Semiconductor device and power amplifier using the same

Information

  • Patent Grant
  • 6724020
  • Patent Number
    6,724,020
  • Date Filed
    Wednesday, April 23, 2003
    21 years ago
  • Date Issued
    Tuesday, April 20, 2004
    20 years ago
Abstract
A semiconductor device comprising a bipolar transistor having an emitter layer consisting of a semiconductor containing indium, and a protective insulating film containing silicon and oxygen which is formed on the surface of the guard ring of the emitter layer, wherein the protective insulating film has a density of oxygen of less than 7×1022 cm−3. This semiconductor device prevents performance deterioration and ensures high performance in a power amplifier.
Description




BACKGROUND OF THE INVENTION




The present invention relates to a semiconductor device and a power amplifier using the same.




In recent years, with the rapid growth in demand for mobile communication equipment, research and development of compound semiconductor devices for power amplifiers used in mobile communication equipment has been actively conducted. As one of such compound semiconductor devices, a hetero junction bipolar transistor (hereinafter called “HBT”) which has a high current drivability has been used.




AlGaAs has been widely used as a material for HBT emitter layers. However, there is an increasing trend to develop HBTs which use InGaP instead of AlGaAs because the former is more reliable in use over a long period that the latter. An example of an HBT which uses an InGaP emitter layer has been disclosed, for example, in Japanese Patent Laid-Open Publication No. 07-106343.




This prior art is illustrated in FIG.


15


. An n-type GaAs emitter protective layer


306


is formed on an n-type InGaP emitter layer


305


; an SiO


2


side wall


313


is formed on the area of the n-type GaAs emitter protective layer


306


which corresponds to the guard ring


312


of the n-type InGaP emitter layer


305


. The n-type GaAs emitter protective layer


306


prevents direct contact between the n-type InGaP emitter layer


305


and the SiO


2


side wall


313


, thereby avoiding an increase in a leakage current.




SUMMARY OF THE INVENTION




The present invention has an object to provide a semiconductor device in which, in a bipolar transistor having an emitter layer consisting of a semiconductor containing indium, a GaAs emitter protective layer is not used as a protective layer for preventing an increase in a leakage current between the emitter and base, and also provide a power amplifier using the same.




The above-said object can be achieved by covering the emitter layer guard ring surface of the bipolar transistor having an emitter layer consisting of a semiconductor containing indium, with a protective insulating film which contains silicon (Si) and oxygen (O) and has a density of oxygen of less than 7×10


22


cm


−3


.




It is also acceptable that the density of oxygen of the protective insulating film is 3×10


22


cm


−3


is or less, or 8×10


21


cm


−3


or less.




Also, the protective insulating film may further contain nitrogen (N) or hydrogen (H) as well.











BRIEF DESCRIPTION OF THE DRAWINGS




Preferred embodiments of the present invention will be described in detail based on the followings, wherein:





FIG. 1

is a sectional view illustrating a semiconductor device according to the present invention;





FIG. 2

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 3

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 4

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 5

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 6

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 7

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 8

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 9

is a sectional view illustrating the manufacturing method for an embodiment of a semiconductor device according to the present invention;





FIG. 10

is a sectional view of an embodiment of a semiconductor device according to the present invention;





FIG. 11

is a graph of reverse current against the density of oxygen in the protective insulating film;





FIG. 12

is a circuit diagram for a power amplifier;





FIG. 13

is a graph of a reverse current Ib against the reverse voltage Vbe in the insulating film formed under forming condition 4 shown in Table 1;





FIG. 14

is a graph of reverse current Ib against the reverse voltage Vbe in the insulating film formed under forming condition 2 shown in Table 1; and





FIG. 15

is a sectional view illustrating a conventional semiconductor device.











DESCRIPTION OF THE PREFERRED EMBODIMENTS





FIG. 1

is a sectional view illustrating an HBT which uses InGaP as an emitter layer material. In the figure, reference numeral


50


represents a GaAs base layer;


51


an InGaP emitter layer;


52


a GaAs ballast layer;


53


an InGaAs emitter contact layer;


54


a base electrode;


55


an emitter electrode;


80


a protective insulating film; and


90


an emitter wiring. The collector layer, the sub-collector layer and the collector electrode in the HBT are omitted in

FIG. 1

for simpler illustration. The base electrode


54


contacts the base layer


50


due to diffusion of its material into the emitter layer


51


so as to make an Ohmic contact. Although the base electrode


54


contacts the emitter layer


51


, it is not necessary to take into consideration the electric current path from the base electrode


54


through the emitter layer


51


, the ballast layer


52


and the emitter contact layer


53


to the emitter electrode


55


. This is because the region (guard ring)


61


, which does not form a junction with the ballast layer


52


, of the InGaP emitter layer


51


is depleted and has a high resistance, and also because the interface


65


between the guard ring


61


and the base electrode


54


is a Schottky junction and has a high resistance. The surface


70


of the guard ring


61


is covered with a protective insulating film


80


to prevent progress in natural oxidation and any etchant infiltration failure in the manufacturing process.





