This application claims priority based on Japanese Patent Application No. 2023-200008 filed on Nov. 27, 2023, and the entire contents of the Japanese patent applications are incorporated herein by reference.
A certain aspect of the embodiments is related to a semiconductor device and a Doherty amplifier circuit.
There has been known an N (N is 3 or more)-way Doherty amplifier circuit using a main amplifier and two or more peak amplifiers (for example, Patent Documents 1 and 2). The N-way Doherty amplifier circuit includes an impedance converter for electrically connecting an output terminal of the main amplifier and an output terminal of the first peak amplifier, and an impedance converter for electrically connecting the output terminal of the main amplifier and an output terminal of the second peak amplifier (for example, Patent Document 1: U.S. Pat. No. 8,022,760, and Patent Document 2: U.S. Pat. No. 10,601,375).
A semiconductor device according to the present disclosure includes: a package that includes a base and an output lead; a first semiconductor chip that is mounted on the base and includes a main amplifier for amplifying a first signal into which an input signal is divided and a first output pad for outputting an amplified first signal; a second semiconductor chip that is mounted on the base and includes a first peak amplifier for amplifying a second signal into which the input signal is divided and a second output pad for outputting an amplified second signal; a third semiconductor chip that is mounted on the base and includes a second peak amplifier for amplifying a third signal into which the input signal is divided and a third output pad for outputting an amplified third signal; a first impedance converter that is mounted on the base, and has a first end electrically connected to the first output pad and the output lead, and a second end electrically connected to the second output pad and the third output pad; a first matching circuit that is mounted on the base, and matches impedances of the first output pad and the first end with each other; and a second matching circuit that is mounted on the base, and matches impedances of the second output pad and the second end with each other.
However, it is difficult to realize the matching circuit for matching the impedances between the main amplifier and the impedance converter with each other and the matching circuit for matching the impedances between the first peak amplifier and the impedance converter with each other.
The present disclosure has been made in view of the above problems, and an object of the present disclosure is to realize matching circuits in the N-way Doherty amplifier circuit.
First, the contents of the embodiments of this disclosure are listed and explained.
Specific examples of a semiconductor device and a Doherty amplifier circuit according to embodiments of the present disclosure will be described below with reference to the drawings. It should be noted that the present disclosure is not limited to these examples, but is defined by the claims and is intended to include all modifications within the meaning and scope equivalent to the claims.
As an example of the Doherty amplifier circuit, a description will be given of a high-output high-frequency amplifier circuit used in a base station of mobile communication. In this case, the frequency of the high-frequency signal is, for example, 0.5 GHz or more and 10 GHz or less.
As illustrated in
The signals S1 through S3 pass through paths 15a through 15c, respectively. The path 15a includes a phase adjuster 23, a matching circuit 12a, the main amplifier 10a, and a matching circuit 14a (first matching circuit). The path 15b includes a phase adjuster 24, a matching circuit 12b (second matching circuit), the peak amplifier 10b, and a matching circuit 14b. The path 15c includes a matching circuit 12c (third matching circuit), the peak amplifier 10c, and a matching circuit 14c.
Phase adjusters 23 and 24 adjust a phase between paths 15a through 15c. The matching circuits 12a to 12c match the impedances seen from the divider 16 toward the matching circuits 12a to 12c with the impedances seen from the matching circuits 12a to 12c toward the main amplifier 10a, the peak amplifier 10b (first peak amplifier), and the peak amplifier 10c (second peak amplifier), respectively.
The main amplifier 10a and the peak amplifiers 10b and 10c amplify the signals S1 to S3, respectively, and output the amplified signals S4 to S6, respectively. The matching circuits 14a to 14c match the impedances seen from the main amplifier 10a and the peak amplifiers 10b and 10c toward the matching circuits 14a to 14c with the impedances seen from the matching circuits 14a to 14c toward the nodes N1 to N3, respectively.
