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**Atmospheric Chemistry and Physics**
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**Research article**
17 Apr 2019

**Research article** | 17 Apr 2019

Deriving stratospheric age of air spectra using an idealized set of chemically active trace gases

^{1}Institute for Atmospheric and Environmental Sciences, Goethe University Frankfurt, Frankfurt am Main, Germany^{2}Deutsches Zentrum für Luft- und Raumfahrt (DLR), Institut für Physik der Atmosphäre, Oberpfaffenhofen, Germany^{3}Meteorological Institute Munich, Ludwig Maximilian University of Munich, Munich, Germany

^{1}Institute for Atmospheric and Environmental Sciences, Goethe University Frankfurt, Frankfurt am Main, Germany^{2}Deutsches Zentrum für Luft- und Raumfahrt (DLR), Institut für Physik der Atmosphäre, Oberpfaffenhofen, Germany^{3}Meteorological Institute Munich, Ludwig Maximilian University of Munich, Munich, Germany

**Correspondence**: Marius Hauck (hauck@iau.uni-frankfurt.de)

**Correspondence**: Marius Hauck (hauck@iau.uni-frankfurt.de)

Abstract

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Analysis of stratospheric transport from an observational point of view is frequently realized by evaluation of the mean age of air values from long-lived trace gases. However, this provides more insight into general transport strength and less into its mechanism. Deriving complete transit time distributions (age spectra) is desirable, but their deduction from direct measurements is difficult. It is so far primarily based on model work. This paper introduces a modified version of an inverse method to infer age spectra from mixing ratios of short-lived trace gases and investigates its basic principle in an idealized model simulation. For a full description of transport seasonality the method includes an imposed seasonal cycle to gain multimodal spectra. An ECHAM/MESSy Atmospheric Chemistry (EMAC) model simulation is utilized for a general proof of concept of the method and features an idealized dataset of 40 radioactive trace gases with different chemical lifetimes as well as 40 chemically inert pulsed trace gases to calculate pulse age spectra. It is assessed whether the modified inverse method in combination with the seasonal cycle can provide matching age spectra when chemistry is well-known. Annual and seasonal mean inverse spectra are compared to pulse spectra including first and second moments as well as the ratio between them to assess the performance on these timescales. Results indicate that the modified inverse age spectra match the annual and seasonal pulse age spectra well on global scale beyond 1.5 years of mean age of air. The imposed seasonal cycle emerges as a reliable tool to include transport seasonality in the age spectra. Below 1.5 years of mean age of air, tropospheric influence intensifies and breaks the assumption of single entry through the tropical tropopause, leading to inaccurate spectra, in particular in the Northern Hemisphere. The imposed seasonal cycle wrongly prescribes seasonal entry in this lower region and does not lead to a better agreement between inverse and pulse age spectra without further improvement. Tests with a focus on future application to observational data imply that subsets of trace gases with 5 to 10 species are sufficient for deriving well-matching age spectra. These subsets can also compensate for an average uncertainty of up to ±20 % in the knowledge of chemical lifetime if a deviation of circa ±10 % in modal age and amplitude of the resulting spectra is tolerated.

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Hauck, M., Fritsch, F., Garny, H., and Engel, A.: Deriving stratospheric age of air spectra using an idealized set of chemically active trace gases, Atmos. Chem. Phys., 19, 5269–5291, https://doi.org/10.5194/acp-19-5269-2019, 2019.

1 Introduction

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Stratospheric meridional circulation, referred to as Brewer–Dobson circulation (BDC), is a key process for the comprehension of air mass transport throughout the atmosphere. The spatial distributions and atmospheric lifetimes of various greenhouse gases and ozone-depleting substances, such as halocarbons, are strongly influenced by this large-scale motion (Butchart and Scaife, 2001; Solomon et al., 2010). Therefore, the BDC affects not only the chemical composition of the stratosphere but also the radiative budget of the complete atmosphere. The BDC is a combination of a residual mean circulation with net mass flux and eddy-induced isentropic bidirectional mixing (Plumb, 2002; Shepherd, 2007; Butchart, 2014). Air is transported mainly through the tropical tropopause and then advected to higher latitudes, where it eventually descends. Primary drivers are tropospheric planetary- and synoptic-scale Rossby waves that propagate upward and transfer their momentum by breaking in the extratropical middle stratosphere (Haynes et al., 1991; Holton et al., 1995). At the same time, this wave drag induces stirring processes that are especially enhanced in this “surf zone” (McIntyre and Palmer, 1984). It has been shown that the tropical upward mass flux has a distinct seasonal cycle with a maximum during northern hemispheric (NH) wintertime, when wave excitation is largest (Rosenlof and Holton, 1993; Rosenlof, 1995).

A problem that arises especially regarding observational investigation of
the stratospheric circulation is the impossibility of direct measurements of
the underlying dynamics, i.e., slow overturning circulation. However, a
suited tool for quantification, which can be derived from observations of
chemically very long-lived trace gases and directly compared to model
results, is the concept of mean age of air (AoA; Hall and Plumb, 1994;
Waugh and Hall, 2002). Mean AoA can be understood as the average period of
time that elapsed for an air parcel at any arbitrary location since passing
a certain reference point. Usually, the reference is either earth's surface
or the tropical tropopause layer. Mean AoA provides not only insight into
the current overall strength of the BDC but also allows for an
investigation of temporal changes. If the circulation intensity varies over
time, the value of mean AoA will also show this trend but will be inversely
proportional (Austin and Li, 2006). Different models predict an enhanced
stratospheric circulation indicated by a negative trend of mean AoA (Garcia
and Randel, 2008; Li et al., 2008; Oman et al., 2009; Shepherd and
McLandress, 2011) in response to strengthened wave drag by rising greenhouse
gas concentrations. On the other hand, sparse observationally derived mean
AoA from balloon-borne SF_{6} and CO_{2} data by Engel et al. (2009)
show an insignificant positive change between 1975 and 2005 in northern
midlatitude stratosphere above 24 km altitude. Recently, this trend is
further affirmed by Engel et al. (2017), where existing data are extended
and still show an insignificant trend for the same spatial region. Ray et
al. (2014) reexamined these data of SF_{6} and CO_{2} using a
simplified tropical leaky pipe model and even found a statistically
significant positive trend in mean AoA at similar ranges of altitude and
latitude as Engel et al. (2009). The analyses of satellite data by
Stiller et al. (2012) and Haenel et al. (2015) additionally indicate
that the temporal changes in mean AoA exhibit hemispheric asymmetries.
Analysis of in situ trace gas measurements of N_{2}O, O_{3} and model
trajectories by Bönisch et al. (2011) suggest an increased tropical
upwelling combined with an enhanced transport from the tropical into the
extratropical lower stratosphere. These results suggest that the strength
of the BDC is not changing uniformly. Similar findings are presented by
Hegglin et al. (2014) using merged satellite H_{2}O data. In fact,
Birner and Bönisch (2011) propose a separation of the residual mean
circulation into two distinct branches conveying air from the tropics into
the extratropics. The shallow branch is mainly effective in the lower
stratosphere, while air in the middle and upper stratosphere is primarily
affected by the deep branch. Since more recent studies of models (Okamoto
et al., 2011; Oberländer-Hayn et al., 2015), reanalyses (Monge-Sanz et
al., 2013; Abalos et al., 2015) and observations (Ray et al., 2014; Haenel
et al., 2015; Engel et al., 2017) still exhibit some inconsistencies about
possible future changes in the strength of the circulation pathways, further
analyses are necessary. Recent studies of model and satellite observations
also suggest that a southward (Stiller et al., 2017) and upward
(Oberländer-Hayn et al., 2016) shift of the BDC might be key factors
for these inconsistencies.

For an even more thorough analysis of stratospheric transport, the usage of a full transit time distribution is of advantage. The interaction of mean residual transport and bidirectional mixing as well as the influence of shallow and deep branch is expressed in this distribution, which is also referred to as age spectrum (Hall and Plumb, 1994; Waugh and Hall, 2002). At any given point in the stratosphere, the age spectrum denotes the fraction of fluid elements in an air parcel that had a certain transit time from the reference point to the chosen location. It can be considered a probability density function (PDF), with the mean AoA being the first moment of this distribution. An important advantage is that changes in the different ranges of transit times of the BDC can be visualized with a comparison of age spectra at different points in time. Variations of the shallow branch influence the age spectrum mostly at short transit times (ca. 1 to 2 years – Birner and Bönisch, 2011), whereas changes in the deep branch influence mostly at long transit times (ca. 4 to 5 years – Birner and Bönisch, 2011). Additionally, the effect of aging by mixing (Garny et al., 2014) on the tail of the spectrum may also be assessed during such an analysis. In model experiments, the age spectrum can be gained via periodically occurring pulses of a chemically inert trace gas. For mean AoA, either a linearly increasing chemically inert trace gas or the mean of the age spectrum can be applied. In reality, only few very long-lived trace gases exhibit a linear trend in the first approximation and can be utilized to gain mean AoA (Andrews et al., 2001a). When deriving mean AoA from observations of very long-lived trace gases with non-linear increase, however, assumptions about the shape of the age spectrum are required, where mostly the pioneering work of Hall and Plumb (1994) is considered. The underlying age spectrum for this calculation is only an approximation, which might not be representative in all cases and could bias the inferred mean AoA. A directly inferred complete age spectrum may constitute an improvement and could give further insight into transport processes. This information might be extracted from mixing ratios of long- and short-lived trace gases in an air parcel, as for such species, residual transport, mixing and chemical depletion are inevitably associated with each other. The state of depletion of these gases provides an estimate of the elapsed transit time since passing the reference point. In addition, trace gases with varying chemical depletion are only sensitive to certain transport pathways and thus contribute mainly to the age spectrum for transit time ranges up to their respective chemical lifetime (Schoeberl et al., 2000, 2005). The complete age spectrum may then theoretically be derived as a combination of those pieces of information, provided that a sufficient number of distinct mixing ratios are known. Since the amount of air parcels with transit times larger than 10 years is likely to be low even in the uppermost part of the stratosphere, trace gases with lifetimes of up to 10 years should be sufficient for retrieving a meaningful age spectrum. That makes short-lived trace gases a suitable tool, as a variety of species with diverse lifetimes were frequently measured during past airborne research campaigns. Unfortunately, to the best of our knowledge, there are only few publications about possible techniques to finally convert the information of the mixing ratios of short-lived trace gases into stratospheric age spectra (Schoeberl et al., 2005; Ehhalt et al., 2007) and none that include seasonality in transport. When analyzing seasonal variation in stratospheric dynamics by inferring age spectra from observations, though, a proper consideration of the seasonal cycle is also required to achieve reliable results.