FIG. 12

shows an example of a power amplifier for mobile communication equipment which has, as basic elements, HBTs using InGaP as an emitter layer material. In this power amplifier, a signal inputted through a signal input terminal


120


is sequentially amplified by HBTs


100


,


101


and


102


connected through matching networks


110


,


111


,


112


and


113


before being outputted from a signal output terminal


125


. In this figure, reference numerals


141


to


146


represent choke inductors,


150


a collector wiring and


160


a base wiring.




When the power amplifier as shown in

FIG. 12

was incorporated in a 1-GHz class system such as a GSM (Global System for Mobile Communication) and operated at a high power (several watts), its amplification factor gradually decreased.




In order to find the cause of this problem, the DC characteristics of the HBTs used in the power amplifier were investigated. It has been found that the amplification factors for HBTs


100


,


101


and


102


decreased and, among them, the final stage HBT


102


showed a particularly remarkable decrease in amplification factor. Further, an examination of DC characteristics between terminals in the final stage HBT


102


has revealed that regarding the characteristics of the reverse current between the emitter and base, the emitter-base leakage current after amplification factor decrease (characteristic curve


202


) is larger than that before amplification factor decrease (characteristic curve


201


) as shown in FIG.


13


.




Then, in order to find the cause of the increase in leakage current between the emitter and the base, an investigation was also made as to how the reverse current between the emitter and base (per square centimeter emitter area) changes as the density of oxygen in the protective insulating film


80


is varied. Here, −5V was applied as the reverse voltage.




The density of oxygen in the protective insulating film was calculated from its constituent element atomic ratio and atomic density measured by the RBS (Rutherford Back Scattering) and HFS (Hydrogen Forward Scattering) methods. Supposing that the constituent elements of the protective insulating film are Si, O, N, and H (ingredients of the film material) and its composition is Si


l


O


p


N


q


H


r


, constituent element atomic ratio l, p, q, r, as well as constituent element atomic density n


all


can be calculated. n


all


represents a total number of Si, O, N and H atoms contained per cubic centimeter. The density of oxygen n


o


can be obtained from the equation n


o


=n


all


×p/(l+p+q+r).





FIG. 11

shows the result of the investigation: if the density of oxygen is in the range from 0 to 3×10


22


cm


−3


, when −5V reverse voltage is applied, the reverse current is almost constant (10


−3


A/cm


2


or so). If the density of oxygen is larger than that, the reverse current sharply increases.

FIG. 11

is a graph in which current values are plotted for densities of oxygen: −0, 8×10


21


, 7×10


22


and 1×10


23


cm


−3


. These protective insulating film forming conditions are summarized in Table 1.

















TABLE 1











Forming




Forming




Forming




Forming







Condition 1




Condition 2




Condition 3




Condition 4




























Density of oxygen




−0




8 × 10


21


cm


−3






7 × 10


22


cm


−3






1 × 10


23


cm


−3








Reverse




−10


−3


A/cm


2






−10


−3


A/cm


2






10


3


A/cm


2






10


4


A/cm


2








Current




(1) 4% SiH


4






(1) 4% SiH


4






(1) 5% SiH


4






(1) 4% SiH


4








(Vbe = 5 V)




(diluted




(diluted




(diluted




(diluted







with N


2


;




with N


2


;




with He;




with N


2


;






Gas used




500 sccm)




450 sccm)




100 sccm)




500 sccm)






(flow rate)




(2) NH


3






(2) N


2


O




(2) N


2


O




(2) O


2









(30 sccm)




(200 sccm)




(220 sccm)




(3500 sccm)










(3) N


2












(2000 sccm)






Degree of vacuum




49 Pa




49 Pa




40 Pa




Atmospheric Pressure






Substrate




250° C.




250° C.




250° C.




390° C.






Temperature






Supply




RF power




RF power




RF power




Heat






Energy




150 W




150 W




50 W














Under the forming condition 1, a trace of oxygen actually remains in the insulating film forming device though no compound gas (which generates oxygen) is introduced as a material into the device.




