Radio frequency limiter

Abstract

Radiofrequency limiter The invention relates to a radiofrequency limiter, comprising an input port (IN), an output port (OUT), a plurality of transistors (T1…TN) connected in parallel between the input port (IN) and the output port (OUT), the transistors (T1…TN) being configured to be biased only between their gate and their source during operation of the limiter, and a plurality of self-inductances (L1…LN), connected in series between the input port (IN) and the output port (OUT), alternately with each of the transistors (T1…TN), each transistor gate being connected to a voltage source (VLim) via an adjustment resistor (RLim1…RLimN), characterized in that a diode (Det1…DetN) is connected between each drain and each adjustment resistor (RLim1...RLimN). Figure for abstract: Fig. 5

Description

Title of the invention: Radiofrequency limiter Technical field

[0001] The invention relates to the field of radiofrequency power limiters, used in particular in radiofrequency transmission / reception (T / R) modules of airborne systems.

[0002] The power limiter is a device whose objective is to clip its output power in the presence of high input power levels. Generally located in the reception chains, in front of sensitive elements such as low noise amplifiers (LNA - Low Noise Amplifier), its use has become essential to protect against possible attacks (intentional or not) from increasingly powerful electromagnetic sources ([Fig.l]). LNAs are generally made using technologies of the AsGa, Si or more recently GaN type. AsGa and Si technologies make it possible to obtain reduced noise levels but do not allow excessively high power levels (around 0.5 W).

[0003] Limiters are generally made from PIN and / or Shottky diodes. These diodes have the advantage of being low cost while offering good power handling.

[0004] The limiter structures most commonly used and using PIN and / or Shottky diodes are generally based on "head-to-tail" diode architectures ([Fig.2]) in order to clip the positive half-wave and the negative half-wave of the signal, or on parallel diode architectures ([Fig.3]). In both cases, these architectures use the non-linearity of the diodes to reflect and therefore clip the RF signal from a certain power level.

[0005] The problem is that their integration is becoming increasingly difficult in equipment due to miniaturization constraints. Although available in certain MMIC (Monolithic Microwave Integrated Circuit) integrated circuit technologies, these technologies do not allow the integration of limiters with other functions such as LNAs, which in fact reduces the possibility of compacting receivers.

[0006] [1] presents a solution to meet the needs cited above. It describes a MMIC limiter made in GaN technology from field effect transistors not polarized between their drain and their source, called cold FETs (FET for "Field Effect Transistor"). These transistors are placed in parallel between the RF input and the RF output of the limiter and alternately with self-inductances (placed in series between the RF input and the RF output).

[0007] Although fulfilling its function in TX mode (transmission mode, mode in which the limiter is at maximum attenuation in order to isolate the LNA from the TX channel), The structure described in [1] has the disadvantage of not sufficiently clipping its output power in RX mode (reception mode in which the limiter must both protect the LNA and present the lowest possible insertion losses to guarantee the performance of the RX chain). Indeed, as illustrated in [Fig.4], in RX mode, when the input power Pin increases (in the presence of an attack, for example), the output power Pout does not reach a plateau, and continues to increase. The limitation level is not sufficient. Indeed, it is advisable not to exceed 20 dBm at the output, so as not to damage the low noise amplifiers of the reception chain which would be made of AsGa.

[0008] There is therefore a need to obtain a radiofrequency limiter which offers good power handling, while having good compactness. Summary of the invention

[0009] An object of the invention is therefore a radiofrequency limiter, comprising an input port, an output port, a plurality of transistors connected in parallel between the input port and the output port, the transistors being configured to be biased only between their gate and their source during operation of the limiter, and a plurality of self-inductances, connected in series between the input port and the output port, alternately with each of the transistors, each transistor gate being connected to a voltage source via an adjustment resistor, a diode being connected between each drain and each adjustment resistor.

[0010] Advantageously, the anode of the diode is connected between two self-inductances, and the cathode of the diode is connected to the adjustment resistor.

[0011] Advantageously, the voltage source is configured to apply a voltage close to the pinch-off voltage of the transistors at the gate of each transistor.

[0012] Advantageously, a protective resistor is connected directly on the one hand to the gate of the transistor and on the other hand to the diode and to the adjustment resistor.

[0013] Advantageously, the limiter is integrated in high-power MMIC technology based on Gallium Nitride (GaN).

[0014] Advantageously, the adjustment resistors do not all have the same value.

[0015] Advantageously, the value of the adjustment resistor closest to the input port is greater than the values ​​of the other adjustment resistors.

[0016] The invention also relates to a transmission / reception module, comprising a aforementioned radiofrequency limiter.

[0017] The invention also relates to the use of the aforementioned radiofrequency limiter or the aforementioned transmission / reception module, as a variable attenuation pad controllable by varying the voltage generated by the voltage source.

[0018] Advantageously, the voltage range varies between the pinch voltage of the transistors and 0 V. Description of the figures

[0019] Other characteristics, details and advantages of the invention will emerge on reading the description given with reference to the appended drawings given by way of example.

[0020] [Fig. 1], already described, illustrates the basic diagram of a transmission module reception incorporating a limiter.