This paper presents an application and evaluation of a modified version of the method by Schoeberl et al. (2005; Schoeberl's method) with a reduced set of fit parameters and an imposed seasonal cycle to account for seasonality in stratospheric transport. The modified technique is applied as a proof of concept to an idealized simulation of the ECHAM/MESSy Atmospheric Chemistry (EMAC) model (Jöckel et al., 2006, 2010). Section 2 provides insight into the method and the model simulation. In Sect. 3, resulting age spectra and related quantities are analyzed and assessed with respect to future application to observational data. Finally, there is a summary, conclusion and outlook in Sect. 4.

2 Methodology

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A frequent basis for the estimation of age spectra, which is also utilized in
Schoeberl et al. (2005) and Ehhalt et al. (2007), is the mathematical
description of a mixing ratio *χ*(** x**,

$$\begin{array}{}\text{(1)}& \mathit{\chi}\left(\mathit{x},t\right)=\underset{\mathrm{0}}{\overset{\mathrm{\infty}}{\int}}\mathit{\chi}\left({\mathit{x}}_{\mathrm{0}},t-{t}^{\prime}\right)\cdot {e}^{-{\scriptscriptstyle \frac{{t}^{\prime}}{\mathit{\tau}\left({t}^{\prime}\right)}}}\cdot G\left(\mathit{x},t,{t}^{\prime}\right)\cdot \mathrm{d}{t}^{\prime}.\end{array}$$

Here, *t*^{′} is the transit time through the stratosphere, $\mathit{\chi}\left({\mathit{x}}_{\mathrm{0}},t-{t}^{\prime}\right)$ the mixing ratio time series at the tropical
tropopause (entry mixing ratio), *τ*(*t*^{′}) the chemical
lifetime and $G\left(\mathit{x},t,{t}^{\prime}\right)$ the age spectrum. Usually, a PDF is integrated from
−∞ to ∞, but since negative transit times are physically
undefined for our analysis, zero is taken instead. To simplify the derivation,
a constant annual mean entry mixing ratio $\stackrel{\mathrm{\u203e}}{{\mathit{\chi}}_{\mathrm{0}}}=\stackrel{\mathrm{\u203e}}{\mathit{\chi}({\mathit{x}}_{\mathrm{0}},t-{t}^{\prime})}$ is assumed. This keeps the balance between a physically
accurate description and practicability for observational studies, since
time series of short-lived species at the tropical tropopause are hard to
attain. Equation (1) then becomes

$$\begin{array}{}\text{(2)}& \mathit{\chi}\left(\mathit{x},t\right)=\stackrel{\mathrm{\u203e}}{{\mathit{\chi}}_{\mathrm{0}}}\cdot \underset{\mathrm{0}}{\overset{\mathrm{\infty}}{\int}}{e}^{-{\scriptscriptstyle \frac{{t}^{\prime}}{\mathit{\tau}\left({t}^{\prime}\right)}}}\cdot G\left(\mathit{x},t,{t}^{\prime}\right)\cdot \mathrm{d}{t}^{\prime}.\end{array}$$

One of the first approaches to obtain the age spectrum from such an equation
in an unidimensional case without chemical loss was made by Hall and Plumb
(1994). In their study, the vertical diffusion equation with a constant
diffusion coefficient was used to calculate the distribution as Green's
function in response to a Dirac delta distribution at the tropical
tropopause. The result is an inverse Gaussian PDF that describes transport
reasonably well. Their results show moreover that the ratio of the second
and first moment of the age spectrum is rather constant in certain
stratospheric regions, a relationship that is still used for the
observational estimation of mean AoA from SF_{6} or CO_{2}.
Mathematically, the age spectrum in Hall and Plumb (1994) is described as
follows:

$$\begin{array}{}\text{(3)}& G\left(z,{t}^{\prime}\right)={\displaystyle \frac{z}{\mathrm{2}\sqrt{\mathit{\pi}K{t}^{\prime \mathrm{3}}}}}\cdot {e}^{\left({\scriptscriptstyle \frac{z}{\mathrm{2}H}}-{\scriptscriptstyle \frac{K{t}^{\prime}}{\mathrm{4}{H}^{\mathrm{2}}}}-{\scriptscriptstyle \frac{{z}^{\mathrm{2}}}{\mathrm{4}K{t}^{\prime}}}\right)},\end{array}$$

with *K* as the constant diffusion coefficient, *z* as the vertical coordinate and
*H* as the scale height of the air density *ϱ*. The latter can either be
gained from an density-altitude fit ($\mathit{\varrho}={\mathit{\varrho}}_{\mathrm{0}}\cdot {e}^{-\frac{z}{H}}$)
or approximated by a constant value. The first moment
Γ (i.e., mean) and the central second moment Δ^{2} (i.e., variance) are then defined as (Hall and Plumb, 1994)

$$\begin{array}{}\text{(4)}& {\displaystyle}& {\displaystyle}\mathrm{\Gamma}\left(z\right)=\underset{\mathrm{0}}{\overset{\mathrm{\infty}}{\int}}G\left(z,{t}^{\prime}\right)\cdot {t}^{\prime}\cdot \mathrm{d}{t}^{\prime},\text{(5)}& {\displaystyle}& {\displaystyle}{\mathrm{\Delta}}^{\mathrm{2}}\left(z\right)={\displaystyle \frac{\mathrm{1}}{\mathrm{2}}}\cdot \underset{\mathrm{0}}{\overset{\mathrm{\infty}}{\int}}G\left(z,{t}^{\prime}\right)\cdot ({t}^{\prime}-\mathrm{\Gamma}(z){)}^{\mathrm{2}}\cdot \mathrm{d}{t}^{\prime}.\end{array}$$

Transfer of Eq. (3) to complex stratospheric
transport is quite difficult, as Hall and Plumb (1994) state that their
inverse Gaussian solution for one-dimensional diffusion is restricted to
long-lived trace gases (Holton, 1986; Plumb and Ko, 1992) in a setup with
only annual mean transport. In such cases, the diffusion coefficient *K* has
to be considered to be a measure of net vertical advection and mixing rather than
simply small-scale diffusion. Their age spectra therefore do not incorporate
any seasonal or inter-annual variability in transport. Model studies of
annual and seasonal age spectra (Reithmeier et al., 2008; Li et al., 2012a, b; Ploeger and Birner, 2016) have shown that age spectra
exhibit multiple modes representing seasonal fluctuations of stratospheric
transport (see Sect. 2.2). However, even though the inverse Gaussian
solution of Hall and Plumb (1994) does not include multiple peaks
intrinsically and might not provide a perfect solution at any point in the
stratosphere, it can certainly provide a robust approximation of the general
(smoothed) shape of these multimodal spectra in models (e.g., Fig. 3 in
Li et al., 2012a, Fig. 7 in Li et al., 2012b, or Fig. 5 in Ploeger and
Birner, 2016). A prescribed age spectrum shape, even if only a fit, is
indeed valuable for observational studies with very limited data. If the
general shape is well constrained a priori, all information from trace gases
measurements will solely be used to tune the spectrum until it is as close
as possible to real transport. Approaches of this kind require fewer data
than cases with a fully unconstrained shape, where more information about
transport processes is needed. Together with the relatively low amount of
free parameters of the inverse Gaussian distribution in Hall and Plumb
(1994), these are important factors of why Eq. (3)
has been the basis of many studies focusing on the retrieval of age spectra
from observational data.

Ehhalt et al. (2007) used the formalism of Hall and Plumb (1994) to
derive a method where mixing ratios of short-lived trace gases are
correlated against those of very long-lived ones. This correlation is
identical to a vertical profile in a trace-gas-based coordinate system.
Technically, the method can also be applied using other vertical coordinates
such as altitude, pressure or potential temperature as long as there is an
exponential decay in the vertical space. In order for this to work, a
height-independent chemical lifetime has to be assumed, as Eq. (2) only then turns into a Laplace transform of
the age spectrum and makes for a constant vertical diffusion coefficient.
This is quite an elegant approach, since it allows for an analytical
solution of the equation. The study concluded that the resulting age spectra
from data between 30 and 35^{∘} N in the lowermost
stratosphere are most probably valid for transit times of up to 1 year.
Application of Ehhalt's method is restricted to this very narrow region
around the subtropical and midlatitude tropopause. Complete global
stratospheric transport, though, cannot be described by a height-independent
diffusion coefficient and constant chemical depletion. Schoeberl et al. (2000) had already proposed a generalized solution to this problem by
discretizing Eq. (2) for long-lived trace gases
with chemistry along an average Lagrangian path and solving the
corresponding system of linear equations. This strategy does not require a
prescribed age spectrum, but our tests with the method show that the matrix
that has to be inverted is close to singular and does not lead to
numerically stable solutions even considering appropriate solvers. In a very
recent study by Podglajen and Ploeger (2019), this method is modified
leading to a stable matrix inversion and promising results. Schoeberl et
al. (2005) took a different approach by allowing both
transit-time-dependent lifetimes and a vertically varying diffusion
coefficient in the age spectrum of Hall and Plumb (1994). They insert Eq. (3) into Eq. (2),
replace *t*^{′} by $({t}^{\prime}-{t}_{\mathrm{off}})$, and perform a multiparameter least-squares
fit on *z*, *K* and *t*_{off} to find a matching age spectrum by minimizing
the sum of squared deviations between the observed and inverted trace gas
mixing ratio in their model. The temporal offset *t*_{off} is introduced to
incorporate the effect that diffusion does not show an instantaneous
response to advected trace gases. In comparison to Ehhalt's method,
Schoeberl's method provides major advantages, as it is still straightforward
to use but with a less restrictive approximation of ongoing physical
mechanisms. It holds a much larger area of applicability in the
stratosphere. A similar approach for long-lived trace gases (deseasonalized
CO_{2}) has been applied by Andrews et al. (1999) with reasonable
results.