When the protective insulating film forming condition 1 or 2 in Table 1 was used, the reverse current as shown in

FIG. 11

was 10


−3


A/cm


2


or so, which demonstrates an improvement, or a decrease by 7 digits, as compared with the case in which the forming condition 4 was used. Even when forming condition 3 (plasma chemical vapor deposition) was used, the reverse current was 10


3


A/cm


2


, which is smaller than 10


4


A/cm


2


in the case of the forming condition 4 (thermal chemical vapor deposition).




When HBTs which have an insulating film (made under the forming condition 2) were used for HBTs


100


,


101


and


102


as shown in

FIG. 12

, no current amplification factor deterioration was observed. The initial DC characteristic of the reverse current between the emitter and base is shown as a characteristic curve in FIG.


14


. This characteristic remained almost unchanged even after operation at high power (several watts). The reason for this may be that, since the protective insulating film used has a low density of oxygen (3×10


22


cm


−3


or less), generation of much indium oxide did not occur on the surface of the InGaP emitter layer and thus the initial reverse current was small and with no current leakage path proliferation.




Embodiment 1




A semiconductor device according to one embodiment of the present invention is explained below referring to FIG.


10


. Here, an HBT consists of the following layers formed on the main side surface of a semi-insulating GaAs substrate


1


one upon another in order: n type GaAs sub-collector layer


2


A (thickness: 600 nm; dopant: silicon; impurity concentration: 5×10


18


cm


−3


); n type GaAs collector layer


3


A (thickness: 800 nm; dopant: silicon; impurity concentration: 1×10


16


cm


−3


) p type GaAs base layer


4


A (thickness: 70 nm; dopant: carbon; impurity concentration: 3×10


19


cm


−3


); n type In


x


Ga


1-x


P emitter layer


5


A (x: 0.5; thickness: 30 nm; dopant: silicon; impurity concentration: 3×10


17


cm


−3


); n type In


Y


Ga


1













y


As emitter contact layer


6


A (y: 0 around the junction with the n type In


x


Ga


1-x


P emitter layer


5


A, 0.5 around the area adjacent to the emitter electrode


10


; thickness: 400 nm; dopant: silicon; impurity concentration: 3×10


17


cm


−3


around the junction with the n type In


x


Ga


1-x


P emitter layer


5


A, 5×10


18


cm


−3


around the area adjacent to the emitter electrode


10


); first emitter electrode


10


and second emitter electrode


11


A; base electrode


11


; and collector electrode


12


.


21


A denotes a protective insulating film (made under forming condition 2 as shown in Table 1) with a density of oxygen of 8×10


21


cm


−3


which protects the main side surface of the emitter layer


5


A.


22


A denotes an insulating film which protects the junction between the emitter layer


5


A and base layer


4


A and the surface of the collector layer


3


A.


23


represents an insulating film including an insulator coating (SOG) made to prevent defects such as discontinuity and short-circuits in making collector wiring


30


and base wiring, while


24


represents an insulating film including an SOG made to prevent defects such as discontinuity and short-circuits in making emitter wiring


31


. Here, the base wiring, which forms an electrical junction with the base electrode


11


in a cross section other than that shown in

FIG. 10

, is not shown in the figure.




The method for manufacturing this semiconductor device is explained below by reference to

FIGS. 2

to


9


. First, an epitaxial film is formed on the main side surface of a semi-insulating GaAs substrate


1


by placing the following layers one upon another in the order of mention using the MOCVD method: n type GaAs sub-collector layer


2


(thickness: 600 nm; dopant: silicon; impurity concentration: 5×10


18


cm


−3


); n type GaAs collector layer


3


(thickness: 800 nm; dopant; silicon; impurity concentration: 1×10


16


cm


−3


); p type GaAs base layer


4


(thickness: 70 nm; dopant: carbon; impurity concentration: 3×10


19


cm


−3


); n type In


x


Ga


1-x


P emitter layer


5


(x: 0.5; thickness: 30 nm; dopant: silicon; impurity concentration: 3×10


17


cm


−3


); n type In


y


Ga


1













y


As emitter contact layer


6


(y: 0 around the junction with the n type In


x


Ga


1-x


P layer


5


, 0.5 around the area adjacent to the emitter electrode


10


; thickness: 400 nm; dopant: silicon; impurity concentration: 3×10


17


cm


−3


around the junction with the n type In


x


Ga


1-x


P layer


5


, 5×10


18


cm


−3


around the area adjacent to the emitter electrode


10


). Then, as shown in

FIG. 2

, WSi


z


(z: approx. 0.3; thickness: 300 nm) is formed by sputtering and then patterning is done by photolithography, followed by plasma etching to make a first layer emitter electrode


10


.




