throbber
Ulllted States Patent [19]
`F0ng et al.
`
`US005939831A
`[11] Patent Number:
`[45] Date 0f Patent:
`
`5,939,831
`Aug. 17, 1999
`
`[54] METHODS AND APPARATUS FOR PRE-
`STABILIZED PLASMA GENERATION FOR
`
`5,273,609 12/1993 Moslehi ....................... .. 315/111.21 X
`5,282,899
`2/1994 Balmashnov et al. .
`118/723 R
`
`MICROWAVE CLEAN APPLICATIONS
`
`Inventors: Gary Fong, cupertino; Fong Chang,
`Los Gatos; Long Nguyen, Fremont, all
`of Calif.
`
`[73] Assignee: Applied Materials, Inc., Santa Clara,
`Calif
`
`5,403,434
`
`4/1995 Moslehi . . . . . . . . . . . . . . . . .
`
`. . . . .. 134/12
`
`.438/905 X
`5,468,686 11/1995 Kawamoto ..
`YaChl ................................ ..
`X
`FOREIGN PATENT DOCUMENTS
`
`4-199816
`7/1992 Japan .............................. .. 315/111.21
`Primary Examiner—R0bert Pascal
`Assistant Examiner—Justin P. Bettendorf
`Attorney, Agent, or Firm—ToWnsend & Townsend & CreW
`
`NOV‘ 13’ 1996
`[22] Flled:
`[51] Int. Cl? ...................................................... .. B08B 6/00
`[52] US. Cl. .................... .. 315/11121; 134/11; 438/714;
`438/905
`315/111 21. 438/714
`905:13’4/1 1 12’
`’
`i
`’
`'
`
`iiiiiiiiiiiii
`
`’
`
`[58] Field of Search
`
`The present invention provides systems, methods and appa
`rams for high temperature (at least about 50W800° C-)
`Processing of Semiconductor wafers- The Systems, methods
`and apparatus of the present invention alloW multiple pro
`cess steps to be performed in situ in the same chamber to
`reduce total processing time and to ensure high quality
`processing for high aspect ratio devices. Performing mul
`tiple process steps in the same chamber also increases the
`control of the process parameters and reduces device dam
`age. In particular, the present invention can provide high
`temperature deposition, heating and efficient cleaning for
`forming dielectric ?lms having thickness uniformity, good
`gap ?ll Capability, high density, 10W moisture, and other
`desired characteristics.
`
`20 Claims, 42 Drawing Sheets
`
`[56]
`
`References Cited
`
`U-S- PATENT DOCUMENTS
`204/165
`4 576 692 3/1986 Fukura et al
`iiiiiiiiiiiiii ":"i38/714 X
`475797623
`4/1986 Suzuki et a1:
`156/643
`4,872,947 10/1989 Wang et al.
`118/719
`4,951,601
`8/1990 Maydan e161. ..
`156/345
`5,082,517
`1/1992 Moslehi ......... ..
`5,266,364 11/1993 Tamura et al. ........................ .. 427/571
`
`150
`[ PROCESSOR H MEMORY
`
`70
`
`[
`
`— r
`OTHER J
`COMPONENTS -~
`
`65
`
`IO\
`
`43
`__~-
`
`51 1273
`
`GAS
`MlXlNG
`BLOCK
`
`I 4/
`'
`
`2B0
`
`REMOTE
`MICROWAVE
`L SM
`P A A
`SYSTEM
`
`55
`
`57
`
`-~
`
`65
`
`my“
`
`l\ \i
`
`

`
`s“ w 3 U 6
`
`a 0
`P \\ 6
`
`Hm /
`m // \\\ \
`
`7| \
`
`we m i u w 0/. /o_ \ A m a _ F. 5
`
`mm H. F \
`
`mm m X t c m \ \
`
`% Don _\I m8 JIM . \l\
`1 S m D
`n, M _ Lm _ M 01w \
`
`9 s _ ‘ _
`
`M M .W/ m \
`
`w M 0%. mm J \
`
`4 VI \
`
`1 M 1 nu . \
`
`
`
`.AhUU 5 2 GK OI. /
`
`5,939,831
`
`
`
`.m mmmm / Mummy
`
`5'!
`
`Ru 0 5 0
`
`BLAME \
`wAM /
`
`2
`
`h / o . ....w_
`
`6 ?mnou \o _l 5
`Pox]. 0| 2
`
`S n. J “
`
`2 FL
`
`M w 5 \
`
`FIG. IA.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 2 0f 42
`
`5,939,831
`
`EH
`
`\Illei \
`
`
`
`IIIHIQ/WI .
`
`F76‘. IB
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 3 of 42
`
`5,939,831
`
`28:35
`
`U\St
`
`zésmzg33
`
`_Ea:SE
`
`_22:9_32.22:35:35mm:
`
`8
`
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 4 0f 42
`
`5,939,831
`
`21 E
`
`528 SE28
`@2550 5E 52%
`
`.9 GR
`
`2K s1 2. a.
`
`
`
`as? 522; $225
`
`5225 @2533: me
`
`OB_\ 2.2 \
`
`
`
`
`
`522; 522.5 522% 5925
`
`
`
`5 \ 5052a :32:
`
`£85 525;:
`
`E 2: mg £02;
`
`255% 5225
`
`
`
`QT 505% E02:
`
`532 :2:
`
`
`
`358 :2: 5:8 55: 358 :22”: $528 3 E8: 5523
`
`
`
`
`
`2252;
`
`