There are, however, two points concerning the method's formulation that are
worthy of discussion. First, the vertical coordinate *z* should be
considered to be a measure of position in the atmosphere to ensure that the
result represents the age spectrum exactly at the given location. We propose
excluding it from the fit so that all information about transport is
inverted into the time- and space-dependent diffusion coefficient
*K*(** x**,

$$\begin{array}{ll}{\displaystyle \frac{\mathit{\chi}\left(\mathit{x},t\right)}{\stackrel{\mathrm{\u203e}}{{\mathit{\chi}}_{\mathrm{0}}}}}:=R& {\displaystyle}=\underset{\mathrm{0}}{\overset{\mathrm{\infty}}{\int}}{e}^{-\frac{{t}^{\prime}}{\mathit{\tau}\left({t}^{\prime}\right)}}\cdot {\displaystyle \frac{z}{\mathrm{2}\sqrt{\mathit{\pi}K(\mathit{x},t){t}^{\prime \mathrm{3}}}}}\\ \text{(6)}& {\displaystyle}& {\displaystyle}\cdot {e}^{\left(\frac{z}{\mathrm{2}H}-\frac{K(\mathit{x},t){t}^{\prime}}{\mathrm{4}{H}^{\mathrm{2}}}-\frac{{z}^{\mathrm{2}}}{\mathrm{4}K(\mathit{x},t){t}^{\prime}}\right)}\cdot \mathrm{d}{t}^{\prime}.\end{array}$$

The ratio of measured mixing ratio and entry mixing ratio will from now on
be called *R*. This is the main equation for the modified inverse method.
The transport parameter
*K*(** x**,

$$\begin{array}{}\text{(7)}& \underset{\mathrm{0}}{\overset{\mathrm{\infty}}{\int}}G(\mathit{x},{t}^{\prime},t)\cdot \mathrm{d}{t}^{\prime}=\mathrm{1}.\end{array}$$

The inverse method yields the important benefit that the procedure can be
applied to punctual data rather than complete vertical profiles of mixing
ratios (Ehhalt's method). This is particularly relevant for observational
data, since complete vertical profiles at a fixed latitude are hard to
retrieve from airborne measurements. By using the inverse method, every data
point can be evaluated separately and provides information without depending
on values above or below it. The modified inverse method allows for a
sophisticated analysis of stratospheric transport by providing a possibility
to estimate age spectra from short-lived trace gases with reduced numerical
effort. We tested the applicability of Ehhalt's method within the model
setup of this paper and found results that are in accordance with Ehhalt et
al. (2007). As the method proves to be indeed restricted to the lowest part
of the stratosphere, we decided not to consider it further on. All methods
discussed here are limited to a transit-time-independent transport parameter
*K*(** x**,

When studying seasonal variability in transport processes, it was already
mentioned that the tropical upward mass flux has a distinct seasonal cycle,
with a clear maximum during NH wintertime and a minimum in NH summer
(Rosenlof, 1995). This cycle is also visible in age spectra, as recent
transport model studies have shown (e.g., Reithmeier et al., 2008; Li et
al., 2012a; Ploeger and Birner, 2016). The annual mean shape of the pulse
spectra is well approximated by an inverse Gaussian distribution with one
obvious mode. But age spectra for single seasons show several modes
representing the variable flux of mass into stratosphere during the
different seasons. This is an important feature, especially for species with
a seasonal cycle (e.g., CO_{2}). The inverse method does not reproduce
those multiple peaks intrinsically when inferring seasonal mean spectra,
since Eq. (3) is the formulation of a monomodal
inverse Gaussian PDF. The amplitude of the age spectra is likely to differ
in all four seasons as a feedback to seasonal variability in trace gas
mixing ratios but yet is only monomodal.

A possible approach to derive a multimodal spectrum for a specific season is
to scale the age spectrum in Eq. (6)
appropriately. Rosenlof (1995) found that the strength of the tropical
mass flux into the stratosphere across the tropical tropopause at 70 hPa has
its maximum in NH winter and its minimum in NH summer. The strength of this
upward mass transport is reflected in the maxima and minima of the age
spectrum. Knowing how the upward mass flux varies within a year might be
used to adjust the age spectrum of a specific season. On the basis of the
first three columns of Table 4 in Rosenlof (1995), the average ratio of
the mass flux in each season relative to the remaining three is derived, which is, for instance, winter relative to summer etcetera. The intrinsic
monomodal spectrum of each season will then be adjusted using these flux
ratios at every point in transit time. When considering, for example, an
arbitrary monomodal summer spectrum, its amplitude has to be modulated by
approximately +25 % for transit times that correspond to spring and
fall and by circa +60 % for transit times that represent winter
according to the flux ratio. For every transit time in between a proper
intermediate ratio has to be applied. Finally, no scaling takes place at
transit times that correspond to the respective season of the spectrum
(summer in the example – see down below for further detail). All this can
be realized mathematically by a cosine, which is phase shifted to fit for a
specific season. That results in the definition of a transit-time-dependent
scaling factor *S* for each season:

$$\begin{array}{}\text{(8)}& S\left({t}^{\prime}\right)=\left(A+B\cdot \mathrm{cos}\left({\displaystyle \frac{\mathrm{2}\mathit{\pi}}{\mathrm{365}\phantom{\rule{0.25em}{0ex}}\text{days}}}\cdot {t}^{\prime}+C\right)\right).\end{array}$$

Herein, *A*, *B* and *C* denote constant factors that are only depending on
the considered season. Due to the fact that increasing transit time is
equivalent to going back in time, NH winter (December–January–February or
DJF) is followed by NH fall (September–October–November or SON), then NH
summer (June–July–August or JJA) and finally NH spring (March–April–May or
MAM). In order to estimate the uncertainty of the tropical upward mass flux
in Rosenlof (1995), the dataset is compared to data of the ERA-Interim
reanalysis (Dee et al., 2011), the MERRA-2 reanalysis (Gelaro et al.,
2017), the JRA-55 reanalysis (Kobayashi et al., 2015), the NCEP CFSR
reanalysis (Saha et al., 2010) and also the EMAC simulation. The
resulting tropical upward mass fluxes at 70 hPa are shown in
Fig. 1a. The relative seasonal cycle is quite similar
throughout all datasets although the absolute values differ, with EMAC
having the strongest mass flux and Rosenlof (1995) the weakest. EMAC is
also the only case where the maximum is situated in SON rather than DJF, but
only with a small difference. Since it is only of interest for Eq. (8) how the seasons scale relative to each other,
all data show that this behavior appears to be quite similar. The scaling
components *A* and *B* are derived in such a way that they provide a robust
approximation of the seasonal cycle in Rosenlof (1995). The resulting
constants are depicted together with the phase shift *C* in Table 1.
When approximating the combined data of all reanalyses and
EMAC similarly, the resulting scaling factors agree within 15 % with the
scaling factor of the Rosenlof (1995) data. The scaled age spectrum
${G}_{\mathrm{seas}}(\mathit{x},{t}^{\prime},t)$ is then given by

$$\begin{array}{ll}{\displaystyle}{G}_{\mathrm{seas}}\left(\mathit{x},{t}^{\prime},t\right)& {\displaystyle}={\displaystyle \frac{z}{\mathrm{2}\sqrt{\mathit{\pi}K(\mathit{x},t){t}^{\prime \mathrm{3}}}}}\cdot {e}^{\left(\frac{z}{\mathrm{2}H}-\frac{K\left(\mathit{x},t\right){t}^{\prime}}{\mathrm{4}{H}^{\mathrm{2}}}-\frac{{z}^{\mathrm{2}}}{\mathrm{4}K\left(\mathit{x},t\right){t}^{\prime}}\right)}\\ {\displaystyle}& {\displaystyle}\cdot \left(A+B\cdot \mathrm{cos}\left({\displaystyle \frac{\mathrm{2}\mathit{\pi}}{\mathrm{365}\phantom{\rule{0.25em}{0ex}}\text{days}}}\cdot {t}^{\prime}+C\right)\right)\\ \text{(9)}& {\displaystyle}& {\displaystyle}=G\left(\mathit{x},{t}^{\prime},t\right)\cdot S\left({t}^{\prime}\right).\end{array}$$

As above, it is always ensured that the integral of the consequent spectrum ${G}_{\mathrm{seas}}(\mathit{x},{t}^{\prime},t)$ satisfies Eq. (7). The age spectrum ${G}_{\mathrm{seas}}(\mathit{x},{t}^{\prime},t)$ is manually normalized (${G}_{\mathrm{seas}}^{N}(\mathit{x},{t}^{\prime},t)$) after the scaling process by

$$\begin{array}{}\text{(10)}& {G}_{\mathrm{seas}}^{N}\left(\mathit{x},{t}^{\prime},t\right)={\displaystyle \frac{{G}_{\mathrm{seas}}(\mathit{x},{t}^{\prime},t)}{{\int}_{\mathrm{0}}^{\mathrm{\infty}}{G}_{\mathrm{seas}}(\mathit{x},{t}^{\prime},t)\cdot \mathrm{d}{t}^{\prime}}}.\end{array}$$

