A high-frequency amplifier includes: a carrier amplifier which amplifies a first signal; a peak amplifier which amplifies a second signal; a first matching circuit which is connected to the output terminal of the carrier amplifier; a second matching circuit which is connected to the output terminal of the peak amplifier; a first transmission line which is connected between the first matching circuit and the second matching circuit, and has an electric length that is less than ¼ of the wavelength of the center frequency of a predetermined frequency band. The phase rotation by a series inductor which is included in each of the first matching circuit and the second matching circuit and has one end that has been grounded is opposite to the phase rotation by the first transmission line.

FIELD

The present disclosure relates to high-frequency amplifiers, and particularly to high-frequency amplifiers represented by Doherty amplifiers.

BACKGROUND

A Doherty amplifier configured to include, in combination, a carrier amplifier that performs an AB-class operation or a B-class operation and a peak amplifier that performs C-class operation has been known as a highly-efficient high-frequency amplifier for use in radio communication, etc. In the Doherty amplifier, only the carrier amplifier operates in an operation area in which output power is low, both the carrier amplifier and the peak amplifier operate in an operation area in which output power is high, and the output signals of the carrier amplifier and the peak amplifier are combined.

In order to combine the output signals, in the Doherty amplifier, a first transmission line is connected between the output terminal of the carrier amplifier and the output terminal of the peak amplifier. The first transmission line has an electric length that is ¼ of the wavelength of the center frequency of a communication frequency band. Here, as problems that occur when the first transmission line having the ¼ wavelength is used, there are following problems: decrease in wide-band characteristics caused by dispersion of the load impedance of the carrier amplifier; decrease in efficiency caused by increase in the loss of high-frequency power; and furthermore, increase in the circuit scale because of increase in the length of the transmission line. It is to be noted that a “load impedance” of a certain circuit element is an impedance in the case where the output side (that is, the load side) is seen from the circuit element. In addition, “dispersion” means a frequency dependence, and “to disperse” means that the frequency dependence increases.

In view of this, conventionally, various techniques have been proposed in order to design a Doherty amplifier which operates in a wide frequency band.

In the technique of Patent Literature 1, a second transmission line is connected between a first transmission line and the output terminal of a peak amplifier. The second transmission line has an electric length that is ½ of the wavelength of the center frequency of a communication frequency band. In this way, in an operation area in which the peak amplifier does not operate and the output power of the Doherty amplifier is low, the frequency characteristics of the load impedance of a carrier amplifier are compensated, and the wide-band characteristics of the Doherty amplifier are improved.

CITATION LIST

Patent Literature

SUMMARY

Technical Problem

However, in the technique in Patent Literature 1, in an operation area in which both the carrier amplifier and the peak amplifier operate and the output power of the Doherty amplifier is high, no output signal of the carrier amplifier flows into the second transmission line, and thus the frequency characteristics of the load impedance of the carrier amplifier are not compensated. For this reason, in such an operation area in which output power is high, there is still a problem in decrease in the wide-band characteristics of the Doherty amplifier. Furthermore, in the technique in Patent Literature 1, problems remain in decrease in the efficiency of the Doherty amplifier and increase in the circuit size. It is to be noted that an “efficiency” of an amplifier means a power conversion efficiency (that is, the ratio of an output power with respect to an input power).

In view of this, the present disclosure has an object to provide a high-frequency amplifier which operates in a wider frequency band, provides a higher efficiency, and is more compact than conventional ones.

Solution to Problem

In order to achieve the above object, a high high-frequency amplifier according to an aspect of the present disclosure is a high-frequency amplifier which amplifies a first signal and a second signal in a predetermined frequency band to output amplified signals from an output terminal. The high-frequency amplifier includes: a first amplifier which amplifies the first signal; a second amplifier which amplifies the second signal; a first matching circuit which is connected to an output terminal of the first amplifier; a second matching circuit which is connected to an output terminal of the second amplifier; a first transmission line which is connected between the output terminal of the first matching circuit and the output terminal of the second matching circuit, the first transmission line having an electric length that is less than ¼ of a wavelength of a center frequency of the predetermined frequency band; a second transmission line which is connected to one of an input terminal of the first amplifier or an input terminal of the second amplifier, the second transmission line having an electric length that is less than ¼ of the wavelength of the center frequency of the predetermined frequency band; and a third transmission line which is connected between one end of the first transmission line and the output terminal, the third transmission line having an electric length that is ¼ of the wavelength of the center frequency of the predetermined frequency band. In the high-frequency amplifier, a phase rotation by one of the first matching circuit or the second matching circuit connected to an other of the output terminal of the first amplifier and the output terminal of the second amplifier is opposite to a phase rotation by the first transmission line.

In order to achieve the above object, a high-frequency amplifier according to another aspect of the present disclosure is a high-frequency amplifier which amplifies a first signal and a second signal in a predetermined frequency band to output amplified signals from an output terminal. The high-frequency amplifier includes: a substrate; one or two semiconductor chips mounted on the substrate; a first amplifier which is disposed on the one or two semiconductor chips and amplifies the first signal; a second amplifier which is disposed on the one or two semiconductor chips and amplifies the second signal; an eighth transmission line which is disposed on the one or two semiconductor chips and has one end connected to an output terminal of the first amplifier; a ninth transmission line which is disposed on the one or two semiconductor chips and has one end connected to an output terminal of the second amplifier; a first capacitor disposed on the one or two semiconductor chips; a second capacitor disposed on the one or two semiconductor chips; a fourth transmission line which is disposed on the substrate and has one end connected to an other end of the eighth transmission line; a fifth transmission line which is disposed on the substrate and has one end connected to an other end of the ninth transmission line; a first transmission line which is connected between the one end of the fourth transmission line and the one end of the fifth transmission line which are disposed on the substrate, the first transmission line having an electric length that is less than ¼ of a wavelength of a center frequency of the predetermined frequency band; a second transmission line which is connected to one of an input terminal of the first amplifier or an input terminal of the second amplifier, the second transmission line having an electric length that is less than ¼ of the wavelength of the center frequency of the predetermined frequency band; and a third transmission line which is connected between the one end of the first transmission line and the output terminal, the third transmission line having an electric length that is ¼ of the wavelength of the center frequency of the predetermined frequency band. In the high-frequency amplifier, an other end of the fourth transmission line and the first capacitor are connected to each other, and an other end of the fifth transmission line and the second capacitor are connected to each other.

Advantageous Effects

According to the present disclosure, a high-frequency amplifier which operates in a wider frequency band, provides a higher efficiency, and is more compact than conventional ones is provided.