The combiner 18 includes impedance converters 20 to 22. The impedance converter 20 (first impedance converter) is connected between the nodes N1 and N2. The impedance converter 21 (second impedance converter) is connected between the nodes N2 and N3. The impedance converter 22 is connected between the node N1 and an output terminal Tout. The combiner 18 combines the signals S4 to S6 to each other and outputs the synthesized signal to the output terminal Tout as an output signal Sout.
The main amplifier 10a and the peak amplifiers 10b and 10c are, for example, FETs (Field Effect Transistors), and are, for example, GaN HEMT (Gallium Nitride High Electron Mobility Transistor) or LDMOS (Laterally Diffused Metal Oxide Semiconductor).
Conditions for the operation of the Doherty amplifier circuit 100 are as follows, as illustrated in
A circuit configuration satisfying the above conditions 1 to 5 will be described.
As illustrated in
At the saturation powers of the transistors Q1 to Q3, a load impedance Zopt at which the output power is maximum (this is referred to as output matching) and a load impedance Zmod at which the efficiency is maximum (this is referred to as efficiency matching) are positioned on substantially a real axis on the Smith chart. That is, the reactance components of the load impedances Zopt and Zmod are substantially zero. For example, if a Doherty amplifier circuit is assumed in which the center frequencies of the operating bands are 2 GHz, the maximum output powers of the transistors Q1 to Q3 are 200 W and the maximum output power of the output signal Sout is 600 W, Zopt is about 2Ω and Zmod is Zopt×M (M is about 1 to 5).
The impedance converters 20 to 22 and 25a to 25c shift the phase at the center frequency of the operating band by 90°. Thus, the impedance located substantially on the real axis of the Smith chart is converted into an impedance located at a different position substantially on the real axis of the Smith chart. The characteristic impedances of the impedance converters 20 to 22 and 25a to 25c are set by the impedances before and after the conversion. For example, in a 2-way Doherty amplifier circuit, the phase may be shifted by 180° by the impedance converters 25b and 20. Since there is no node to which the peak amplifier 10c is connected, the impedance converters 25b and 20 need not be divided. On the other hand, in the N (N is 3 or more)-way Doherty amplifier circuit, the node N2 for electrically connecting the peak amplifier 10c exists between the impedance converters 20 and 25b. Therefore, the impedance converters 25b and 20 each having a phase shifted by 90° are separated from each other, and the node N2 is provided therebetween.
As illustrated in
For example, a description will be given of a case where the saturation power of the main amplifier 10a and the peak amplifiers 10b and 10c are the same as each other. At the power P3, the output powers of the main amplifier 10a and the peak amplifiers 10b and 10c are assumed to be the maximum powers Pmax. The following assumptions were made. At the power P2, the output power of the main amplifier 10a is Pmax/2, and the output power of the peak amplifier 10b is Pmax/4. At the power P1, the output power of the main amplifier 10a is Pmax/3. The output powers of the main amplifier 10a and the peak amplifiers 10b and 10c when the input powers Pin are the power P1 to P3, respectively, can be set as appropriate in addition to the above. Assume that the load impedance Z0 is 50Ω and the impedance Z4 is 16.7Ω. The load impedance Z0 and the impedance Z4 can also be set as appropriate. The configurations of the matching circuits 14a to 14c are assumed to be the same as each other. The configurations of the matching circuits 14a to 14c can be set as appropriate.
At the power P1, the impedance seen from the node N1 toward the impedance converter 20 is almost infinite, so the impedance Z2a is 16.7Ω and the same as the impedance Z4. The impedance converter 25a converts the impedance Z2a of 16.7Ω into the impedance Z1a of Zmod. This allows the main amplifier 10a to operate with efficiency matching.
