raised by the buried layer voltage.
The above are merely preferred embodiments of the present invention, and are not intended to limit the present invention. Various modifications and alterations to this invention will become apparent to those skilled in the art. Any modification, equivalent replacement, or improvement made within the spirit and principle of the present invention should be included in the protection scope of the present invention.

Claims (2)

1. A method for describing well resistance, comprising: described using the following formula:
<mrow> <mi>R</mi> <mrow> <mo>(</mo> <mi>V</mi> <mo>)</mo> </mrow> <mo>=</mo> <mi>R</mi> <mn>0</mn> <mo>*</mo> <mi>F</mi> <mn>1</mn> <mrow> <mo>(</mo> <mi>V</mi> <mo>(</mo> <mrow> <mi>n</mi> <mn>1</mn> <mo>,</mo> <mi>n</mi> <mn>2</mn> </mrow> <mo>)</mo> <mo>)</mo> </mrow> <mo>*</mo> <mi>F</mi> <mn>2</mn> <mrow> <mo>(</mo> <mi>V</mi> <mo>(</mo> <mrow> <mi>n</mi> <mn>2</mn> <mo>,</mo> <mi>n</mi> <mn>3</mn> </mrow> <mo>)</mo> <mo>)</mo> </mrow> <mo>*</mo> <mfrac> <mrow> <mi>L</mi> <mo>-</mo> <mn>2</mn> <mi>d</mi> <mi>l</mi> <mo>*</mo> <mi>F</mi> <mn>3</mn> <mrow> <mo>(</mo> <mi>V</mi> <mo>(</mo> <mrow> <mi>n</mi> <mn>2</mn> <mo>,</mo> <mi>n</mi> <mn>3</mn> </mrow> <mo>)</mo> <mo>)</mo> </mrow> </mrow> <mrow> <mi>W</mi> <mo>-</mo> <mn>2</mn> <mi>d</mi> <mi>w</mi> <mo>*</mo> <mi>F</mi> <mn>4</mn> <mrow> <mo>(</mo> <mi>V</mi> <mo>(</mo> <mrow> <mi>n</mi> <mn>2</mn> <mo>,</mo> <mi>n</mi> <mn>3</mn> </mrow> <mo>)</mo> <mo>)</mo> </mrow> </mrow> </mfrac> </mrow>
wherein,
F1(V(n1,n2))=1+VC1*V(n1,n2)+VC2*V(n1,n2)2
F2(V(n2,n3))=1+VC3*V(n2,n3)+VC4*V(n2,n3)2
F3(V(n2,n3))=1+VC5*V(n2,n3)+VC6*V(n2,n3)2
F4(V(n2,n3))=1+VC7*V(n2,n3)+VC8*V(n2,n3)2
in the formula, V (n1, n2) represents the voltage between two nodes n1 and n2, and V (n2, n3) represents the voltage between two nodes n2 and n 3; n1 is a high potential end of a well resistor, n2 is a low potential end of the well resistor, and n3 is a buried potential end; l is the resistance length, W is the resistance width, dl is the resistance length deviation caused by process errors, dw is the resistance width deviation caused by process errors, R0 is the resistance value of a trap resistor square, VC1 and VC2 are first-order and second-order voltage coefficients of a conventional trap resistor, VC3 and VC4 are first-order and second-order voltage coefficients of a buried layer voltage influencing the extraction of the trap resistor, VC5 and VC6 are first-order and second-order voltage coefficients of the trap resistor length influenced by the buried layer voltage elevation, and VC7 and VC8 are first-order and second-order voltage coefficients of the trap resistor width influenced by the buried layer voltage elevation; VC 1-VC 8 are trap resistance coefficients.
2. The method for describing a well resistance according to claim 1, wherein: the trap resistivity extraction method comprises the following steps:
a) when the potential of the buried layer under the trap is 0 potential, extracting trap resistance coefficients dl, dw, VC1, VC2 and R0 through an R (V) calculation formula;
b) when the potential of a buried layer under a trap is raised, selecting trap resistance test values under 3-5 different buried layer voltages, selecting a trap resistor with the length and width both larger than 10 mu m, and removing the influence of 2dw and 2dl in an R (V) calculation formula through an R (V) calculation formula because the resistor width and the resistor length are large, and extracting trap resistance coefficients VC3 and VC 4;
c) selecting trap resistance test values of 3-5 different buried layer voltages, selecting a group of trap resistances with the same length and the width of more than 10 mu m and different widths through an R (V) calculation formula, and extracting trap resistance coefficients VC7 and VC 8;
d) selecting trap resistance test values of 3-5 different buried layer voltages, selecting a group of trap resistances with the same width and the length of more than 10 mu m and extracting trap resistance coefficients VC5 and VC6 through an R (V) calculation formula.
CN201310752999.0A 2013-12-31 2013-12-31 The description method of trap resistance Active CN104749511B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201310752999.0A CN104749511B (en) 2013-12-31 2013-12-31 The description method of trap resistance