It is mandatory that *t*^{′} must be given in days in Eqs. (8) and (9) for a
correct result. A year is approximated only by 365 days. Fig. 1b illustrates the evolution of the complete scaling
factor *S* with transit time during 1 year. All scaling factors equal 1
for transit times 0 years and all integer multiples of 1 year (i.e., 2, 3 years,
etc.). In that way, the spectrum of the considered season remains
unmodified within its season of origin during the scaling process and is
then only altered when re-normalizing the whole spectrum uniformly. As
intended, JJA has the weakest upward mass transport of the year, with all
other seasons being scaled up relatively, while DJF exhibits the strongest
flux with downscaling during every other season. The intermediate periods
MAM and SON display a similar scaling only with the phase shift that was
striven for by introducing parameter *C*. Besides this, the scaling factor
correctly shows its desired maximum on any curve at transit times that
represent DJF, whereas the corresponding minimum always appears at summer
transit times. When inserting this new formulation into the basic equation of the
inverse method (Eq. 6), the modified version
becomes

$$\begin{array}{}\text{(11)}& {R}_{\mathrm{seas}}=\underset{\mathrm{0}}{\overset{\mathrm{\infty}}{\int}}{e}^{-{\scriptscriptstyle \frac{{t}^{\prime}}{\mathit{\tau}\left({t}^{\prime}\right)}}}\cdot {G}_{\mathrm{seas}}^{N}(\mathit{x},{t}^{\prime},t)\cdot \mathrm{d}{t}^{\prime}.\end{array}$$

The numerical procedure to find a matching age spectrum is described in Appendix A. Implementing both Eqs. (11) and (6), it can be estimated whether the seasonal cycle distorts the result or contributes to a better approximation of the pulse age spectra with respect to seasonality. In theory, the annual mean spectrum should be equivalent in both versions of the inverse method if the imposed seasonal cycle works correctly. The lowermost stratosphere is hereby likely to be a critical region where tropospheric air also enters through the extratropical tropopause. This mechanism violates the assumption of a single entry through the tropical tropopause, which is the basis of the inverse method. Transport through the extratropical tropopause also exhibits a distinct seasonal cycle, especially in the Northern Hemisphere (Appenzeller et al., 1996), possibly leading to wrongly scaled spectra when using the scaling factor presented above. The inverse method is thus likely to produce distorted age spectra when applied in this critical region. The seasonal cycle is not included in the fitting procedure as a free parameter but imposed based on mean values of the tropical upward transport. The inverse method is also not able to incorporate any temporal variabilities in the seasonality of the flux.

The use of model data for a general proof of concept of the method's capabilities is very suitable, since the idealized setup yields the advantage of lifetimes being independent of transit time and transport pathways. Scientific focus in this study is on the method's potential to capture stratospheric transport with its underlying assumptions in a solely dynamical model setup. The model of choice is EMAC, being a potent and very well-performing chemistry climate model which has been used in many studies regarding stratospheric transport and chemistry.

The ECHAM/MESSy Atmospheric Chemistry (EMAC) model is a numerical chemistry
and climate simulation system that includes sub-models describing
tropospheric and middle atmosphere processes and their interaction with
oceans, land and human influences (Jöckel et al., 2010).
It uses the second version of the Modular Earth Submodel System (MESSy2) to link
multi-institutional computer codes. The core atmospheric model is the
fifth-generation European Centre Hamburg general circulation model
(Roeckner et al., 2006). For the present study we applied EMAC (ECHAM5
version 5.3.02, MESSy version 2.53.0) in the T42L90MA resolution, i.e., with
a spherical truncation of T42 (corresponding to a quadratic Gaussian grid of
approximately 2.8^{∘} by 2.8^{∘} in latitude and longitude) with 90 vertical
hybrid pressure levels up to 0.01 hPa. The free-running time-slice
simulation covers a period of 20 model years and is performed without
chemistry and ocean models, i.e., sea surface temperatures and radiatively
active trace gases are prescribed. This is a valid approach, since the study
focuses on transport of passive trace gases as well as conceptual tests of
the inverse method. As a lower boundary, observations of sea surface
temperatures and sea ice concentrations from the Hadley Centre Sea Ice and
Sea Surface Temperature dataset (HADISST) are fixed at monthly mean values
averaged from 1995 to 2004. Additionally, greenhouse gases are prescribed at
the constant value of year 2000. The climatology is therefore set to the
state of the year 2000 and has no temporal trend over the whole model
period. Still, seasonal and inter-annual variability is present. Here,
monthly and zonal average data are used and analyzed from December of year 9
to November of year 19. All data in this range are then finally averaged
with respect to seasons, on the one hand, and annually, on the other hand, over
the complete period of 10 years to gain solid statistics.

In order to retrieve age spectra from the model itself, 40 chemically
completely inert trace gases are included that are released as a pulse every
3 months at the tropical surface between 12.5^{∘} N and
12.5^{∘} S, starting in January of year 1. After 10 years, every
pulse tracer has been pulsed once, the cycle starts again with resetting
the first tracer back to 0 in October of year 9, it is pulsed again in
January of year 10, etc. From this period on, complete age spectra that
range over the full period of 10 years can be inferred by creating a map of
the boundary impulse response (BIR) for every point on the model grid. This
concept is first described by Haine et al. (2008) and refined for
transient simulations by Ploeger and Birner (2016). An illustration of
such a map from our EMAC simulation is shown in Fig. 2, where a horizontal
cut (backward in source time) through the complete map gives the age
spectrum at a specific field time. This provides an age spectrum with a
temporal resolution of 3 months. Finer resolutions would require further
pulse tracers (120 for a resolution of 1 month) and are numerically
expensive. Li et al. (2012a) presented a sophisticated simulation with 12 pulse
tracers released in every month of 1 model year simulated over 20 years
field time, which is then cyclically repeated to cover a period of 20 years
source time. This computationally efficient procedure provides
seasonal age spectra with a high temporal resolution of 1 month by
neglecting inter-annual variability in the spectra. The simulation presented
in this paper, however, features inter-annual variability. To keep the
balance between numerical costs and scientific value, a resolution of 3 months
in source time is selected as being the absolute minimum for an
investigation of seasonality, where each season is represented by one point
per year of transit time. Together with the pulse tracers, a linearly
increasing completely inert trace gas (clock tracer) is implemented to
derive the mean AoA as a lag time that the surface mixing ratio needs to
reach an arbitrary location in the stratosphere. In general, the clock
tracer mean AoA will be larger than the first moments of the intrinsic pulse
tracer age spectra. This is a direct consequence of the transit time being
limited to 10 years. The tail of the age spectrum is underestimated and an
extension is required. The formulation by Ploeger and Birner (2016),

$$\begin{array}{}\text{(12)}& G\left(\mathit{x},{t}^{\prime},t\right)=\left\{\begin{array}{ccc}G\left(\mathit{x},{t}^{\prime},t\right)& \mathrm{for}& {t}^{\prime}<\mathrm{10}\phantom{\rule{0.25em}{0ex}}\text{years}\\ G\left(\mathit{x},{t}_{\mathit{\omega}}^{\prime},t\right)\cdot {e}^{-{\scriptscriptstyle \frac{({t}^{\prime}-{t}_{\mathit{\omega}}^{\prime})}{\mathit{\omega}}}}& \mathrm{for}& {t}^{\prime}>\mathrm{10}\phantom{\rule{0.25em}{0ex}}\text{years}\end{array}\right.,\end{array}$$

is applied to all seasonal pulse spectra to correct them for transit times up to 300 years
(see Appendix A). *ω* is a scale time derived from an exponential fit of
the age spectrum between ${t}_{\mathit{\omega}}^{\prime}$ and 10 years transit time.
${t}_{\mathit{\omega}}^{\prime}$ is set to 5 years as threshold for the fit, in
accordance with Ploeger and Birner (2016). The extended age spectra are
then normalized to be mathematically correct.

For the application of the inverse method, a further set of 40 trace gases
is included with prescribed constant lifetimes ranging from 1 month up to
118 months by steps of 3 months. This simplification allows for an
investigation of the method's basic principle by eliminating the variability
in chemical depletion. These trace gases are constantly released in the same
source region as the pulse tracers with a mixing ratio of 100 %. Figure 3
visualizes annual mean vertical profiles of five of these radioactive
tracers at 85, 55 and 10^{∘} N relative to
the tropopause. The dashed line marks the level of 10 hPa, where multiple
short-lived trace gases have a mixing ratio of less than 10 %. As this is
critically close to the accuracy of the inversion, no reliable information
will be gained by the respective tracers. 10 hPa marks the upper boundary
for the analysis in this paper. The maxima are located above the tropopause
at extratropical latitudes, which is not intuitive, since one would expect them
to be within the tropopause layer. This might be caused by an inhomogeneous
distribution of these trace gases in the troposphere due to their sole
initialization in the tropical boundary layer in combination with
cross-tropopause transport. Since their mixing ratio is lower in the
extratropical troposphere than in the tropics (source region), mixing of
this air mass into the corresponding region of the stratosphere could be
the cause of the reduced burden in the extratropical tropopause layer.
Profiles in the Southern Hemisphere exhibit a qualitatively identical
behavior (not shown).