DESCRIPTION OF EMBODIMENTS

FIG.1is a circuit diagram of high-frequency amplifier10according to a comparison example. Arrows and symbols Zci and Zpi (i is a numerical number) denoted near the arrows in the diagram indicate impedances (that is, load impedances) when seen from the positions of the symbols in the directions of the arrows. High-frequency amplifier10is a Doherty amplifier which amplifies a first signal and a second signal in a predetermined frequency band to output amplified signals from output terminal22. High-frequency amplifier10includes carrier amplifier (CA)11, peak amplifier (PA)12, first matching circuit13, second matching circuit16, first transmission line20, second transmission line19, third transmission line21, output terminal22, first input terminal23, and second input terminal24. First matching circuit13includes series inductor14and parallel capacitor15whose one end is grounded. Second matching circuit16includes series inductor17and parallel capacitor18whose one end is grounded. It is to be noted that a “series inductor” is an inductor which is inserted on a transmission path from an input terminal to an output terminal. In addition, a “parallel capacitor” is a capacitor which is connected between a transmission path from an input terminal to an output terminal and a reference potential (that is, a ground potential). In addition, “to ground” covers not only being Direct Current (DC) grounded (that is, being DC grounded to a reference potential) but also being grounded at high frequency (that is, being connected to a reference potential via a capacitor, or the like whose impedance is extremely low in a predetermined frequency band).

Carrier amplifier11is an amplifier which performs an AB-class operation or a B-class operation and amplifies the first signal, and operates in the entire range of the output power of high-frequency amplifier10. Peak amplifier12is an amplifier which operates a C-class operation and amplifies the second signal, and operates in an area in which the output power of high-frequency amplifier10is high. First transmission line20is connected between the output terminal of carrier amplifier11and the output terminal of peak amplifier12, and has an electric length that is ¼ of the wavelength of the center frequency of the predetermined frequency band. Characteristic impedance Zo1 of first transmission line20is 50Ω. In high-frequency amplifier10, the length of first transmission line20is as long as the ¼ wavelength, and thus there is a problem that the load dispersion of the carrier amplifier is large and the wide-band characteristics decrease. In addition, there is a problem that the loss of high-frequency power is large, and the efficiency of the amplifier decreases. In addition, increase in the circuit area becomes a problem.

Second transmission line19is connected to the input side of peak amplifier12, and is set to have an electric length that is the same as the electric length of first transmission line20in order to compensate the phase rotation by first transmission line20. In this case, the length of second transmission line19is as long as the ¼ wavelength, there are problems of the large loss of high-frequency power and decrease in amplification gain. In addition, increase in the circuit area becomes a problem. It is to be noted that the “phase rotation” by a certain circuit element is the difference between the phase angle of a signal input to the circuit element and the phase angle of a signal that is output from the circuit element (that is, the difference corresponds to a value according to (the phase angle of the output signal)−(the phase angle of the input signal)).

Now, the connection part between first transmission line20and second matching circuit16is assumed to be terminal X. Third transmission line21is connected between terminal X and output terminal22, and has an electric length that is ¼ of the wavelength of the center frequency of the predetermined frequency band. Characteristic impedance Zo3 of third transmission line21is a value (for example, 35.36Ω) for converting an impedance (for example, 25Ω) of terminal X to an impedance (for example, 50Ω) of output terminal22.

When peak amplifier12operates (when the PA is on), Zc14 is designed to have a value according to 50 Ω+j0Ω. When peak amplifier12does not operate (when the PA is off), Zc14 is designed to have a value according to 25 Ω+j0Ω.

Here, a description is given of a specific circuit constant in the case where GaN having a total gate width of 3 mm is used for each of carrier amplifier11and peak amplifier12in high-frequency amplifier10. In the center frequency of 4.5 GHz of a predetermined frequency band, the optimum characteristics are obtained by making the following settings of: Zc11=10 Ω+j43Ω, and Zp11=10 Ω+j43Ω when the PA is on; and Zc11=6 Ω+j39Ω when the PA is off. It is to be noted that the obtainable characteristics are described with reference toFIGS.4A,4B,5A, and5B. For this reason, it is only necessary that: the inductance of series inductor14be set to 2.2 nH; the capacitance of parallel capacitor15be set to 1.4 pF; the inductance of series inductor17be set to 2.2 nH, and the capacitance of parallel capacitor18be set to 1.4 pF.

FIG.2illustrates Smith charts each indicating impedance conversion in high-frequency amplifier10according to the comparison example. More specifically,FIG.2indicates impedance conversion by first matching circuit13and first transmission line20. When the PA illustrated in (a) ofFIG.2is on, conversion from Zc14=50 Ω+j0Ω to Zc11=10 Ω+j43Ω is performed. Here, conversion from Zc14 to Zc13 is not performed with 50Ω maintained, because the characteristic impedance of first transmission line20is 50Ω. When the PA illustrated in (b) ofFIG.2is off, conversion from Zc14=25 Ω+j0Ω to Zc11=6 Ω+j39Ω is performed. By first transmission line20, conversion from Zc14=25 Ω+j0Ω to Zc13=100 Ω+j0Ω is performed,

FIG.3is a diagram illustrating the phase angle of the matching circuit included in high-frequency amplifier10according to the comparison example. When the PA is on, the phase angle of Zc14 is 0°, the phase angle of Zc11 is 189°, and the phase difference between Zc14 and Zc11 is 189° (the solid line inFIG.3). Likewise, when the PA is off, the phase difference between Zc14 and Zc11 is 201° (the broken line inFIG.3). In either case, there is a large phase difference exceeding 180°. In this way, in high-frequency amplifier10, since the phase difference from terminal X to carrier amplifier11is large, there is a problem that dispersion of Zc11 is large (the dispersion of Zc11 is described later with reference toFIG.4A).

FIG.4Ais a Smith chart indicating the dispersion of Zc11 when the PA is on in high-frequency amplifier10according to the comparison example.FIG.4Aindicates the dispersion of Zc11 at frequencies 4.3 GHz, 4.5 GHz, and 4.7 GHz. When the dispersion of Zc11 is large, for example, when the optimum design is made to have center frequency 4.5 GHz, frequencies 4.3 GHz and 4.7 GHz at both ends are outside the optimum design, and the characteristics of high-frequency amplifier10at the frequencies decrease. When the variation amount of Zc11 (ΔZc11) from 4.3 GHz to 4.7 GHz is seen, ΔZc11=−1.4 Ω+j6.7Ω is satisfied.

FIG.4Bindicates frequency characteristics of efficiency when the PA is on in high-frequency amplifier10according to the comparison example. Although efficiency 70% is obtained at center frequency 4.5 GHz, the efficiency decreases to 60% at frequencies 4.3 GHz and 4.7 GHz at the both ends. This decrease in characteristics stems from the fact that ΔZc11 is large as indicated inFIG.4A,

FIG.5Ais a Smith chart indicating the dispersion of Zc11 when the PA is off in high-frequency amplifier10according to the comparison example. When ΔZc11 from frequency 4.3 GHz to frequency 4.7 GHz is seen, ΔZc11=−1.6 Ω+j8.6Ω is satisfied. InFIG.5B, efficiency 50% is obtained at center frequency 4.5 GHz, the efficiency decreases to 42% at frequencies 4.3 GHz and 4.7 GHz at the both ends. This decrease in characteristics stems from the fact that ΔZc11 is large.

