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Har

vard

Uni

vers

ity

New

Pre

curs

ors

for A

LD

of H

igh-

k D

iele

ctric

s

Roy

G. G

ordo

n,Je

an-S

ébas

tien

Lehn

, Yiq

unLi

u,

Kyo

ung

H. K

im, Z

heng

wen

Li a

nd M

icha

el C

oulte

rH

arva

rd U

nive

rsity

Cam

brid

ge, M

A

Hua

zhiL

i, R

alph

Pug

h an

d D

eoSh

enai

Roh

m a

nd H

aas

Com

pany

Nor

th A

ndov

er, M

A

Har

vard

Uni

vers

ity

ALD

HfO

2fr

om s

tabl

e H

fam

idin

ate

prec

urso

rs

Stab

le, a

mor

phou

s hi

gh-k

die

lect

rics

=> L

aLuO

3ha

s th

e be

st p

rope

rtie

s

Vola

tile

Prec

urso

rs fo

r Lan

than

um O

xide

ALD

of L

a 2O

3an

d La

AlO

3

Vola

tile

Prec

urso

rs fo

r Lut

etiu

m O

xide

Out

line

Har

vard

Uni

vers

ity

Hig

h-k

HfO

2or

ZrO

2w

ith v

ery

low

ele

ctric

al le

akag

e ne

eded

Why

Mor

e St

able

Hfa

nd Z

rPre

curs

ors?

Car

bon

impu

rity

in fi

lms

incr

ease

s le

akag

e

Ther

mal

dec

ompo

sitio

n of

org

anic

pre

curs

ors

adds

C to

film

s

Ther

mal

dec

ompo

sitio

n de

stro

ys u

nifo

rmity

and

con

form

ality

Dep

ositi

on T

~ 3

50 o C

nee

ded

for H

fAlO

xw

ith A

LD A

l 2O3

Hfa

lkyl

amid

epr

ecur

sors

dec

ompo

se to

o qu

ickl

y at

350

o C

Har

vard

Uni

vers

ity

Haf

nium

tetr

akis

(N,N

’-dim

ethy

lform

amid

inat

e)

Neg

ligib

le re

sidu

e af

ter T

G

CH

3

N

NC

H3

H

H3C

N

N CH

3H

CH

3N

N CH

3H

CH

3

N

NH

3C

H

Hf

=> S

uffic

ient

vol

atili

ty a

nd th

erm

al s

tabi

lity

for A

LD

TG d

ata

for

Hf(M

e 2-fm

d)4

Tem

pera

ture

(oC

)

Remaining mass (%)

187

o C

Har

vard

Uni

vers

ityHaf

nium

Am

idin

ates

CH

3

N

NC

H3

R

H3C

N

N CH

3R

CH

3N

N CH

3R

CH

3

N

NH

3C

R

Hf

bmd

pmd

amd

fmd

187

141

H

246

<20

CH

2CH

2CH

3

251

80C

H2C

H3

221

171

CH

3

TG T

½o C

Mel

ting

Poi

nt,o

CR

R =

CH

2CH

2CH

3(p

ropy

l) is

a li

quid

Hfp

recu

rsor

20 o C

R =

H is

the

mos

t vol

atile

; liq

uid

in b

ubbl

er >

141

o CSo

lid a

t 20

o C, s

olub

le fo

r use

in d

irect

liqu

id in

ject

ion

Har

vard

Uni

vers

ity

Ther

mal

Sta

bilit

y of

Hfa

nd Z

rPre

curs

ors

No

deco

mpo

sitio

n of

Hf

or Z

ram

idin

ates

dur

ing

1000

hou

rs a

t 200

o C:

Hfa

nd Z

ram

ides

com

plet

ely

deco

mpo

sed

in a

few

hou

rs

at 2

00 o C

:

Prec

urso

rs d

isso

lved

in m

esity

lene

-d12

, hea

ted,

an

d N

MR

spe

ctra

take

n pe

riodi

cally

020406080100

120

02

46

810

1214

Tim

e (h

)

% of complex remaining

Zr(N

Me2

)4Zr

(NEt

2)4

Hf(N

Me2

)4H

f(NM

eEt)4

020406080100

120

020

040

060

080

010

00Ti

me

(h)

% of complex remainingZr

(MM

M)4

Hf(M

MM

)4

Hf(M

EM)4

Zr(M

e 2-a

md)

4H

f(Me 2

-am

d)4

Hf(M

e 2-p

md)

4

Har

vard

Uni

vers

ity

Ther

mal

Sta

bilit

y of

Hfa

nd Z

rAm

idin

ates

No

deco

mpo

sitio

n du

ring

140

hour

s at

250

o CD

ecom

posi

tion

afte

r ~2

00 h

ours

at 2

80 o C

=> H

fand

Zra

mid

inat

es m

uch

mor

e st

able

than

am

ides

020406080100

120

050

100

150

200

250

300

350

Tim

e (h

)

% of complex remaining

Zr(M

MM

)4

Hf(M

MM

)4

020406080100

120

020

4060

8010

012

014

0Ti

me

(h)