`
`U.S. Patent
`
`Aug. 17, 1999
`
`Sheet 5 0f 42
`
`5,939,831
`
`RECEIVE DESIRED
`TEMPERATURE Tdes
`
`/ I67
`
`MEASURE CURRENT
`TEMPERATURE TIk)
`
`592 W
`
`$590
`
`TEMPERATURE
`REGULATOR
`ALGORITHM
`
`APPLY
`POWER PIk+I)
`
`,sae
`
`1588
`
`584
`/DIFFERENCE
`NO
`ETWEEN DESIRED
`-——-@0 CURRENT TEMPERA
`TURES EXCEEDS A PRE'
`DETERMINED BOUNDARY VALUE?
`YES
`DETERMINE DESIRED AND
`MEASURED RAMP RATES
`(T'desIk) &T'(k))
`
`I
`DETERMINE
`TEMPERATURE RAMP
`RATE ERROR
`
`DETERMINE POWER P(k+I)
`USING A CONTROL FUNCTION,
`IF PIk+I)-P(k) IS WITHIN
`SATURATION LIMITS
`
`I
`
`DAMPEN SYSTEM RESPONSE
`TO ADJUST PIk+I) USING A
`SATURATION FUNCTION IF
`P(k+l)-P(k) EXCEEDS
`SATURATION LIMITS
`
`FIG‘. IE.
`
`

`
`U.S. Patent
`
`Aug. 17, 1999
`
`Sheet 6 0f 42
`
`5,939,831
`
`233
`
`210*
`
`220 \i”
`
`l
`
`2l5
`
`219
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 7 0f 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 8 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 9 0f 42
`
`5,939,831
`
`$250
`
`FIG. 5.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 10 0f 42
`
`5,939,831
`
`I/ 225
`
`280
`
`210
`
`' ——-
`
`240
`
`4?
`
`O
`
`245
`
`FIG‘. 6A.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 11 0f 42
`
`5,939,831
`
`295
`
`320
`30|
`20
`
`500
`
`E,‘
`
`FIG. 68.
`
`F161 66‘.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 12 0f 42
`
`5,939,831
`
`FIG 7B.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 13 0f 42
`
`5,939,831
`
`FIG‘.
`
`8.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 14 of 42
`
`5,939,831
`
`30
`
`405
`
`493
`
`495
`
`440
`
`403
`
`25
`
`420
`
`20°
`
`'
`
`.
`
`
`
`455
`
`.
`
`Iii
`‘'2
`v .‘§I'——.—.l---lD_‘x.
`
`r
`'1-' '“n"'"'=fi
`3" gin
`
`n“}ik!‘
`E $‘ 4:3
`
`53:3
`39549:
`1'
`_ ‘ .
`597- 445
`7/-5
`\\
`:{aE ! 5.’./4
`475
`4n
`4l3_
`
`I‘:
`-I:
`
`
`"V
`{a.‘\I.:...I,g,I.I.%1s
`
`#2
`
`.
`
`l -'
`
`4.
`
`464
`
`5|!
`
`" [TV 466
`
`/
`
`409
`
`
`
`H
`
`m
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 15 0f 42
`
`5,939,831
`
`HUME Us |‘\\
`/// %
`\\mmtt“
`
`5 4 >
`
`32%
`\\\\\\\
`g 3
`Z
`
`1b 4
`/
`
`93
`
`455
`
`A / ////////w////
`
`\ \
`
`445
`
`465"
`
`I y
`
`r \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \\
`
`.V 1.
`
`/////////////////
`
`7
`
`464 /
`
`\\\
`
`503
`
`1 H6. 10.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 16 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 17 0f 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 18 0f 42
`
`5,939,831
`
`_\ \\\
`
`
`//_\\ \\\\
`_\\\\\\\
`
`\ \ \
`\ \ \ \
`
`\
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 19 0f 42
`
`5,939,831
`25 /
`
`\
`\
`\
`\
`
`\
`\
`
`/
`SOI/
`FIG /5A.
`
`FIG I58.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 20 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 21 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 22 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 23 of 42
`
`5,939,831
`
`FIG‘.
`
`/76‘.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 24 of 42
`
`5,939,831
`
`FIG.
`
`/70.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 25 of 42
`
`5,939,831
`
`F/G’.
`
`I6’.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 26 of 42
`
`5,939,831
`
`
`
`I006
`
`
`
`FIG?
`
`/96:
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 27 of 42
`
`5,939,831
`
`/IOIO
`
`I030
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 28 of 42
`
`5,939,831
`
`IIO4
`
`H02
`
`/
`
`H04
`
`n04
`
`H04
`
`H06
`
`H08
`
`H00
`
`F7; 203.
`
`l|02
`
`H08
`
`H00
`
`F/G 2061
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 29 of 42
`
`5,939,831
`
`uoz
`
`/ I
`
`IIO
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 30 of 42
`
`5,939,831
`
`/H02
`
`n04
`
`nos
`
`mo
`
`"04
`
`U99
`
`FIG 20/’.
`
`H04
`
`/1102
`"06
`
`mo
`
`"04
`
`H08
`
`F/6'. 206'.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 31 of 42
`
`5,939,831
`
`MICROWAVE CHAMBER P MONITOR
`
`0 N2=0
`o N2=500SCCM
`A N2=l0O0SCCM
`
`2600
`
`3300
`
`I800
`
`I400
`
`I000
`‘D0
`
`
`
`
`
`SATURATIONPOWER(W)
`
`5E
`BSG B WT. °/o AND CARRIER TYPE
`
`
`
`5..‘o;50.0‘o;i
`
`
`
`
`
`CARRIERCONCENTRATION(CM-3)
`
`-0- |.90|°/o-
`
`'0-4.694“/r
`
`-0~5.024°/o-
`
`—'-6.l3|“/o+
`'-V"5.l3|"/o"
`
`-+ 8.084°/o+
`
`'
`
`ooooooooooooooooooooooooooooooooooo -p
`
`IOI4 L‘.
`0.0
`
`0|
`
`0.5
`02
`DEPTH (um)
`
`04
`
`05
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 32 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 33 of 42
`
`5,939,831
`
`I025
`
`I022
`
`.02:
`
`Si -(l0N COUNTS)
`
`0--(ION COUNTS)
`
`[05
`
`104
`