A problem for the comparison of the spectra is that all pulse spectra are
referred to earth's surface, whereas the inverse method uses the tropical
tropopause as a reference layer. When trying to refer inverse spectra to the
surface, results broaden significantly and do not match the pulse spectra.
This is likely a consequence of the solution given by Hall and Plumb
(1994) that uses one-dimensional diffusion to approximate transport above
the tropopause and might not be sufficient for application in the tropical
troposphere. Still, to make the spectra comparable, the annually averaged
mean AoA from the clock tracer at the tropical tropopause is derived for the
evaluated field time period. It is considered to be the mean transit time
from surface to the tropopause within the model. This quantity
(∼0.19 years) is then subtracted from all clock tracer mean AoA
as well as transit times of the pulse age spectra, ensuring that the first
transit time value is still 0 years. Resulting negative values are omitted. The
tropopause is directly extracted from EMAC for the complete analysis, with
the exact definition being described in Jöckel et al. (2006). To
reduce errors in spectra, mean AoA and variance when approaching the
tropopause, data are omitted up to 30 K above the tropopause, as this is
described as a transition layer with major tropospheric influence (Hoor et
al., 2004; Bönisch et al., 2009). Possible inadequacies of the inverse
method and of the artificial seasonal cycle in the lowermost stratosphere
(see Sect. 2.2) are incorporated by introducing a threshold of 1.5 years of
clock mean AoA for the evaluation of the inverse method. The clock tracer
provides the most accurate intrinsic value of mean AoA available in the
model. Above the threshold, the tropopause is reasonably far off and
seasonality should, in theory, mostly be steered by the tropical upward mass
flux. In the model data, the tropical region is defined as average between
12.5^{∘} N and 12.5^{∘} S to be consistent with the source
region of the pulse and radioactive tracers. The entry mixing ratios for the
inverse method are derived within this area as annual mean values.

Atmospheric pressure is in general not a suitable choice when investigating
transport processes and especially mixing. In the stratosphere,
bidirectional stirring occurs mainly parallel to isentropic surfaces, which
makes potential temperature the best choice for such a study. To include an
adequate description of all transport mechanisms, the local potential
temperature difference to the tropopause is calculated for every
stratospheric model grid point and used as vertical coordinate *z* for the
inverse method. The scale height *H* is then fitted properly along this
introduced coordinate.

3 Results

Back to toptop
The following section provides the results of the model study to evaluate
the performance of the inverse method. Annual and seasonal spectra are
presented for three different pressure levels (70, 10 and 140 hPa)
in the midlatitudes at 55^{∘} N for pulse and inverse spectra,
the latter being presented with and without the seasonal cycle. This is a major region of
interest, where both branches of the BDC are present and mixing is
especially enhanced due to wave breaking. Many observational campaigns focus
specifically on the northern midlatitudes with abundant trace gas
measurements. Age spectra are derived in this specific region in order to
deeply understand ongoing transport processes. In the second part, the first and
second moments of the distributions are shown to compare resulting spectra
on a larger scale, both annual and seasonal. The moments are derived using
Eqs. (4) and (5)
and constitute a suitable analytical tool, since an inverse Gaussian PDF can
be well approximated by its mean and width. The width of a spectrum around
its first moment is computed as the square root of the spectrum's variance.
There is also a brief analysis of the ratio of the second to first moment
($\frac{{\mathrm{\Delta}}^{\mathrm{2}}}{\mathrm{\Gamma}}$ or ratio of moments), which
is used to infer mean AoA from measurements of very long-lived trace gases.
The pulse and inverse spectra's performance is assessed and evaluated with
respect to the results of Hall and Plumb (1994). Finally, tests of
applicability to observational data are presented, which include the number
of trace gases necessary for the inversion as well as an estimation of how
uncertainties in the knowledge of chemical lifetimes influence resulting age
spectra and might be compensated.

Figure 4 shows age spectra at 70 hPa and 55^{∘} N. Since 70 hPa is
the origin of the tropical upward mass flux, the seasonal cycle should in
theory work best on this pressure surface. The annual mean inverse spectrum
without a seasonal cycle (dashed–dotted line in panel a) complies
well with the annual pulse spectrum (black solid line), with slightly
reduced amplitude and overestimated tail. The modal age (transit time at
maximum) of the inverse spectrum agrees qualitatively with the modal age of
the pulse spectrum. Including the seasonal cycle into the spectrum (dashed
line in panel a) does not noticeably alter the annual mean curve,
as it exhibits nearly identical modal age and amplitude. This is an
indicator that the formalism of the seasonal cycle modifies the seasons but
cancels out the annual average. The seasonal pulse spectra (solid curves in
panels b to e) indicate that the seasonal cycle of
tropical upward transport is important at this pressure level as multiple
distinct maxima and minima are evolving with deviating modal ages. The
inverse spectra without a seasonal cycle (dashed–dotted – panels b
to e) also show diminished amplitudes for all seasons but still
approximate the pulse spectra quite reliably. Yet the inverse spectra
without a seasonal cycle do not reflect transport seasonality due to their
prescribed monomodal shape, and a comparison of modal ages with the
multimodal seasonal pulse spectra is not useful. When including the seasonal
cycle, however, the results (dashed – panels b to e)
coincide remarkably with the pulse spectra, exhibiting equivalent minima and
maxima at according transit times, but still with slightly enhanced tails
and underestimated amplitudes (especially SON). The timing of modal ages for
the different seasons agrees with the pulse spectra within 0.1 years, and
the resemblance of the amplitudes has also increased. The transit time of
the secondary and ternary peaks are then prescribed with 1 year of distance
and match the pulse spectra qualitatively well. It seems that the prescribed
seasonal cycle constitutes a reasonable choice for describing seasonality in
transport at this altitude. Also, it is evident that exclusion of *t*_{off}
in the formalism of the inverse method still leads to matching spectra, all
with a similar offset. Clock mean AoA values range between 2.51 years (maximum
– DJF) and 1.92 years (minimum – JJA) and are located above the threshold of
1.5 years (see Sect. 2.3).

Age spectra around the previously defined upper boundary (10 hPa) of the
inverse method at 55^{∘} N are depicted in Fig. 5. At this pressure
level, the tail of the spectrum is important to fully describe transport.
Annual mean inverse spectra with and without a seasonal cycle (panel a)
show a similar performance, both with underestimated amplitude
and enhanced tail with respect to the pulse spectra, but no significant
differences between them. Also, the imposed cycle leads to similar modal
ages for the annual mean spectra. Qualitative agreement of the annual
inverse spectra with the annual mean pulse spectrum is nevertheless fairly
good, although the modal age does not agree with the pulse peaks. Again, the
inverse spectra derived here show an offset without explicit inclusion of
*t*_{off}, similar to that found in the pulse spectra. The inverse spectra
without a seasonal cycle (dashed–dotted – panels b to e)
exhibit only small differences between their seasonal amplitudes. Since the
annual mean of inverse and pulse spectra are very similar, it is likely that
the seasonal pulse spectra would show a similar behavior if smoothed. The
inverse spectra without a seasonal cycle show, just as in Fig. 4 for the 70 hPa
level, underestimated amplitudes and slight overly pronounced tails.
Again, a comparison of modal ages between the monomodal inverse and
multimodal pulse spectra is not useful. Including the seasonal cycle (dashed
– panels b to e), the resulting spectra prove to be
similar to the pulse spectra only with slightly enhanced peaks for transit
times greater than 4 years, which is probably a consequence of the coarse
resolution of the spectra or of the scaling factor overestimating the actual
influence of the tropical upward mass flux. The modal ages of the inverse
spectra's maxima agree with the pulse spectra within up to 0.15 years. Some
minor peaks appear between 1 and 2 years of transit time in the inverse
spectra, which are not found in the pulse spectra. On the one hand, this may be caused by the
coarse temporal resolution of the pulse spectra. On the
other hand, the minor peaks could be an artefact in the inverse spectra due
to the prescribed cycle. Again, the seasonal cycle provides an improvement
such that the inverse spectra concur reasonably with the pulse spectra in
this region of the stratosphere in contrast to monomodal spectra. The
corresponding clock mean AoA values range from 5.42 years (maximum – SON) to
5.16 years (minimum – DJF) and are clearly above the threshold of 1.5 years
(see Sect. 2.3).

Finally, age spectra for the lower stratosphere on the 140 hPa level are
shown in Fig. 6. The temporal resolution of 3 months in the pulse spectra is
quite critical for an evaluation in the lower stratosphere. The annual mean
inverse spectrum without the seasonal cycle (dashed–dotted – panel a) fits the annual mean pulse spectrum (solid line) very well,
exhibiting qualitatively similar amplitude and modal age. An exact
comparison of the modal age is not useful due to very small transit times
and comparatively large uncertainties. As above, the tail of the inverse
spectrum seems to be slightly overestimated compared to the pulse spectrum.
It is evident that now all seasonal pulse age spectra (solid – panels b to e) display a very similar modal age, with one
clearly pronounced peak and only minor secondary maxima. This implies that
seasonality is dominated in this area by a local seasonal cycle in the
extratropical cross-tropopause transport and not by the tropical upward
mass flux. Inverse spectra without a seasonal cycle (dashed–dotted – panels b to e) reproduce that shift between the seasons
qualitatively, but yielding a much larger difference among the seasonal
amplitudes, with an underestimated SON (slightly DJF) and overly pronounced
MAM and JJA. The annual curve (dashed–dotted – panel a) compares well
with the pulse spectrum nevertheless, indicating that over- and
underestimation cancel out coincidentally. Since seasonality seems to be
controlled by local entrainment into the stratosphere in this region in the
midlatitudes, a comparison of spectra including the artificial seasonal
cycle (dashed – panels b to e) with the pulse spectra
reveals seasonal differences that are inordinately distinct and very similar
to the inverse spectra without a seasonal cycle. Also, all inverse spectra
again exhibit a slightly overestimated tail. The extratropical
cross-tropopause transport violates the assumption of single entry in the
inverse method, which does not reproduce the pulse spectra correctly. The
imposed cycle prescribes seasonality wrongly, as it cannot include
variability in local transport trough the tropopause. The cycle of this
extratropical transport across the tropopause is visible in Fig. 6 of
Appenzeller et al. (1996) and differs significantly from the variability
in the tropical upward mass flux. Hence, a modification of the imposed
seasonal cycle would be necessary to include this effect. All these findings
coincide well with our defined threshold, since 140 hPa at 55^{∘} N
corresponds to a clock mean AoA between 1.04 years (maximum – MAM) and 0.52 years
(minimum – SON) and falls below the introduced threshold of 1.5 years (see
Sect. 2.3).

