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International Journal of Antennas and Propagation

Volume 2011 (2011), Article ID 438478, 12 pages

http://dx.doi.org/10.1155/2011/438478

## The Noise Performance of a Multiple-Input-Port and Multiple-Output-Port Low-Noise Amplifier Connected to an Array of Coupled Antennas

Excem, 12 Chemin des Hauts de Clairefontaine, 78580 Maule, France

Received 19 May 2011; Revised 17 July 2011; Accepted 18 July 2011

Academic Editor: Hon Tat Hui

Copyright © 2011 Frédéric Broydé and Evelyne Clavelier. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

We address the noise characterization of a multiple-input-port and multiple-output-port (MIPMOP) device receiving signals from an array of antennas. A definition of the noise figures and natural noise figures of a MIPMOP device is provided, and the resulting properties are detailed in the impedance and admittance representations. We compute the natural noise figures of a low-noise MIPMOP amplifier comprising a MIMO series-series feedback amplifier (MIMO-SSFA), designed for a wireless receiver front-end.

#### 1. Introduction

In this paper, we consider a linear multiple-input-port and multiple-output-port (MIPMOP) device havinginput ports and output ports, connected to an -port source, such as an array ofcoupled antennas, and to an -port load. The MIPMOP device could be passive, but our motivation lies in the case where it provides amplification. We want to characterize the noise performance of the MIPMOP device in a small bandwidth around a given frequency . The case is covered in detail in the literature since more than 50 years [1, 2] and will be referred to as the two-port case.

The theory and measurement methods developed for the two-port case can be applied to a MIPMOP device only when all the following conditions are met:(i)the MIPMOP device is made of uncoupled two-ports;(ii)the ports of the -port source are uncoupled;(iii)the ports of the -port source are uncoupled.

The first condition is obvious. However, it is important to note that the theory of the two-port case is irrelevant when the second or the third conditions are not met.

Let us for instance consider the multiport antenna array and the multiport wireless receiver shown in Figure 1, which may be used in a multiple-input and multiple-output (MIMO) or single-input and multiple-output (SIMO) wireless communication system. In Figure 1, is the impedance matrix seen by the receiver, and is the input impedance matrix of the receiver. The physical size of the antenna array is often limited by the application, for example in the case of portable transceivers. Antenna coupling may in such a case be so large that the nondiagonal entries cannot be ignored when one computes the directivity patterns and correlations of the channels [3, 4]. A large coupling between the antennas will also impact the noise performance of the receiver front-end because the noise power *delivered* by an input port may excite other input ports via antenna coupling.

A conventional wireless receiver front-end uses a MIPMOP device consisting ofuncoupled two-port low-noise amplifiers (LNAs) presenting a diagonal . Even though the noise figure of each LNA as a two-port can be defined and measured, it gives no information on the true noise performance of the receiver front-end because it does not take the above-mentioned LNA noise coupled through the antenna array into account. This has been investigated by several authors [5–9].

A type of nonconventional wireless receiver front-end uses a MIPMOP passive matching network to obtain a nondiagonal . For instance, a passive lossless MIPMOP device can be used to provide reflectionless matching to its antenna ports (i.e., ) and to uncoupled two-port LNAs at its output [10]. More importantly, a passive lossless MIPMOP device can be used to provide hermitian matching to its antenna ports (i.e., where the star denotes the hermitian adjoint) and hermitian matching to uncoupled two-port LNAs at its output [11–14]. This possibility is very interesting since hermitian matching provides a maximum power transfer and decorrelated output voltages in the case of 2-dimensional Rayleigh channels (because the matching network modifies the directional patterns such that they are orthogonal over the azimuth). This type of passive MIPMOP device can also theoretically be used to obtain noise matching [15, 16]. However, a passive MIPMOP device having a prescribed nondiagonal is a complex circuit in which losses must be taken into account to obtain a realistic design [17, 18]. Such losses degrade the noise performance.

Another type of nonconventional wireless receiver front-end comprises a MIPMOP LNA presenting a nondiagonal [19]. This scheme is new [20]. Also, it offers more flexibility than a design using a passive lossless MIPMOP device having its output ports connected to uncoupled two-port LNAs. Thus, better characteristics are expected with an optimized MIPMOP LNA.