`.73 I020

`
`1;
`
`E
`E Io”

`3
`
`mus
`
`In W
`
`I016
`
`o
`
`100
`
`200
`
`400
`300
`DEPTH (ANGSTROMS)
`
`500
`
`F/G. 228.
`
`DOSE or B= 4.59e|5 ATDMS/CM
`
`2
`
`E
`=
`105$
`9
`E
`E
`02 §
`
`1
`
`10'
`
`[00
`600
`
`
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 34 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 35 of 42
`
`5,939,831
`
`CARRIER
`CONCENTRATION
`(0:13)
`
` 0
`
`.2
`
`.25
`
`.3
`
`.05
`
`.I
`
`.I5
`
`DEPTH - MICRONS
`
`F/6‘. 23.4.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 36 of 42
`
`5,939,831
`
`1500
`
`NE»
`
`I200
`
`900
`
`S >
`
`,__:
`
`E 600
`
`E 300
`
`o8
`
`
`
`50
`
`900
`
`950
`RTP TEMPERATURE <°c)
`
`moo
`
`I050
`
`F/6. 230.
`
`102'
`3 I020
`5
`g .o|9
`E
`E-:- m‘3
`g
`H
`g 10
`
`E .016
`§ I015
`
`RTP TEMPERATURE
`(60 SEC ANNEAL)
`—<=—9oo°c
`-0- 950"C
`+ 975°C
`+ uooo°c
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 37 of 42
`
`5,939,831
`
`%0
`
`|‘\) $ $
`
`5 co
`
`5 o
`
`
`
`sumRESISTIVITY(11/cm?)
`
`B WT. %= 6.l5l
`
`3 wr.°/.= 6.15!
`
`.014
`o.o
`
`0.:
`
`0.2
`
`0.3
`
`0.4
`
`0.5
`
`DEPTH (um)
`
`F/6 236'.
`
`‘E
`
`E '
`
`32
`
`§ §
`
`

`
`U S Patent
`
`Aug. 17,1999
`
`Sheet 38 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 39 of 42
`
`5,939,831
`
`FIG. 24B.
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 40 of 42
`
`5,939,831
`
`
`
`
`
`canace.cam.cocmcommgcomeconcage
`
`
`
`mnymw.mu\pu‘
`
`._-=o.zwm==zm>«;
`
`8382
`._-:°.¢mm:=zu><;
`accmcommooo¢
`
`.a_:2.ESE.28...}
`
`.a:_8.E5?.5:11
`
`
`
`_s_=8.ma.525._1111
`
`.a:_8.E59.E.3«Inc:
`
`
`
`ms:55.s_:,a£<2.5.2
`
`‘’/o JONVHHOSHV
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 41 of 42
`
`5,939,831
`
`

`
`U.S. Patent
`
`Aug. 17,1999
`
`Sheet 42 of 42
`
`5,939,831
`
`so
`
`AT:oSN
`
`
`
`3§=s_§;fim.Gxh.
`
`838%2.:83
`
`.s:§:_.s§:2
`
`zozaomaSE.552
`
`zo:_8.§SE.5:
`
`2.3234.35&3<.zn
`
`) EONVHHOSBV
`
`

