Supplementary text S1 Description of the method to calculate

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Supplementary text S1
Description of the method to calculate confidence limits for excess deaths and age
adjusted excess deaths rates
Let consider:
ο‚·
ο‚·
ο‚·
π‘¦π‘‘π‘Žπ‘” the number of observed deaths in month t (1…12) of flu-year a (1…24) and age
group g (1…8);
πΈπ‘Ž the estimate of the epidemic period of flu-year a
π·π‘Žπ‘” the periods of months where an excess of deaths in π‘¦π‘‘π‘Žπ‘” is attributed to the
epidemic period of flu-year a
1. Compute the monthly rate of deaths adjusted for a 30.4 days month:
π‘¦π‘‘π‘Ž
π‘Ÿπ‘‘π‘Žπ‘” = (
30.4)⁄π‘π‘Žπ‘”
π‘šπ‘‘
2. Compute the time series π‘§π‘‘π‘Žπ‘” = 𝑙𝑛(π‘Ÿπ‘‘π‘Žπ‘” ) in order to stabilize de variance;
∗
3. Compute π‘§π‘‘π‘Žπ‘”
the time series of natural logarithm of the death rare in month t (1…12)
of flu-year a (1…24) and age group g (1…8) without the epidemic periods πΈπ‘Ž , i.e.
∗
π‘§π‘‘π‘Žπ‘”
= {(𝑑, π‘Ž) ∉ πΈπ‘Ž };
∗
4. For each age group g (1…8) a cyclical regression model is fitted to π‘§π‘‘π‘Žπ‘”
, the model is
′
then used to predict the number of deaths for the πΈπ‘Ž periods. A new time series π‘§π‘‘π‘Žπ‘”
is
∗
then build by inputting the missing values of π‘§π‘‘π‘Žπ‘” with cyclical regression model
predictions;
′
5. For each age group g an seasonal ARIMA model is fitted to the time series π‘§π‘‘π‘Žπ‘”
. Then
′
compute the time series π‘§Μ‚π‘‘π‘Žπ‘” representing the fitted values using the adjusted seasonal
ARIMA model will represent the natural logarithm of the monthly death rate baseline
without the effect of the epidemic periods πΈπ‘Ž and the respective upper 95%
′
confidence limit given by π‘§Μ‚π‘‘π‘Žπ‘”
+ 𝑝0.975 πœŽΜ‚π‘’π‘” , where πœŽΜ‚π‘’π‘” is the standard deviation of the
seasonal ARIMA model residuals and 𝑝0.975 the 0.975 percentile of the standard
normal distribution;
6. Log baseline and upper 95% confidence limits are anti log:
′
′
π‘Ÿπ‘‘π‘Žπ‘”
= exp⁑(π‘§Μ‚π‘‘π‘Žπ‘”
)
′
′
π‘Ÿπ‘’π‘π‘‘π‘Žπ‘”
= exp⁑(π‘§Μ‚π‘‘π‘Žπ‘”
+ 𝑝0.975 πœŽΜ‚π‘’π‘” )
7. The π·π‘Žπ‘” are then obtained as the periods included in πΈπ‘Ž where
′
π‘Ÿπ‘‘π‘Žπ‘” > π‘Ÿπ‘’π‘π‘‘π‘Žπ‘”
8. Compute excess rate and absolute excess deaths attributable to influenza epidemics
for (𝑑, π‘Ž, 𝑔) ∈ π·π‘Žπ‘” :
′
Excess rate - 𝑒π‘₯𝑐_π‘Ÿπ‘‘π‘Žπ‘” = π‘Ÿπ‘‘π‘Žπ‘” − π‘Ÿπ‘‘π‘Žπ‘”
Absolute excess deaths - 𝑒π‘₯𝑐_π‘¦π‘‘π‘Žπ‘” = 𝑒π‘₯𝑐_π‘Ÿπ‘‘π‘Žπ‘” × π΄π‘‘π‘Žπ‘”
where π΄π‘‘π‘Žπ‘” =
π‘šπ‘‘ ×π‘π‘Žπ‘”
30.4
9. Compute total excess deaths in the epidemic period πΈπ‘Ž for age group g, i.e. in period
π·π‘Žπ‘” :
Absolute excess deaths in π·π‘Žπ‘” : 𝑒π‘₯𝑐_π‘¦π‘Žπ‘” = ∑𝑑∈π·π‘Žπ‘” 𝑒π‘₯𝑐_π‘¦π‘‘π‘Žπ‘”
10. Compute total excess deaths in epidemic period πΈπ‘Ž (all age groups)
8
𝑒π‘₯𝑐_π‘¦π‘Ž = ∑
𝑔=1
𝑒π‘₯𝑐_π‘¦π‘Žπ‘”
11. Compute age-standardized excess rates for epidemic period πΈπ‘Ž :
8
𝑒π‘₯𝑐_π‘¦π‘Žπ‘”
𝑒π‘₯𝑐_π‘Ÿπ‘Ž = ∑
𝑀𝑔 ×
π‘π‘Žπ‘”
𝑔=1
Where 𝑀𝑔 is the weight of age group g in the reference population used (world population
2000);
12. Confidence interval for the total excess deaths in epidemic period πΈπ‘Ž - 𝑒π‘₯𝑐_π‘¦π‘Ž :
8
𝑒π‘₯𝑐_π‘¦π‘Ž = ∑
𝑔=1
𝑒π‘₯𝑐_π‘¦π‘Žπ‘”
Let start by finding the distribution of 𝑒π‘₯𝑐_π‘¦π‘Žπ‘” , if
′
′
𝑒π‘₯𝑐_π‘¦π‘Žπ‘” = ∑ (π‘Ÿπ‘‘π‘Žπ‘” − π‘Ÿπ‘‘π‘Žπ‘”
) × π΄π‘‘π‘Žπ‘” = ∑ π‘Ÿπ‘‘π‘Žπ‘” π΄π‘‘π‘Žπ‘” − ∑ π‘Ÿπ‘‘π‘Žπ‘”
π΄π‘‘π‘Žπ‘”
𝑑,π‘Ž∈π·π‘Žπ‘”
𝑑,π‘Ž∈π·π‘Žπ‘”
𝑑,π‘Ž∈π·π‘Žπ‘”
Assuming that the observed rates π‘Ÿπ‘‘π‘Žπ‘” are fixed, we only need to find the distribution of
′
∑𝑑,π‘Ž∈π·π‘Žπ‘” π‘Ÿπ‘‘π‘Žπ‘”
π΄π‘‘π‘Žπ‘” .