In view of this, a high high-frequency amplifier according to an embodiment of the present disclosure is an amplifier which amplifies a first signal and a second signal in a predetermined frequency band to output amplified signals from an output terminal. The high-frequency amplifier includes: a first amplifier which amplifies the first signal; a second amplifier which amplifies the second signal; a first matching circuit which is connected to an output terminal of the first amplifier; a second matching circuit which is connected to an output terminal of the second amplifier; a first transmission line which is connected between the output terminal of the first matching circuit and the output terminal of the second matching circuit, the first transmission line having an electric length that is less than ¼ of a wavelength of a center frequency of the predetermined frequency band; a second transmission line which is connected to one of an input terminal of the first amplifier or an input terminal of the second amplifier, the second transmission line having an electric length that is less than ¼ of the wavelength of the center frequency of the predetermined frequency band; and a third transmission line which is connected between one end of the first transmission line and the output terminal, the third transmission line having an electric length that is ¼ of the wavelength of the center frequency of the predetermined frequency band. In the high-frequency amplifier, a phase rotation by one of the first matching circuit or the second matching circuit connected to an other of the output terminal of the first amplifier and the output terminal of the second amplifier is opposite to a phase rotation by the first transmission line. In this way, the phase rotation by the first matching circuit is opposite to the phase rotation by the first transmission line, and thus the dispersion of load impedance of the carrier amplifier is reduced. Thus, the amplifier can operate in a wider frequency band, provide a higher efficiency, and be more compact than conventional ones.

Hereinafter, the embodiment of the present disclosure is explained using the drawings. It is to be noted that each of embodiments to be described below indicates one specific example of the present disclosure. Frequencies, impedances, characteristic impedances, constants of circuit components, materials, etc. indicated in the embodiments below are examples, and thus do not intend to limit the present disclosure. In addition, the respective diagrams are not always illustrated precisely. In the diagrams, substantially the same dements are assigned with the same reference signs, and overlapping descriptions may be omitted or simplified. Predetermined frequency bands are frequency bands for use in communication, and for example frequency bands up to 3 THz for use in radio communication.

FIG.6is a circuit diagram of high-frequency amplifier30according to Embodiment 1. High-frequency amplifier30is a Doherty amplifier which amplifies a first signal and a second signal in a predetermined frequency band (for example, a frequency band whose center frequency is 4.5 GHz) to output amplified signals from output terminal22. High-frequency amplifier30includes carrier amplifier11which is an example of a first amplifier, peak amplifier12which is an example of a second amplifier, first matching circuit33, second matching circuit36, first transmission line40, second transmission line39, third transmission line21, output terminal22, first input terminal23, and second input terminal24, First matching circuit33includes series inductor34and parallel capacitor35whose one end is grounded. Second matching circuit36includes series inductor37and parallel capacitor38whose one end is grounded.

Carrier amplifier11and peak amplifier12for use in high-frequency amplifier30are each configured with, for example, a device which performs high-frequency amplification. The device is a FET, a BJT, or the like including Gall, GaAs, SiGe, Si, or the like. Transmission lines (first transmission line40, second transmission line39, and third transmission line21) are, for example, microstrip lines or strip lines. The transmission lines are configured with a substrate material for use in a general high-frequency circuit that is a ceramic group, a resin group, or the like, and transmission paths which include a material such as Cu whose electrical characteristics are excellent and which is for transmitting high-frequency signals. In an actual circuit, parallel inductors35and38are grounded via a capacitor for grounding, the capacitor for grounding is not illustrated in the diagram. In addition, a line for supplying power from a power source is not illustrated.

Hereinafter, high-frequency amplifier30according to this embodiment is described focusing on differences from high-frequency amplifier10according to the comparison example. In high-frequency amplifier10according to the comparison example, first matching circuit13includes series inductor14and parallel capacitor15whose one end is grounded. In comparison, in high-frequency amplifier30according to this embodiment, first matching circuit33includes series inductor34and parallel inductor35whose one end is grounded. In addition, in high-frequency amplifier10according to the comparison example, second matching circuit16includes series inductor17and parallel capacitor18whose one end is grounded. In comparison, in high-frequency amplifier30according to this embodiment, second matching circuit36includes series inductor37and parallel inductor38whose one end is grounded. In addition, a “parallel inductor” is an inductor which is connected between a transmission path from an input terminal to an output terminal and a reference potential (that is, a ground potential).

Here, as for high-frequency amplifier30according to this embodiment, a description is given of a specific circuit constant in the case where GaN having a total gate width of 3 mm (that is, the same GaN as in high-frequency amplifier10according to the comparison example) is used for each of carrier amplifier11and peak amplifier12.

Conditions for obtaining the optimum characteristics at frequency 4.5 GHz are the same as in high-frequency amplifier10. The conditions are: Zc21=10 Ω+j43Ω, and Zp21=10 Ω+j43Ω when the PA is on; and Zc21=6 Ω+j39 when the PA is off. To satisfy these conditions, it is only necessary that the inductance of series inductor34be set to 0.82 nH, the inductance of parallel inductor35be set to 0.89 nH, the inductance of series inductor37be set to 0.82 nH, and the inductance of parallel inductor38be set to 0.89 nH. It is excellent that the electric length of first transmission line40is set not to the ¼ wavelength but to less than the ¼ wavelength, and is set to a 1/10 wavelength of the center frequency of the predetermined frequency band here. In addition, the electric length of second transmission line39is set to the same electric length as the electric length of first transmission line40, that is, to the 1/10 wavelength, in order to compensate the phase rotation by first transmission line40. The characteristic impedance of first transmission line40and the characteristic impedance of second transmission line39are both 50Ω. Since the electric length of first transmission line40is shorter than in the comparison example, the dispersion of Zc21 is small, and the wide-band characteristics increase. In addition, loss in high-frequency power is small, and the efficiency of the amplifier increases. Furthermore, it is possible to reduce the size of the circuit.

FIG.7illustrates Smith charts each indicating impedance conversion in high-frequency amplifier30according to Embodiment 1. More specifically,FIG.7indicates impedance conversion by first matching circuit33and first transmission line40. As illustrated in (a) ofFIG.7, conversion from Zc24=50 Ω+j0Ω to Zc21=10 Ω+j43Ω is performed when the PA is on. Seeing the details, the conversion from Zc24 to Zc23 is caused by first transmission line40whose characteristic impedance is 50Ω, and thus Zc24 and Zc23 are both 50Ω. The conversion from Zc23 to Zc22 is caused by parallel inductor35whose one end is grounded, and thus the rotation is a counterclockwise rotation. In (a) ofFIG.2, compared with the conversion from Zc13 to Zc12 performed in the clockwise rotation direction, the conversion from Zc23 to Zc22 is performed in the rotation direction opposite to the clockwise rotation direction. In addition, the conversion from Zc22 to Zc21 is caused by series inductor34. In comparison with the conversion from Zc12 to Zc11 in (a) ofFIG.2, the inductance of series inductor34is reduced from 2.2 nH to 0.82 nH, and thus the amount of the conversion from Zc22 to Zc21 is small.