Then, as shown in

FIG. 3

, using the first layer emitter electrode


10


as a mask, then n type In


Y


Ga


1-y


As layer


6


is etched with phosphoric acid etching solution (H


3


PO


4


(85 weight %): H


2


O


2


(30 weight %): H


2


O=1:2:40) to make it an emitter contact layer


6


A, followed by forming an insulating film


20


all over by the thermal CVD method. The forming condition of the thermal CVD method used for forming the insulating film


20


is as follows: three types of gas are used (4% SiH


4


diluted with N


2


, and O


2


and N


2


and their flow rates are 500 sccm, 3,500 sccm and 2,000 sccm, respectively); atmospheric pressure and 390° C. substrate temperature.




Then, a resist pattern


40


is made by photolithography and the insulating film


20


is processed by plasma etching with a hydrofluoric acid solution to make it


20


A, as shown in FIG.


4


.




Next, Pt (20 nm), Ti (10 nm), Mo (30 nm), Ti (50 nm), Pt (50 nm), and Au (120 nm) are deposited one upon another in the order of mention by evaporation before forming a base electrode


11


using the lift-off method. An Ohmic contact between the base layer


4


and the base electrode


11


is made by a thermal sintering process based at a later process. The base electrode


11


is formed on the first layer emitter electrode


10


by self-alignment, so also formed on the emitter electrode


10


is a second layer emitter electrode


11


A which consists of Pt, Ti, Mo, Ti, Pt and Au deposited one upon another in the order of mention (FIG.


5


).




Then, a protective insulating film


21


which protects the surface of the n type In


x


Ga


1-x


P emitter layer


5


is formed all over using the plasma CVD method under forming condition 2 in Table 1 (two types of gas, 4% SiH


4


diluted with N


2


and N


2


O whose flow rates are 450 sccm and 200 sccm, respectively, are used; degree of vacuum 49 Pa; substrate temperature 250° C.; supply energy RF power 150W) (FIG.


6


).




Then, patterning is done by photolithography and then insulating films


21


and


20


A are processed by plasma etching. At this stage, the insulating film


20


A is completely removed. Next, the n type In


x


Ga


1-x


P emitter layer


5


is etched with hydrochloric acid, and the p type GaAs base layer


4


and n type GaAs collector layer


4


are etched with phosphoric acid etching solution (H


3


PO


4


(85 weight %): H


2


O


2


(30 weight %): H


2


O=1:2:40) to make them an emitter layer


5


A, a base layer


4


A, and a collector layer


3


A, respectively (FIG.


7


).




Next, using the thermal CVD method, the whole surface is covered with an insulating film under the following forming condition: three types of gas are used (4% SiH


4


diluted with N


2


, and O


2


and N


2


whose flow rates are 500 sccm, 3,500 sccm and 2,000 sccm, respectively) atmospheric pressure; and 390° C. substrate temperature. Then, after patterning by photolithography, this insulating film is processed by plasma etching to make it


22


A. Using this insulating film


22


A as a mask, a channel which reaches the n type GaAs sub-collector layer


2


is formed using a phosphoric acid etching solution as mentioned above to make a collector electrode


12


by depositing AuGe (60 nm), W (10 nm), Ni (10 nm), and Au (300 nm) one upon another by evaporation in the order of mention (FIG.


8


). An Ohmic contact of the collector electrode


12


with the n type GaAs sub-collector layer


2


is made by alloying at about 390° C.




Then an insulating film is formed all over the surface using the plasma CVD method under the following forming condition: two types of gas, 4% SiH


4


diluted with N


2


and N


2


O whose flow rates are 450 sccm and 200 sccm, respectively, are used; degree of vacuum 49 Pa; substrate temperature 250° C.; and supply energy RF power 150W, then to smoothen the surface to prevent such defects as discontinuity and short-circuits, rotary coating with SOG is done. Further, using the plasma CVD method (forming condition: two types of gas, 4%SiH


4


diluted with N


2


and N


2


O whose flow rates are 450 sccm and 200 sccm respectively, are used; degree of vacuum 49 Pa; substrate temperature 250° C.; and supply energy RF power 150W), an insulating film is formed all over the surface to make an insulating film


23


which contains SOG; then an opening is made by plasma etching; Mo (50 nm) and Au (800 nm) are deposited on it by evaporation in the order of mention before a collector wiring


30


and a base wiring (not shown in the figure) are made by photolithography (FIG.


9


).