`
`1
`METHODS AND APPARATUS FOR PRE-
`STABILIZED PLASMA GENERATION FOR
`MICROWAVE CLEAN APPLICATIONS
`
`CROSS-REFERENCE TO RELATED
`APPLICATIONS
`
`This application is related to concurrently filed and com-
`monly assigned patent application Ser. No. 08/749,283 (filed
`Nov. 13, 1996) entitled “HEATER/LIFT ASSEMBLY FOR
`HIGH TEMPERATURE PROCESSING CHAMBER,” hav-
`ing Jonathan Frankel, Hari Ponnekanti, Inna Shmurun, and
`Visweswaren Sivaramakrishnan listed as co-inventors; and
`to concurrently filed and commonly assigned patent appli-
`cation Ser. No. 08/746,748 (filed Nov. 13, 1996) entitled
`“CHAMBER LINER FOR HIGH TEMPERATURE PRO-
`
`CESSING CHAMBER,” having Jonathan Frankel and
`Visweswaren Sivaramakrishnan listed as co-inventors; and
`to concurrently filed and commonly assigned patent appli-
`cation Ser. No. 08/747,830 (filed Nov. 13, 1996) entitled
`“SUBSTRATE PROCESSING APPARATUS WITH
`BOTTOM-MOUNTED REMOTE PLASMA SYSTEM,”
`having Gary Fong and Irwin Silvestre listed as co-inventors;
`and to concurrently filed and commonly assigned patent
`application Ser. No. 08/749,284 (filed Nov. 13, 1996)
`entitled “LIFT ASSEMBLY FOR HIGH TEMPERATURE
`
`PROCESSING CHAMBER,” having Jonathan Frankel
`listed as inventor; and to concurrently filed and commonly
`assigned patent application Ser. No. 08/749,286 (filed Nov.
`13, 1996) entitled “SYSTEMS AND METHODS FOR
`DETECTING END OF CHAMBER CLEAN IN ATHER-
`
`MAL (NONPLASMA) PROCESS,” having Visweswaren
`Sivaramakrishnan and Gary Fong listed as co-inventors; and
`to concurrently filed and commonly assigned patent appli-
`cation Ser. No. 08/749,925 (filed Nov. 13, 1996) entitled
`“LID ASSEMBLY FOR HIGH TEMPERATURE PRO-
`
`CESSING CHAMBER,” having Jonathan Frankel, Inna
`Shmurun, Visweswaren Sivaramakrishnan, and Eugene
`Fukshanski listed as co-inventors; and to concurrently filed
`and commonly assigned patent application Ser. No. 08/748,
`095 (filed Nov. 13, 1996) entitled “METHODS AND APPA-
`RATUS FOR CLEANING SURFACES IN ASUBSTRATE
`
`PROCESSING SYSTEM,” having Gary Fong, Li-Qun Xia,
`Srinivas Nemani, and Ellie Yieh listed as co-inventors; and
`to concurrently filed and commonly assigned patent appli-
`cation Ser. No. 08/747,982 (filed Nov. 13, 1996) entitled
`“METHODS AND APPARATUS FOR GETTERING
`FLUORINE FROM CHAMBER MATERIAL
`
`SURFACES,” having Li-Qun Xia, Visweswaren
`Sivaramakrishnan, Srinivas Nemani, Ellie Yieh, and Gary
`Fong listed as co-inventors; and to concurrently filed and
`commonly assigned patent application Ser. No. 08/748,960
`(filed Nov. 13, 1996) entitled “METHODS AND APPARA-
`TUS FOR DEPOSITING PREMETAL DIELECTRIC
`LAYER AT SUB-ATMOSPHERIC AND HIGH TEM-
`
`PERATURE CONDITIONS,” having Li-Qun Xia, Ellie
`Yieh, and Srinivas Nemani listed as co-inventors; and to
`concurrently filed and commonly assigned patent applica-
`tion Ser. No. 08/746,631 (filed Nov. 13, 1996) entitled
`“METHODS AND APPARATUS FOR SHALLOW
`
`TRENCH ISOLATION,” having Ellie Yieh, Li-Qun Xia,
`and Srinivas Nemani listed as co-inventors; and to concur-
`rently filed and commonly assigned patent application Ser.
`No. 08/746,657 (filed Nov. 13, 1996) entitled “SYSTEMS
`AND METHODS FOR CONTROLLING THE TEMPERA-
`
`TURE OF AVAPOR DEPOSITION APPARATUS,” having
`Jonathan Frankel listed as inventor; and to concurrently filed
`and commonly assigned patent application Ser. No. 08/748,
`
`10
`
`15
`
`20
`
`25
`
`30
`
`35
`
`40
`
`45
`
`50
`
`55
`
`60
`
`65
`
`5,939,831
`
`2
`
`883 (filed Nov. 13, 1996) entitled “SYSTEMS AND METH-
`ODS FOR HIGH TEMPERATURE PROCESSING OF
`
`SEMICONDUCTOR WAFERS,” having Visweswaren
`Sivaramakrishnan, Ellie Yieh, Jonathan Frankel, Li-Qun