As illustrated in (b) ofFIG.7, conversion from Zc24=25 Ω+j0Ω to Zc21=6 Ω+j39Ω is performed when the PA is off. Seeing the details, in comparison with the amount of the conversion from Zc14 to Zc13 which corresponds to the ¼ wavelength and is caused by first transmission line20in (b) ofFIG.2, the amount of the conversion from Zc24 to Zc23 caused by first transmission line40corresponds to the 1/10 wavelength. The conversion from Zc23 to Zc22 is caused by parallel inductor35whose one end is grounded, and thus the rotation is a counterclockwise rotation. Compared with the conversion from Zc13 to Zc12 indicated in (b) ofFIG.2, the conversion from Zc23 to Zc22 is performed in a counterclockwise rotation. In addition, the conversion from Z22 to Z21 is caused by series inductor34, and thus the amount of the conversion is small compared with the amount of the conversion from Zc12 to Zc11 in (b) ofFIG.2.

FIG.8is a diagram indicating phase angles of the matching circuit included in high-frequency amplifier30according to Embodiment 1. When the PA is on, the phase difference between Zc24 and Zc21 is only 7° (the solid line inFIG.8), The phase difference is significantly reduced compared with phase difference 189° of high-frequency amplifier10according to the comparison example indicated inFIG.3. In high-frequency amplifier10according to the comparison example, the phase difference by first transmission line20is 90°, and since the phase difference by first matching circuit13is added thereto, the sum of the phase differences is inevitably 90° or more. In comparison, in high-frequency amplifier30according to this embodiment, the sum of the phase difference by first matching circuit33and the phase difference by first transmission line40is less than 90°. It can be said that this is a clear difference. The factor is analyzed below.

Specifically, in high-frequency amplifier30according to this embodiment, the phase difference between Zc24 and Zc23 is 36°. The phase difference is significantly reduced compared with 90° that is the phase difference between Zc14 and Zc13. This is an effect of the length of first transmission line40being reduced to the 1/10 wavelength. The conversion by first matching circuit33is a phase rotation from Zc23 to Zc21, and the phase difference is −16° according to 20°-36°. The phase rotation by first matching circuit33is directionally opposite to the phase rotation by first transmission line40, and thus has a function of compensating the phase difference of first transmission line40, Seeing this more specifically, the reason why the phase difference by first matching circuit33is negative is that the phase difference by parallel inductor35whose one end is grounded is negative. The phase difference is −36° according to 0°-36° when the conversion from Zc23 to Zc22 is seen. In this way, including a constituent element having a phase rotation which is directionally opposite to the phase rotation of first transmission line40is effective for compensating the phase difference by first transmission line40. The smallness of the phase difference between Zc22 and Zc21 reflects the smallness of the inductance of series inductor37.

In the same diagram, also when the PA is off, in high-frequency amplifier30according to this embodiment, the phase difference between Zc24 and Zc21 is significantly reduced compared with the phase difference of high-frequency amplifier10according to the comparison example illustrated inFIG.2(the broken line inFIG.8). The reasons for this include: that the length of first transmission line40is reduced as in the case where the PA is on; that first matching circuit33compensates the phase difference of first transmission line40; that parallel inductor35which is a constituent element of first matching circuit33has a phase rotation which is directionally opposite to the phase rotation by first transmission line40; and that the inductance of series inductor37is small.

FIG.9Ais a Smith chart indicating the dispersion of Zc21 when the PA is on in high-frequency amplifier30according to Embodiment 1.FIG.9Aindicates the dispersion of Zc21 at frequencies 4.3 GHz, 4.5 GHz, and 4.7 GHz. Zc21 at each of the frequencies is a value according to a corresponding one of 9.3 Ω+j41.5Ω, 10.0 Ω+j43.1Ω, and 10.7 Ω+j44.6Ω. When ΔZc21 from frequency 4.3 GHz to 4.7 GHz is seen, ΔZc21=1.4 Ω+j3.1Ω is satisfied. The dispersion is reduced compared with the dispersion in high-frequency amplifier10according to the comparison example illustrated inFIG.4A. This is because first matching circuit33compensates the phase rotation by first transmission line40as indicated inFIG.8. In other words, first matching circuit33functions to reduce dispersion of Zc21 by first transmission line40.

FIG.9Bindicates frequency characteristics of efficiency when the PA is on in high-frequency amplifier30according to Embodiment 1, Although efficiency 72% is obtained at center frequency 4.5 GHz. As known through comparison withFIG.4B, the efficiency is improved by 2% from the efficiency obtained by high-frequency amplifier10according to the comparison example. This is because the high-frequency loss is reduced by reducing the length of first transmission line40. At frequencies 4.3 GHz and 4.7 GHz at the both ends, efficiency 67% is maintained. This is the effect of the reduction in dispersion of ΔZc21 as illustrated inFIG.9A.

FIG.10Ais a Smith chart indicating dispersion of Zc21 when the PA is off in high-frequency amplifier30according to Embodiment 1. When ΔZc21 from frequency 4.3 GHz to 4.7 GHz is seen, ΔZc21=0.5 Ω+j3.3Ω is satisfied. The dispersion is reduced compared with the dispersion in high-frequency amplifier10according to the comparison example illustrated inFIG.5A. In other words, first matching circuit33functions to reduce dispersion of Zc21 by first transmission line40.

FIG.10Bindicates frequency characteristics of efficiency when the PA is on in high-frequency amplifier30according to Embodiment 1, Although efficiency 52% is obtained at center frequency 4.5 GHz. As known through comparison withFIG.43, the efficiency is improved by 2% from the efficiency obtained by high-frequency amplifier10according to the comparison example. This is because the high-frequency loss is reduced by reducing the length of first transmission line40. At frequencies 4.3 GHz and 4.7 GHz at the both ends, efficiency 48% is maintained. This is the effect of the reduction in ΔZc21 as illustrated inFIG.10A.

Although the electric length of first transmission line40is set to the 1/10 wavelength, it is to be noted that the same effect is provided as long as the electric length of first transmission line40is less than the ¼ wavelength. As an example, the electric length of first transmission line40is set to a ⅛ wavelength of the center frequency of the predetermined frequency band, other circuit constants are adjusted to the optimum ones, and dispersion of Zc21 is verified. When ΔZc21 from frequency 4.3 GHz to frequency 4.7 GHz is seen, ΔZc21=1.2 Ω+j4.5Ω is satisfied when the PA is on, and ΔZc21=0.3 Ω+j4.8Ω is satisfied when the PA is off. Also in the case where the electric length of first transmission line40is set to the ⅛ wavelength, the dispersion is reduced compared with the dispersion in high-frequency amplifier10according to the comparison example illustrated inFIG.4AandFIG.5A, The values of ΔZc21 in the respective cases where the electric lengths of first transmission line40are set to the 1/10 wavelength, the ⅛ wavelength, and the ¼ wavelength are indicated collectively in Table 1 below.