At the power P2, the impedance Z4 of 16.7Ω is divided into the impedance Z2a of 25Ω and the impedance Z3a of 50Ω. The impedance converter 20 converts the impedance Z3a of 50Ω into the impedance Z3b of 12.5Ω. Since the impedance seen from the node N2 toward the impedance converter 21 is almost infinite, the impedance Z2b is 12.5Ω, which is the same as the impedance Z3b. At the power P2, the power of the main amplifier 10a and the peak amplifier 10b are Pmax/2 and Pmax/4, respectively. Therefore, in order to make the main amplifier 10a and the peak amplifier 10b have output-matching, the impedances Z1a and Z1b are 2×Zopt and 4×Zopt, respectively. The impedance converter 25a converts the impedance Z2a of 25Ω into the impedance Z1a of 2×Zopt. The impedance converter 25b converts the impedance Z2b of 12.5Ω into the impedance Z1b of 4×Zopt. This allows the main amplifier 10a and the peak amplifier 10b to operate with output matching.
At the power P3, the impedance Z4 of 16.7Ω is divided into the impedance Z2a of 50Ω and the impedance Z3a of 25Ω. The characteristic impedance of the impedance converter 20 is 25Ω, and the impedance converter 20 converts the impedance Z3a of 25Ω into the impedance Z3b of 25Ω. The impedance Z3b of 25Ω is divided into the impedance Z2b of 50Ω and the impedance Z2c of 50Ω. The characteristic impedance of the impedance converter 21 is 50Ω, and the impedance converter 21 converts the impedance Z3c of 50Ω into the impedance Z2c of 50Ω. In this way, the impedances Z2a to Z2c are all 50Ω. The impedance converters 25a to 25c convert the impedances Z2a to Z2c of 50Ω so that the impedances Z1a to Z1c are both equal to Zopt. This allows the main amplifier 10a and the peak amplifiers 10b and 10c to operate with output matching.
As described above, by using the impedance converters 20 to 22 and 25a to 25c, the Doherty amplifier circuit 100 can be operated as illustrated in
The semiconductor device used in the first embodiment will be described.
In
When the input powers Pin are the powers P1, P2, and P3, the characteristic impedances of the impedance converters 25a to 25c are about V (Zopt×Zmod) in order to achieve a well-balanced wide band. When Zopt is about 2Ω, the characteristic impedances of the impedance converters 25a to 25c are 2Ω to 4Ω. The remainders of the impedance converters 25a to 25c from which the drain-source capacitance Cds of
A semiconductor device for realizing such matching circuits 14a to 14c will be described.
As illustrated in
The planar shape of the frame 32 is substantially a rectangle. Leads 34a to 34c (input leads) are provided on the − side of the frame 32 in the X direction. The lead 35 (output lead) is provided on the + side of the frame 32 in the X direction. The leads 34a to 34c and 35 are metal layers such as copper or metal plates. The signals S1 to S3 are input to the leads 34a to 34c, respectively, and the output signal Sout is output from the lead 35.
The lead 34a, the capacitive component 65, the semiconductor chip 40a (first semiconductor chip), the line component 45, and the high dielectric component 50 are arranged in the X direction in correspondence with the path 15a. The lead 34b, the capacitive component 65, the semiconductor chip 40b (second semiconductor chip), the line component 45, and the high dielectric component 50 are arranged in the X direction in correspondence with the path 15b. The lead 34c, the capacitive component 65, the semiconductor chip 40c (third semiconductor chip), the line component 45, and the high dielectric component 50 are arranged in the X direction in correspondence with the path 15c. The line component 60 is mounted between the high dielectric component 50 and the frame 32 so as to extend in the Y direction.
Each of the semiconductor chips 40a to 40c includes a semiconductor substrate 41, pads 42 and 43 provided on the upper surface of the semiconductor substrate 41, and an electrode 44 provided on the lower surface of the semiconductor substrate 41. The pads 42 and 43 and the electrode 44 are a gate electrode, a drain electrode, and a source electrode, respectively, and the pad 42 is an input pad. The pads 43 of the semiconductor chips 40a, 40b, and 40c are a first output pad, a second output pad, and a third output pad, respectively. The transistors Q1 to Q3 illustrated in
The capacitive component 65 includes a dielectric substrate 66, an electrode 67 provided on an upper surface of the dielectric substrate 66, and an electrode 68 provided on a lower surface of the dielectric substrate 66. The electrodes 67 and 68 interposing the dielectric substrate 66 form a capacitor. The dielectric substrate 66 is, for example, an alumina substrate or a barium titanate substrate. The electrodes 67 and 68 are metal layers, such as gold layers.