`Xia, Gary Fong, Srinivas Nemani, Irwin Silvestre, Inna
`Shmurun, and Tim Levine listed as co-inventors; and to
`concurrently filed and commonly assigned patent applica-
`tion Ser. No. 08/748,094 (filed Nov. 13, 1996) entitled
`“METHOD AND APPARATUS FOR FORMING ULTRA-
`SHALLOW DOPED REGIONS USING DOPED SILICON
`
`OXIDE FILMS,” having Ellie Yieh, Li-Qun Xia, Paul Gee,
`and Bang Nguyen listed as co-inventors. Each of the above
`referenced applications are assigned to Applied Materials
`Inc., the assignee of the present invention, and each of the
`above referenced applications are hereby incorporated by
`reference.
`
`BACKGROUND OF THE INVENTION
`
`The present invention relates to semiconductor process-
`ing. More specifically, the invention relates to a method and
`apparatus for forming dielectric films over high aspect ratio
`features at temperatures greater than about 500° C., with the
`dielectric films having low moisture content and low shrink-
`age. Embodiments of the present invention are particularly
`useful to deposit doped dielectric films, such as borophos-
`phosilicate glass (BPSG) films, borosilicate glass (BSG)
`films, or phosphosilicate glass (PSG) films, and to form
`ultra-shallow doped regions used, for example, as source/
`drain junctions or as channel stop diffusions in shallow
`trench isolation. In addition, embodiments of the present
`invention may also be used to deposit doped dielectric films
`used as premetal dielectric (PMD) layers, intermetal dielec-
`tric (IMD) layers, or other dielectric layers. Further embodi-
`ments of the present invention may further be used to deposit
`undoped dielectric films, such as undoped silicate glass
`(USG) films used as shallow trench isolation filling oxides,
`insulating layers, capping layers, or other layers.
`One of the primary steps in fabricating modem semicon-
`ductor devices is forming a dielectric layer on a semicon-
`ductor substrate. As is well known, such a dielectric layer
`can be deposited by chemical vapor deposition (CVD). In a
`conventional thermal CVD process, reactive gases are sup-
`plied to the substrate surface where heat-induced chemical
`reactions (homogeneous or heterogeneous) take place to
`produce a desired film. In a conventional plasma process, a
`controlled plasma is formed to decompose and/or energize
`reactive species to produce the desired film. In general,
`reaction rates in thermal and plasma processes may be
`controlled by controlling one or more of the following:
`temperature, pressure, and reactant gas flow rate.
`Semiconductor device geometries have dramatically
`decreased in size since such devices were first introduced
`
`several decades ago. Since then, integrated circuits have
`generally followed the two-year/half-size rule (often called
`“Moore’s Law”) which means that the number of devices
`which will fit on a chip doubles every two years. Today’s
`wafer fabrication plants are routinely producing 0.5 pm and
`even 0.35 pm feature size devices, and tomorrow’s plants
`soon will be producing devices having even smaller feature
`sizes. As device feature sizes become smaller and integration
`density increases, issues not previously considered crucial
`by the industry are becoming of greater concern.
`In
`particular, devices with increasingly high integration density
`have features with high (for example, greater than about 3:1
`or 4:1) aspect ratios. (Aspect ratio is defined as the height-
`to-spacing ratio of two adjacent steps.)
`Increasingly stringent requirements for processes in fab-
`ricating these high integration devices are needed in order to
`
`