′
′
2
From the seasonal ARIMA model we know that π‘§Μ‚π‘‘π‘Žπ‘”
∼ 𝑁(π‘§π‘‘π‘Žπ‘”
, πœŽπ‘’π‘”
) so
′
′
′
2
π‘Ÿπ‘‘π‘Žπ‘”
= 𝑒 π‘§Μ‚π‘‘π‘Žπ‘” ∼ πΏπ‘œπ‘” − 𝑁(π‘§π‘‘π‘Žπ‘”
, πœŽπ‘’π‘”
)
and
′
′
2
π΄π‘‘π‘Žπ‘” π‘Ÿπ‘‘π‘Žπ‘”
∼ πΏπ‘œπ‘” − 𝑁(𝑙𝑛(π΄π‘‘π‘Žπ‘” ) + π‘§π‘‘π‘Žπ‘”
, πœŽπ‘’π‘”
)
And by the Fenton and Wilkinson approximation
2
′
′
′ ,𝜎 ′ )
∑ π‘Ÿπ‘‘π‘Žπ‘”
π΄π‘‘π‘Žπ‘” = ∑ π‘¦π‘‘π‘Žπ‘”
∼ β‘πΏπ‘œπ‘” − 𝑁 (πœ‡π‘¦π‘Žπ‘”
π‘¦π‘Žπ‘”
𝑑,π‘Ž∈π·π‘Žπ‘”
𝑑,π‘Ž∈π·π‘Žπ‘”
Where
′
πœŽπ‘¦2π‘Žπ‘”
(𝑒
′ = 𝑙𝑛
2
πœŽπ‘’π‘”
− 1)
∑𝑑,π‘Ž∈π·π‘Žπ‘” 𝑒 2(𝑙𝑛(π΄π‘‘π‘Žπ‘” )+π‘§π‘‘π‘Žπ‘”)
[∑𝑑,π‘Ž∈π·π‘Žπ‘” 𝑒
(
′
𝑙𝑛(π΄π‘‘π‘Žπ‘” )+π‘§π‘‘π‘Žπ‘”
]
2
+1
)
and
′ = 𝑙𝑛 (∑𝑑,π‘Ž∈𝐷
πœ‡π‘¦π‘Žπ‘”
𝑒
π‘Žπ‘”
′
𝑙𝑛(π΄π‘‘π‘Žπ‘” )+π‘§π‘‘π‘Žπ‘”
2
πœŽπ‘’π‘”
⁑) +
2
−
𝜎2′
π‘¦π‘Žπ‘”
2
Consider now:
8
𝑒π‘₯𝑐_π‘¦π‘Ž = ∑
8
𝑒π‘₯𝑐_π‘¦π‘Žπ‘” = ∑
𝑔=1
[∑
𝑔=1
𝑑,π‘Ž∈π·π‘Žπ‘”
8
8
=∑
∑
𝑔=1
𝑑,π‘Ž∈π·π‘Žπ‘”
π‘¦π‘‘π‘Žπ‘” − ∑
π‘¦π‘‘π‘Žπ‘” − ∑
∑
𝑔=1
𝑑,π‘Ž∈π·π‘Žπ‘”
𝑑,π‘Ž∈π·π‘Žπ‘”
′
π‘Ÿπ‘‘π‘Žπ‘”
π΄π‘‘π‘Žπ‘” ] =
′
π‘Ÿπ‘‘π‘Žπ‘”
π΄π‘‘π‘Žπ‘”
Considering that ∑8𝑔=1 ∑𝑑,π‘Ž∈π·π‘Žπ‘” π‘¦π‘‘π‘Žπ‘” is fixed then we must find the distribution of
′
′
′
∑8𝑔=1 ∑𝑑,π‘Ž∈π·π‘Žπ‘” π‘Ÿπ‘‘π‘Žπ‘”
π΄π‘‘π‘Žπ‘” = ∑8𝑔=1 ∑𝑑,π‘Ž∈π·π‘Žπ‘” π‘¦π‘‘π‘Žπ‘”
= ∑8𝑔=1 π‘¦π‘Žπ‘”
.