The line component 45 includes a dielectric substrate 46, a line pattern 47 provided on an upper surface of the dielectric substrate 46, and an electrode 48 provided on a lower surface of the dielectric substrate 46. The line pattern 47 and the electrode 48 form a transmission line. The dielectric substrate 46 is, for example, an alumina substrate. The line pattern 47 and the electrode 48 are metal layers such as gold layers.
The high dielectric component 50 includes a high dielectric substrate 51, an electrode 52 provided on an upper surface of the high dielectric substrate 51, and an electrode 53 provided on a lower surface of the high dielectric substrate 51. The electrodes 52 and 53 interposing the high dielectric substrate 51 form a capacitor. The high dielectric substrate 51 has a larger relative dielectric constant than an alumina substrate, such as a barium titanate substrate. The electrodes 52 and 53 are metal layers such as gold layers.
The line component 60 includes a dielectric substrate 61, line patterns 62a and 62b provided on the upper surface of the dielectric substrate 61, and electrodes 63 provided on the lower surface of the dielectric substrate 61. The line pattern 62a and the electrode 63 form a transmission line TL01. The line pattern 62b and the electrode 63 form a transmission line TL02. Transmission lines TL01 and TL02 correspond to impedance converters 20 and 21, respectively. The width of the transmission line TL01 in the X direction is larger than the width of the transmission line TL02 in the X direction. Thereby, the characteristic impedance of the transmission line TL01 is lower than the characteristic impedance of the transmission line TL02. Both ends of the transmission line TL01 in the Y direction correspond to ends 20a (first end) and 20b (second end) of the impedance converter 20, respectively. Both ends of the transmission line TL02 in the Y direction correspond to the ends 21a (third end) and 21b (fourth end) of the impedance converter 21, respectively. The electrodes 44, 48, 53, 63 and 68 are bonded to the base 31 by a conductive bonding layer 38 such as a brazing filler metal or a metal paste.
Bonding wires 71 electrically connect the leads 34a to 34c to the electrode 67. Bonding wires 72 electrically connect the electrode 67 and the pad 42. Bonding wires 73 electrically connect the pads 43 to the line pattern 47. Bonding wires 74 electrically connect the line pattern 47 to the electrode 52. Bonding wire 75a electrically connect the electrode 52 of the path 15a to the end 20a of the line pattern 62a. Bonding wires 75b electrically connect the electrode 52 of the path 15b to the end 20b of the line pattern 62a and the end 21a of the line pattern 62b. Bonding wires 75c electrically connect the electrode 52 of the path 15c to the end 21b of the line pattern 62b. Bonding wires 76 electrically connect the end of the line pattern 62a to the lead 35. The bonding wires 71 to 76 are metal wires such as gold wires or aluminum wires.
The bonding wires 71 and 72 function as inductors, and the capacitive component 65 functions as a capacitor. Thus, the bonding wires 71 and 72 and the capacitive component 65 correspond to each of the matching circuits 12a to 12c of the T-type LCL circuit.
Next, the matching circuits 14a to 14c will be described by taking the matching circuit 14a as an example. The matching circuits 14b and 14c have the same configuration as the matching circuit 14a.
The inductor L1 corresponds to the bonding wires 73 and 74 and the line component 45. The transmission line TL1 corresponds to the high-dielectric component 50. The drain-source capacitance Cds of the transistor Q1 and the matching circuit 14a form the impedance converter 25a.
The inductor L1 may be formed only by a bonding wire. When the inductor L1 is formed using the bonding wire, the bonding wire is made longer in order to increase the inductance of the inductor L1. In this case, the bonding wire may be fused when a large current flows through the bonding wire. Therefore, the length of the bonding wires 73 and 74 is reduced by providing the line component 45.