% of complex remaining

Zr(M

MM

)4

Hf(M

MM

)4

Zr(M

e 2-a

md)

4H

f(Me 2

-am

d)4

Zr(M

e 2-a

md)

4H

f(Me 2

-am

d)4

Har

vard

Uni

vers

ity

Vapo

rizat

ion

Rat

es o

f Haf

nium

Am

idin

ates

Hig

hest

rate

with

Hft

etra

kis(

N,N

’-dim

ethy

lform

amid

inat

e)

=> H

igh

evap

orat

ion

rate

s fr

om th

erm

ally

sta

ble

liqui

ds

Har

vard

Uni

vers

ity

ALD

of H

fO2

from

Am

idin

ate

Prec

urso

rs

ALD

Con

ditio

ns

Typi

cal b

ubbl

er te

mpe

ratu

res

100-

150

o C(m

p 14

1 o C

)

ALD

with

H2O

sel

f-lim

iting

at ~

0.1

nm p

er c

ycle

ALD

“w

indo

w”

~150

to ~

400

o C

Elec

tric

al P

rope

rtie

s (n

on-o

ptim

ized

)

Die

lect

ric c

onst

ant >

16

Bre

akdo

wn

field

~6

MV/

cm

Har

vard

Uni

vers

ity

Stab

le A

mor

phou

s H

igh-

k D

iele

ctric

s

2.5

2.0

22D

yScO

3

4.4

3.5

3.9

SiO

2

4.9

2.8

8A

l 2O3

2.1

2.1

32La

LuO

3

2.5

2.0

22G

dScO

3

2.6

2.0

20La

2Hf 2O

7

3.2

1.9

18La

AlO

3

3.4

1.5

12H

fSiO

4

Val

ence

band

offs

etC

ondu

ctio

nba

nd o

ffset

k

=> L

aLuO

3ha

s th

e be

st p

rope

rtie

s!

Har

vard

Uni

vers

ity

Adv

anta

ges

of L

aLuO

3as

hig

h-k

diel

ectr

ic

Hig

h di

elec

tric

cons

tant

(k~3

2) fo

r am

orph

ous

pha

se

Sha

rp in

terfa

ce w

ith S

i, an

d no

low

-k in

terla

yer

Sta

ys a

mor

phou

s an

d do

esn’

t for

mal

loys

with

Sio

r Ge

afte

r res

pect

ive

S/D

act

ivat

ion

anne

als

Bot

h ba

nd o

ffset

s w

.r.t S

iare

larg

e (2

.1 e

V),

help

ing

to a

chie

ve lo

w le

akag

e cu

rren

ts

Har

vard

Uni

vers

ity

Am

idin

ate

Prec

urso

rs fo

r Lan

than

ides

Ln

NN

NN

NN

R2

R1

R2

R2

R1

R1

R3

R3

R3

The

R1

and

R2

are

alky

l gro

ups:

isop

ropy

l, te

rt-b

utyl

, eth

yl, e

tc.

The

choi

ces

of R

naf

fect

the

vola

tility

, rea

ctiv

ity a

nd s

tabi

lity.

R3

can

be a

n al

kyl g

roup

or h

ydro

gen

Har

vard

Uni

vers

ity

Ther

mog

ravi

met

ricA

naly

sis

of

Lant

hanu

m A

mid

inat

es

NH C

N

N CH

NN

HCN

La

NC

N

N CN

NCN

LaCH

3

CH

3H

3C

NC

N

N CN

NCN

LaCH

3

CH

3H

3CH3C

CH

3 CH

3

CH

3C

H3

H3C

=> V

apor

izat

ion

tem

pera

ture

incr

ease

s w

ith m

olec

ular

mas

s

Har

vard

Uni

vers

ity

Vapo

r Pre

ssur

es o

f Lan

than

um P

recu

rsor

s

=> L

a(iP

r 2-fm

d)3

is m

ost

vola

tile

La c

ompo

und

know

n,

60 m

Torr

at 1

00 o C

La(iP

rCp)

3

NH C

N

N CH

NN

HCN

La

Har

vard

Uni

vers

ity

ALD

of L

a 2O

3 => 0

.16

nm p

er c

ycle

=> n

eglig

ible

del

ay

in n

ucle

atio

n on

SiH

NH C

N

N CH

NN

HCN

La

tris

(N,N

’-diis

opro

pyl-

form

amid

inat

o)la

ntha

num

(i Pr 2

-fmd)

3La

Prec

urso

rs:

H2O

and

Har

vard

Uni

vers

ity

Gro

wth

per

La

Cyc

le fo

r ALD

LaA

lO3

Bub

bler

tem

pera

ture

90

to 1

20 o C

Subs

trat

e te

mpe

ratu

re 3

00 o C

Gro

wth

eve

n at

bub

bler

te

mpe

ratu

re <

100

o C

=> A

LD s

atur

atio

n at

0.

