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第四章 有限元素分析

4.8 封裝效應:類型二

本部分探討構裝體對於電晶體(類型二)之影響,首先比較電晶 體製程部分二維與三維模型之結果,在三維模型部分取兩個切面作為 比較,圖4-39 為兩切面之示意圖,圖 4-40、4-41 為 X 方向之應力比 較,圖 4-42、4-43 為 Y 方向之應力比較。比較兩切面之結果,可發 現切面二之應力梯度分布較近似於二維模型,因切面二位於正中央其 受外圍處材料改變之影響較小。

圖 4-39 切面示意圖

1

SIGE_TRANSISTOR OF SUB LEVEL FOUR ELEMENTS

MAT NUM

1

SIGE_TRANSISTOR OF SUB LEVEL FOUR ELEMENTS

MAT NUM

切面一 切面二

2D model 3D model cut plane 1

1

MX MN

SIGE_TRANSISTOR OF SUB LEVEL FOUR -2000

-1600 -1200

-800 -400

0 400

8001000 NODAL SOLUTION

STEP=8 SUB =6 TIME=8 SX (AVG) RSYS=0 DMX =.132E-04 SMN =-4952 SMX =1047

1

MNMX

SIGE_TRANSISTOR

-2000 -1600

-1200 -800

-400 0

400 800 NODAL SOLUTION

STEP=8 SUB =6 TIME=8

SMX =1060 SX (AVG) RSYS=0 DMX =.160E-04 SMN =-4917

1000

圖4-41 X 方向應力分布 (切面二)

圖4-42 Y 方向應力分布 (切面一)

圖4-43 Y 方向應力分布 (切面二)

1

MX MN

SIGE_TRANSISTOR OF SUB LEVEL FOUR -2000

-1600 -1200

-800 -400

0 400

800 1000 NODAL SOLUTION

STEP=8 SUB =6 TIME=8 SX (AVG) RSYS=0 DMX =.

SMN =-SMX =9

132E-04 4952 25.62

1

MNMX

SIGE_TRANSISTOR -2000

-1600 -1200

-800 -400

0 400

800 1000 NODAL SOLUTION

STEP=8 SUB =6 TIME=8

SMX =1060

2D model 3D model cut plane 2

3D model cut plane 1 2D model

SX (AVG) RSYS=0 DMX =.160E-04 SMN =-4917

1

MX MN

SIGE_TRANSISTOR -2000

-1600 -1200

-800 -400

0 400

800 1000 NODAL SOLUTION

STEP=8 SUB =6 TIME=8 SY (AVG) RSYS=0 DMX =.160E-04 SMN =-3084 SMX =1620 1

MN MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR -2000

-1600 -1200

-800 -400

0

400 1000

800 NODAL SOLUTION

STEP=8 SUB =6 TIME=8 SY (AVG) RSYS=0 DMX =.132E-04 SMN =-2423 SMX =2073

3D model cut plane 2 2D model

1

MX MN

SIGE_TRANSISTOR -2000

-1600 -1200

-800 -400

0 400

800 1000 NODAL SOLUTION

STEP=8 SUB =6 TIME=8 SY (AVG) RSYS=0 DMX =.160E-04 SMN =-3084 SMX =1620 1

MN MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR -2000

-1600 -1200

-800 -400

0 400

800 1000 NODAL SOLUTION

STEP=8 SUB =6 TIME=8 SY (AVG) RSYS=0 DMX =.132E-04 SMN =-2423 SMX =1627

接著考慮構裝體之封裝效應,依據前一章所述之構裝體全域模

圖 4-44 構裝體全域模型應力分布

型及各階層之次模型,將構裝體之效應加到電晶體上,兩效應相加的 部分則使用初始應力法,圖4-44 所示為構裝體全域模型三方向與 von Mises 之應力分布,圖 4-45~4-51 所示為第一層至第四層次模型三方 向與von Mises 之應力分布。

