CST – Computer Simulation Technology

Electrical Performance of High Speed Signaling in Coupled Microstrip Lines

Differential (DIFF) transmission lines are perhaps one of the most commonly used passive interconnect structures for high speed data transmission. Typically there are two configurations of DIFF transmission lines used to transfer signals in printed circuit boards (PCBs) and/or packages: stripline and microstrip line. A stripline represents a guiding structure which provides a pure transverse electromagnetic (TEM) mode of propagation. The transmission line is shielded between two metal layers (typically the power and ground plane), and therefore also provides excellent performance in terms of EMC/EMI. A microstrip line is routed on a dielectric substrate and referenced to a ground plane. Because of the inhomogeneous substrate/air interface, only a quasi TEM propagation mode develops in the line. This can produce larger signal degradation in high speed signals and also cause higher radiation levels because of the absence of shielding....

In this work [1], the modal propagation characteristics and the corresponding effect on the signal integrity (SI) performance of a coupled DIFF microstrip line pair is analyzed. First, a test prototype is built for model-to-hardware correlation. The DIFF net is 15 inches long, 4.7 mils wide, has a copper thickness of 1.18 mils and it is routed on the bottom layer of a 10-layer PCB, as illustrated in Figure 1 along with the port numbering.

Figure 1: Test board used for the correlation study with the DIFF microstrip line highlighted

Due to the complexity of the original board and for the purpose of only validating the numerical code, a small section around the DIFF net of interest is chosen. This assumption is no longer valid in presence of very dense routing nets in combination with small dimensions and at very high frequencies. However in this particular case the impact of the size of the power structure on the numerically evaluated results is negligible.

An nth higher order Debye model is used to model the electrical properties of the dielectric substrate (4 points were originally available). Surface roughness was also taken into account by means of the Hammerstad and Jensen formulation based on the calculation of an additional element for the attenuation coefficient, which results in an increased value for the metal losses. Results of the calculated S-parameters are illustrated in Figure 2 and a very good agreement between measured data and CST MICROWAVE STUDIO® (CST MWS) simulation results is achieved in the considered frequency range 0-12 GHz.

Figure 2: Measured vs. simulated S-parameters: return loss (S11), insertion loss (S21), NEXT (S31) and FEXT (S41)

A ‘dip’ (cancellation frequency) can be observed in the insertion loss profile at around 6.7 GHz in the single-ended (SE) excitation case. On the other hand, the mixed mode (DIFF) insertion loss shows a straight profile, as shown in Figure 3. The fairly large difference between the modal group delays of the even/odd modes for the DIFF pair can also be observed.

Figure 3: Insertion loss (S21) for SE excitation vs. mixed mode DIFF excitation (left), Even and odd-mode group delay (right)

This behavior is related to the fact that the even and odd modes propagate at different speeds due to the non-homogenous nature of the microstrip interconnect. As these two independent modes propagate along the line, there are locations and frequencies, where the phase difference will reach odd multiples of 180 degrees. At these frequencies and locations a cancellation of the nodal voltages is observed. By computing the modal propagation delay difference, multiplying by the trace length and calculating the mean of the result as a general approximation for all frequencies, a certain delta propagation delay (tpd) for the entire trace length can be obtained. The cancellation frequencies (fr), can be calculated by the following approximation [2]:

fr = (2n+1) / 2tpd

Applying the above formula to the measured group delay results for the test board gives a delta propagation delay of 75 ps which equates to a cancellation frequency of 6.67 GHz. This agrees very well with the measured/simulated value of 6.7 GHz as shown in Figure 2-3.

In order to gain further insight into the dip in the SE insertion loss response of the DIFF microstrip line, a simplified version of the original geometry is developed as shown in Figure 4. The DIFF microstrip traces are designed for a differential impedance of 100 ohms with a trace width of 0.3 mm, a spacing of 0.7 mm, conductor (copper) thickness of 1 oz and a substrate (FR-4, permittivity = 4.3) thickness of 30 mils. The trace length considered is 3.15 inches while the board size is 3.94 × 0.4 inches.

Figure 4: Section of the simplified DIFF microstrip trace geometry

The simulated SE S-parameter results for the simplified DIFF trace demonstrate a significant dip in the insertion loss curve at around 9.64 GHz (not shown). This model is henceforth used as a baseline for the subsequent sensitivity analysis. It should be noted that a solder mask layer with a variable thickness and dielectric permittivity is added to the base model for future simulations.

The first parametric study looks at the effect of varying the permittivity of the solder mask material within a range of 1-10. The thickness of the solder mask layer is fixed at 3.93 mils. From the SE insertion loss results presented in Figure 5 the cancellation frequency is seen to shift higher in frequency as the permittivity of the solder mask is increased. For permittivity values of 7 and greater it is pushed out beyond the 20 GHz frequency range of interest and results in a straight insertion loss profile.