In order to reduce the characteristic impedance of the impedance converters 25a to 25c in
As described above, the characteristic impedances of the matching circuits 14a to 14c can be reduced. As a method of reducing the characteristic impedance of the matching circuits 14a to 14c, first to third comparative examples will be described.
When the matching circuits 14a to 14c are provided on the circuit substrate 39 on which the semiconductor device 102 is mounted as in the first comparative example, if a transmission line having a low characteristic impedance is provided on the circuit substrate, the width of the line becomes wider. This is because the dielectric substrate of the circuit substrate 39 has a relatively low dielectric constant and is thick. For example, the width of the line is about 40 mm. This increases the size of the circuit substrate. If the characteristic impedance of the matching circuit 14a is increased (for example, to 10Ω), the band of the matching circuit 14a is narrowed. If a line having a wide width is used, the width of the line for connecting the matching circuits 14a to 14c to the impedance converter 20 also becomes wide. If a shunt capacitor is used without using the line, resonance occurs due to inductances of vias of the circuit substrate 39 for shunt connection. The characteristic impedances of the impedance converters 20 and 21 need not be as low as the characteristic impedances of the matching circuits 14a to 14c. However, when the impedance converters 20 and 21 are provided on the circuit substrate 39, the following problems occur as shown in second and third comparative examples.
As illustrated in
In the second comparative example, in order to compensate the drain-source capacitance Cds by providing the inductor L2, the impedance converter 25a for shifting the phase by 90° may be provided in the pad 43 and the subsequent portions. However, since the bonding wire 79a passes over the capacitive component 55d, the inductance of the inductor L0a becomes larger than the inductance of the inductor L0 of the first comparative example. When the inductance of the inductor L0a is large, it is difficult to design an impedance converter that has a desired characteristic impedance and shifts the phase by 90° by using the matching circuit 14a having the capacitor and the inductor and the inductor L0a, making it difficult to achieve the wide band.
As illustrated in
In the third comparative example, the matching circuit 14a is provided in the package 30. This makes it possible to realize the matching circuit 14a having a low characteristic impedance. However, the parasitic capacitance of the lead 35 is large. Therefore, the high-frequency characteristic of the lead 35 is largely deviated from the ideal transmission line. This makes it difficult to design an impedance converter that has a desired characteristic impedance and shifts the phase by 90° using the matching circuit 14a and the lead 35, and makes it difficult to achieve a wide band.
As an example, when the center frequency f0 is 2 GHZ, the characteristic impedances of the impedance converters 20, 21, and 22 are 3.9Ω, 7.9Ω, and 11.4Ω, respectively. The characteristic impedances of the matching circuits 14a to 14c are 2.63Ω, and the shift angle of the phase is 37.2°. A description will be given of an example in which the impedance converters 20, 21 and 22 are provided on the circuit substrate 39 as in the first comparative example.
As described above, according to the first embodiment, the impedance converter 20 and the matching circuits 14a and 14b are mounted on the base 31 as illustrated in
By mounting the impedance converter 20 and the matching circuits 14a and 14b on the base 31 in this way, the matching circuits 14a and 14b having low characteristic impedances can be realized. This allows the impedance converters 25a and 25b to shift the phase between the signal source of the transistor Q1 and the node N1 and the phase between the signal source of the transistor Q2 and the node N2 by 90°. Therefore, the N-way Doherty amplifier circuit 100 can be realized. In addition, the circuit substrate 39 can be reduced in size.
The impedance converter 21 is mounted on the base 31. The end 21a of the impedance converter 21 is electrically connected to the end 20b of the impedance converter 20, is short-circuited, and has the same potential as the end 20b of the impedance converter 20. The end 21b of the impedance converter 21 is electrically connected to the pad 43 of the semiconductor chip 40c. The matching circuit 14c matches the impedances of the pad 43 and the end 21b of the semiconductor chip 40c with each other.
