Borderless vias with HSQ gap filled metal patterns having...

Semiconductor device manufacturing: process – Coating of substrate containing semiconductor region or of... – Insulative material deposited upon semiconductive substrate

Reexamination Certificate

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C438S622000, C438S624000, C438S637000, C438S761000, C438S763000, C438S692000

Reexamination Certificate

active

06319859

ABSTRACT:

TECHNICAL FIELD
The present invention relates to a high density, multi-metal layer semiconductor device with reliable interconnection patterns. The invention has particular applicability in manufacturing high density multi-metal layer semiconductor devices with design features of 0.25 microns and under.
BACKGROUND ART
The escalating requirements for high densification and performance associated with ultra large scale integration semiconductor devices require design features of 0.25 microns and under, such as 0.18 microns, increased transistor and circuit speeds, high reliability and increased manufacturing throughput. The reduction of design features to 0.25 microns and under challenges the limitations of conventional interconnection technology, including conventional photolithographic, etching and deposition techniques.
Conventional methodology for forming patterned metal layers comprises a subtractive etching or etch back step as the primary metal patterning technique. Such a method involves the formation of a first dielectric layer on a semiconductor substrate, typically monocrystalline silicon, with conductive contacts formed therein for electrical connection with an active region on the semiconductor substrate, such as a source/drain region. A metal layer, such as aluminum or an aluminum alloy, is deposited on the first dielectric layer, and a photoresist mask is formed on the metal layer having a pattern corresponding to a desired conductive pattern. The metal layer is then etched through the photoresist mask to form the conductive pattern comprising metal features separated by gaps, such as a plurality of metal lines with interwiring spacings therebetween. A dielectric layer is then applied to the resulting conductive pattern to fill in the gaps and the surface is planarized, as by conventional etching or chemical-mechanical polishing (CMP) planarization techniques.
As shown in
FIGS. 1 and 2
, conventional practices comprise depositing metal layer
11
on dielectric layer
10
which is typically formed on a semiconductor substrate containing an active region with transistors (not shown) After photolithography, etching is then conducted to form a patterned metal layer comprising metal features
11
a
,
11
b
,
11
c
and
11
d
with gaps therebetween. A dielectric material
12
, such as spin on glass (SOG), is typically deposited to fill in the gaps between the metal features, and baked at a temperature of about 300° C. to about 450° C., for a period of time up to about two hours, depending upon the particular SOG material employed, to effect planarization. Planarization, as by CMP, is then performed.
As feature sizes, e.g., metal lines and interwiring spacings, shrink to 0.25 microns and below, such as 0.18 microns, it becomes increasingly difficult to satisfactorily fill in the interwiring spacings voidlessly and obtain adequate step coverage. It also becomes increasingly difficult to form a reliable interconnection structure. A through-hole is typically formed in a dielectric layer to expose an underlying metal feature, wherein the metal feature serves as a landing pad occupying the entire bottom of the through-hole. Upon filling the through-hole with conductive material, such as a metal plug to form a conductive via, the entire bottom surface of the conductive via is in direct contact with the metal feature. Such a conventional technique is illustrated in
FIG. 3
, wherein metal feature
30
of a first patterned metal layer is formed on first dielectric layer
31
and exposed by through-hole
32
formed in second dielectric layer
33
. In accordance with conventional practices, through-hole
32
is formed so that metal feature
30
encloses the entire bottom opening, thereby serving as a landing pad for metal plug
34
which fills through-hole
32
to form conductive via
35
. Thus, the entire bottom surface of conductive via
35
is in direct contact with metal feature
30
. Conductive via
35
electrically connects metal feature
30
and metal feature
36
which is part of a second patterned metal layer. As shown in
FIGS. 2 and 3
, the side edges of a metal feature or conductive line, e.g.,
30
A,
30
B, and
36
A, and
36
B, taper somewhat as a result of etching.
The reduction of design features to the range of 0.25 microns and under requires extremely high densification. The conventional practice of forming a landing pad completely enclosing the bottom surface of a conductive via utilizes a significant amount of precious real estate on a semiconductor chip which is antithetic to escalating high densification requirements. In addition, it is extremely difficult to voidlessly fill through-holes having such reduced dimensions because of the extremely high aspect ratio, i.e., height of the through-hole with respect to diameter of the through-hole. Accordingly, conventional remedial techniques comprise purposely widening the-diameter of the through-hole to decrease the aspect ratio. As a result, misalignment occurs wherein the bottom surface of the conductive via is not completely enclosed by the underlying metal feature. This type of via is called a “borderless via”, which also conserves chip real estate.
The use of borderless vias, however, creates new problems. For example, as a result of misalignment, the SOG gap filling layer is penetrated by etching when forming a through-hole, due to the low density and poor stability of SOG. As a result of such penetration, moisture and gas accumulate thereby increasing the resistance of the interconnection. Moreover, spiking can occur, i.e., penetration of the metal plug to the substrate, causing a short. For example, adverting to
FIG. 4
, first dielectric layer
41
is formed on substrate
40
and a first metal pattern comprising a first metal feature, e.g., metal line
45
, is formed on first dielectric layer
21
gap filled with SOG
42
. Dielectric layer
43
is then deposited and a through-hole formed therein exposing a portion of the upper surface and at least a portion of a side surface of first metal feature
45
and exposing a portion of SOG
42
. Upon filling the through-hole with a metallic plug
44
, typically comprising an initial barrier layer (not shown) and tungsten, spiking occurs, i.e., penetration through to substrate
40
, thereby causing shorting.
Another problem generated by reducing the size of metal lines below about 0.25 microns is that it becomes increasingly difficult to voidlessly gap fill interwiring spacings with a dielectric material, such as SOG. Hydrogen silsesquioxane (HSQ) offers many advantages for use in interconnect patterns. HSQ is relatively carbon free, thereby avoiding poison via problems. Moreover, the absence of carbon renders it unnecessary to etch back HSQ below the upper surface of the metal lines to avoid shorting. In addition, HSQ exhibits excellent planarity and is capable of gap filling interwiring spacings less than 0.15 microns employing conventional spin-on equipment. HSQ undergoes a melting phase at approximately 200° C., but does not convert to the high dielectric constant glass phase until reaching temperatures of about 400° C. for intermetal applications and about 700° C. to about 800° C. for premetal applications.
However, the use of HSQ presents problems, particularly in borderless via applications. Typically, when forming a borderless via, a photoresist mask is deposited and the through-hole etched to expose a portion of an upper surface and a portion of a side surface of a metal line. The photoresist mask is then stripped employing an oxygen (O
2
)-containing plasma. It was found that the O
2
-containing plasma employed to strip the photoresist mask degraded the HSQ layer so that, upon subsequent introduction of a barrier material, such as titanium nitride or titanium-titanium nitride, spiking occurred, i.e., the barrier material penetrated through the HSQ layer.
HSQ typically contains between about 70% and about 90% Si—H bonds. However, upon exposure to an O
2
-containing plasma, a considerable number of Si—H bonds are broken and Si—OH bonds are formed. Upon tr

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