Directional coupler

A coupler of distributed type including a first conductive line carrying a main signal between two end terminals, a second conductive line coupled to the first one and between two terminals of which flows a sampled signal, proportional to the main signal, and two capacitors respectively connecting the two terminals of each of the lines.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to the field of couplers which are used to capture a portion of a signal conveyed by a transmission line for, in particular, measurement or control purposes. The present invention more specifically relates to the field of radiofrequency couplers between a transmit amplifier and an antenna, especially applied to mobile telephony.

2. Discussion of the Related Art

FIG. 1very schematically illustrates the general structure of a distributed coupler1, that is, with transmission lines of the type to which the present invention applies, as opposed to couplers with localized inductive and capacitive elements.

Coupler1is interposed between an amplifier2(PA) for amplifying a signal Tx to be transmitted, and a transmit antenna3. The function of coupler1is to extract, between terminals CPLD and ISO of a secondary line12, a signal proportional to the signal transiting over a main transmission line11, that is, between terminals IN and DIR, respectively connected to the output of amplifier2and to the input of antenna3.

Signal G extracted by coupler1is exploited by a circuit4(DET), for example to control the power of amplifier2or to turn it off in case of a need for protection, for example, in case of a disappearing of antenna3.

This is an example of application to mobile telephony where the highest power consumption is due to the transmission chain and where the circuit power consumption is generally desired to be minimized. In receive mode, a mobile phone exploits a low-noise amplifier (LNA), the gain of which is generally fixed and for which a coupler is accordingly not necessary.

The coupler ofFIG. 1is a bidirectional coupler in that it detects a signal present on transmission line11in both directions: a forward signal (FWD) transiting from IN to DIR will be coupled towards output CPLD, and a reverse signal (REV) transiting from DIR to IN will be coupled towards output ISO. In practice, the voltages present on terminals CPLD and ISO are rectified to generate gain correction signal G.

A distributed coupler of the type shown inFIG. 1is characterized by its coupling and its directivity. The coupling characterizes the difference between the amplitude of the main signal circulating on line11and the amplitude of the signal sampled from line12. The directivity characterizes the difference between the amplitude of signal FWD, which translates as a signal coming out of terminal CPLD, and the amplitude of signal REV circulating from DIR to IN, which translates as a signal coming out of terminal ISO. The greater the amplitude difference between terminals CPLD and ISO, the greater the coupler directivity and the easier it is to detect a possible problem of antenna3translating as a reflection of the signal carried by line11. Indeed, in case of a problem on the antenna (for example a disappearing thereof), the power that cannot come out is reflected, which results in an increase in the signal on terminal ISO. By detecting the potential of terminal ISO with respect to a threshold, a problem can be detected on the antenna and the transmit amplifier can then be cut off to avoid damaging it, since said amplifier generally cannot stand receiving a reflected power.

In an ideal coupler and in normal operation, the amplitude maximum of the coupled line would be present on terminal CPLD and a zero voltage would be present on terminal ISO. However, in practice, the voltage of terminal ISO is not zero, but it is generally attenuated by on the order of −30 dB with respect to the voltage of terminal DIR.

Further, a low coupling is generally searched to avoid sampling too large a portion of the output for the detection. Generally, terminal CPLD reproduces a signal attenuated by on the order of from −15 to −20 dB with respect to the signal transiting from terminal IN to terminal DIR.

Accordingly, the directivity of a conventional coupler is on the order of from −10 dB to −15 dB (−30−(−20) to −30−(−15)).

Now, especially to ease the detection of a problem on the antenna, a higher directivity is desired.

To improve the directivity, the coupler can be enlarged by making conductive sections11and12close to a length of λ/4, where λ represents the wavelength corresponding to the central frequency of the desired coupler passband. However, developing a distributed coupler at a λ/4 length results in a very bulky coupler and increases insertion losses.

FIG. 2shows a conventional embodiment of a coupler10with an improved directivity. This coupler of distributed type comprises two conductive lines11and12and two capacitors Cp respectively connecting terminals iN and CPLD and terminals DIR and ISO. Such capacitors enable increasing the coupler directivity by drawing the values of the line impedances closer to one another. However, a disadvantage of such a solution is that at frequencies of several hundreds of MHz, the capacitance values are very small (on the order of one femtofarad). In practice, such values make the implementation almost impossible since the values of capacitances Cp come close to the values of stray capacitances which can then not be neglected. Now, the features of the coupler significantly degrade as soon as it is departed from the values selected, according to the coupler passband, for capacitors Cp.

Examples of couplers of the type described in relation withFIG. 2are described in U.S. Pat. No. 4,937,541 and in German patent application 19749912, both of which are incorporated herein by reference.

SUMMARY OF THE INVENTION

The present invention aims at providing a coupler with distributed lines of improved directivity.

The present invention especially aims at providing a radiofrequency coupler which does not require use of capacitors of very small value (on the order of one fF).

The present invention also aims at providing a coupler having a reduced bulk.

To achieve these and other objects, the present invention provides a coupler of distributed type comprising a first conductive line carrying a main signal between two end terminals, a second conductive line coupled to the first one and between two terminals of which flows a sampled signal, proportional to the main signal, and two capacitors respectively connecting the two terminals of each of the lines.

According to an embodiment of the present invention, the lines are of same length.

According to an embodiment of the present invention, the capacitors are of same values.

According to an embodiment of the present invention, the lines are sized in λ/4 for a central band frequency greater than the frequency band for which the coupler is intended.