By mounting the impedance converter 21 and the matching circuit 14c on the base 31 in this way, the matching circuit 14c having a low characteristic impedance can be realized. This allows the impedance converter 25c to shift the phase between the signal source of the transistor Q3 and the node N3 by 90°. Therefore, the N-way Doherty amplifier circuit 100 can be realized. The impedance converter 21 may not be necessarily provided.
The end 20a of the impedance converter 20 is electrically connected to the pad 43 of the semiconductor chip 40a via the bonding wires 73, 74, and 75a (first bonding wires). The end 20a of the impedance converter 20 is electrically connected to the lead 35 via the bonding wires 76 (second bonding wire). This allows the bonding wires 73, 74, and 75a to be used as a part of the matching circuit 14a. The bonding wires 76 may electrically connect the node N1 to the outside of the package 30.
The end 20b of the impedance converter 20 is electrically connected to the pad 43 of the semiconductor chip 40b via the bonding wires 73, 74, and 75b (third bonding wires). The end 21b of the impedance converter 21 is electrically connected to the pad 43 of the semiconductor chip 40c via the bonding wires 73, 74, and 75c (fourth bonding wires). This allows the bonding wires 73, 74 and 75b to be used as a part of the matching circuit 14b. The bonding wires 73, 74 and 75c may be used as a part of matching circuit 14c.
The impedance converter 20 includes the line pattern 62a provided on the line component 60, and the impedance converter 21 includes the line pattern 62b provided on the line component 60. This allows the transmission lines TL01 and TL02 to be used to form the impedance converters 20 and 21. By using the line patterns 62a and 62b, the characteristic impedances and the electrical lengths of the impedance converters 20 and 21 can be accurately realized.
The impedance converter 20 shifts the phase of the center frequency f0 of the operating band by 90° between the ends 20a and 20b, and the impedance converter 21 shifts the phase of the center frequency f0 of the operating band by 90° between ends 21a and 21b. Thus, the impedance converters 20 and 21 can convert the impedance on the real axis of the Smith chart into a different impedance on the real axis.
The matching circuit 14a shifts the phase of the center frequency f0 by 90° between the signal source of the main amplifier 10a and the end 20a. The matching circuit 14b shifts the phase of the center frequency f0 by 90° between the signal source of the peak amplifier 10b and the end 20b. The matching circuit 14c shifts the phase of the center frequency f0 by 90° between the signal source of the peak amplifier 10c and the end 20b. Thus, the impedance converters 25a to 25c including the matching circuits 14a to 14c, respectively, can convert the impedance on the real axis of the Smith chart into the difference impedance on the real axis.
As illustrated in
The phase of the center frequency f0 may not be exactly shifted by 90°. For example, the phase of rotation is 70° or more and 110° or less, or 85° or more and 95° or less. The impedance on the real axis does not have to be strictly on the real axis (that is, the reactance component is 0). An absolute value of a reactance component of the impedance may be 1.0 times or less or 0.2 times or less a resistance component thereof.
Assume that the target characteristic impedances of the impedance converters 20 and 21 are Z01 and Z02, respectively, the capacitances of the capacitors C01 to C03 are C01 to C03, respectively, and the inductances of the inductors L01 and L02 are L01 and L02, respectively. Here, L01=Z01/(2×π×f0), L02=Z02/(2×π×f0), C01=(2×π×f0)/Z01, C02=(2×π×f0)/Z01+(2×π×f0)/Z02, and C03=(2×π×f0)/Z02 are set. This allows the characteristic impedances Z01 and Z02 of the impedance converters 20 and 21 to be set to target values.
As illustrated in
Although the matching circuit 14a is described as an example of the matching circuits 14a to 14c, the matching circuits 14b and 14c can be formed in the same manner. The same applies to second to fourth alternative examples of the matching circuits 14a to 14c described later.