When the electric length of first transmission line40is set to less than the ¼ wavelength, ΔZc21 between when the PA is on and when the PA is off is reduced compared with ΔZc21 in high-frequency amplifier10according to the comparison example including first transmission line20whose electric length is the ¼ wavelength. As a result, high-frequency amplifier30according to this embodiment can be configured to operate in a wider frequency band, provide a higher efficiency, and be more compact than high-frequency amplifier10according to the comparison example.

As described above, high-frequency amplifier30according to this embodiment is a high-frequency amplifier which amplifies a first signal and a second signal in a predetermined frequency band to output amplified signals from output terminal22. High-frequency amplifier30includes: a first amplifier which amplifies the first signal; a second amplifier which amplifies the second signal; first matching circuit33which is connected to an output terminal of the first amplifier; second matching circuit36which is connected to an output terminal of the second amplifier; first transmission line40which is connected between the output terminal of first matching circuit33and the output terminal of second matching circuit36, first transmission line40having an electric length that is less than ¼ of a wavelength of a center frequency of the predetermined frequency band; second transmission line39which is connected to one of an input terminal of the first amplifier or an input terminal of the second amplifier (the second amplifier in this embodiment), second transmission line39having an electric length that is less than ¼ of the wavelength of the center frequency of the predetermined frequency band; and third transmission line21which is connected between one end of first transmission line40and output terminal22, third transmission line21having an electric length that is ¼ of the wavelength of the center frequency of the predetermined frequency band. In the high-frequency amplifier, a phase rotation by one of first matching circuit33or second matching circuit36(first matching circuit33in this embodiment) connected to an other of the output terminal of the first amplifier and the output terminal of the second amplifier is opposite to a phase rotation by first transmission line40.

In this way, since the electric length of first transmission line40is less than the ¼ wavelength, the loss of high-frequency power in first transmission line40is small, the efficiency of high-frequency amplifier30increases, and high-frequency amplifier30can be compact. Furthermore, a phase rotation by one of first matching circuit33or second matching circuit36(first matching circuit33in this embodiment) connected to an other of the output terminal of the first amplifier and the output terminal of the second amplifier is opposite to a phase rotation by first transmission line40. Thus, the phase rotation by first transmission line40is compensated (that is, cancelled) by the one of first matching circuit33or second matching circuit36(first matching circuit33in this embodiment). Specifically, a sum of (i) an amount of phase rotation by the one of first matching circuit33or second matching circuit36(first matching circuit33in this embodiment) connected to the other of the output terminal of the first amplifier and the output terminal of the second amplifier and (ii) an amount of phase rotation by first transmission line40is less than 90°. Thus, the one of first matching circuit33or second matching circuit36(first matching circuit33in this embodiment) connected to the other of the output terminal of the first amplifier and the second amplifier is capable of reducing dispersion which is a frequency dependence of an impedance at an output side when seen from the output terminal of the first amplifier. Thus, the wide-band characteristics of the high-frequency amplifier increase.

Here, the first amplifier is carrier amplifier11, and the second amplifier is peak amplifier12. In this way, the Doherty amplifier which can operate in a wider frequency band, provide a higher efficiency, and be more compact than conventional ones is implemented.

In addition, first matching circuit33and second matching circuit36include a fourth transmission line and a fifth transmission line, respectively. The fourth transmission line and the fifth transmission line each have a grounded end. Here, at least one of the fourth transmission line or the fifth transmission line (the both in this embodiment) includes an inductor (parallel inductors35and38). In this way, first matching circuit33or second matching circuit36(first matching circuit33in this embodiment) which causes a phase rotation in a direction opposite to the direction of a phase rotation by first transmission line40is easily implemented using the inductor.

It is to be noted that first matching circuit33and second matching circuit36have series inductor34and series inductor37, respectively. In this way, first matching circuit33and second matching circuit36which cause a phase rotation in a direction opposite to the direction of a phase rotation by first transmission line40can be configured using at least the two inductors, respectively.

FIG.11is a circuit diagram of high-frequency amplifier50according to Embodiment 2. Descriptions are given focusing on differences from high-frequency amplifier30according to Embodiment 1 illustrated inFIG.6. High-frequency amplifier50illustrated in the diagram includes: fourth transmission line55whose one end is grounded instead of parallel inductor35illustrated inFIG.6; and fifth transmission line58whose one end is grounded instead of parallel inductor38also inFIG.6, As for fourth transmission line55and fifth transmission line58, it is possible to obtain desired characteristics by setting the line length of each line to a 1/15 wavelength at frequency 4.5 GHz. In addition, in high-frequency amplifier50illustrated in the diagram, eighth transmission line54and ninth transmission line57having equivalent impedance conversion are used respectively instead of series inductor34and series inductor37illustrated inFIG.6, It is to be noted that each of fourth transmission line55, fifth transmission line58, eighth transmission line54, and ninth transmission line57is a microstrip line or a strip line.

The phase rotation by fourth transmission line55whose one end is grounded is equivalent to parallel inductor35whose one end is grounded, and it is possible to obtain impedance conversion similar to those indicated inFIGS.7and8. In this way, inductors can be handled as kinds of transmission lines. Furthermore, high-frequency amplifier50is capable of obtaining efficiency characteristics similar to efficiency characteristics indicated inFIGS.9A and93, andFIGS.10A and10B, In addition, first matching circuit53and second matching circuit56include fourth transmission line55and fifth transmission line58, respectively. Fourth transmission line55and fifth transmission line58each have a grounded end. In this way, first matching circuit53which causes a phase rotation opposite to the phase rotation by first transmission line40is easily implemented using fourth transmission line55such as a microstrip line.

FIG.12is a circuit diagram of high-frequency amplifier60according to Embodiment 3. In general, high-frequency amplifier30illustrated inFIG.6and high-frequency amplifier60illustrated inFIG.12may be distinguished from each other as a forward Doherty amplifier and as an inverse Doherty amplifier, respectively. Descriptions are given focusing on differences from high-frequency amplifier30. The connection part between first transmission line40and first matching circuit33is assumed to be terminal Y. Third transmission line21is connected between terminal Y and output terminal22. Second transmission line39is connected to the input side of carrier amplifier11, and is set to have an electric length that is the same as the electric length of first transmission line40in order to compensate a phase rotation by first transmission line40.

As for first transmission line40, although a conventional inverse Doherty amplifier requires a transmission line having the ¼ wavelength, it is possible to reduce the wavelength to less than the ¼ wavelength in high-frequency amplifier60according to this embodiment. Furthermore, there are following features similar to those described with reference toFIG.7andFIG.8: that second matching circuit36compensates the phase difference of first transmission line40; that parallel inductor38having a grounded end which is a constituent element of second matching circuit36has a phase rotation which is directionally opposite to the phase rotation by first transmission line40; and that the inductance of series inductor37is smaller than the inductance of the conventional inverse Doherty amplifier. As a result, also in high-frequency amplifier60, it is possible to obtain efficiency characteristics similar to the efficiency characteristics indicated inFIGS.9A and9B, andFIGS.10A and10Bby making the optimum settings to first matching circuit33, second matching circuit36, first transmission line40, and second transmission line39.