According to an embodiment of the present invention, each conductive line is formed of at least two parallel sections between its end terminals, the sections of the two lines being interlaced.

According to an embodiment of the present invention, the capacitor electrodes are formed in the same two metallization levels as those in which are formed the conductive lines.

According to an embodiment of the present invention, the capacitors have values ranging between 0.1 and 10 pF, the central frequency of the coupler ranging between a few tens of MHz and a few tens of GHz.

DETAILED DESCRIPTION

The same elements have been referred to with the same reference numerals in the different drawings. For clarity, only those elements that are necessary to the understanding of the present invention have been shown in the drawings and will be described hereafter. In particular, the signals crossing the coupler, as well as what exploitation is made of the measurements by the coupled line have not been detailed, the present invention being implementable whatever application is made of the signals issued by the coupler.

A feature of the present invention is to provide capacitors, no longer to connect the respective ends of a line to the ends of the other line, but to interconnect the respective ends of a same line.

Such an arrangement enables, for a same frequency band, improving the directivity while using capacitors of higher values than in the conventional case ofFIG. 2.

The fact that the capacitors have substantially higher values makes the coupler (especially its directivity) less sensitive to variations in the capacitor values due to technological dispersions or due to the presence of stray capacitances which remain on the order of one femtofarad.

FIG. 3shows a coupler20according to a first embodiment of the present invention. It shows two parallel conductive lines11,12like in the embodiment ofFIG. 2. Line11forms the main line of terminals IN and DIR. Line12corresponds to the coupled line of terminals CPLD and ISO.

According to the present invention, a first capacitor Cs connects terminals IN and DIR while a second capacitor Cs connects terminals CPLD and ISO.

Lines11and12have the same lengths and capacitors Cs both have the same value.

The sizing of the conductive lines and of the capacitors depends on the application and more specifically on the central frequency of the passband desired for the coupler. In a simple example, sections11and12have lengths corresponding to λ/4, where λ represents the wavelength of the central frequency of the band. In this case, the addition of capacitors Cs reduces the bandwidth, but already improves the directivity. Further, they enable subsizing the λ value, due to the offset that they introduce on the central frequency.

According to a preferred embodiment of the present invention, advantage is taken of the presence of the capacitors to decrease the length of conductive sections11and12with respect to the size that they would have in λ/4 with respect to the central frequency of the desired passband. Such an embodiment enables decreasing the coupling (which is maximum at λ/4), and thus reducing the amplitude of the signal measured on the coupled line with respect to the main line. This thus reduces the power consumption (signal portion) which is not directly useful for the transmission.

FIG. 4shows a second preferred embodiment of a distributed coupler30according to the present invention.

According to this embodiment, a structure known as a Lange coupler, in which the two conductive sections11′ and12′ are interdigited, is used. In the example ofFIG. 4, sections each comprising two parallel branches111and112, respectively121and122, interleaved with the branches of the other line, have been provided. In such a structure, each section is, from the electrical point of view, formed of two parallel sections111and112, respectively121and122, between terminals IN and DIR, respectively CPLD and ISO. Perpendicular extensions114and124of the conductive tracks connect one end of sections112and122, for example, to terminals IN and ISO, respectively. Conductive sections (bridges)113and123connect the respective free ends of sections112and122to terminals DIR and CPLD, respectively.

In an embodiment in integrated circuit form, connections113and123are formed by vias (not shown) and conductive tracks in a second metallization level with respect to the metallization level in which are formed tracks111,112,114,121,122, and124.

According to the present invention, terminals IN and DIR, respectively CPLD and ISO, are connected to each other by capacitors Cs.

An advantage of this embodiment is that the forming of the capacitors takes advantage of the fact that the conductive lines are already formed in two separate metallization levels. Accordingly, these two metallizations levels and the dielectric separating them can be used to form the integrated capacitors Cs specific to the present invention.

In a conventional Lange coupler, that is, without capacitors Cs, the sizing corresponds to individual sections111,112,121, and122of length λ/4 for a central frequency corresponding to wavelength λ. Such a coupler is generally used to increase the coupling by decreasing stray capacitances.

According to the present invention, due to capacitors Cs, the Lange coupler can be sized for a substantially higher frequency (that is, with a substantially smaller length λ/4), to obtain the desired operating frequency. In this case, the coupling is decreased and the coupler directivity is increased.

The dimensions of a coupler according to the present invention are chosen according to the application. To take into account that fact that capacitors Cs must have values greater than the stray capacitances, a coupler of the present invention is more specifically dedicated to frequencies ranging between a few tens of MHz and a few tens of GHz. Capacitors Cs then have values ranging between 0.1 and 10 picofarads.

As a comparison, a Lange coupler with no capacitor and a Lange coupler according to the present invention with capacitors Cs of a 3.3-pF capacitance, with section lengths adapted to a 820-MHz frequency, have been formed on a board. Respective directivities of 7 and 28 dB have been obtained.

An advantage of the present invention is that the addition of capacitors Cs slightly increases the coupling while considerably increasing (by more than 10 dB) the directivity. Further, the isolation is improved and insertion losses increase only very slightly (less than 0.5 dB).

In an integrated forming of the structure ofFIG. 4, the surface area taken up by such a coupler is substantially the same as for a conventional coupler, the surface area necessary to the capacitor forming being compensated for by the decrease in the length of the conductive sections.

Of course, the present invention is likely to have various alterations, modifications, and improvements which will readily occur to those skilled in the art. In particular, the dimensions to be given to the different conductive sections of the coupler as well as to the capacitors are within the abilities of those skilled in the art based on the functional indications given hereabove.