In both nonconventional front-end designs, and are nondiagonal, so that there is no possibility of applying the two-port noise theory to anything. Thus, a noise theory of MIPMOP devices must be used.

In their theory of linear noisy networks, Haus and Adler presented many results which are applicable to MIPMOP devices [21]. However, they did not define an adequate figure of merit, since their purpose was the systematic description of the noise performance of a two-port linear amplifier. More recently, Randa [22] introduced a definition of the noise figures of a MIPMOP device. This definition generalizes the definition used in the two-port case, but it is not directly related to a signal-to-noise ratio.

Randa expressed the noise figures using the S-parameter representation of the device. This formalism is adequate for RF measurements used for the noise characterization of a MIMOP device. However, a noise theory of MIPMOP devices, presented in the impedance and admittance representations, is more appropriate for circuit design. Basic elements of this theory and a validation are available [23]. In this paper, starting from the definitions in Sections 2 and 3, we further develop this noise theory in Sections 3 to 5. In Section 6, this theory is applied to the design of a MIPMOP LNA connected to an array of coupled antennas.

#### 2. Notations

We use rms values throughout the paper. We use to denote the transpose of a matrix to denote the complex conjugate of to denote the hermitian adjoint , and tr to denote the trace of .

In the small bandwidth , we define the column-vector of the input noise currents flowing into the positive terminals of the input ports of the MIPMOP device and the column vector of the input noise voltages between the positive and negative terminals of the input ports. We use and to denote the column vectors of the short-circuit input noise currents and of the open-circuit input noise voltages , respectively. We also define the column vector of the output noise currents flowing into the positive terminals of the output ports and the column vector of the output noise voltages between the positive and negative terminals of the output ports. We use and to denote the column vectors of the short-circuit output noise currents and of the open-circuit output noise voltages , respectively. Let us write

For the case , we obtain the equivalent circuit *a* of Figure 2, consisting of noise voltage sources and one noiseless ()-port. Such an equivalent circuit corresponds to the impedance representation, since
where **Z** is the impedance matrix of the MIPMOP device, of size . Alternatively, we obtain the equivalent circuit shown in Figure 2, consisting of noise current sources and one noiseless ()-port. Such an equivalent circuit corresponds to the admittance representation, since
where is the admittance matrix of the MIPMOP device. We easily obtain

The second-order statistics of the noise produced by the MIPMOP device is determined by the covariance matrix of the open-circuit noise voltages or equivalently by the covariance matrix of the short-circuit noise currents , where the brackets indicate an average over an ensemble of noise processes. The covariance matrices are related by

These relations are important for noise computations because they can be used to switch between the impedance and admittance representations to easily take into account additional series-connected or shunt-connected circuit elements [24, 25].

#### 3. Noise Figures of MIPMOP Devices

In the definition of the noise figure of a two-port, the spectral density of the available power of the noise delivered by the source is where is Boltzmann’s constant and K. In the case of devices having multiple input ports, we have to consider that the noises delivered by the different ports of the -port source may be correlated and may have different noise temperatures.

*Definition 1. *If * α* is an integer such that , the noise figure of the MIPMOP device for the output

*is the ratio of the self-power spectral density at the output*

*α**to the portion of this self-power spectral density that is due to the input noise, evaluated for the case where (a) the available power spectral density of the -port source is and (b) the available power of the noise delivered by the load is zero.*

*α*The noise figures defined above are identical to the one defined by Randa [22] using the scattering representation, except that the condition (a) is not required in his definition. We use this condition because it guaranties that our definition becomes the usual definition in the two-port case, as shown in Section 4.

Let us first assume that the impedance matrix of the source is , that the column vector of the open-circuit noise voltages produced by the source is , and that the impedance matrix of the noiseless load is . We have where is used to denote the null matrix of size . We use (3) and (7) to write Consequently, we have

By (2), we directly obtain so that where is the identity matrix of size . Since by (1), (2), and (7) we have , we can write

Using (9) in (12), we obtain the matrix of the self- and cross-complex powers received by the -port load, in the impedance representation

Let us use and to denote the column vectors of noise voltages and noise currents of the source, respectively. In the case of hermitian matching, we have

Thus, the matrix of the self- or cross-complex powers which the -port source would deliver to a noiseless -port load providing hermitian matching is We therefore have

The available power of the -port source, denoted by , is equal to the real power which it delivers to a noiseless -port load providing hermitian matching [12]. The available power of the -port source is where we have used (14). Thus, where we have used the characteristic noise matrix of the source in the impedance representation [21, chapter 3], defined as

Consequently,in the impedance representation, the noise figure may be written where , and is the entry of row and column of , where is computed for = −tr and where

Alternatively, we can use to denote the admittance matrix of the source, to denote the column vector of the short-circuit noise currents produced by the source, and the admittance matrix of the noiseless load. We have We use (4) and (22) to write

Proceeding as above to obtain (13), we get the matrix of the self- and cross-complex powers received by the -port load, in the admittance representation

The matrix of the self- or cross-complex powers which the -port source would deliver to a noiseless -port load providing hermitian matching is given by

We therefore have

The available power of the -port source is where is the characteristic noise matrix of the source in the admittance representation, given by

Thus, in the admittance representation, the noise figure is given by where and is computed for and

#### 4. Properties of the Noise Figures

The above-defined noise figures of a MIPMOP device do not depend on the particular representation used to express them, since the definition is based on a ratio of real powers. We also note that and do not depend on the representation chosen.

The four following properties indicate that our definition of the noise figures of a MIPMOP device is an adequate generalization of the well-known definition for a two-port.

*Property 1. *In the case , is the noise figure defined for the two-port, which does not depend on or .

*Proof. *For , Definition 1 is the standard definition of for a two-port [22, Section 2.1].

We note that for , using (18), (27) and , we get the usual single-port noise source formulas where the bar indicates the complex conjugate.

*Property 2. *In the case , if the -port source is made of uncoupled and uncorrelated identical single-port sources of internal impedance , if the MIPMOP device is made of uncoupled identical two-ports having the noise figure for the source impedance , and if the -port load is made of uncoupled single-port loads of impedance , then for any *α* such that . Thus, in this case, does not depend on or .

*Proof. *We use (15) and (19) to write
Consequently, for , we have

Let us use to denote the impedance matrix of one of said identical two-ports and to denote an entry of . We have
We also have

Using (20), (33), (35) and (36), after some derivations, we get
which can be shown to be equal to .

The Property 2 indicates that the noise figures given by (20) and (29) are intensive quantities: each noise figure does not change when the number of identical uncoupled systems is changed.

*Property 3. *If a MIPMOP device B is made of a cascade consisting of a lossless passive input network having input ports and output ports, of a MIPMOP device A having input ports and output ports and of a lossless passive output network, then the sum of the noise figures of the MIPMOP device B is equal to the sum of the noise figures of the MIPMOP device A.

*Proof. *This is the direct consequence of the following facts:(i)the lossless passive output network does not change the total real power delivered to the -port load;(ii)the lossless passive input network does not change the available power of the -port source because it is possible to prove (see the appendix) that hermitian matching occurs at its input ports if and only if hermitian matching occurs at its output ports.

*Property 4. *In the configuration considered in the Property 3, if we also require that the lossless passive output network is made of uncoupled lossless passive two-ports, each having an input port connected to the output port *α* of the MIPMOP device A and an output port corresponding to the output port *α* of the MIPMOP device B, then, for any *α* such that , the noise figure of the MIPMOP device B for the output *α* is equal to the noise figure of the MIPMOP device A for the output .

*Proof. *Each lossless passive two-port does not change the real power delivered to each port of the -port load.

The Property 4 is a generalization to MIPMOP devices of a property of noisy two-ports which is a direct consequence of the Friis formula for cascaded noisy two-ports [1, 2]. We note that the configurations considered in the properties 3 and 4 can be used for computing the noise figures of a MIPMOP amplifier consisting of an active MIPMOP circuit inserted between two MIPMOP matching circuits having negligible losses.

Notwithstanding the fact that is a vector, we have to keep in mind that there are three important differences between the usual definition of the noise figure for a two-port and the definition introduced in Section 3 for a MIPMOP device:(i)for each depends on the correlations between the ports of the -port source;(ii)for each depends on the -port load, that is to say, on or on in the case of a linear -port load [23, Section 3];(iii)since there is no obvious generalization of the concept of signal-to-noise ratio to MIPMOP devices, the noise figures of a MIPMOP device cannot be viewed as a direct measure of the degradation of a signal-to-noise ratio.

#### 5. Natural Noise Figures of a MIPMOP Device

We are going to introduce a definition of the *natural noise figures* of the MIPMOP device, based on two properties.

*Property 5. *If the -port source is a noisy passive linear network at the temperature , then the available power spectral density of the -port source is . Additionally, we have

*Proof. *The covariance matrix is hermitian and positive definite, and is hermitian. Consequently [26, Section 7.6.5], there exists a nonsingular matrix such that is real and diagonal and .

As pointed out in [21, page 29], this transformation may be obtained with a lossless imbedding. We may introduce the impedance matrix of the resulting network, the column vector of its open-circuit noise voltages and write
where denotes the diagonal matrix of size having the entries , and where are real. We then introduce the impedance matrix such that

If we use (42) in (40), we find that

Thus, is the impedance matrix of a lossless network. We now connect a lossless network of impedance matrix in series with the network of impedance matrix and obtain a network of impedance matrix
this network having the column vector of the open-circuit noise voltages . We consequently haveuncoupled resistances at the temperature , which proves that are positive and

Using (41), we obtain
Using (40) we then find that

*Property 6. *If the -port source produces the noise of a noisy passive network at the temperature , the constraint (a) of the Definition 1 is automatically satisfied.

*Proof. *If we use (15), (18), and (38), we find that
which proves the property. Alternatively, we could have used (25), (27), and (39), to obtain
and reached the same conclusion.

*Definition 2. *If the -port source produces the noise of a noisy passive network at the temperature , the noise figures of Definition 1 will be referred to as the *natural noise figures*.

In the laboratory, it is possible to use a nearly ideal noisy passive network at the temperature , and to measure natural noise figures in this manner. However, this parameter does not necessarily correspond to the application situation. For instance the noise collected by multiple antennas will in general not comply with (48) and (49).

The following property relates to a special case where the natural noise figures are easier to determine using standard measuring instruments. Let us use(i) to denote the noise figure between an input and an output , defined as the usual noise figure of a two-port, evaluated in the case where all unused inputs and outputs are connected to uncoupled and uncorrelated single-port terminations for which the available power spectral density is ;(ii) to denote the noise figure between an output, used as an input, and an output, defined as the usual noise figure of a two-port, evaluated in the case where all unused inputs and outputs are connected to uncoupled and uncorrelated single-port terminations for which the available power spectral density is.

*Property 7. *In the case where the -port source is made of uncoupled and uncorrelated single-port sources, and where the -port load is made of uncoupled and uncorrelated single-port loads, the natural noise figures are given by

*Proof. *All single-port sources and loads being assumed uncoupled and uncorrelated to each other, let us use

(i) to denote the self-power spectral density at the output * α*, evaluated for the case where (c) the inputs are connected to single-port sources, (d) the available power spectral density of each single-port source is , (e) the outputs are connected to single-port loads, and (f) the available power spectral density of each single-port load is zero;(ii) to denote the self-power spectral density at the output

*, evaluated for the case where (g) the MIPMOP device is noiseless, (c) the inputs are connected to single-port sources, (h) the available power spectral density of each single-port source is zero except the single-port source connected to the input for which the available power spectral density is , (e) the outputs are connected to single-port loads, and (f) the available power spectral density of each single-port load is zero.*

*α*In the case defined above, we have so that

is not the usual noise figure of a two-port, evaluated in the case where all unused inputs and outputs are connected to single-port terminations, because, in this case, the unused single-port loads also contribute to the self-power spectral density at the output . Let us use to denote the self-power spectral density at the output , evaluated for the case where (g) the MIPMOP device is noiseless, (c) the inputs are connected to single-port sources, (j) the available power spectral density of each single-port source is zero, (e) the outputs are connected to single-port loads, and (k) the available power spectral density of each single-port load is zero except the single-port load connected to the output for which the available power spectral density is . We have

So that we obtain

Using (54) in (52) leads us to (50).

Note that in the case where the contribution of the single-port loads to the self-power spectral density at the output is negligible, that is, we may assume that

In [23], (56) was incorrectly presented as an exact formula. However, (56) was a good approximation of the exact formula (50) for the MIPMOP amplifier considered in [23].

#### 6. A MIPMOP LNA Connected to an Antenna Array

We will now apply our results to the 1880 MHz MIPMOP LNA shown in Figure 3, having signal input terminals and signal output terminals. It is intended to be used as a wireless receiver front-end. The core of this MIPMOP LNA is a new circuit called MIMO series-series feedback amplifier (MIMO-SSFA) described below [23, 27, 28]. Referring to the impedance matrices defined in Figure 1, the MIPMOP LNA is designed to provide hermitian matching between and .

The antenna array is a circular array of four parallel half-wave dipole antennas (side-by-side configuration) for 1880 MHz. The radius of the array is 0.3 mm, so that it presents a 0.424 mm spacing between the nearest array elements. This antenna array has been presented in [19]. The impedance matrix of the antenna array is computed as

For a zenithal angle , and if we assume that the array sees four uncoupled scalar loads of 73.0 Ω, the power delivered by each antenna and the average power are shown in Figure 4 as a function of the azimuth for an incident field of 1 V/m peak. The average power oscillates between 3.3 W and 4.2 W as a function of the angle of arrival whereas, in the same field, a single dipole antenna in free space would deliver 4.4 W to a 73.0 Ω load.

We assume that each antenna is connected to the MIPMOP amplifier via a two-conductor interconnection (for instance a coaxial cable) behaving as a two-conductor transmission line. The antenna number is connected to the near-end of the interconnection number of length, characteristic impedance , phase velocity , and attenuation constant . The far-end of the interconnection number is connected to the input port number of the MIPMOP amplifier. Let us define the characteristic impedance matrix of the set of interconnections as

Let us also define the transmission matrix of the set of interconnections as

After some derivation [19], we get

If we assume that four identical 54 mm-long interconnections are used, having, at MHz, a propagation velocity of 0.6 , a characteristic impedance of 80 Ω, and an attenuation of 1.667 dB/m, the resulting impedance matrix seen by the MIPMOP LNA at is equal to

We note that if we compare (57) and (61), the relative difference between diagonal entries is small, but the nondiagonal entries are thoroughly modified.

The MIMO-SSFA consists of active subcircuits (ASC) and a feedback network. Each ASC comprises a packaged low-noise pseudomorphic HEMT (Q311 to Q314) and a drain resistor (R311 to R314) providing resistive loading to improve stability. The feedback network consists of the 4 inductors L411 to L414, coupled by mutual induction. This coupling is the only phenomenon leading to a nondiagonal input impedance matrix. The MIPMOP LNA also comprises an input matching network (C211 to C214 and L221 to L224) and an output matching network (C521 to C524 and L511 to L514).

The MIMOP LNA shown in Figure 3 has been designed in such a way that when each output port is connected to a grounded 50 Ω resistor, the amplifier provides an impedance close to [29, Section 5]. At MHz, the resulting voltage gain matrix of the MIPMOP amplifier and are

The comparison of (61) and (63) shows that hermitian matching is almost exactly reached between the receiver’s end of the interconnections and the inputs of the MIPMOP LNA. We computed the power delivered to each 50 Ω resistor and the average power shown in Figure 5, in the configuration used for Figure 4 [19, Section 8.2].

Assuming that the input and output matching networks are lossless, we have computed the noise figures for three configurations of the MIPMOP amplifier, in a worksheet of a generic calculation program. A technique used several times in this worksheet is the following: (6) being possibly used to obtain the appropriate representation, the covariance matrix of a series or parallel connection of two uncorrelated circuits is obtained as a sum of covariance matrices [24, 25].

In this manner we successively determined:(1)the covariance matrix of the open-circuit voltages of an ASC comprising a transistor and a series drain resistor, this matrix being denoted by (2)the covariance matrix of the open-circuit voltages of the MIMO-SSFA, using and the assumption that the feedback network of the MIMO-SSFA behaves as a noisy passive network at the temperature , so that according to (38) the covariance matrix of the open circuit voltages at the terminals of the feedback network is where is the impedance matrix of the feedback network, the real part of which is determined by losses in the inductors L411 to L414;(3)the noise figures of the MIMO-SSFA, using (20) applied to given by (65);(4)the matrices and of the MIPMOP LNA, once parallel and series circuit elements of the input and output matching networks are included;(5)the noise figures of the MIPMOP LNA, using (20) applied to or (29) applied to .

Since we assume that the input and output matching networks are lossless, we expect that the steps (3) and (5) provide the same result, according to the Property 4. We indeed always obtain the same noise figures, in the three configurations defined below.

In the first configuration, we have canceled the mutual induction between the inductors L411 to L414, the resulting MIPMOP amplifier being driven by a source having a diagonal impedance matrix equal to Ω. Consequently, the four channels are uncoupled. All computed natural noise figures are equal to about 1.134 dB, irrespective of the choice of diagonal load impedance matrix. We checked that in line with the Property 2, this result is the same as the one obtained for one channel treated as a two-port.

In the second configuration, we have kept zero mutual inductances between the inductors L411 to L414, but the input of the resulting MIPMOP amplifier sees the impedance matrix given by (61). All computed natural noise figures are equal to about 1.218 dB, for a load impedance matrix equal to 50 Ω. Consequently, the couplings between the antennas increase the noise figures, as qualitatively explained in the introduction. We also observed that, as expected, these noise figures depend on the choice of the diagonal load impedance matrix.

In the third configuration, the mutual inductances between the inductors L411 to L414 had their nominal values, the MIPMOP amplifier being driven by a source having an impedance matrix equal to given by (61). This configuration is the MIPMOP LNA designed in [29] and used in [19], as said above. In this configuration, all natural noise figures are equal to about 1.896 dB, for a load impedance matrix equal to 50 Ω. We again observed that, as expected, these noise figures depend on the choice of the diagonal load impedance matrix.

It must again be emphasized that, for the second and third configurations, there is no direct relationship between the computed natural noise figures and a measure of the degradation of a signal-to-noise ratio, as pointed out in the introduction and at the end of Section 4.

#### 7. Conclusion

In this paper, we have defined the noise figures of a MIPMOP device in a manner that extends the classical definition applicable to a two-port. This definition has an additional condition compared to the definition used by Randa [22]. When the -port source connected to the input ports of the MIPMOP device is a passive multiport source at , our noise figures are referred to as *natural noise figures,* and the source impedance matrix determines the self- and cross-correlations of the noises applied to the input ports. We have also developed a theory of the noise figures of MIPMOP devices in the impedance and admittance representations.

We have presented an example which shows how this theory can be applied to the design of a MIPMOP LNA connected to an array of coupled antennas and providing hermitian matching. It is worth noting that if mutual induction was not present, Figure 3 would represent four independent single-input and single-output LNA with inductive source degeneration. This scheme is popular because it can simultaneously provide a high gain and a low noise figure [30–33]. Since introducing mutual induction between coils does not involve any additional circuit element, the 4-input and 4-output MIPMOP LNA shown in Figure 3 has the same number of circuit elements as four independent 2-port LNAs with inductive source degeneration.

In the example treated in Section 6, we observe that given by (58) is quite different from given by (63) and given by (57), so that multiple reflections will take place. This phenomenon is inherent to hermitian matching. It does not cause problems when the interconnections between the antennas and the MIPMOP LNA are sufficiently short.

#### Appendix

#### A Theorem on Linear MIPMOP Devices

A linear MIPMOP device having input ports and output ports is characterized by the admittance matrices , and such that where is used to denote the column vector of the input currents, is used to denote the column vector of the output currents, is used to denote the column vector of the input voltages, and is used to denote the column vector of the output voltages. We can also write where is the admittance matrix defined and used in Section 2. If the output ports of the MIPMOP device are connected to an -port load presenting the impedance matrix , the input ports of the MIPMOP device present an admittance matrix which may referred to as the loaded input admittance matrix and is given by If the input ports of the MIPMOP device are connected to an -port source presenting the impedance matrix , the output ports of the MIPMOP device present an admittance matrix which may be referred to as the loaded output admittance matrix and is given by

The real power received by the linear MIPMOP device is given by Thus, the MIPMOP device is lossless if and only if

If we assume that the linear MIPMOP device provides hermitian matching at the input ports, by (A.4) we get If we assume that is invertible, we get

If we now assume that the MIPMOP device is lossless, by (A.7) we get

If we compare (A.5) and (A.10), we find the following theorem on simultaneous hermitian matching at the input ports and at the output ports (bilateral hermitian matching) of a lossless device: if is invertible, hermitian matching at the input ports entails hermitian matching at the output ports. By symmetry, if is invertible, hermitian matching at the output ports entails hermitian matching at the input ports.

We note that this theorem does not use reciprocity.

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