Figure 5: SE insertion loss for different solder mask permittivity (eps_solder) values

This behavior can be explained by observing the modal group delay for the even and odd modes. The SE insertion loss curves for the base model (Case A) and the case where the solder mask dielectric constant is set to a value of 8 (Case B) are plotted together in Figure 6 for clarity along with the respective group delay curves for the even and odd modes. It can be observed that including a high permittivity solder mask layer causes a significant decrease in the odd mode phase velocity while the even mode phase velocity also decreases by a smaller amount. The net effect is that the group delay for the two modes ends up being almost equal for Case B. Based on these results the delta propagation delay for Case A is calculated to be 53.76 ps which corresponds to a cancellation frequency of 9.3 GHz. This is in agreement with the simulated result of 9.64 GHz. Similarly, the delta propagation delay for Case B is found to be 9.8 ps which corresponds to a cancellation frequency of 51 GHz. This frequency lies outside the frequency band of interest thereby resulting in a straight insertion loss profile for this case as seen in Figure 6.

Figure 6: SE insertion loss for Case A and Case B (left), Corresponding group delay curves for the even and odd modes (right)

By observing the propagation phase for the two modes as shown in Figure 7 for Case A and Case B, a 180 degree phase difference at 9.64 GHz for Case A can be observed which corresponds to the location of the cancellation frequency. However for Case B there is a negligible phase difference between the two modes within the simulated frequency range.

The second parametric sweep looks at the effect of varying the thickness of the solder mask layer. A permittivity of 4.3 which matches the permittivity of the substrate is used for this set of simulations. As can be observed from the SE insertion loss results presented in Figure 8, the cancellation frequency is increased as the solder mask layer thickness increases. This is due to the fact that a thicker solder mask layer with a sufficiently high permittivity value will encapsulate a larger portion of the fields associated with the odd propagation mode and therefore reduce the odd mode propagation velocity. This in turn reduces the difference between the even and odd mode phase velocities resulting in a lower delta propagation delay value which translates to a higher cancellation frequency as shown earlier.

The effect of varying the spacing between the DIFF traces is investigated next. No solder mask layer is considered for these simulations. It can be seen (Figure 8) that the cancellation frequency increases as the spacing between the traces is increased. This is because the coupling between the traces decreases as the spacing increases and this reduced coupling results in reduction in the difference between the even and odd mode phase velocities thereby leading to a lower delta propagation delay value. This is turn causes the cancellation frequency to increase.

Figure 7: Group delay (phase) curves for the even and odd modes for (a) Case A (b) Case B

Figure 8: SE insertion loss for different solder mask thickness (t_mask) values (top), SE insertion loss for different spacing (gap) values (bottom)

Finally, the variation of the differential impedance of the DIFF traces as a result of the three sensitivity studies is shown in Figure 9. It can be seen that the variation in the DIFF impedance is relatively small for the cases where the solder mask permittivity and the thickness are changed. However there is a large variation for the case where the gap between the DIFF traces is changed. These results demonstrate that the differential impedance is less sensitive to the electrical properties of the solder mask layer than to changing the spacing between the DIFF traces. Therefore careful selection of the dielectric material and thickness of the solder mask layer can help improve the insertion loss response of coupled microstrip DIFF pairs, thereby leading to improved signal integrity performance.

Figure 9: DIFF trace impedance for variable solder mask permittivity (top left), solder mask layer thickness (top right), DIFF trace spacing (bottom)


[1] D. Kostka, A.C. Scogna, F. Paglia, B. Mutnury, "Electrical performance of high speed signaling in coupled microstrip lines," in Proc. of IEEE Electrical Performance of Electronic Packaging and Systems (EPEPS), 2011.

[2] G. Blando, G. Miller, I. Novak, “Losses induced by asymmetry in differential transmission lines,” in Proc. of DesignCon, 2007.

Rate this Article

0 of 5 Stars
5 Stars
4 Stars
3 Stars
2 Stars
1 Stars
contact support

Your session has expired. Redirecting you to the login page...

We use cookie to operate this website, improve its usability, personalize your experience, and track visits. By continuing to use this site, you are consenting to use of cookies. You have the possibility to manage the parameters and choose whether to accept certain cookies while on the site. For more information, please read our updated privacy policy

Cookie Management

When you browse our website, cookies are enabled by default and data may be read or stored locally on your device. You can set your preferences below:

Functional cookies

These cookies enable additional functionality like saving preferences, allowing social interactions and analyzing usage for site optimization.

Advertising cookies

These cookies enable us and third parties to serve ads that are relevant to your interests.