As described above, high-frequency amplifier60according to this embodiment is an inverse Doherty amplifier. Similarly to Embodiment 1, since the electric length of first transmission line40is less than the ¼ wavelength, the loss of high-frequency power in first transmission line40is small, the efficiency of high-frequency amplifier30increases, and high-frequency amplifier60can be compact. Furthermore, a phase rotation by one of first matching circuit33or second matching circuit36(second matching circuit36in this embodiment) connected to an other of the output terminal of the first amplifier and the output terminal of the second amplifier is opposite to a phase rotation by first transmission line40, Thus, the phase rotation by first transmission line40is compensated (that is, cancelled) by the one of first matching circuit33or second matching circuit (first matching circuit33in this embodiment) Thus, the one of first matching circuit33or second matching circuit36(second matching circuit36in this embodiment) connected to the other of the output terminal of the first amplifier and the second amplifier is capable of reducing dispersion which is a frequency dependence of an impedance at an output side when seen from the output terminal of the second amplifier. Thus, the wide-band characteristics of the high-frequency amplifier increase.

FIG.13is a circuit diagram of high-frequency amplifier70according to Embodiment 4. In high-frequency amplifier70, fourth transmission line55and fifth transmission line58are connected to power source terminal75and power source terminal76, respectively. First capacitor72whose one end is grounded is connected between power source terminal75and fourth transmission line55. Second capacitor74whose one end is grounded is connected between power source terminal76and fifth transmission line58. In this way, fourth transmission line55and fifth transmission line58have one end grounded at high frequency. Thus, also in high-frequency amplifier70, it is possible to obtain characteristics similar to those obtained by high-frequency amplifier30according to Embodiment 1. As such, it is possible to reduce the size of the circuit by utilizing fourth transmission line55and fifth transmission line58for the purposes of both impedance matching and supply of power from the power sources.

As described above, in addition to the configuration of high-frequency amplifier50according to Embodiment 2, high-frequency amplifier70according to this embodiment includes first capacitor72and second capacitor74. First capacitor72is a capacitor which is for grounding one end of fourth transmission line55and is connected between the one end of fourth transmission line55and a reference potential, Second capacitor74is a capacitor which is for grounding one end of fifth transmission line58and is connected between the one end of fifth transmission line58and a reference potential. In this way, fourth transmission line55and fifth transmission line58are grounded at high frequency, and high-frequency amplifier70is capable of exerting the same effects as the effects exerted by high-frequency amplifier50according to Embodiment 2.

In addition, in high-frequency amplifier70according to this embodiment, at least one of fourth transmission line55or fifth transmission line58(the both in this embodiment) is used also in the application of supplying power from the power sources in addition to the application of impedance conversion. In this way, it is possible to reduce the number of circuit elements required for high-frequency amplifier70, and thus to reduce the size of the circuit.

FIG.14is a circuit diagram of high-frequency amplifier77according to Embodiment 5, High-frequency amplifier77is different from high-frequency amplifier70according to Embodiment 4 illustrated inFIG.13in that inductor78for a first power source is connected between power source terminal75and point S which is a connection point between fourth transmission line55and first capacitor72. In high-frequency amplifier70according to Embodiment 4, the length of fourth transmission line55is selected by prioritizing impedance matching. Thus, when the length of fourth transmission line55is short, there is a problem that a high-frequency signal leaks from power source terminal75to the power source side. In this embodiment, as illustrated inFIG.14, the use of inductor78for the first power source makes it possible to prevent leakage of a high-frequency signal. Likewise, inductor79for a second power source is connected between power source terminal76and point S′ which is a connection point between fifth transmission line58and second capacitor74. The use of inductor79for the second power source makes it possible to prevent leakage of a high-frequency signal to the power source side.

As described above, in addition to the configuration of high-frequency amplifier according to Embodiment 4, high-frequency amplifier77according to this embodiment includes inductor78for the first power source and inductor79for the second power source. Inductor78for the first power source is connected between the power source and the connection point between fourth transmission line55and first capacitor72. Inductor79for the second power source is connected between the power source and the connection point between fifth transmission line58and second capacitor74. In this way, it is possible to prevent leakage of the high-frequency signal from high-frequency amplifier77to the power source side.

The background that leads to the present disclosure is described using the Smith chart indicating a load impedance area in each of high-frequency amplifiers according to Embodiments 1 to 5, Here, a description is given with reference to Embodiment 1. High-frequency amplifier30illustrated inFIG.6is characterized in that parallel inductor35and parallel inductor38whose one end is grounded are used as first matching circuit33and as second matching circuit36, respectively. First matching circuit33and second matching circuit36can be used only in the case where the load impedances of carrier amplifier11and peak amplifier12are in a matching available area (a hatched area) which is, as illustrated inFIG.15, an area except inside of a circle which (i) has, as a center, a midpoint between a point of R=50Ω and a short-circuited point and (ii) passes through the point of R=50Ω and the short-circuited point (in short, the equal admittance circle which passes though the point of R=50Ω. In the Doherty amplifiers which have been studied mainly for high-output applications, amplifier loads are inside such circles because the sizes of the transistors handled are large. Thus, it has been impossible to use first matching circuit33and second matching circuit36which are included in high-frequency amplifier30.

In the fifth-generation communication (so-called 5G) whose future development has been expected, the number of antennas to be used in a radio base station apparatus increases significantly (for example, from conventionally required four antennas to 256 antennas), In such radio base station apparatus, high-frequency signals to be output from a plurality of high-frequency amplifiers are output by beam forming using an array antenna, thus there is a tendency that the individual high-frequency amplifiers have low output power performances. Moreover, it becomes important that the amplifier to be used operates in a wider frequency band, provides a higher efficiency, and is more compact, more than ever before. In order to solve this problem, we have arrived at the high-frequency amplifier according to the present disclosure.

Here, a detailed description is given of a relationship between decrease in output power by a high-frequency amplifier and a high-frequency amplifier according to the present disclosure. The study by the Inventors have shown that, when FETs having a total gate width of 5 mm are used in the case where GaN FETs are used for high-frequency transistors, the optimum loads are within the matching available area illustrated inFIG.15. The saturation power that is output by each GaN FET having the total gate width of 5 mm is 30 W. The saturation output by high-frequency amplifier30obtainable when the GaN FET is used for each of carrier amplifier11and peak amplifier12is 60 W. This can be said for all the high-frequency amplifiers disclosed in this Specification.

As described above, in the high-frequency amplifier according to this embodiment, at least one of an impedance at an output side when seen from the output terminal of the first amplifier or an impedance at an output side when seen from the output terminal of the second amplifier is outside the equal admittance circle which passes through a point that satisfies R=50Ω on the Smith chart. In order to satisfy this, it is desirable that each of the first amplifier and the second amplifier includes a FET formed using GaN, and a maximum high-frequency output power of the FET be less than or equal to 30 W. In this way, the high-frequency amplifier according to this embodiment can be used for a radio base station apparatus for applications such as the fifth-generation communication which outputs a high-frequency signal using an array antenna.