[0021] [Fig. 2], already described, illustrates the basic diagram of a head- diode limiter. spade.

[0022] [Fig. 3], already described, illustrates the basic diagram of a diode limiter in parallel.

[0023] [Fig.4], already described, illustrates the power response of the limiter as described in [1] for several attenuation levels.

[0024] [Fig.5] illustrates the basic diagram of the invention.

[0025] [Fig.6] illustrates the equivalent diagram of the limiter in RX mode.

[0026] [Fig.7] illustrates the equivalent diagram of the limiter in TX mode.

[0027] [Fig.8] illustrates the evolution of the output power as well as the response in transmission depending on the limiter input power in RX mode.

[0028] [Fig.9] illustrates the transmission response and reflection coefficients in low RF power level input / output of the limiter in RX mode.

[0029] [Fig. 10] illustrates the transmission response and input reflection coefficients / low RF power output from the limiter in TX mode.

[0030] [Fig. 11] illustrates the evolution of the output power as well as the response in transmission depending on the limiter input power in TX mode.

[0031] [Fig. 12] illustrates the evolution of the output power as well as the response in transmission as a function of input power, for a single frequency and for different VLim control levels. Detailed description of the invention

[0032] In [Fig.5], the input port IN is a connection point that allows the signal to be received at the output of the circulator. The output port OUT is another connection point that allows the limited signal to be made available to the low noise amplifiers LNA of the reception path.

[0033] The limiter comprises a plurality of cells (Celll...CellN) connected in parallel, as well as a plurality of self-inductances (L1...LN) connected in series, alternating with the cells. The number of cells results from a compromise between the desired limitation level and the insertion losses that can be accepted.

[0034] Each cell comprises a transistor (Tl.. .TN) which is said to be "cold", because it is polarized only between the gate and the source during operation of the limiter. Indeed, no polarization voltage is seen by the drain. The source of each transistor is connected to a reference potential (ground). As illustrated in [Fig.5], the drain of each transistor is connected directly to one of the self-inductances.

[0035] The gate of each transistor is connected to the control potential VLim, the value of which will modulate the attenuation level. Protective resistors (RGi.. .RGN) can be connected directly to the gate of the transistor (Tl.. .TN), to isolate the control circuit from the microwave signal.

[0036] In each cell, a detection diode (Detl.. .DetN) is connected to the voltage source (VLim) via an adjustment resistor (RLimi• • -Ri) which makes it possible to play on the limitation level of the function, as indicated below. Thus, each detection diode (Detl.. .DetN) is connected between the drain of the transistor and an adjustment resistor (RLimi• • -RumN)- Preferably, the anode of the diode (Detl.. .DetN) is connected between two self-inductances (L1.. .LN), and the cathode of the diode (Detl.. .DetN) is connected to the gate of the transistor (Tl.. .TN) (possibly via the protection resistor (RGi...RGN)), and to the adjustment resistor (RLiml.. .RLimN).

[0037] The limiter end self-inductors and capacitors, immediately adjacent to the input port and output port, are illustrated to account for the input and output wiring leads, which may introduce parasitic inductances and capacitances.

[0038] At low power level and for a voltage VLim allowing the transistors and the detection diodes to be blocked (VLhn=Vp pinch voltage), the limiter is equivalent to a transmission line.

[0039] Each cell is then equivalent to a resistance Roff (resistance causing insertion losses) and a capacitance Coff in parallel (parasitic capacitance limiting the operating frequency), as illustrated in [Fig.6]. The choice of the size of the transistors of the different cells will condition the value of the capacitance Coff and consequently the cut-off frequency of the limiter.

[0040] With the increase of the input Pin level, the detection diodes will start to conduct and will modify the gate bias of the transistors. The voltage seen by each of the gates will be equal to VLim - RLim.IDiode with VLim the control voltage and IDiode the current crossed by each diode.

[0041] The transistors will then gradually move from a blocked state (high impedance) to a passing state (low impedance) thus increasing the insertion losses, and giving a compression appearance to the limiter, similar to what is obtained on an amplifier. The equivalent model of the limiter at the end of the input pin variation range is then equivalent to that described in the diagram in [Fig.7].

[0042] According to a preferred embodiment, the adjustment resistors (RLimi • • -Ri.imd do not all have the same value, which makes it possible to trigger the change of state of the cells at different times.

[0043] More preferably, the value of the adjustment resistor RLimi closest to the input port IN is greater than the values ​​of the other adjustment resistors (RLim2- • • RLimN). Indeed, the first cell Celll is driven by the highest power. It is therefore advantageous to have a higher resistance value for this cell.

[0044] This effect is illustrated by [Fig.8], which shows respectively the evolution of the insertion losses and the output power Pout as a function of the input power Pin. These performances are obtained for a control voltage VLhn=Vp, corresponding to operation in RX mode (passing mode) and for RF signal frequencies varying between 6 and 12 GHz.

[0045] A very clear improvement in the limitation level can be observed compared to what was obtained until now with the limiter as described in [1] (see [Fig.4]). The output power level remains in fact lower than 16 dBm for input power levels of up to 46 dBm.