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201310752999.0A CN104749511B (en) 2013-12-31 2013-12-31 The description method of trap resistance

Publications (2)

Publication Number Publication Date
CN104749511A CN104749511A (en) 2015-07-01
CN104749511B true CN104749511B (en) 2017-10-24

Family

ID=53589492

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201310752999.0A Active CN104749511B (en) 2013-12-31 2013-12-31 The description method of trap resistance

Country Status (1)

Country Link
CN (1) CN104749511B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110400791B (en) 2018-04-25 2021-12-10 华为技术有限公司 Polycrystalline silicon resistor

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1888926A (en) * 2005-06-29 2007-01-03 上海华虹Nec电子有限公司 Method for extracting N-trap electric resistance device voltage depending coefficient
CN101894177A (en) * 2010-06-08 2010-11-24 上海新进半导体制造有限公司 Method and system for establishing diffused resistor voltage coefficient extraction and simulation model
CN102521466A (en) * 2011-12-28 2012-06-27 上海新进半导体制造有限公司 Method and system for simulation of diffusion resistor

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6828632B2 (en) * 2002-07-18 2004-12-07 Micron Technology, Inc. Stable PD-SOI devices and methods
US20080140379A1 (en) * 2003-05-22 2008-06-12 Xoomsys, Inc. Approximations for simulations of systems
US7375000B2 (en) * 2005-08-22 2008-05-20 International Business Machines Corporation Discrete on-chip SOI resistors

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1888926A (en) * 2005-06-29 2007-01-03 上海华虹Nec电子有限公司 Method for extracting N-trap electric resistance device voltage depending coefficient
CN101894177A (en) * 2010-06-08 2010-11-24 上海新进半导体制造有限公司 Method and system for establishing diffused resistor voltage coefficient extraction and simulation model
CN102521466A (en) * 2011-12-28 2012-06-27 上海新进半导体制造有限公司 Method and system for simulation of diffusion resistor

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
CMOS模拟集成温度传感器的设计;钟灿;《中国优秀硕士学位论文全文数据库 信息科技辑》;20070715(第1期);22-23 *
电源芯片中CMOS带隙基准源与微调的设计与发现;李永红;《中国优秀硕士学位论文全文数据库 信息科技辑》;20051115(第7期);20-22 *
集成电路(IC)中电阻的设计;吕江平;《集成电路通讯》;20050930;第23卷(第3期);18-22 *
高压MOSFET的BSIM3 I-V模型研究与改进;任铮;《中国优秀硕士学位论文全文数据库 信息科技辑》;20061015(第10期);27-28 *

Also Published As

Publication number Publication date
CN104749511A (en) 2015-07-01

Similar Documents

Publication Publication Date Title
CN106558543B (en) Semiconductor structure of electrostatic discharge protection device and manufacturing method thereof
CN107679261B (en) Modeling method for parasitic resistance between source and drain of MOS device and substrate
CN103575998B (en) A kind of method for testing resistance without junction transistors
US9263438B2 (en) Apparatus related to a diode device including a JFET portion
CN101673728B (en) Model and method for measuring resistance of contact holes or through holes in bipolar transistor components
CN102693959B (en) Grid resistor test structure for MOS transistor
Pan et al. Understanding and modeling of diode voltage overshoots during fast transient ESD events
CN104377143B (en) A kind of method of test MOS device trap resistance
TW201250986A (en) Super-high-voltage resistor on silicon
US11948967B2 (en) Polysilicon resistor
CN104749511B (en) The description method of trap resistance
CN111435657B (en) Tracking temperature compensation for X/Y stress independent resistors
JP5512581B2 (en) Semiconductor device
US20120293191A1 (en) HVMOS Reliability Evaluation using Bulk Resistances as Indices
CN105989935B (en) Electrical resistor
US7982282B2 (en) High efficiency amplifier with reduced parasitic capacitance
CN112614824A (en) Resistance unit, high-precision resistor adopting same and sampling circuit
JP5945124B2 (en) Power circuit
CN106960802B (en) A kind of the test device and test method of semiconductor static electric current
EP2534690A1 (en) Systems and methods for a continuous-well decoupling capacitor
Khandelwal et al. ASM-ESD–A comprehensive physics-based compact model for ESD Diodes
US20170154949A1 (en) Diffused resistor
CN109376483B (en) LOD stress effect SPICE modeling method
JP6292929B2 (en) Semiconductor device, method of manufacturing the semiconductor device, and inspection method
CN111341834B (en) Test structure and semiconductor device

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant