Electronic networks, such as integrated circuits (ICs), are employed to perform a variety of electronic functions, such as filtering microwave or radio frequency signals. In evaluating the performance of a particular network, it may be desirable to measure its electrical accuracy. One manner by which the electrical accuracy of a network can be measured is by determining the scattering parameters (S-parameters) of the network. The S-parameters of a network are indicative of the degree of signal transmission and reflection at the ports of the network.
Typically, to determine the S-parameters of a network, an analysis tool, such as a network analyzer, is used to measure waveform parameters simultaneously at the input and output ports of the network. For example, to measure the waveform parameters at the ports of the network, probes can be utilized to establish electrical contact between the ports and the network analyzer. Establishing electrical contact with probes, however, can be problematic in that the ports of the network may be electrically conductive pads that may be extremely small, such as having a pitch of 250 microns or less. This issue can become compounded in a network having pads located on opposite surfaces of an IC die, package substrate or printed circuit board. Accordingly, to establish a clean and reliable connection with the pads usually requires a high degree of precision.
According to one embodiment of the present invention, a system for determining S-parameters of a network includes an S-parameter calculator that computes the S-parameters of the network based on waveform parameters determined through single port measurements at each of plural ports of the network.
According to another embodiment of the present invention, a system for determining S-parameters of a multi-port network includes a reflection coefficient engine that provides a subset of available reflection coefficients associated with ports of the multi-port network. The system also includes an S-parameter calculator that computes a set of the S-parameters for the multi-port network based on the subset available reflection coefficients provided by the reflection coefficient engine.
According to yet another embodiment of the present invention, a method for determining S-parameters of a network includes determining waveform parameters based on single port measurements performed at plural ports of the network, and determining S-parameters of the network based on the waveform parameters.
According to still another embodiment of the present invention, a computer-readable medium having computer-executable instructions can receive waveform parameters based on single port measurements performed at plural ports of the network, and determine S-parameters of the network based on the waveform parameters.
According to another embodiment of the present invention, a computer-readable medium having computer-executable instructions can determine reflection coefficients based on single port measurements performed at ports of the network, and determine S-parameters of the network based on the reflection coefficients.
The present disclosure relates generally to a system and method for determining S-parameters for an electronic network, which can have two or more ports. A set of reflection coefficients are derived for the network based on waveform parameters. The waveform parameters, for example, can be measured by a network analyzer or other test equipment using single port measurements (e.g., measure parameters at one port while the other port(s) is either open or shorted). The S-parameters of the network can be determined from a subset of the reflection coefficients. According to one embodiment of the present invention, the S-parameters are determined based on those coefficients derived from single port measurements of the network.
In characterizing the DUT 12, the S11parameter is related to signal reflection at the input port P1, which is a function of the input impedance of the DUT, and models how the DUT reflects the input signal V1. The S22 parameter of the DUT 12 is related to signal reflection at the output port P2, which is a function of the output impedance of the DUT in relation to the impedance of the load Z0, and models signal reflection at the output port P2. The S12 parameter models the reverse gain of the DUT 12. The S21parameter is the insertion or forward gain of the DUT 12.
To illustrate operation of the circuit 10, it can include a source 14 that supplies an input signal (e.g., a sine wave at a desired frequency) having a voltage V1 to an input port P1 of the DUT 12. An output port P2 of the DUT 12 provides an output signal V2 based on the input signal V1. In the example of
Waveform parameters (e.g., amplitude or voltage) of the DUT 12 can be measured at the input port P1 and at the output port P2. The waveform parameters include the transmitted portion V1m of the input signal V1, i.e., the portion of the input signal V1 transmitted to the DUT 12 from the source 14. The waveform parameters also include the reflected portion V1pof the input signal V1, i.e., the portion of the input signal V1 reflected back toward the source 14 from the DUT. The waveform parameters can also include the transmitted portion V2m of the output signal V2, i.e., the portion of the output signal V2 transmitted to the load Z0 from the DUT 12, and the reflected portion V2p of the output signal V2, i.e., the portion of the output signal reflected back toward the DUT from the load Z0.
The amplitude of V1p depends on the amount of mismatch between the output impedance of the source 14 and the input impedance of the DUT 12. The amplitude of V1p increases according to the mismatch between the output impedance of the source 14 and the input impedance of the DUT 12. If the input impedance of the DUT 12 and the output impedance of the source 14 are matched and the output impedance and the load Z0 are matched, for example, there will be no reflection of the input signal V1, namely, V1p=0 and V1m=V1/2, assuming the source 14 has a 50 Ohm series resistance.
Similarly, the amplitude of V2p depends on the amount of mismatch between the output impedance of the DUT 12 and the impedance of the load Z0. The amplitude of V2p increases with the mismatch between the output impedance of the DUT 12 and the impedance of the load Z0. If the impedance of the load Z0 and the output impedance of the DUT 12 are matched and the input impedance and the output impedance of the source 14 are matched, there will be no reflection of the output signal V2, namely, V2p=0 and V2m=V2/2, assuming the source 14 has a 50 Ohm series resistance.
The S-parameters of the DUT 12 are related to waveform parameters V1m, V1p, V2m, and V2p, which, for a two port network, can be expressed as follows:
According to an aspect of the present invention, reflection coefficients Γ for the DUT 12 can be determined through single port measurements of waveform parameters of the DUT. The reflection coefficients may then be used to determine the S-parameters of the DUT 12 and reconstruct the S-parameter matrix of Eq. 1. As mentioned above, the waveform parameters are measured at one particular port, such as while the other port(s) are either left open or are shorted.
The following sets forth an example derivation of equations that can be employed to determine the reflection coefficients and the S-parameters through single port measurements:
If the output port P2 is left open, V2m=V2p. This being the case, the S-parameter matrix of Eq. 1 may be reduced to the following:
V1m=S11·V1p+S12·V2p Eq. 2
V2p=S21·V1p+S22·V2p Eq. 3
V2p may be solved as a function of V1p and Eq. 3 can be rewritten as follows:
Eq. 4 can be substituted in Eq. 2 and Eq. 2 can be rewritten as follows:
Eq. 5 can be rewritten to express a reflection coefficient (Γ2open) that represents a ratio of transmission to reflection for the open condition of the output port P2 as follows:
If the output port P2 is shorted, V2m=−V2p. In the shorted condition of the output port P2, the S-parameter matrix of Eq. 1 may be reduced to the following:
V2p may be solved as a function of V1p and Eq. 8 can be rewritten as follows:
Eq. 9 can be substituted in Eq. 7 to provide:
Eq. 10 further can be rewritten to express a reflection coefficient (Γ2short), which represents a ratio of transmission to reflecttion for the shorted condition of the output port P2. Γ2short can be expressed as follows:
If the input port P1 is left open, V2m=V2p. An equation for determining the reflection coefficient with the input port P1 open could be derived in a manner similar to the derivation of Eq. 6, described above. The equations describing the DUT 12 simplify since the DUT in the example of
If the output port P2 is shorted, V1m=−V1p. An equation for determining the reflection coefficient (Γ1short) which is a ratio of transmission to reflection, for the shorted condition of the input port P1 can be derived in a manner similar to the derivation of Eq. 11, described above. Since the DUT 12 is a passive device, as mentioned above, symmetry permits the following equation (Eq. 13) to be extrapolated from Eq. 11, as follows:
Additionally, since the DUT 12 is a passive two-port network, there is no forward or reverse gain, such that S12=S21. Therefore, for a two port network having the S-parameters S11, S12, S21, and S22, any three unknown S-parameters can be employed to solve for the remaining S-parameter. That is, only three of the four Eqs. 6, 11, 12, and 13 are required to calculate the S-parameters of the DUT 12. Thus, it will be appreciated that the S-parameters of the two-port DUT 12 can be determined based on a subset of three of the four single port measurements described above. That is, the complete S-parameter model for the DUT 12 can be computed by employing any three of the four reflection coefficients Γ1open, Γ1short, Γ2open, and Γ2short derived from such single port measurements.
By way of further example, the following illustrates the derivation of equations for determining S-parameters using three of the four determined reflection coefficients, namely Γ1open, Γ2open, and Γ2short. For instance, Eqs. 6, 11, and 12 are used to solve the S-parameter matrix of Eq. 1 for each of the S-parameters S11, S12, S21, and S22. It will be appreciated, however, that any three of the four reflection coefficients Γ1open, Γ1short, Γ2open, and Γ2short and, thus, any corresponding three of Eqs. 6, 11, 12, and 13, could be used to solve the S-parameter matrix of Eq. 1. Similarly, it will be appreciated that the S-parameters can be determined using different combinations of three reflection coefficients, which could allow for averaging or verification of the determined S-parameters.
Solving the S-parameter matrix of Eq. 1 for S22 using Eqs. 6, 11, and 12 produces the following equation:
Combining Eq. 11 and Eq. 12 produces the following:
Solving Eq. 15 for S11 produces the following:
Substituting Eq. 14 into Eq. 16 produces Eq. 17, as follows:
Because the DUT 12 is a passive two-port network (e.g., S12=S21), Eq. 12 can be rewritten as follows:
Eq. 18 can be solved for S12 to produce the following:
S12=(Γ1open−S11·Γ1open−S22+S11·S22)1/2 Eq. 19
Substituting equations 14 and 17 into equation 19 for S22 and S11, respectively, produces Eq. 20 as follows:
In view of the above example derivation, it is demonstrated that selected equations (e.g., Eqs. 14, 17, and 20) can thus be employed to determine the S-parameters S11, S12, S21, and S22 of the DUT 12 based on single port waveform parameter measurements at the respective ports P1 and P2. The determined S-parameters in turn can be used to construct the S-parameter matrix of Eq. 1.
Those skilled in the art will appreciate that various types and configurations of probes exist, and that any such probe can be employed, such depending on the type and configuration of the DUT 12. The source 14 could be separate from the network analyzer 22, as shown in
An S-parameter calculator 30 is operatively associated with the network analyzer 22. The S-parameter calculator 30 is programmed and/or configured to ascertain S-parameters for the DUT 12 based on a subset of possible reflection coefficients derived from single port measurements at ports P1 and P2. For example, the S-parameter calculator 30 can compute the S-parameters by implementing selected equations (e.g., as listed above) based on values measured or otherwise obtained by the network analyzer 22.
The calculator 30 can be implemented as computer executable instructions within the network analyzer 22 or in an associated computer or analysis tool. The S-parameter calculator 30, for example, may take the form of a host computer, such as a PC, or a portion of the network analyzer dedicated to performing S-parameter calculations based on the measured values. Additionally, the S-parameter calculator 30 could even be embodied as manual calculations of the S-parameters based on the values measured by the network analyzer 22.
In an initial configuration of the system 20 shown in the example of
The system 20 of
When the output port P2 is shorted, the network analyzer 22 can measure V1m and V1p at the input port P1 via the probe 24. The S-parameter calculator 30 can determine the reflection coefficient Γ2short (e.g., via implementation of Eq. 11) based on the single port measurement at port P1 while P2 is shorted.
The arrangement of the system 20 of
Additionally, the S-parameter calculator 30 can be programmed and/or configured to compute or otherwise determine the S-parameters S11, S12, S2l , and S22 of the DUT 12 based on at least a subset of the single port measurements identified with respect to
It is to be understood and appreciated that, since the reflection coefficients Γ vary as a function of the waveform parameters, equations employed to define the S-parameters (e.g., Eqs. 14, 17, and 20) could be rewritten in terms of the measured waveform parameters instead of reflection coefficients. As a result, the S-parameters could be determined directly as functions of the measured waveform parameters, without explicitly determining the reflection coefficients.
In view of the above embodiments of
To this point, the present invention has been described mostly in terms of determining S-parameters of a two-port network. It will be appreciated, however, that the system and methodology of the present invention could be implemented to determine the S-parameters of a network having more than two ports. This is because, in a multi-port network where the forward and reverse gain S-parameters are equal, equations for determining the reflection coefficients and thus the S-parameters of the network may be determined. While the determination of such equations may involve complex algebraic and other mathematical operations, the equations are nonetheless ascertainable based on the teachings contained herein.
The S-parameter calculator 42 is operatively connected to a source of data 50, which includes measurement information for a multi-port network. For example, the data 50 includes measurement data (e.g., measured waveform parameters) based on which reflection coefficients can be computed for the multi-port network. The data 50 can be stored in a computer-readable medium, such as a volatile storage device (e.g., RAM, DRAM etc.) or a non-volatile storage device (e.g., a hard disk drive, CD-ROM, etc.). The data can be provided in real time, such as by measurements implemented by a network analyzer or, alternatively, it can be stored for subsequent processing by the S-parameter calculator 42. The S-parameter calculator 42 is operative to construct an S-parameter matrix for the DUT and provide an indication of S-parameters, indicated as 52, based on the measurement data 50.
The S-parameter calculator 42 includes an S-parameter matrix construction engine 60 and a reflection coefficient engine 62. The S-parameter calculator 42 also includes a selector 64 for selecting parameters that define the operations to be performed by the reflection coefficient engine 62. The selector 64 may also select parameters that define the operation of the matrix construction engine 60. For instance, the selector 64 can select an appropriate set of equations 66 based on the user input 46 provided by to user interface 44. The selector 64, for example, may be operable to select from a set of available equations 66, such as those described above (e.g., Eqs. 6, 11, 12, and 13), for determining reflection coefficients of the DUT based on the data 50. Additionally or alternatively, the selector can select appropriate equations from an available set of equations 68 for computing the S-parameters. For example, the equations 66 and 68 can be stored as a library of predetermined equations from which the selector 64 can access necessary equations based on the user inputs 46.
By way of further example, as shown in
A more conservative approach for a two-port network, can employ four of reflection coefficient equations 66 (e.g., Eqs. 6, 11, 12, and 13) to provide multiple sets of S-parameters, which can be correlated or compared to provide error checking and/or averaging. The equation selector 64 may also be operable to select other equations 68, such as those described above (e.g., Eqs. 14, 17, and 20), for determining the S-parameters 52 based on the computed reflection coefficients. The matrix construction engine 60 thus computes the S-parameters based on applying the selected set of equations 66 and 68 to the measurement data 50.
In view of the foregoing structural and functional features described above, a methodology 80 for determining the S-parameters of the DUT 12, in accordance with an embodiment of the present invention, will be better appreciated with reference to
The methodology 80 begins at 82. This can include defining attributes of a DUT (e.g., number of ports, the types and quantities of measurements, etc.). This can result in initializing variables to their starting values and instantiating objects in associated software. At 84, reflection coefficients equations are selected. For a two port network, for example, the reflection coefficients can include Γ1open, Γ1short, Γ2open, Γ2short. The reflection coefficients are selected for use in the determination of the S-parameters of a DUT (e.g., the DUT 12 of
At 86, the reflection coefficients are determined based on the equations selected at 84 using the waveform parameters, such as described above. Alternatively, at 86, all or a selected number of reflection coefficients could be determined based on the waveform parameters available to the system without requiring selection. For example, in determining reflection coefficients for the two-port DUT described above, if waveform parameters sufficient to determine reflection coefficients Γ1open, Γ1short, Γ2open, and Γ2short are available, all four of these reflection coefficients can be determined at 86. If, however, a subset of waveform parameters sufficient to determine only three reflection coefficients are available, then only three reflection coefficients may be determined at 86.
At 88, S-parameter equations are selected. The S-parameter equations enable S-parameters (e.g., S11, S12, S21, S22) of the DUT to be determined. As described above, the S-parameters may be determined through a variety of equations that incorporate different combinations of the reflection coefficients, such as determined at 86. Thus, the number of S-parameter equations selected may vary, depending on factors such as the number of ports of the DUT and the available reflection coefficients, as determined at 86.
At 90, the S-parameters are determined based on the equations selected at 88. Alternatively, the S-parameters could be determined at 90 without requiring selection of S-parameter equations at 88, such as accessing appropriate equations automatically based on the reflection coefficients available methodology 80. For example, in determining S-parameters for a two-port DUT, such as described above, a subset of some or all S-parameter equations can be utilized, which can vary according to the available reflection coefficients. As a result, where more reflection coefficients than needed are available, the S-parameters can be determined at 90 to provide redundant verification of the results and/or averaging. In a situation where a subset of less than all available reflection coefficients exists, fewer available S-parameter equations can still be utilized to ascertain the full S-parameter matrix. At 92, the S-parameters (S11, S12, S21, S22) determined from the equations implemented at 90 are provided. The S-parameters further can be provided at 92 after performing a comparison of the S-parameters that may have been computed based on different sets of reflection coefficients. This comparison can be utilized to provide an indication of the accuracy of the results. The methodology then ends at 94.
What have been described above are examples of the present invention. It is, of course, not possible to describe every conceivable combination of components or methodologies for purposes of describing the present invention, but one of ordinary skill in the art will recognize that many further combinations and permutations of the present invention are possible. Accordingly, the present invention is intended to embrace all such alterations, modifications and variations that fall within the spirit and scope of the appended claims.
This application is related to co-pending and commonly assigned U.S. patent application to Yang et al., which was filed contemporaneously with this application and entitled “SYSTEM AND METHOD FOR DETERMINING S-PARAMETERS USING A MATCHED LOAD,” Attorney Docket No. 200314668-1, the disclosure of which is incorporated herein by reference.