`
`5,939,831
`
`3
`produce high quality devices, and conventional substrate
`processing systems are becoming inadequate to meeting
`these requirements. One requirement is that the dielectric
`films formed in the process of fabricating such devices need
`to be uniformly deposited over these high aspect ratio
`features without leaving substantial gaps or voids. Another
`requirement is that these films need to exhibit low shrinkage
`so that subsequent heating and/or wet etching steps do not
`cause voids to open up in the deposited film. However,
`conventional substrate processing systems that
`typically
`deposit dielectric films at temperatures less than about 450°
`C. are unable to produce low moisture films having good
`gap-filling capabilities without opening substantial voids in
`subsequent heating and/or wet etching steps. As is well
`known, these gaps or voids may contribute to device per-
`formance unreliability and other problems. Dielectric films
`used, for example, as PMD or IMD layers in such devices
`need good high aspect ratio gap-fill capability to avoid
`problems caused by these gaps or voids. A further require-
`ment is that metal contamination into the wafer during the
`processing steps be minimized to avoid short circuits and
`other problems in the devices. As is well known, conven-
`tional substrate processing systems using in situ plasma
`during processing experience physical sputtering of ions
`which attack chamber surfaces, such as aluminum walls,
`resulting in metal contamination of the substrate. Use of in
`situ plasma is therefore undesirable. An improved substrate
`processing system, which does not use in situ plasma, is
`needed to provide dielectric films with the desired charac-
`teristics of low moisture, high density, low shrinkage, good
`high aspect ratio gap-filling capability.
`In addition to meeting these stringent requirements, sub-
`strate processing systems must be able to meet the higher
`demands for forming ultra-shallow doped regions, which are
`necessary for high integration devices with shrinking device
`geometries. With the advent of smaller device geometries,
`ultra-shallow doped regions in semiconductors are needed
`for various applications including, for example, source/drain
`junctions, channel stop diffusions for shallow trench
`isolation, etc. For example, MOS devices with channel
`lengths of less than 0.8 gm often require source/drain
`junctions having depths less than about 250 nanometers
`(nm) for adequate device performance. For transistors sepa-
`rated by trench isolation structures of about 0.35 pm depth,
`ultra-shallow channel stop regions having a depth on the
`order of hundreds of nm are usually required. For applica-
`tions requiring ultra-shallow doped regions, it is important
`to provide uniform dopant distribution in the doped regions
`and good control of junction depth.
`Current approaches to forming ultra-shallow doped
`regions, such as ion implantation and gaseous diffusion, are
`inadequate in some applications. With these current
`approaches, the ability to control dopant distribution and
`junction depth is limited, especially as the doped regions
`become shallower. With an approach like ion implantation,
`controlling dopant distribution is made difficult due to the
`built-up concentration of ions at the surface of the semicon-
`ductor material. Also, ion implantation causes damage to the
`semiconductor surface, and methods for repairing this sub-
`strate damage often make it more difficult to control dopant
`distribution and junction depth for ultra-shallow doped
`regions. For example, ions bombarded at relatively high
`energy levels have a tendency to tunnel or channel through
`the semiconductor material and cause damage such as point
`defects. These point defects, which may lead to irregular and
`nonuniform junction depths, may be fixed by annealing the
`implanted semiconductor material at high temperatures
`
`10
`
`15
`
`20
`
`25
`
`30
`
`35
`
`40
`
`45
`
`50
`
`55
`
`60
`
`65
`
`4
`
`(greater than about 900° C.). Annealing the implanted semi-
`conductor material, however, may further increase the junc-
`tion depth beyond that desired. With an approach like
`gaseous diffusion, controlling dopant distribution and junc-
`tion depth is difficult to control in forming ultra-shallow
`doped regions. As technology progresses to even smaller
`geometry devices, an alternative approach that is able to
`control the dopant uniformity and junction depth in ultra-
`shallow doped regions is needed.
`In forming ultra-shallow doped regions, one alternative
`approach to the current approaches of ion implantation and
`gaseous diffusion is the use of a doped dielectric film as a
`dopant diffusion source.
`In this alternative approach, a
`doped dielectric film is deposited onto a substrate and used
`as a source of dopants which are diffused into the substrate
`to form ultra-shallow doped regions. For example, doped
`dielectric films are deposited at temperatures less than 500°
`C.
`in a deposition chamber, and subsequently heated at
`temperatures greater than 500° C. in a different chamber,
`such as an annealing furnace, to perform the dopant diffu-
`sion to form the doped region. Controlling thickness,
`uniformity, and moisture content of the doped dielectric film
`is important in efficiently forming ultra-shallow doped junc-
`tions in the semiconductor material. Specifically, controlling
`the thickness and uniformity of the deposited doped dielec-
`tric film provides some control over the amount of dopants
`available for diffusion. Limiting the thickness of doped
`dielectric films used as diffusion sources also helps to
`increase wafer throughput by saving deposition (and subse-
`quent etching) time. Moreover, a uniformly deposited film
`with even dopant uniformity can provide a more controlled
`diffusion of dopants from the film into the substrate. As is
`well known, moisture in doped dielectric films reacts with
`dopants to bind them in a crystal structure, resulting in fewer
`dopants available for diffusion into the substrate to form
`doped regions. It is desirable to use doped dielectric films
`having a low moisture content, since these films have more
`dopants available for use in the diffusion.
`Several problems are encountered with conventional sub-
`strate processing systems when using a doped dielectric film
`as a dopant diffusion source. One problem is that
`it
`is
`difficult to obtain a high degree of control over film thick-
`ness and uniformity when using conventional systems to
`deposit the doped dielectric film. Another problem is that it
`is often difficult to ensure that adequate amounts of dopants
`in the doped dielectric film are available for diffusion into
`the substrate to form the ultra-shallow doped regions. A
`further problem is the existence of native oxides, which act
`as a barrier layer preventing dopants from diffusing into the
`substrate from the doped dielectric film, on substrate sur-
`faces where the ultra-shallow doped regions are to be
`formed. These problems are discussed in further detail
`below.
`
`Despite the advantages of using doped dielectric films as
`dopant diffusion sources to form ultra-shallow doped
`regions, the problem of being unable to control thickness
`and uniformity of the deposited doped dielectric film when
`using conventional deposition systems is of particular con-
`cern for two primary reasons. First,
`the inability to
`adequately control thickness and uniformity of the deposited
`doped dielectric film using conventional methods and appa-
`ratus undesirably results in a diminished ability to control
`the dopant uniformity and junction depth of the ultra-
`shallow doped region formed. For example, in a conven-
`tional sequential CVD chamber, a substrate rests on a belt
`and travels through various portions of the chamber. In each
`portion of the chamber, a layer having a certain thickness
`
`