Since the seasonal cycle leads to an improvement of the inverse spectra except for the lower stratosphere and no significant changes in the annual mean state, all of the following results of the inverse method will include the imposed cycle.

The percentage differences of the annual pulse and inverse mean AoA to the clock tracer are given in Fig. 7. The pulse mean AoA (panel a) matches the clock mean AoA very well except for the lower stratosphere. This is expected for sharp peaks of the age spectrum, such as in Fig. 6, where the temporal resolution of 3 months might not be sufficient and leads to inaccurate mean AoA. The tail correction of the spectra as well as their sole initialization in the tropics might also contribute to these deviations. For lower pressures, however, the approximation of the tail correction seems to be adequate with matching mean AoA values. The main differences between pulse and clock mean AoA also appear to follow the shaded area (panel b) of the 1.5-year threshold (see Sect. 2.3). If globally averaged for the pulse spectra, this results in deviations of −0.61 % above the threshold and +14.5 % below it. These findings imply that the tail correction works mostly as intended and only needs to be applied with caution around the tropopause region. The inverse mean AoA (Fig. 7b) is biased towards larger values, with the largest positive differences at polar and tropical latitudes. Negative differences are only found in the southern midlatitude lowermost stratosphere, which fall below the threshold of 1.5 years of mean clock AoA (dashed) for the most part. This is most probably linked to inaccurate seasonal spectra, which do not cancel out on annual average. Below the threshold, a global difference of +44.3 % is derived, whereas above the threshold this deviation reduces to +13.3 %. The bias may be attributed to the prescribed inverse Gaussian shape of the inverse spectra and is already indicated in the enhanced tails of all inverse spectra (Figs. 4 to 6). Since the annual mean is distorted towards larger mean AoA, it is likely that the seasonal fields show a similar behavior. To compare their structure and the reproduction of pulse spectra and clock tracer qualitatively, percentage changes relative to the annual mean state are evaluated.

Figure 8 shows mean AoA of the clock tracer and the pulse and inverse spectra as a latitude–pressure cross section. The left column gives the absolute annual average, and the remaining four columns give the percentage deviations of all seasons from each annual mean. The seasonal patterns of pulse spectra and clock tracer are matching very well with a few differences in the lowermost stratosphere (especially DJF and JJA). This coincides with the results of Fig. 7. The structures of mean AoA for the inverse method match the pulse spectra and clock tracer in each season very well qualitatively above the dashed area. Only the amplitude of the seasonal changes seems to be enhanced in direct comparison. This indicates that the seasonality that could already be detected in Figs. 4 and 5 extends mostly to the global scale. A clear boundary of those seasonal patterns is visible in the lower stratosphere around the threshold of 1.5 years of clock mean AoA (see, in particular, MAM or SON in the north). Below, the contours do not agree with the pulse spectra and clock tracer in multiple seasons and spatial regions and display an opposite sign to the pulse or clock tracer, especially in MAM and SON in the north. These differences generally emerge particularly in the Northern Hemisphere and are only visible to a small extent in the Southern Hemisphere (e.g., DJF – polar below 100 hPa). This is again consistent with the results of Appenzeller et al. (1996). They state that the net mass flux across the northern extratropical tropopause is largest downward in late MAM and largest upward in SON, whereas the upward mass flux across the tropical tropopause has its maximum in DJF and minimum in JJA. This local entry cannot be described by an annual mean entry mixing ratio at the tropical tropopause and is not well represented in the inverse method. The seasonal cycles of transport at the tropical and the extratropical tropopause differ distinctly so that the imposed seasonal cycle is not appropriate and leads to distorted inverse spectra (see Fig. 6). A combination of both effects is most probably the reason for the differences of the inverse method from clock tracer and pulse spectra in the northern midlatitude lower stratosphere in MAM and SON. In DJF and JJA, however, the strength of the extratropical cross-tropopause transport is vanishingly low (Appenzeller et al., 1996) so that an assumption of single entry through the tropical tropopause should be appropriate, leading to changes in inverse mean AoA that match clock tracer and pulse spectra. This seasonal cycle in extratropical cross-tropopause transport is much less pronounced in the Southern Hemisphere, being a plausible reason for a better performance of the inverse method there. The lower stratosphere proves to be a critical region for the inverse method on the global scale also, where further improvements are necessary. The deviations of inverse mean AoA from the pulse mean AoA and clock tracer at the tropical tropopause, however, are more likely only a result of the choice of an annual mean entry mixing ratio for the inverse method. The first moment of a distribution is an integrated measure of the complete spectrum and, as expected, the cross sections of mean AoA for the inverse method without a seasonal cycle (not shown) are identical in structure and strength to the ones presented in Fig. 8. The seasonal cycle only modulates seasons of weak and strong transport properly, while keeping the average over the complete transit time period unchanged, similar to the annual mean spectrum.

The following analysis focuses on three fixed latitudes, since the results
presented in Fig. 8 have already shown a good performance of the inverse
method beyond 1.5 years of clock mean AoA in both hemispheres. 85,
55 and 10^{∘} N are selected because the Northern
Hemisphere appears to be more challenging to the method and is better
covered by in situ measurement campaigns. The analysis on fixed latitudes is
also advantageous, as the second moment of a PDF is strongly dependent on its
first moment. An interpolation of mean AoA as vertical coordinate would be
required for a global cross section, which might lead to inaccuracies and
errors. Figure 9 depicts the width of spectra as function of their mean AoA
for pulse (panels a, b and c) and inverse (panels d, e and f) spectra. Mean AoA serves as
vertical coordinate. Filled diamonds represent data of vertical levels above
the threshold of 1.5 years. For a better comparison, the pulse width is also
given as grey shading in the bottom-row graphics. Seasonal differences of
the pulse spectra widths appear to be marginal below mean AoA of 3 years at
all latitudes. The width of a spectrum at a given mean AoA is similar and
independent of the chosen latitude. With increasing mean AoA, curves begin
to fan out for the different seasons, especially at 85^{∘} N. The
curves at 55 and 85^{∘} N seem to be skewed towards
smaller widths for larger mean AoA, indicating that the spectra become
slightly tighter around their means at the upper boundary of the analyzed
area. The inverse method again captures these effects quite well with
similar curvatures, although the resulting spectra are systematically wider,
just as presented in Figs. 4 to 6. A steady width ensues at larger mean AoA
than for the pulse spectra. When the necessary threshold of 1.5 years is
applied, primarily the obvious outliers and only few possibly matching data
points are omitted (unfilled diamonds) at 85 and 55^{∘} N.
That improves the overall agreement of the inverse and pulse width.
Seasonal fluctuations in the tropics are comparatively high over the
complete data range. Since the entry mixing ratio is significantly important
for transport in that region, the annual mean entry mixing ratio is most
probably the cause of this variability. At 55 and 85^{∘} N,
however, the seasonality is of minor influence below 4 years of mean
AoA, just as for the pulse spectra. Beyond that level, the curves start to
fan out similarly, but with a stronger signal in particular at polar regions
above 5 years. Coherently, the difference between pulse and inverse
spectra regarding the initial point of curves fanning out is approximately
the mean AoA bias of +13.3 % detected in Fig. 7. It might be concluded
that the inverse method also reproduces the pulse width in a qualitative
manner but is biased towards larger values, equivalent to the results for mean
AoA and midlatitude spectra. The lowermost stratosphere likewise arises as
a critical region with false width below the threshold. Since width is also an
integrated value, exclusion of the imposed seasonal cycle gives an identical
outcome.

The ratio of second to first moment $\frac{{\mathrm{\Delta}}^{\mathrm{2}}}{\mathrm{\Gamma}}$ is crucial for some observational studies of mean
AoA with mixing ratios of SF_{6}. Volk et al. (1997) propose a
second-order fit to describe the temporal trend of this trace gas.
They derive a relation to calculate mean AoA in the stratosphere up to
20 km
altitude between 60^{∘} N and 70^{∘} S as a function of the
fit parameters and the variance of the underlying age spectrum. A ratio of
moments of 1.25 years with an uncertainty of 0.5 years is then chosen, according to
Hall and Plumb (1994) and Waugh et al. (1997), to prescribe the
dependence on the variance. This technique has since been refined and
applied in further research (Engel et al., 2002, 2009, 2017;
Bönisch et al., 2009) and is still used to this day
albeit with different parameterizations. However, due to developments in
climate modeling during the past 24 years, the EMAC model might include
more processes on a finer grid than the models of Hall and Plumb (1994)
and Waugh et al. (1997). This study offers the possibility to reassess the
ratio of moments in a modern climate model also with focus on possible
seasonal variability. Figure 10 depicts the absolute pulse
and inverse ratio of moments for all four seasons and annual mean. The pulse
results (top row) differ in terms of numbers from the results presented in
Fig. 9 of Hall and Plumb (1994) as well as from the 1.25 years applied by
Volk et al. (1997) below 20 km. The spatial distribution of the ratio of
moments is nevertheless quite similar to Hall and Plumb (1994), with similar
large areas of constant values in the lower stratosphere in both hemispheres
in all seasons, but with increased vertical gradients at the same time. The
seasonal cycle of transport affects the distribution of the ratio of moments
slightly, with a maximum in DJF and a minimum in JJA on both hemispheres.
Values in the Southern Hemisphere appear to be slightly larger in the lowermost
stratosphere compared to the north. On the basis of Fig. 10,
an annual mean ratio of moments of approximately 2.0 years for the same
spatial region as in Volk et al. (1997) is detected. The inverse method
(bottom row) does not reproduce the ratio from the pulse spectra in any
season with globally divergent structures and numbers. This is likely caused
by the biased mean AoA and width presented in the previous sections. Since
the shape of the annual mean ratio of moments of the pulse spectra compares
well with absolute annual clock, pulse and also inverse mean AoA (Fig. 8),
it seems plausible that the inverse spectra variance is more likely the
driving factor of arising deviations. The mathematical fact that variations
in mean AoA always contribute squared to the second moment (Eq. 5) stresses this assumption. Again, removing
the imposed seasonal cycle from the inverse method yields identical results.