Then, an insulating film is formed all over the surface using the plasma CVD method (forming condition: two types of gas, 4%SiH


4


diluted with N


2


and N


2


O whose flow rates are 450 sccm and 200 sccm respectively are used; degree of vacuum 49 Pa; substrate temperature 250° C.; and supply energy RF power 150W), then, rotary coating of the whole film surface with SOG is done to smoothen the surface to prevent such defects as discontinuity and short-circuits. Further, using the plasma CVD method (forming condition: two types of gas, 4%SiH


4


diluted with N


2


and N


2


O whose flow rates are 450 sccm and 200 sccm respectively, are used; degree of vacuum 49 Pa; substrate temperature 250° C.; and supply energy RF power 150W), an insulating film is formed all over the surface to make an insulating film


24


which contains SOG; then an opening is made by plasma etching; Mo (50 nm) and Au (800 nm) are deposited on it by evaporation in the order of mention before an emitter wiring


31


is made by photolithography to complete a semiconductor device as shown in FIG.


10


.




Embodiment 2





FIG. 12

is a circuit diagram for a power amplifier based on a semiconductor device according to the present invention. In the figure, reference numerals


100


,


101


and


102


represent HBTs connected in parallel which each uses a semiconductor device according to the present invention.


110


,


111


,


112


and


113


represent matching networks,


120


a signal input terminal,


125


a signal output terminal,


141


,


142


,


143


,


144


,


145


and


146


represent choke inductors,


150


a collector wiring, and


160


a base wiring.




The circuit shown in

FIG. 12

is the same as that for the power amplifier whose amplification factor has decreased due to high power operation as mentioned earlier except that HBTs


100


,


101


and


102


each uses a semiconductor device according to the present invention. Therefore, in this circuit, the phenomenon of an amplification factor decrease caused by high power operation was not observed. This demonstrates that according to the present invention, in a power amplifier, performance deterioration can be prevented and thus high performance can be ensured.



Claims
  • 1. A semiconductor device comprising a bipolar transistor having an emitter layer consisting of a semiconductor containing indium, and a protective insulating film containing silicon and oxygen which is formed on a surface of a guard ring of the emitter layer such that a reverse current between the emitter layer and a base is substantially 10−3 A/cm2.
  • 2. The semiconductor device as defined in claim 1, wherein the protective insulating film further contains nitrogen.
  • 3. The semiconductor device as defined in claim 2, wherein the protective insulating film further contains hydrogen.
  • 4. The semiconductor as defined in claim 1, wherein the bipolar transistor is formed on a semi-insulating compound semiconductor substrate and is a hetero junction bipolar transistor.
  • 5. The semiconductor as defined in claim 4, wherein the emitter layer is an n-type InxGa1-xP layer (0<x<1), and the hetero junction bipolar transistor further has a sub-collector layer which is an n-type GaAs layer, a collector layer which is an n-type GaAs layer, a base layer which is a p-type GaAs layer, and an emitter contact layer which is an n-type InyGa1-yAs layer (0<y<1).
  • 6. A power amplifier comprising a plurality of semiconductor devices on input and output sides, wherein at least one of the semiconductor devices located nearest to the output side is a semiconductor device comprising a bipolar transistor, said bipolar transistor has an emitter layer consisting of a semiconductor containing indium, and a protective insulating film containing silicon and oxygen which is formed on a surface of a guard ring of the emitter layer, wherein a reverse current between the emitter and the base is 10−3 A/cm2 or more and less than 10−3 A/cm2.
Priority Claims (1)
Number Date Country Kind
2000-169050 Jun 2000 JP
Parent Case Info

This application is a continuation application of U.S. application Ser. No. 09/863,343 filed on May 24, 2001 now U.S. Pat. No. 6,576,937.

US Referenced Citations (10)
Number Name Date Kind
4731340 Chang et al. Mar 1988 A
4800415 Simmons et al. Jan 1989 A
4996165 Chang et al. Feb 1991 A
5185274 Chang et al. Feb 1993 A
5682046 Takahashi et al. Oct 1997 A
5780922 Mishra et al. Jul 1998 A
5837589 McNamara et al. Nov 1998 A
5907165 Hamm et al. May 1999 A
6043520 Yamamoto et al. Mar 2000 A
6392258 Hirata et al. May 2002 B1
Foreign Referenced Citations (1)
Number Date Country
07-106343 Jul 1994 JP
Non-Patent Literature Citations (1)
Entry
Yutaka Kamei, Makoto Baba and Shigetaka Fujita, “space Charge in Polyimide Film after Water Absorption”, Proceedings of the 6th International Conference on Properties and Applications of Dielectric Materials (Jun. 21-26, 2000).
Continuations (1)
Number Date Country
Parent 09/863343 May 2001 US
Child 10/420764 US