[0046] [Fig.9] illustrates the transmission response and reflection coefficients in Low RF power input / output of the limiter when the limiter is in RX mode. The limiter architecture provides a response that is substantially identical to that of a transmission line below the structure cutoff frequency, with transmission losses of less than 1.4 dB over 6 GHz of band, as well as excellent adaptation to RF accesses in this operating band.

[0047] It is recalled that in RX mode (reception mode), the limiter must have the lowest possible insertion losses to guarantee the performance of the reception chain, while protecting the low noise amplifiers LNA in the event of an attack.

[0048] [Fig. 10] shows the transmission response as well as the reflection coefficients at low level RF input / output (in the linear operating zone) of the limiter when in TX mode (maximum attenuation). The attenuation level is approximately 48 dB which allows good isolation of the low noise amplifiers LNA of the RX chain from the HPA amplifiers of the TX chain when the latter transmit.

[0049] [Fig. 11] illustrates the evolution of insertion losses as well as output power of the limiter according to the invention as a function of the input power Pin in TX mode and for frequencies between 6 and 12 GHz. These results are obtained for a voltage VLim applied between the gate and the source of the transistors Tl.. .TN equal to 0 V. The gain curve illustrates that attenuation is constant, regardless of frequency or input power.

[0050] The curves presented show that the limiter perfectly fulfills its limitation role, whether in TX or RX mode, and for input power levels much higher than those presented in [1].

[0051] As indicated previously, the control voltage VLim makes it possible to switch the transistors from a high impedance mode (RX mode, VLim=Vp, minimum attenuation) to a low impedance mode (TX mode, VLim=0V, maximum attenuation), and vice versa. The invention also makes it possible to use the radiofrequency limiter as a variable attenuation pad by applying a voltage VLim between 0 and Vp.

[0052] [Fig. 12] shows the evolution of the output power as a function of the input power (left figure) as well as the transmission response (gain, right figure) of the limiter according to the invention for different voltage levels VLim corresponding to different attenuation levels.

[0053] The fact that the limiter can integrate this functionality brings several advantages. Firstly, it saves the need for a variable attenuator that would potentially need to be added, which increases the level of integration. Secondly, it improves the performance of the RX chain because this additional functionality saves the insertion losses of an additional component.

[0054] Thus, it is possible to design a transmission / reception module in which the radio frequency limiter and the low noise amplifier network are implemented on a single MMIC.

[0055] The radiofrequency limiter according to the invention can be integrated in high-power MMIC technology based on Gallium Nitride (GaN), which makes it possible to offer good power handling and a high level of integration.

[0056] The invention also relates to the use of the aforementioned radiofrequency limiter, as a variable attenuation pad controllable by varying the voltage VLim generated by the voltage source.

[0057] Reference cited

[0058] [1] FR 3 013 536 B1

Claims

Claims

1. A radio frequency limiter, comprising an input port (IN), an output port (OUT), a plurality of transistors (Tl.. .TN) connected in parallel between the input port (IN) and the output port (OUT), the transistors (Tl.. .TN) being configured to be biased only between their gate and their source during operation of the limiter, and a plurality of self-inductances (L1.. .LN), connected in series between the input port (IN) and the output port (OUT), alternating with each of the transistors (Tl.. .TN), each transistor gate being connected to a voltage source (VLim) via an adjustment resistor (R,,^1...Ri,^), characterized in that a diode (Detl.. .DetN) is connected between each drain and each adjustment resistor (RLimi...RLimN).

2. Radio frequency limiter according to claim 1, wherein the anode of the diode (Detl.. .DetN) is connected between two self-inductances (L1.. .LN), and the cathode of the diode (Detl.. .DetN) is connected to the adjustment resistor (RLimi...RLimN).

3. Radio frequency limiter according to one of the preceding claims, in which the voltage source (VLim) is configured to apply a voltage close to the pinch voltage of the transistors (Tl...TN) at the gate of each transistor (T1...TN).

4. Radio frequency limiter according to one of the preceding claims, in which a protective resistor (RG1. . .Rgn) is connected directly on the one hand to the gate of the transistor (Tl.. .TN) on the other hand to the diode (Detl.. .DetN) and to the adjustment resistor (R,,imi...Ri.imN)

5. Radiofrequency limiter according to one of the preceding claims, in which it is integrated in high-power MMIC technology based on Gallium Nitride (GaN).

6. Radiofrequency limiter according to one of the preceding claims, in which the adjustment resistors (R,,im1.. .R, imN) do not all have the same value.

7. Radio frequency limiter according to claim 6, wherein the value of the adjustment resistor (RLimi) closest to the input port (IN) is greater than the values ​​of the other adjustment resistors (RLim2.. .RLimN).

8. Transmitting / receiving module, comprising a radiofrequency limiter according to one of the preceding claims.

9. Use of the radiofrequency limiter according to one of claims 1 to 7 or of the transmission / reception module according to claim 8, as a variable attenuation pad controllable by varying the voltage generated by the voltage source (VLim).

10. Use of the radiofrequency limiter according to the preceding claim, in which the voltage range varies between the pinch voltage of the transistors and 0 V.

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