1 1

MN

MX X Y

Z

-129.664-105.045-80.427 -55.808-31.189

-6.571 18.048 42.667 67.286

91.904 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SX (AVG) RSYS=0 DMX =.279979 SMN =-129.664 SMX =91.904

NODAL SOLUTION STEP=2 SUB =1 TIME=2 SY (AVG) RSYS=0 DMX =.279979 SMN =-36.42 SMX =34.969

MN

MX X

Y Z

-36.42-28.488-20.556 -12.624-4.692

3.24 11.172 19.104 27.037

34.969

1

MN MX

X Y

Z

-129.033-104.438 -79.842

-55.246 -30.651

-6.055 18.541

43.137 67.732

92.328 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SZ (AVG) RSYS=0 DMX =.279979 SMN =-129.033 SMX =92.328

1

MN X MX Y

Z

.58098614.735 28.89

43.044 57.198

71.353 85.507

99.661 113.816 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SEQV (AVG) DMX =.279979 SMN =.580986 SMX =127.97

Sxx Syy

Szz von Mises stress

127.97

1

MN MX

-720.558-592.41 -464.261

-336.113 -207.964

-79.816 48.333

240.556 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SX (AVG) RSYS=0 DMX =.079084 SMN =-720.558 SMX =240.556

1

圖4-45 第一層次模型應力分布 (I)

圖4-46 第一層次模型應力分布 (II)

MN MX

-1819 -1515 -1210

-905.788 -601.279

-296.769 7.74

464.504 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SY (AVG) RSYS=0 DMX =.079084 SMN =-1819 SMX =464.504

1

-720.558-592.41 -464.261

-336.113 -207.964

-79.816 48.333 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SX (AVG) RSYS=0 DMX =.079084 SMN =-720.558 SMX =240.556

240.556

Sxx

1

-1819 -1515 -1210

-905.788 -601.279

-296.769 7.74 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SY (AVG) RSYS=0 DMX =.079084 SMN =-1819 SMX =464.504

464.504

Syy

1

MXMN

-717.516 -584.664

-451.811 -318.958

-186.105 -53.253

79.6 278.879 NODAL SOLUTION

STEP=2

DMX =.079084 SMN =-717.516 SMX =278.879 SUB =1 TIME=2 SZ (AVG) RSYS=0

1

MN MX

2.945 195.93

388.915 581.9

774.885 967.869

1161 1354

1450 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SEQV (AVG) DMX =.079084 SMN =2.945 SMX =1450

1

-717.516 -584.664

-451.811 -318.958

-186.105 -53.253

79.6 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SZ (AVG) RSYS=0 DMX =.079084 SMN =-717.516 SMX =278.879

278.879

Szz

von Mises stress

1

MX

2.945 195.93

388.915 581.9

774.885 967.869

1161 1354 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SEQV (AVG) DMX =.079084 SMN =2.945 SMX =1450

1450

圖 4-47 第二層次模型應力分布(I)

圖4-48 第二層次模型應力分布(II)

1

MN MX

-134.814-88.642 -42.47

3.701 49.873

96.045 142.217

211.474 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SX (AVG) RSYS=0 DMX =.078047 SMN =-134.814 SMX =211.474

1

MX MN

-17.577-12.371 -7.166

-1.96 3.246

8.452 13.658

21.466 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SY (AVG) RSYS=0 DMX =.078047 SMN =-17.577 SMX =21.466

1

MN

-134.814-88.642 -42.47

3.701 49.873

96.045 142.217

211.474 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SX (AVG) RSYS=0 DMX =.078047 SMN =-134.814 SMX =211.474

1

-17.577-12.371 -7.166

-1.96 3.246

8.452 13.658

21.466 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SY (AVG) RSYS=0 DMX =.078047 SMN =-17.577 SMX =21.466