The reason for the deviation from Hall and Plumb (1994) and Volk et al. (1997)
may not only be coarser resolution and lesser complexity of the
models compared to EMAC. The tail of the age spectrum is vital for a
mathematically and physically correct description of transport. The width of
annual mean pulse and inverse spectra with tail lengths of 10, 20, 50
and 300 years is shown as a function of mean AoA at 55^{∘} N in Fig. 11.
Unfilled diamonds denote data below 1.5 years of clock mean AoA. The tail of
the spectrum needs to be properly specified with an appropriate length.
There seems to be no distinct difference for the pulse spectra between a
tail length of 50 and 300 years, whereas in case of the inverse method there
still appears to be some small shift towards larger mean AoA and increased width.
This is expected, since the maximum transit time is selected in accordance
with the integral over the spectrum (see Appendix A). When using the intrinsic
tail length of 10 years, the ratio of moments of pulse and inverse spectra
have similar orders of magnitude as presented by Hall and Plumb (1994). A
maximum transit time between 10 and 20 years was also used in Hall and Plumb
(1994; Timothy M. Hall, private communication, 2018). The spatial distribution of
the inverse ratio of moments agrees very well with the pulse results if
using a tail length of 10 years for both. Thus, on the one hand, a fully included tail is
needed for physically precise results. On the other hand,
the width in Fig. 11 exhibits a much stronger dependence on the tail length
than mean AoA, making variations in variance even more likely to be the primary
factor for the discrepancies between inverse method and pulse spectra in
Fig. 10.

Results of the proof of concept presented above have shown that the inverse
method in combination with the imposed seasonal cycle is in principle
capable of deriving seasonal age spectra correctly, except for the region
below 1.5 years of mean AoA. However, when it comes to real atmospheric data,
application of the method becomes even more challenging. One of the most
critical factors is the chemical lifetime of the gases used in the
inversion which is strongly dependent on time and space, tainted with
seasonal and inter-annual variability and only known with limited accuracy.
The inverse method in its form postulated above (Eq. 11) can include variability in lifetimes, since
the lifetime *τ* is designed to be transit-time dependent, although a
constant lifetime is used for all tracers implemented in this study.
Transit-time dependence is a more approximate choice compared to real space
dependence, since two distinct spatial pathways could in theory exhibit
an equal transit time but different lifetimes along them. However, as discussed
in Engel et al. (2018), a good average correlation between chemical loss
and time spent in the stratosphere is expected. Extension of the method to
variable chemistry could involve the ansatz of Schoeberl et al. (2000, 2005), who reduced the depletion of trace gas species to
chemistry along average Lagrangian paths starting at the reference point to
any location in the stratosphere (see Sect. 4).

A further limitation of the method when applying it to observational data is the number of trace gases necessary for the inversion to work properly. In reality, it is impossible to find 40 trace gases with lifetimes ranging from 1 to 118 months evenly spaced in steps of 3 months. Considering data and measured species of modern airborne research campaigns, it is more likely to find a set of 10 trace gases at most, which span a range of 10 years in chemical lifetime. On this basis, three subsets of tracers with 10, 5 and 3 trace gas species are selected and shown in Table 2 together with their corresponding lifetimes to investigate the effects of reducing the number of trace gases and introducing uncertainty in the knowledge of the lifetime. Three trace gases are considered to be the minimum in order to constrain different parts of the age spectrum (e.g., left flank of the peak, right flank and tail). A reduction of trace gases removes, on the one hand, redundant information about transport and strongly diminishes the amount of data but, on the other hand, also increases the risk of errors during the inversion leading to wrong age spectra. This is especially precarious if chemical depletion is spatially varying and inaccurately estimated.

To test the influence of uncertainties in assumed lifetimes, a Monte Carlo
approach has been used in which chemical lifetimes are varied
pseudo-randomly. In this simulation the mean lower error margin is evaluated
by giving a pseudo-randomly selected number of lifetimes in a trace gas
subset a certain preset uncertainty *ϵ*_{lower} (e.g., −20 %). In
a second similar run, the opposite error *ϵ*_{upper} (e.g.,
+20 %) is then applied to retrieve the mean upper margin. All simulations are
repeated 5000 times for each of the three trace gas subsets (Table 2) while
pseudo-randomly varying the lifetimes of some of the species used in the
inversion. This setup will provide a mean deviation of the spectra for all
cases where the exact amount of error-prone lifetimes is unknown. Since the
pseudo-random numbers are distributed uniformly, the simulation mean is
equivalent to a case where the lifetimes of approximately half of the
species in a subset exhibit an error but are pseudo-randomly chosen with equal
probability. Each simulation is designed as a single sensitivity experiment,
where lifetimes are varied constantly in transit time either upwards or
downwards, which provides an estimation of the maximum and minimum error of
an age spectrum for a preset uncertainty. Note that an underestimation of
the lifetime causes the peak of the age spectrum to shift upward and to
smaller transit times, as depletion becomes faster. Errors of ±10 %, ±20 %
and ±50 % have been selected for this
study. Results are shown in Fig. 12 at 55^{∘} N and 70 hPa as annual
mean, but analog results are found at 10 hPa (not shown). As the main
differences for the trace gas subsets occur within the first year of transit
time, only this small slice is presented to make lines distinguishable. The
age spectra of the subsets with 10 (panel a) and also 5 (panel b) trace
gases without error (solid blue line) are in good agreement with the
spectrum of the full tracer set (black line). Modal age increases by 2.5 %
(10 tracers) and by 3.1 % (5 tracers) compared to the full set,
whereas the amplitude changes by −0.03 % (10 tracers) and −2.5 % (5 tracers).
The inversion results are robust even if using only a fourth and
an eighth of all trace gases. In the case of only three trace gases (panel c), the solid blue line exhibits a growing shift of amplitude (−9 %)
and also greater modal age (10 %). Overall agreement is still reasonable
but not as good as for the other two subsets. The shift towards larger modal
age and smaller amplitudes when decreasing the size of the subset is
unexpected and not intuitive. Errors in the knowledge of chemical lifetime
of the trace gases affect all subsets equally, as all non-solid lines in all
three panels show an equivalent behavior relative to the reference spectrum
of each subset (solid blue lines). All averaged percentage uncertainties of
amplitudes and modal ages are depicted in Table 3. An overestimation of
chemical lifetime generally leads to smaller deviations of modal age and
amplitude than an underestimation.

These results imply that a reduced set of trace gases with either 10 (optimum) or 5 (sufficient) species should be recommended in order to retrieve age spectra from observations. Values in Table 3 and also the general shape of the error spectra indicate that on average both of these subsets can also compensate a chemical lifetime uncertainty of up to ±20 % of a random number of species if small deviations of modal age (−10 % or +8 %) and amplitude (−8 % or +12 %) are tolerated. Given the assumptions that the inverse method is based on, the accuracy level of 5 % during the inversion and atmospheric variability when applied to in situ data, this threshold might be considered a reasonable choice. If the number of trace gases with lifetime error is decreased and kept constant, the deviation from the reference spectrum will become smaller due to more compensation by the remaining species. Opposite effects will apply if the number is increased.

4 Summary and conclusion

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This paper presents a modified version of the inverse method by Schoeberl et al. (2005) to derive stratospheric age of air spectra from radioactive trace gases with fewer free parameters. It introduces a formulation of an imposed seasonal cycle in the spectra to approximate seasonality in stratospheric transport. The development process always focuses on achieving the best possible compromise between accuracy and practicability for observational studies with very limited data. The resulting spectra are evaluated in comparison to EMAC pulse spectra. The inverse method is applied on a simplified set of 40 short-lived trace gases with globally constant prescribed lifetimes as proof of concept. Resulting spectra are assessed as well as their first and second moments and the ratio between them. This comparison is conducted for annual mean state and for respective seasonal variation. Data within the transition layer, the first 30 K beyond the tropopause, are always omitted in our study, as the strong tropospheric influence distorts the concept of age of air referred to the tropical tropopause. A threshold of 1.5 years of clock mean AoA is introduced as a region where entry through the local tropopause is not negligible. 10 hPa is selected as upper boundary, since the mixing ratios of trace gases with lifetimes smaller than 2 years are critically close to the accuracy level of the inverse algorithm.