08 n

m p

er L

a cy

cle

NH C

N

N CH

NN

HCN

La

tris

(N,N

’-diis

opro

pyl-

form

amid

inat

o)la

ntha

num

(i Pr 2

-fmd)

3La

Prec

urso

rs:

Me 3

Al,

H2O

and

120

o C11

0o C

100

o C90

o C

Har

vard

Uni

vers

ity

Com

posi

tion

of A

LD L

a xA

l 1-xO

3/2

Gro

wth

con

ditio

ns:

Bub

bler

tem

pera

ture

120

o CSu

bstr

ate

tem

pera

ture

300

o C

=> C

ompo

sitio

n co

ntro

l by

cha

ngin

g ra

tio o

f pr

ecur

sor d

oses

=> 2

x a

s m

any

Al a

tom

s as

La

atom

s pe

r dos

e

NH C

N

N CH

NN

HCN

La

tris

(N,N

’-diis

opro

pyl-

form

amid

inat

o)la

ntha

num

(i Pr 2

-fmd)

3La

Prec

urso

rs:

Me 3

Al,

H2O

and

Har

vard

Uni

vers

ity

Prec

urso

r Rea

ctiv

ity w

ith S

iHSu

rfac

e by

IR

=> C

ompl

etel

y un

iform

sur

face

cov

erag

e by

La

amid

inat

e

Hfa

lkyl

amid

eon

ly

reac

ts w

ith h

alf o

f th

e Si

-H b

onds

on

the

surf

ace

even

af

ter m

any

cycl

es

La a

mid

inat

e re

acts

w

ith n

early

all

the

Si-H

bon

ds in

onl

y 3

cycl

es

Det

ails

of t

he in

frar

ed s

pect

ra w

ere

give

n in

a p

aper

this

mor

ning

by

J. K

won

, M. D

ai, E

. Lan

gere

is, Y

. Cha

bal,

K.-H

. Kim

and

R. G

. Gor

don.

Har

vard

Uni

vers

ity

TEM

sof

ALD

LaA

lO3an

d G

dScO

3

=> S

harp

inte

rfac

es w

ith s

ilico

n w

ithou

t int

erla

yers

=> U

nifo

rm n

ucle

atio

n an

d th

ickn

ess

Har

vard

Uni

vers

ity

Leak

age

Cur

rent

thro

ugh

ALD

La 2

O3

Vapo

r sou

rce:

a s

olut

ion

of th

e La

pre

curs

or (m

p 19

4 o C

)va

poriz

ed w

ith a

n M

KS

MD

D s

yste

m

Low

leak

age

curr

ent s

imila

r to

film

s m

ade

from

a b

ubbl

er.

=> n

eglig

ible

car

bon

cont

amin

atio

n fr

om s

olve

nt

Har

vard

Uni

vers

ity

Ther

mal

Gra

vim

etric

Ana

lysi

s of

Lu

tetiu

m tr

is(N

,N’-d

iisop

ropy

lace

tam

idin

ate)

Evap

orat

ion

with

neg

ligib

le re

sidu

e

=> S

uffic

ient

vol

atili

ty a

nd th

erm

al s

tabi

lity

for A

LD

NC

N

N CN

NCN

LuCH

3

CH

3H

3C

Har

vard

Uni

vers

ity

Ther

mal

Gra

vim

etric

Ana

lyse

s of

La

ntha

num

and

Lut

etiu

m A

mid

inat

es

NH C

N

N CH

NN

HCN

LuN

CN

N CN

NCN

LuCH

3

CH

3H

3C

NC

N

N CN

NCN

LuCH

3

CH

3H

3CH3C

CH

3 CH

3

CH

3C

H3

H3C

=> L

u am

idin

ates

are

slig

htly

mor

e vo

latil

e th

an L

a am

idin

ates

Har

vard

Uni

vers

ity

ALD

of L

u 2O

3an

d La

LuO

3

ALD

exp

erim

ents

and

film

cha

ract

eriz

atio

n ar

e un

derw

ay. .

. .

Har

vard

Uni

vers

ity

Con

clus

ions

Hfa

mid

inat

es a

re m

ore

stab

le th

an H

fam

ides

Hfa

mid

inat

es a

re s

uita

ble

as A

LD p

recu

rsor

s

La a

nd L

u am

idin

ates

are

vol

atile

ALD

pre

curs

ors

LaLu

O3

is a

ver

y pr

omis

ing

high

-k d

iele

ctric

Cur

rent

wor

k on

ALD

of L

aAlO

3, Lu

2O3

and

LaLu

O3

Har

vard

Uni

vers

ity

Am

idin

ate

prec

urso

rs s

uppl

ied

by R

ohm

and

Haa

s C

ompa

ny

MD

D li

quid

del

iver

y sy

stem

sup

plie

d by

MK

S In

stru

men

ts, I

nc.

Infr

ared

dat

a fr

om J

inhe

eK

won

, Min

Dai

, Erik

Lan

gere

is,

Lesz

ekW

ielu

nski

and

Yves

J. C

haba

l, R

utge

rs U

nive

rsity

Supp

orte

d in

par

t by

the

US

Nat

iona

l Sci

ence

Fou

ndat

ion

Ack

now

ledg

emen

ts

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