Sxx

Syy

1 1

NODAL SOLUTION STEP=2 SUB =1

NODAL SOLUTION STEP=2 SUB =1 TIME=2

SZ (AVG) RSYS=0 DMX =.078047 SMN =-134.412 SMX =211.57

TIME=2 SZ (AVG) RSYS=0 DMX =.078047 SMN =-134.412 SMX =211.57

MN MX

-134.412 -88.281

-42.15 3.981

50.112 96.243

142.374 211.57

1

MN

MX

13.838 36.797

59.756 82.715

105.674 128.633

151.591 186.03 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SEQV (AVG) DMX =.078047 SMN =13.838 SMX =186.03

-134.412 -88.281

-42.15 3.981

50.112 96.243

142.374 211.57

1

13.838 36.797

59.756 82.715

105.674 128.633

151.591 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SEQV (AVG) DMX =.078047 SMN =13.838 SMX =186.03

Szz

von Mises stress

186.03

1

MN MX

-143.399 -102.882

-62.365 -21.847

18.67 59.187

99.704 160.48 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SX (AVG) RSYS=0 DMX =.077742 SMN =-143.399 SMX =160.48

1

MN

MX

-14.099 -13.062

-12.025 -10.989

-9.952 -8.915

-7.878 -6.322 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SY (AVG) RSYS=0 DMX =.077742 SMN =-14.099 SMX =-6.322

1

MN MX

-142.997 -102.563

-62.13 -21.696

18.738 59.171

99.605 160.255 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SZ (AVG) RSYS=0 DMX =.077742 SMN =-142.997 SMX =160.255

1

MN

MX

1.592 23.845

46.097 68.349

90.601 112.853

135.106 168.484 NODAL SOLUTION

STEP=2 SUB =1 TIME=2 SEQV (AVG) DMX =.077742 SMN =1.592 SMX =168.484

Sxx Syy

von Mises stress Szz

圖4-49 第三層次模型應力分布

1

MX MN

SIGE_TRANSISTOR OF SUB LEVEL FOUR -769.614

-658.567 -547.52

-436.473 -325.426

-214.378 -103.331

63.239 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SX (AVG) RSYS=0 DMX =.07767 SMN =-769.614 SMX =63.239

1

MN MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR -749.403

-634.403 -519.403

-404.404 -289.404

-174.404 -59.404

113.095 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SY (AVG) RSYS=0 DMX =.07767 SMN =-749.403 SMX =113.095

1

MN MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR -1052

-906.785 -762.033

-617.281 -472.529

-327.777 -183.026

34.102 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SZ (AVG) RSYS=0 DMX =.07767 SMN =-1052 SMX =34.102

1

MN

MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR 1.112

88.516 175.92

263.324 350.727

438.131 525.535

656.641 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SEQV (AVG) DMX =.07767 SMN =1.112 SMX =656.641

Sxx Syy

von Mises stress Szz

圖4-50 第四層次模型應力分布 (切面一)

1

MN MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR -768.909

-660.408 -551.907

-443.407 -334.906

-226.405 -117.905

44.846 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SX (AVG) RSYS=0 DMX =.07767 SMN =-768.909 SMX =44.846

1

MN MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR -749.403

-634.146 -518.889

-403.632 -288.375

-173.118 -57.861

115.024 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SY (AVG) RSYS=0 DMX =.07767 SMN =-749.403 SMX =115.024

1

MN MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR -1052

-904.457 -757.377

-610.297 -463.217

-316.137 -169.057

51.563 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SZ (AVG) RSYS=0 DMX =.07767 SMN =-1052 SMX =51.563

1

MN

MX

SIGE_TRANSISTOR OF SUB LEVEL FOUR 1.289

83.53 165.772

248.013 330.254

412.496 494.737

618.099 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SEQV (AVG) DMX =.07767 SMN =1.289 SMX =618.099

Sxx Syy

von Mises stress Szz

圖4 )

向約為 39.6%,在 Z 方向約為 128%,因此可知封裝效應對於電晶體 -51 第四層次模型應力分布 (切面二

兩效應合併之結果分別顯示於圖 4-52、4-53,最後取電晶體 Z 方向的通道應力值與二維模型比較,圖 4-54 為所取通道應力位置與 電晶體之 Z 方向示意圖。如圖 4-55 所示為製程所產生之應力比較,