`
`5,939,831
`
`5
`may be deposited. Thickness of the deposited film may be
`controlled by changing the belt speed, which provides
`limited control. Further, control over the thickness and
`dopant uniformity of the films deposited on different wafers
`is difficult when attempting to control film thickness and
`dopant concentration using belt speed. That is, the thick-
`nesses of the deposited films on different wafers may vary
`and be unpredictable, leading to wafer-to-wafer unreliabil-
`ity. Second, being able to control
`the thickness of the
`deposited doped dielectric film, even for very thin films, is
`desirable for overall efficiency and increased wafer through-
`put. However, conventional approaches have only been
`capable of forming doped dielectric films with thicknesses
`on the order of thousands of Angstroms
`Also, it may be
`difficult to maintain the thickness of the deposited film as
`thin as possible using systems relying on belt speed to
`control thickness of the deposited film. With thicker films
`deposited conventionally, some dopants may take longer to
`diffuse into the substrate, since they have greater distances
`to travel before reaching the semiconductor material. Also,
`removal of such a thick film used as a dopant diffusion
`source by etching or other technique often increases the total
`time to process the wafer. With growing pressures on
`manufacturers to improve efficiency, it is desirable to form
`the doped dielectric film as thin as possible in order to
`decrease the time needed to deposit and then remove the
`film. It is desirable to have a method and apparatus that can
`easily control the thickness and dopant uniformity of a
`doped dielectric film (less than about 500 A thick at 10.2
`weight percentage dopant variation across the wafer) that is
`used as a dopant diffusion source.
`Another problem with using doped dielectric films as
`dopant diffusion sources for ultra-shallow doped regions is
`that adequate amounts of dopants must be available for
`diffusion into the substrate. Films with high dopant concen-
`tration are often needed to provide adequate amounts of
`dopants for uniform diffusion into the substrate to form
`ultra-shallow junctions. However, moisture absorption and
`outgassing are two problems relating to adequate dopant
`availability. Doped dielectric films, especially those with
`high dopant concentrations, tend to absorb moisture shortly
`after a wafer is exposed to ambient moisture in a clean room
`(e.g. when the wafer is transferred from the deposition
`chamber after deposition of the doped dielectric film to a
`different processing chamber for the next processing step in
`a multiple-step process). The absorbed moisture (H20) then
`reacts with the dopants in the dielectric film, causing the film
`to crystallize. Due to the crystal structure binding the
`dopants within the film, these dopants become unavailable
`for diffusion into the substrate, even after a subsequent
`heating of the wafer by rapid thermal processing or anneal-
`ing in another chamber. Moisture absorption thus reduces
`the amount of dopants for diffusion into the substrate. In
`addition to the moisture absorption problem, outgassing of
`dopants from the doped dielectric film also may occur in
`subsequent heating steps. These dopants diffuse out of the
`film away from the substrate, resulting in fewer dopants
`available to be diffused into the substrate to form ultra-
`
`shallow doped regions.
`Even if adequate dopants are available for diffusion, the
`problem of native oxides remains an important consideration
`when using doped dielectric films as diffusion sources.
`Native oxides existing on the substrate surface where ultra-
`shallow doped regions are to be formed prevent effective and
`uniform dopant diffusion into the silicon. Therefore, native
`oxides, which act as a diffusion barrier layer to the dopants,
`need to be removed. Removing native oxides has been done
`
`10
`
`15
`
`20
`
`25
`
`30
`
`35
`
`40
`
`45
`
`50
`
`55
`
`60
`
`65
`
`6
`using conventional techniques such as wet etching using
`liquid etchants, and dry etching using an in situ plasma.
`However, using liquid etchants is often difficult to control
`and may result in overetching the substrate. Substrates that
`have native oxides cleaned by conventional methods such as
`wet etching have shelf lives of less than about one week
`before native oxides begin to form again, making it desirable
`to process the wafers shortly after the native oxides have
`been removed. Using dry etching to remove native oxides
`with an in situ plasma results in plasma damage to the
`surface of the substrate.
`In addition to causing surface
`plasma damage, in situ plasma dry etching may undesirably
`result in more metal contamination, as discussed earlier.
`Accordingly,
`it is important to efficiently remove native
`oxides without damaging the substrate surface so dopants
`may diffuse into the substrate uniformly for ultra-shallow
`doped regions.
`In addition to providing dense, low moisture dielectric
`films having uniform thickness and high aspect ratio gap-
`filling capability with low metal contamination, improved
`quality and overall efficiency in fabricating integrated circuit
`devices is also important. An important way to improve
`quality and overall efficiency in fabricating devices is to
`clean the chamber effectively and economically. With grow-
`ing pressures on manufacturers to improve processing qual-
`ity and overall efficiency, eliminating the total down-time in
`a multiple-step process without compromising the quality of
`the wafers has become increasingly important for saving
`both time and money. During CVD processing, reactive
`gases released inside the processing chamber form layers
`such as silicon oxides or nitrides on the surface of a substrate
`
`being processed. Undesirable oxide deposition occurs else-
`where in the CVD apparatus, such as in the area between the
`gas mixing box and gas distribution manifold. Undesired
`oxide residues also may be deposited in or around the
`exhaust channel and the walls of the processing chamber
`during such CVD processes. Over time, failure to clean the
`residue from the CVD apparatus often results in degraded,
`unreliable processes and defective substrates. Without fre-
`quent cleaning procedures, impurities from the residue built
`up in the CVD apparatus can migrate onto the substrate. The
`problem of impurities causing damage to the devices on the
`substrate is of particular concern with today’s increasingly
`small device dimensions. Thus, CVD system maintenance is
`important for the smooth operation of substrate processing,
`as well as resulting in improved device yield and better
`product performance.
`Frequently, periodic chamber cleanings between process-
`ing of every N wafers is needed to improve CVD system
`performance in producing high quality devices. Providing an
`efficient, non-damaging clean of the chamber and/or sub-
`strate is often able to enhance performance and quality of the
`devices produced. In addition to improving the quality of the
`above-discussed chamber cleanings (which are done without
`breaking the vacuum seal), preventive maintenance chamber
`cleanings (where the vacuum seal is broken by opening the
`chamber lid to physically wipe down the chamber) are
`performed between multiple periodic chamber cleanings.
`Often, performing the necessary preventive maintenance
`chamber cleanings involves opening the chamber lid and
`any other chamber parts that might obstruct the lid, which is
`a time-consuming procedure that
`interferes with normal
`production processing.
`In light of the above, improved methods, systems and
`apparatus are needed for depositing dense, low moisture
`dielectric films with uniform thicknesses and high aspect
`ratio gap-filling capabilities. Optimally,
`these improved
`
`