The modified inverse spectra match the pulse spectra well both on an annual and
seasonal timescale with its new set of reduced fit parameters for most
parts of the stratosphere. The imposed seasonal cycle improves the already
well-described intrinsic seasonality and reproduces seasonal variation in
the spectra correctly. Multiple peaks of the inverse age spectra at
55^{∘} N coincide with the pulse spectra in time of appearance and
amplitude during all seasons in 70 and 10 hPa. The artificial seasonal
cycle moreover does not change the moments of the distributions, as they are
integrated measures. This extends to the annual mean spectra, which are also
almost unchanged when applying the seasonal cycle. Additionally, a need for
an explicit temporal offset in the formulation of the inverse method is not
detected. In the lower stratosphere at 55^{∘} N and 140 hPa, which is
below the threshold of 1.5 years of mean AoA, the inverse spectra differ from
the pulse spectra on the seasonal scale, whereas the annual mean matches
coincidentally. The imposed seasonal cycle does not contribute to a better
agreement of the seasonal spectra. In the northern extratropics at 140 hPa,
entrainment of air through the local tropopause is important. This process
is not considered in the assumption of single entry through the tropical
tropopause and not included in the inverse method presented here. The
seasonality of the local entry of air through the extratropical tropopause
(Appenzeller et al., 1996) differs strongly from the seasonality in
tropical upward mass flux (Fig. 1). The imposed seasonal cycle leads to
mismatching spectra, as it does not take this seasonal cycle in local
entrainment into account. Global mean AoA as well as spectra's width at
85, 55 and 10^{∘} N reveal that the inverse
method also performs well on the global scale, reproducing the annual state
as well as seasonality for air masses with more than 1.5 years of mean AoA. Below the
threshold, similar problems in the seasonality of the inverse method as at
55^{∘} N arise globally in large areas around the extratropical
tropopause. These mechanisms are enhanced in the Northern Hemisphere and
only occur to some small extent in the south, which is again in accordance
with Appenzeller et al. (1996). Due to its assumptions, the inverse method
and the imposed seasonal cycle are likely not applicable in the lowermost
stratosphere below 1.5 years of mean AoA without further improvements. The
chosen annual mean entry mixing ratio influences results only in close
vicinity to the tropical tropopause. All inverse age spectra exhibit
systematically enhanced tails, leading to larger global mean AoA compared to
pulse spectra and clock tracer and larger width compared to the pulse
spectra, most probably caused by the prescribed inverse Gaussian shape.

The ratio of moments of the pulse and inverse spectra is compared to the results of Hall and Plumb (1994). The ratio of moments of the pulse spectra exceeds their values by a factor of 3 but show a similar spatial structure. Since the results show that the ratio of moments undergoes seasonal variability, an annual average value of 2.0 years for the lower stratosphere in both hemispheres is promoted. This is larger than the values implemented by Volk et al. (1997; 1.25±0.5 years) and Engel et al. (2002; 0.7 years). The large deviation between EMAC and Hall and Plumb (1994) is most probably a result of an underestimated spectrum tail in Hall and Plumb (1994). A properly considered tail is required to fully describe stratospheric transport using age spectra, since the tail affects both mean AoA and width. As the ratio of moments is usually implemented for the derivation of mean AoA from observations (Volk et al., 1997; Engel et al., 2002), these findings might contribute to improved results. The inverse method is not capable of reproducing the pulse spectra's ratio of moments, likely because of the systematic errors in mean AoA and width not scaling accordingly.

With respect to observational data, a set of 40 trace gases with lifetimes
ranging evenly spaced from 1 month to 10 years cannot be found in
reality. Tests with reduced numbers of trace gases show that subsets
consisting of 5 (sufficient) to 10 (optimal) chemically active trace gases
should be used in order to invert consistent and matching age spectra in the
northern midlatitudes. It is recommended that the species in these subsets
are selected so that their average local lifetimes along the transport
pathway cover a period of 10 years uniformly. The analysis shows moreover
that errors in the assumed chemical lifetime, which affect a random number
of trace gases in these subsets, can be compensated during the inversion to
some degree. On average an uncertainty in the knowledge of lifetimes up to
±20 % still leads to reasonable agreement of age spectra if an
amplitude and modal age deviation of approximately ±10 % is
accepted. The more lifetimes are known correctly, the smaller these
deviations will become due to better compensation by the correctly
prescribed species. While the method's presented formalism allows for
varying lifetime in the form of transit-time dependence, actual application
to observations requires further development and analyses. Possible
approaches might include chemistry along average Lagrangian paths (e.g.,
Schoeberl et al., 2000, 2005) in combination with
chemistry transport models. In addition, for the lower stratosphere with
mean AoA below 1.5 years, a fractional approach as proposed by Andrews et
al. (2001b) and Bönisch et al. (2009) for chemically inert trace
gases could be applied, which splits the stratosphere into an upper and
lower section and derives an age spectrum as superposition of the
sub-spectra of each section. If chemical depletion is then approximated by
lifetimes representative of each compartment, this separation of the
stratosphere possibly leads to more reasonable results than in the complete
stratospheric case. In such a case, different entry mixing ratios of
short-lived trace gases at the tropical and extratropical tropopause could
also be prescribed to better represent temporal and spatial variability. A
limiting factor for long-term analyses is the fact that real stratospheric
transport is not stationary and afflicted with a long-term temporal trend
coupled with seasonal and inter-annual variation. This trend can neither be
included in the transport parameter *K*, as it is independent of transit
time, nor in the prescribed seasonal cycle. Despite these additional difficulties
when applying the method to observational data, the basic principle of both
modified inverse method and imposed seasonal cycle proved to work. Further
work is required to make the method finally applicable to measurement data
and possibly contribute to a deepened understanding of stratospheric
transport. In particular, the method's application on more realistic trace
gases should be included in future studies regarding observationally derived
age spectra.

Data availability

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Data availability.

All data can be made accessible on request to the authors.

Appendix A: Numerical implementation

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Deriving the reference ratio *R*_{ref} from observational or modeled data,
*K* will be numerically optimized until *R*_{seas} or *R* is equivalent to
*R*_{ref} within a range of 5 % accuracy. This is possible for a single
trace gas as well as for a set of given species simultaneously. The more
distinct substances with varying lifetimes are included, the more
information about the underlying transport processes of the BDC is
condensed into *K*. To estimate the deviation of *R* from the reference
ratio *R*_{ref} for every trace gas, the mean percentage error (MPE) between
them is minimized and given as follows:

$$\begin{array}{}\text{(A1)}& {\displaystyle \frac{\mathrm{1}}{n}}\cdot \sum _{i}^{n}{\displaystyle \frac{{R}_{\mathrm{ref}}^{i}-{R}^{i}}{{R}_{\mathrm{ref}}^{i}}}\stackrel{!}{=}\mathrm{0}.\end{array}$$

The index *i* denotes a single trace gas within a set of *n* species. To
achieve the optimization numerically, a combination of an algorithm
postulated by Ridders (1979) and Newton's method is applied. This
also justifies the choice of MPE as an measure of error, besides the fact that
it is a robust deviation estimate. Ridders' method is known to be convergent
in any case, if and only if the root (MPE=0) is correctly bracketed.
This implies that there must be always one value of *K* where MPE is less
than 0 and one *K* where MPE is greater than 0. Only then is convergence for
large deviations of *K* from the solution ensured and rapid. When
approaching the solution of *K*, Newton's method is significantly faster
for converging and yet very stable, which is an advantage to keep the
computational effort as small and efficient as possible. If the satisfaction
criterion is reached, the corresponding age spectrum of the matching *K* is
returned. A problem arises when reaching upper or lower boundary regions.
Both algorithms will become unstable in such regions. If the ratio is larger
than 1, which is possible in close proximity to the tropopause where
entrainment of tropospheric air occurs, or nearly equal to 0, no suitable
*K* will be optimized. In this case, the respective points will be omitted
and treated as missing data. Other than in the original method of Schoeberl
et al. (2005), there are no trace gases with a constant mixing ratio of 1
at the tropical tropopause in the model, since in reality there will be
uncertainties, seasonalities and temporal trends affecting this quantity. To
include this effect and test if it influences the performance of the method
critically, the annual mean mixing ratios are calculated at the tropical
tropopause and utilized in respect of future observational approaches. The
scale height *H* is derived from the air density *ϱ* at each
latitude. This can also be done with observed data, as the density is
frequently measured along with trace gases. A critical aspect for the
calculation of age spectra as an inverse Gaussian PDF is the numerical
choice of a value large enough to be equivalent to infinity. That is
especially relevant for the tail of the age spectrum and hence for its
variance, since only at infinity are all possible values considered.
Multiple tests with the spectra have shown that a maximum transit time of
300 years with a resolution of 30 days is sufficient. With this selection,
Eq. (7) settles at 0.999 and does not significantly
change anymore if the maximum is further increased. All spectra are
therefore be integrated from 0 to 300 years.

Author contributions

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Author contributions.

MH wrote the paper, evaluated the model data and developed the ideas presented in this study in close collaboration with AE. FF and HG planned and performed the EMAC model simulation and implemented and tested the method of Schoeberl et al. (2000) mentioned in Sect. 2.1. FF, HG and AE contributed to the preparation of the paper in many discussions.

Competing interests

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Competing interests.

The authors declare that they have no conflict of interest.

Acknowledgements

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Acknowledgements.

This work is supported by the German Research Foundation (DFG) priority program 1294 (HALO) under the project number 316588118. The model simulations were performed on the HPC system Mistral of the German Climate Computation Center (DKRZ) supported by the German Federal Ministry of Education and Research (BMBF). The authors cordially thank Felix Plöger from Forschungszentrum Jülich and Harald Bönisch from the Karlsruhe Institute of Technology (KIT) for their help and the useful discussions regarding the research presented in this paper.

Review statement

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Review statement.

This paper was edited by Rolf Müller and reviewed by three anonymous referees.

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Short summary

The paper presents a modified method to invert mixing ratios of chemically active tracers into stratospheric age spectra. It features an imposed seasonal cycle to include transport seasonality into the spectra. An idealized set of tracers from a model is used as proof of concept and results are in good agreement with the model reference, except for the lowermost stratosphere. Applicability is studied with focus on number of tracers and error tolerance, providing a starting point for future work.

The paper presents a modified method to invert mixing ratios of chemically active tracers into...

Atmospheric Chemistry and Physics

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