As illustrated in
When the capacitance of the capacitor C1a is the same as the drain-source capacitance Cds and the inductance of the inductor L1a is 1/((2×π×f0)2×Cds), the impedance converter 25a shifts the phase of the center frequency f0 by 90°. The characteristic impedance of the impedance converter 25a is 1/(2×π×f0×Cds). In the first alternative example of the matching circuits 14a to 14c, the characteristic impedance cannot be set freely, but the number of components mounted on the base 31 can be reduced.
As illustrated in
The inductance of the inductor L2 is greater than 1/((2×π×f0)2×Cds). As a result, the inductor L2 does not fully compensate the drain-source capacitance Cds. An uncompensated capacitance component is assumed to be ΔCds. The capacitor C2 is a DC cut capacitor, and the capacitance is sufficiently large not to affect inductor L2 at center frequency f0. The inductance of the inductor L1b is 1/(2×π×f0)2×(Cds−ΔCds), and the capacitance of the capacitor C1b is “Cds−ΔCds”. As a result, the impedance converter 25a shifts the phase of the center frequency f0 by 90°. The characteristic impedance of the impedance converter 25a is 1/(2×π×f0×(Cds−ΔCds)). By selecting the value of ΔCds in this way, the characteristic impedance of the impedance converter 25a can be set freely as compared with the case of the first alternative example.
Instead of the inductor L2 and the capacitor C2, the capacitor C2 may be provided without providing the inductor. In this case, the capacitance of the capacitor C2 is represented by ΔCds. The inductance of the inductor L1b is 1/((2×π×f0)2×(Cds+ΔCds)), and the capacitance of the capacitor C1b is Cds+ΔCds. As a result, the impedance converter 25a shifts the phase of the center frequency f0 by 90°. The characteristic impedance of the impedance converter 25a is 1/(2×π×f0×(Cds+ΔCds)). In this case, the characteristic impedance of the impedance converter 25a can be set freely.
As illustrated in
The inductance of the inductor L2 is 1/(2×π×f0)2×Cds). Thus, the inductor L2 compensates for the drain-source capacitance Cds. The phase of the center frequency f0 may be shifted by 90° by using the inductor L1c and the transmission line TL1a. The characteristic impedance of the transmission line TL1a and the phase to be shifted can be set in the same manner as in the high dielectric component 50 illustrated in
As illustrated in
The inductance of the inductor L2 is 1/((2×π×f0)2×Cds). Thus, the inductor L2 compensates for the drain-source capacitance Cds. The phase of the center frequency f0 may be shifted by 90° by using the inductors L1d and L3 and the capacitor C1c. For example, when the characteristic impedance of the impedance converter 25a is Z0, the inductances of the inductors L1d and L3 are set to Z0/(2×π×f0), and the capacitance of the capacitor C1c is set to 1/(2×π×f0×Z0). In this way, the drain-source capacitance Cds is compensated, which facilitates the design of the inductors L1d and L3 and the capacitor C1c.
Although the first embodiment has been described as an example in which the semiconductor substrates 41 of the semiconductor chips 40a to 40c are separated from each other, at least two of the semiconductor substrates 41 of the semiconductor chips 40a to 40c may be provided as a common integral body.
Although the 3-way Doherty amplifier circuit has been described as an example, in the case of an N-way Doherty amplifier circuit, N semiconductor chips, N matching circuits, and N−1 impedance converters may be provided.
Although the saturation powers of the main amplifier 10a and the peak amplifiers 10b and 10c are the same as each other, the saturation powers of the main amplifier 10a and the peak amplifiers 10b and 10c may be different from each other. For example, the saturation power of the peak amplifiers 10b and 10c may be twice that of the main amplifier 10a.
The embodiments disclosed here should be considered illustrative in all respects and not restrictive. The present disclosure is not limited to the specific embodiments described above, but various variations and changes are possible within the scope of the gist of the present disclosure as described in the claims.
Number | Date | Country | Kind |
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2023-200008 | Nov 2023 | JP | national |