2
′
′ , 𝜎 ′ ) so:
From the results above we know that π‘¦π‘Žπ‘”
∼ β‘πΏπ‘œπ‘” − 𝑁 (πœ‡π‘¦π‘Žπ‘”
π‘¦π‘Žπ‘”
8
∑
′
π‘¦π‘Žπ‘”
∼ πΏπ‘œπ‘” − 𝑁 (πœ‡π‘¦π‘Ž′ , πœŽπ‘¦2π‘Ž′ )
𝑔=1
Where by the Fenton and Wilkinson approximation
πœŽπ‘¦2π‘Ž′
∑8𝑔=1 𝑒
= 𝑙𝑛
[
2πœ‡π‘¦′ +𝜎2′
π‘Žπ‘”
π‘¦π‘Žπ‘”
(𝑒
𝜎2′
π‘¦π‘Žπ‘”
− 1)
2
πœ‡ ′ +𝜎2′ ⁄2
(∑8𝑔=1 𝑒 π‘¦π‘Žπ‘” π‘¦π‘Žπ‘” )
8
πœ‡π‘¦π‘Ž′ = 𝑙𝑛 (∑
𝑒
𝑔=1
πœ‡π‘¦′ +𝜎2′ ⁄2
π‘¦π‘Žπ‘”
π‘Žπ‘”
)−
+1
]
πœŽπ‘¦2π‘Ž′
2
The 95%confidence limits for 𝑒π‘₯𝑐_π‘¦π‘Ž are computed using the upper 0.975 and lower 0.025
probability quantiles of the Log-N distribution with πΏπ‘œπ‘” − 𝑁 (πœ‡π‘¦π‘Ž′ , πœŽπ‘¦2π‘Ž′ )
13. –Confidence interval for standardized excess rates for epidemic period πΈπ‘Ž :
8
8
𝑒π‘₯𝑐_π‘¦π‘Žπ‘”
𝑒π‘₯𝑐_π‘Ÿπ‘Ž = ∑
𝑀𝑔 ×
= ∑ π‘Šπ‘Žπ‘” × π‘’π‘₯𝑐_π‘¦π‘Žπ‘” =
π‘π‘Žπ‘”
𝑔=1
𝑔=1
𝑀𝑔
Where π‘Šπ‘Žπ‘” = 𝑁
π‘Žπ‘”
8
=∑
8
π‘Šπ‘Žπ‘” π‘¦π‘Žπ‘” − ∑
𝑔=1
′
π‘Šπ‘Žπ‘” π‘¦π‘Žπ‘”
=
𝑔=1
2
′
′ ,𝜎 ′ )
π‘Šπ‘Žπ‘” π‘¦π‘Žπ‘”
~πΏπ‘œπ‘” − 𝑁 (𝑙𝑛(π‘Šπ‘Žπ‘” ) + πœ‡π‘¦π‘Žπ‘”
π‘¦π‘Žπ‘”
Where by the Fenton and Wilkinson approximation
𝑒π‘₯𝑐_π‘Ÿπ‘Ž ~πΏπ‘œπ‘” − 𝑁(πœ‡π‘Ÿ π‘Ž , πœŽπ‘Ÿ2π‘Ž )
πœŽπ‘Ÿ2π‘Ž
∑8𝑔=1 𝑒
= 𝑙𝑛
[
2𝑙𝑛(π‘Šπ‘Žπ‘” )+πœ‡π‘¦′ +𝜎2′
𝑦
π‘Žπ‘”
π‘Žπ‘”
(∑8𝑔=1 𝑒
𝜎2′
π‘¦π‘Žπ‘”
𝑙𝑛(π‘Šπ‘Žπ‘” )+πœ‡π‘¦′ +𝜎2′ ⁄2
𝑦
π‘Žπ‘”
π‘Žπ‘”
8
πœ‡π‘Ÿ π‘Ž = ⁑𝑙𝑛 (∑
(𝑒
𝑒
𝑔=1
− 1)
2
+1
)
𝑙𝑛(π‘Šπ‘Žπ‘” )+πœ‡π‘¦′ +𝜎2′ ⁄2
π‘¦π‘Žπ‘”
π‘Žπ‘”
]
πœŽπ‘Ÿ2π‘Ž
)−
2
The 95%confidence limits for 𝑒π‘₯𝑐_π‘¦π‘Ž are computed using the upper 0.975 and lower
0.025 probability quantiles of the Log-N distribution with πΏπ‘œπ‘” − 𝑁 (πœ‡π‘¦π‘Ž′ , πœŽπ‘¦2π‘Ž′ )
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