`
`5,939,831
`
`7
`methods and apparatus will also provide a chamber clean
`with low metal contamination. Improved methods and appa-
`ratus are also needed for forming doped dielectric films as
`dopant diffusion sources for ultra-shallow junctions. These
`methods and apparatus should be capable of efficiently
`removing native oxides to ensure effective and uniform
`dopant diffusion from the doped dielectric layer without
`causing significant surface damage to the silicon wafer.
`Further, for some applications it
`is desirable to provide
`multiple deposition and cleaning capabilities in a single
`chamber with a simplified design to minimize the time
`consumed for different types of cleanings. What is needed,
`therefore, are systems and methods that are capable of high
`quality, efficient, high temperature deposition and efficient,
`gentle cleaning. In particular, these systems and methods
`should be designed to be compatible with processing
`requirements for forming devices with high aspect ratio
`features, and for forming ultra-shallow doped regions.
`SUMMARY OF THE INVENTION
`
`The present invention provides systems, methods and
`apparatus for high temperature (at least about 500—800° C.)
`processing of semiconductor wafers. Embodiments of the
`present invention in

This document is available on Docket Alarm but you must sign up to view it.


Or .

Accessing this document will incur an additional charge of $.

After purchase, you can access this document again without charge.

Accept $ Charge
throbber

Still Working On It

This document is taking longer than usual to download. This can happen if we need to contact the court directly to obtain the document and their servers are running slowly.

Give it another minute or two to complete, and then try the refresh button.

throbber

A few More Minutes ... Still Working

It can take up to 5 minutes for us to download a document if the court servers are running slowly.

Thank you for your continued patience.

This document could not be displayed.

We could not find this document within its docket. Please go back to the docket page and check the link. If that does not work, go back to the docket and refresh it to pull the newest information.

Your account does not support viewing this document.

You need a Paid Account to view this document. Click here to change your account type.

Your account does not support viewing this document.

Set your membership status to view this document.

With a Docket Alarm membership, you'll get a whole lot more, including:

  • Up-to-date information for this case.
  • Email alerts whenever there is an update.
  • Full text search for other cases.
  • Get email alerts whenever a new case matches your search.

Become a Member

One Moment Please

The filing “” is large (MB) and is being downloaded.

Please refresh this page in a few minutes to see if the filing has been downloaded. The filing will also be emailed to you when the download completes.

Your document is on its way!

If you do not receive the document in five minutes, contact support at support@docketalarm.com.

Sealed Document

We are unable to display this document, it may be under a court ordered seal.

If you have proper credentials to access the file, you may proceed directly to the court's system using your government issued username and password.


Access Government Site

We are redirecting you
to a mobile optimized page.





Document Unreadable or Corrupt

Refresh this Document
Go to the Docket

We are unable to display this document.

Refresh this Document
Go to the Docket