FIG.16is a layout diagram of high-frequency amplifier80according to Embodiment 6, High-frequency amplifier80according to this embodiment includes the same circuits as those in high-frequency amplifier77according to Embodiment 5 illustrated inFIG.14. Thus,FIG.16corresponds to a specific layout on substrate80a, regarding the circuit diagram of high-frequency amplifier77according to Embodiment 5 illustrated inFIG.14.

The correspondences betweenFIG.14andFIG.16are as follows. Specifically, eighth transmission line54inFIG.14corresponds to line AB inFIG.16. Likewise, fourth transmission line55inFIG.14corresponds to line BC inFIG.16. In addition, first transmission line40inFIG.14corresponds to line BX inFIG.16. First capacitor72for grounding inFIG.14is configured with component capacitor82whose one end is connected to grounding part87inFIG.16, Inductor78for the first power source inFIG.14corresponds to a part at which two elements which are component inductor85and line CD which is an example of the sixth transmission line inFIG.16are connected. Here, using also line CD makes it possible to reduce the inductance of component inductor85, and as a result, it is possible to increase a Q value of component inductor85. The output terminal (point P) of carrier amplifier11and the input terminal (point A) of line AB are connected via a bonding wire. It is to be noted that carrier amplifier11is disposed on semiconductor chip80b.

Likewise, ninth transmission line57inFIG.14corresponds to line A′S″ inFIG.16. Fifth transmission line58inFIG.14corresponds to line B′C′ inFIG.16. Second capacitor74for grounding inFIG.14is configured with component capacitor84whose one end is connected to grounding part88inFIG.16. Inductor79for the second power source inFIG.14corresponds to a part at which two elements which are component inductor86and line C′D′ which is an example of the seventh transmission line inFIG.16are connected. Here, using also line CD′ makes it possible to reduce the inductance of component inductor86, and as a result, it is possible to increase a Q value of component inductor86. The output terminal (point P′) of peak amplifier12and the input terminal (point A′) of line A′B′ are connected via a bonding wire. It is to be noted that peak amplifier12is disposed on semiconductor chip80c.

As known fromFIG.16, in the layout of high-frequency amplifier80according to this embodiment, the following positions are designed to be line symmetric: (i) the positions of carrier amplifier11to power source terminal75, specifically, chip80b, line AB corresponding to eighth transmission line54, line BC corresponding to fourth transmission line55, line CD corresponding to the sixth transmission line, and (ii) the positions of peak amplifier12to power source terminal76, specifically, chip80c, line A′B′ corresponding to ninth transmission line57, line B′C′ corresponding to fifth transmission line58, line CD′ corresponding to the seventh transmission line. In addition, line BX is implemented to have a 1/10 wavelength (approximately 3 mm at frequency 4.5 GHz on substrate80a), and thus the length is short.

As described above, high-frequency amplifier80according to this embodiment is configured to include: component inductor85and line CD which is the example of the sixth transmission line instead of inductor78for the first power source in Embodiment 5; and component inductor86and line C′D′ which is the example of the seventh transmission line instead of inductor79for the second power source in Embodiment 5. In other words, inductor78for the first power source in Embodiment 5 includes the sixth transmission line (line CD), and inductor79for the second power source in Embodiment 5 includes the seventh transmission line (line C′D′).

In this way, it is possible to arrange transmission lines having line length shorter than conventional near carrier amplifier11and peak amplifier12, and thus to reduce the circuit size of high-frequency amplifier80.

Although semiconductor chip80bon which carrier amplifier11is disposed and semiconductor chip80con which peak amplifier12is disposed are separate chips in this embodiment, it is to be noted that configurations are not limited to this, and both carrier amplifier11and peak amplifier12may be disposed on a same chip.

In addition, eighth transmission line54, ninth transmission line57, fourth transmission line55, fifth transmission line58, first transmission line40, second transmission line39(not illustrated inFIG.16) and third transmission line21may be made using a same material (such as copper).

FIG.17is a layout diagram of high-frequency amplifier90according to Embodiment 7. High-frequency amplifier90according to this embodiment includes the same circuits as those in high-frequency amplifier77according to Embodiment 5 illustrated inFIG.14. Thus,FIG.17corresponds to a specific layout on substrate90a, regarding the circuit diagram of high-frequency amplifier77according to Embodiment 5 illustrated inFIG.14.

In high-frequency amplifier90according to this embodiment, not only a FET as carrier amplifier91but also line PQ and first capacitor95are disposed on semiconductor chip90bon which carrier amplifier91is disposed. One end of first capacitor95is connected to the ground on a rear face of semiconductor chip90bvia a through hole (not illustrated inFIG.17). Likewise, not only a FET as peak amplifier92but also line P′Q′ and second capacitor96are disposed on semiconductor chip90con which peak amplifier92is disposed. One end of second capacitor96is connected to the ground on a rear face of semiconductor chip90cvia a through hole (not illustrated inFIG.17).

The correspondences betweenFIG.14andFIG.17are as follows. Specifically, eighth transmission line54inFIG.14corresponds to a part at which line PQ and a bonding wire between point Q and point H are connected inFIG.17. Likewise, fourth transmission line55inFIG.14corresponds to line HJ inFIG.17. First transmission line40inFIG.14corresponds to line HX inFIG.17. First capacitor72for grounding inFIG.14corresponds to first capacitor95disposed on semiconductor chip90binFIG.17. Likewise, ninth transmission line57inFIG.14is configured with line P′Q′ and a bonding wire between point Q′ and point H′. Fifth transmission line58inFIG.14corresponds to line H′J′ inFIG.17. Second capacitor74for grounding inFIG.14corresponds to second capacitor96disposed on semiconductor chip90cinFIG.17, In addition, the line between point3and power source terminal75inFIG.17corresponds to the sixth transmission line, and the line between point J′ and power source terminal76inFIG.17corresponds to the seventh transmission line.

In a high frequency band of a millimeter waveband or above, a wavelength is short, and thus it is possible to dispose a transmission line on a semiconductor chip. In addition, the length of a bonding wire is significant compared with the wavelength, it is possible to configure part of a matching circuit using the bonding wire. In addition, a capacitor for grounding can be implemented using a small capacitance value in the high frequency band, and thus it is possible to dispose the capacitor for grounding on the semiconductor chip.