圖4-56 所示為封裝效應所產生之應力比較,圖 4-57 所示為兩效應合 併之應力比較,圖4-58~4-60 所示為三方向之兩效應合併前後之應力 比較。由圖4-56 發現封裝效應在 X 以及 Z 方向對電晶體之通道應力 影響約為150MPa,Y 方向之影響約為~20MPa;觀察圖 4-58~4-60 中 可看出兩效應合併前後影響的程度,在 X 方向約為 50.8%,在 Y 方

1

MX MN

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200

-800 -400

0 400

8001000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SX (AVG) RSYS=0 DMX =.07767 SMN =-4502 SMX =987.845

1

MN

MX

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200

-800 -400

0 400

8001000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SY (AVG) RSYS=0 DMX =.07767 SMN =-2656 SMX =1990

1

MN MX

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200

-800 -400

0 400

8001000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SZ (AVG) RSYS=0 DMX =.07767 SMN =-2838 SMX =661.933

1

MN

MX

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200

-800 -400

0 400

8001000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SEQV (AVG) DMX =.07767 SMN =1.113 SMX =3851

Syy Sxx

Szz von Mises stress

圖4-52 兩效應合併之應力分布 (切面一)

1

MX MN

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200 -800 -400

0 400

8001000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SX (AVG) RSYS=0 DMX =.07767 SMN =-4569 SMX =876.368

1

MX MN

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200

-800 -400

0 400

8001000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SY (AVG) RSYS=0 DMX =.07767 SMN =-2656 SMX =1728

1

MN MX

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200

-800 -400

0 400

800 1000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SZ (AVG) RSYS=0 DMX =.07767 SMN =-2938 SMX =1376

1

MN

MX

PACKAGE STRESS ZOOM IN SIGE S/D MOSFET -2000

-1600 -1200

-800 -400

0 400

800 1000 NODAL SOLUTION

STEP=2 SUB =6 TIME=2 SEQV (AVG) DMX =.07767 SMN =1.289 SMX =3939

Sxx Syy

Szz von Mises stress

圖4-53 兩效應合併之應力分布 (切面二)

圖 4-54 通道應力位置示意圖

圖4-55 製程所產生之應力比較(2D&3D)

0 100 200 300 400 500 600 700 800 900 1000 Z (nm)

-400 -200 0 200 300 400 600 80

-300 -100 100 500 700 0

St ress ( MP a)

3D Cha nel_stress Sxx n 3D Channel_stress Syy 3D Channel_stress Szz 2D Channel_stress Sxx 2D Channel_stress Syy

1

z y

x

SIGE_TRANSISTOR

Channel Stress:along the direction Z

-200 -150 -100 -50 0 50 100

圖4-56 封裝效應所產生之應力比較

圖4-57 兩效應合併之應力比較

3D Channel_stress Sxx 3D Channel_stress Syy 3D Channel_stress Szz

)a re ss (MP St

0 100 200 300 400 500 600 700 800 900 1000 Z (nm)

0 100 200 300 400 500 600 700 800 900 1000 Z (nm)

-500 -400 -300 -200 -100 100 200 300 400 500 600

700 3D Channel_stress Sxx

3D Channel_stress Syy 3D Channel_stress Szz

)a

re ss ( M P St 0

圖4-58 比較

兩效應合併前後之 X 方向應力

4-59 兩效應合併前後之 Y 方向應力比較

~ 50.8%

0 100 200 300 400 500 600 700 800 900 1000 Z (nm)

-500 -400 -300 -200 -100 0 100

200 Process Channel_stress Sxx

Sum Channel_stress Sxx

) St ress (MP a

-300 -200 -100 0 100 200 300

400 Process Channel_stress Syy

Sum Channel_stress Syy

)

0 100 200 300 400 500 600 700 800 900 1000 Z (nm)

St ress (MP a

~ 39.6%

-400 -300 -200 -100 0 100 200 300 400 500 600 700 800

圖4-60 兩效應合併前後之 Z 方向應力比較

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