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Consequently, the effective reproduction factor 28 becomes Figure 5. This yields a time-independent constant effective reproduction factor.

Since d 0 is positive, the exponential effective reproduction factor at time t 0 34 is greater than unity and provides an approximation for the exact one Figure 4. Figure 4. For comparison, the thin lines show the approximant Figure 5. Gamma-shaped R t 33 compared with the approximate R t 37 red, dashed , using a box-shaped serial interval distribution W s , and the RKI formula Here, we address the question on how relevant it is to take into account the correct shape of serial interval distribution when calculating R t via With the Gaussian evolution 1 and the box-shaped serial interval distribution 36 inserted, we obtain with the help of This aspect is worked out in detail in Appendix 4.

As before, it is useful to consider a regime of exponential growth to come up with a simple approximant for R 0 , now using a box-shaped W s. Inserting the exponential time evolution 7 with constant d 0 and the box-shaped serial interval distribution 36 into Equation 23 , we obtain the time-independent constant effective box reproduction factor that serves an approximant for R 0 ,. As already mentioned, the box-shaped serial interval distribution is better not used to estimate R 0.

It significantly underestimates the R 0 obtained with the gamma serial distribution. The RKI estimates an effective reproduction factor from the daily measured number i t of people that have been recognized to be infected as follows. Here, we again use the continuous version. Because measured data is not available for the future and is not sufficiently reliable if collected within the time frame of a few days, the RKI estimates R t for a time t that lies one 8 days the past.

A connection between 40 and the true effective reproduction number is based on the assumption that the true number of cases is proportional to the measured ones at any time. Using the GM instead of measured numbers for i t , the estimated true number of cases deaths or infections in Equation 40 yields. With 41 at hand, one can predict the RKI version of R t at all times during the first wave of a pandemic. A time of interest is when R drops below unity.

It is this feature of the RKI, shared with the R t for the gamma serial distribution, that may have given rise to the choice of the interval length of 4 days in its definition. Figure 6. The R t factors obtained using i the box-shaped W s and ii the RKI formula greatly overestimate the R t using a gamma-shaped serial interval distribution at times beyond the peak time. Alternative representation of the data already shown in Figure 5. The mismatch increases with decreasing w. A typical w is in the range between 15 and 20 days for most countries [ 1 ] cf.

The Gauss model for the time evolution of the first corona pandemic wave rendered useful in the estimation of peak times, amount of required equipment, and the forecasting of fade out times. At the same time, it is probably the simplest analytically tractable model that allows to quantitatively forecast the time evolution of infections and fatalities during a pandemic wave.

For these descriptions and forecasts, various descriptors, such as doubling times and reproduction factors are currently used in order to judge lockdowns and other non-pharmaceutical measures that aim to prevent spreading of the virus. As different definitions of doubling times and reproduction factors and numbers are used in the literature, we have provided in this manuscript both exact and simple approximate relationships between the two relevant parameters of the Gauss model peak time t max and width w as well as the transient behavior of two versions of doubling times and three variants of reproduction factors R t , including basic reproduction numbers R 0.

Regarding doubling times, we considered both differential doubling times calculated from the daily number of cases and cumulative doubling times calculated from the cumulative case rates. The former differential doubling time is positive for times earlier than the peak time and monotonically increases in the course of time until it diverges as it approaches the peak time.

For later times after the peak time, the differential doubling time is formally negatively valued but corresponds to positively valued half-life. Because of the divergence at the peak time and its negative value beyond, differential doubling times are of limited use only before the peak time of the outburst; instead, in the public discussion, cumulative doubling times are often preferred.

As opposed to doubling times calculated from daily rates, doubling times derived from cumulative numbers of cases are strictly positive, monotonically increase in the course of time, but never diverge, and remain finite at and after the peak time. At times below the peak time, the two doubling times have a similar behavior.

However, the Gaussian cumulative doubling time for times after the peak time is only a formal indicator for the decreasing slope of the cumulative rate of cases. This implies that only the maximal cumulative doubling time 0. Because of these two drawbacks of differential and cumulative doubling times in characterizing the time evolution of the corona wave after its peak time, health agencies, such as the German Robert-Koch-Institute RKI instead refer to the effective reproduction factor of the disease R t , which is the number of cases infected in the current state of a population by a single individual infected person.

As long as this factor remains smaller than unity the number of infections per day decreases with time. The effective reproduction factor is calculated from an integral involving the serial interval distribution W s normalized to unity and the differential case time distribution.

For the GM, the latter is known analytically, and we investigated three different effective Gaussian reproduction factors: i the first is calculated with a gamma-function type serial interval distribution, ii the second is calculated with a flat box-shaped serial interval distribution, and iii the third, referred to as RKI estimate, involves the ratio of two consecutive 4-days time intervals of the monitored daily cases.

All three discussed effective reproduction factors, calculated with the GM, decrease from the base reproduction number R 0 at the beginning of the pandemic wave to very small values at times much larger than the peak time. As the approximated RKI estimate for Germany still, many weeks after the peak times of the infection and death rates, occasionally indicates effective reproduction factors greater than unity, this has to be due to short intraday fluctuations of the rates.

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