As described above, high-frequency amplifier90according to Embodiment 7 is an amplifier which amplifies a first signal and a second signal in a predetermined frequency band to output amplified signals from output terminal22. The high-frequency amplifier includes: substrate90a; one or two semiconductor chips mounted on substrate90a(in this embodiment, semiconductor chips90band90c); a first amplifier which is disposed on semiconductor chip90band amplifies the first signal; a second amplifier which is disposed on semiconductor chip90cand amplifies the second signal; a part (line PQ) of eighth transmission line54which is disposed on semiconductor chip90band has one end connected to an output terminal of the first amplifier; a part (line P′Q′) of ninth transmission line57which is disposed on semiconductor chip90cand has one end connected to an output terminal of the second amplifier; first capacitor95disposed on semiconductor chip90b; second capacitor96disposed on semiconductor chip90c; fourth transmission line55(line HJ) which is disposed on substrate90aand has one end connected to an other end of the part (line PQ) of eighth transmission line54; fifth transmission line58(line H′J′) which is disposed on substrate90aand has one end connected to an other end of the part (line P′Q′) of ninth transmission line57; first transmission line40(line HX) which is connected between the one end (point H) of fourth transmission line55and the one end (point H′) of fifth transmission line58which are disposed on substrate90a, first transmission line40having an electric length that is less than ¼ of a wavelength of a center frequency of the predetermined frequency band; second transmission line39(not illustrated inFIG.17) which is connected to one of an input terminal of the first amplifier or an input terminal of the second amplifier, second transmission line39having an electric length that is less than ¼ of the wavelength of the center frequency of the predetermined frequency band; and third transmission line21(a transmission line between point X and output terminal22) which is connected between the one end of first transmission line40(line HX) and output terminal22, third transmission line21having an electric length that is ¼ of the wavelength of the center frequency of the predetermined frequency band. An other end of fourth transmission line55and first capacitor95are connected to each other, and an other end of fifth transmission line58and second capacitor96are connected to each other. More specifically, the other end of fourth transmission line55and first capacitor95are connected using first bonding wire97, and the other end of fifth transmission line58and second capacitor74are connected using second bonding wire98.

In this way, it is possible to configure parts of a matching circuits using bonding wires, Thus, the lengths of transmission lines required for the matching circuits are reduced. In addition, the capacitors for grounding are disposed on the semiconductor chips on which the amplifiers are disposed, and thus it is possible to design the amplifiers and capacitors as components independent from the other circuits.

Although semiconductor chip90bon which carrier amplifier91is disposed and semiconductor chip90con which peak amplifier92is disposed are separate chips in this embodiment, it is to be noted that configurations are not limited to this, and both carrier amplifier11and peak amplifier12may be disposed on a same chip. In addition, eighth transmission line54, ninth transmission line57, fourth transmission line55, fifth transmission line58, first transmission line40, second transmission line39(not illustrated inFIG.17) and third transmission line21illustrated inFIG.17as examples may be made using a same material (such as copper).

FIG.18illustrates a layout diagram of semiconductor chip101for a carrier amplifier according to Embodiment 8 ((a) ofFIG.18) and a layout diagram of semiconductor chip102for a peak amplifier according to Embodiment 8 ((b) ofFIG.18). Not only a FET for amplification but also line PQ and first capacitor105are disposed on semiconductor chip101for the carrier amplifier illustrated in (a) ofFIG.18. In addition, a bump is disposed at point Q which is the connection point of semiconductor chip101and an outside transmission line, a bump is disposed on upper electrode106which is one end of first capacitor105, and a bump is disposed on lower electrode107which is the other end. Likewise, not only a FET for amplification but also line P′Q′ and second capacitor108are disposed on semiconductor chip102for the peak amplifier illustrated in (b) ofFIG.18. In addition, a bump is disposed at point Q′ which is the connection point of semiconductor chip102and an outside transmission line, a bump is disposed on upper electrode109which is one end of second capacitor108, and a hump is disposed on lower electrode110which is the other end.

FIG.19is a layout diagram of high-frequency amplifier100according to Embodiment 8. High-frequency amplifier100according to this embodiment includes the same circuits as those in high-frequency amplifier77according to Embodiment 5 illustrated inFIG.14. Thus,FIG.19corresponds to a specific layout on substrate100a, regarding the circuit diagram of high-frequency amplifier77according to Embodiment 5 illustrated inFIG.14.

As illustrated in the diagram, semiconductor chip101for the carrier amplifier and semiconductor chip102for the peak amplifier illustrated inFIG.18are mounted on substrate100aby face-down bonding. Here, the mounting is performed in such a manner that the bump on point Q overlaps point H, the bump on upper electrode106overlaps point3, the bump on point Q″ overlaps point H′, and the bump on upper electrode109overlaps point3′. In addition, lower electrodes107and110which are the other ends of first capacitor105and second capacitor108are respectively grounded via substrate100a.

The correspondences betweenFIG.14andFIG.19are as follows. Specifically, eighth transmission line54inFIG.14corresponds to line PQ inFIG.19. Likewise, fourth transmission line55inFIG.14corresponds to line HJ inFIG.19. In addition, first transmission line40inFIG.14corresponds to line HX inFIG.19. Likewise, ninth transmission line57inFIG.14is configured with line P′Q′ inFIG.19. Likewise, fifth transmission line58inFIG.14corresponds to line WY inFIG.19.

In this way, semiconductor chip101for the carrier amplifier has a bump which is a first conductor disposed in the area in which at least part of semiconductor chip101overlaps the other end (that is point3) of fourth transmission line55in a plan view, and semiconductor chip102for the peak amplifier has a bump which is a second conductor disposed in the area in which at least part of semiconductor chip102overlaps the other end (that is point3′) of fifth transmission line58in the plan view. The other end (that is point3) of fourth transmission line55and first capacitor72are connected via the bump which is the first conductor, and likewise, the other end (that is point J′) of fifth transmission line58and second capacitor74are connected via the bump which is the second conductor.

In Embodiment 7, the parts of the matching circuits are configured using first bonding wire97and second bonding wire98. However, further increase in frequency makes it difficult to perform matching because the inductances of the bonding wires are too large. In the case, the inductances of the bumps are much smaller than the inductances of the bonding wires, it is excellent to make contact with an outside circuit using the bumps instead of the bonding wires.

Although the high-frequency amplifiers according to the present disclosure have been described based on Embodiments 1 to 8 above, the present disclosure is not limited to Embodiments 1 to 8. The present disclosure covers and encompasses embodiments that a person skilled in the art may arrive at by adding various kinds of modifications to the above embodiments or by arbitrarily combining some of the constituent elements in the embodiments within the scope of the present disclosure.

For example, although the high-frequency amplifier in each of the above embodiments are designed assuming that a target load impedance is 50Ω, target load impedances are not limited to 50Ω, and a high-frequency amplifier may be designed assuming that a target load impedance is another load impedance such as 75Ω. In the case, it is only necessary to match the characteristic impedances of the respective transmission lines included in the high-frequency amplifier with the target load impedance.

INDUSTRIAL APPLICABILITY

The high-frequency amplifiers according to the present disclosure is available as a Doherty amplifier and an inverse Doherty amplifiers which are compact and highly efficient, and operate in a wide frequency band, and which is for use in radio communication. More specifically, the high-frequency amplifier is available as a high-frequency amplifier for radio base station apparatus for the fifth generation communication.