Open Access

Thermospheric inter-annual variability and its potential connection to ENSO and stratospheric QBO

Earth, Planets and Space201668:77

DOI: 10.1186/s40623-016-0455-8

Received: 3 December 2015

Accepted: 28 April 2016

Published: 10 May 2016


Using a 46-year-long dataset of the thermospheric density during 1967–2012, we examined the inter-annual variability in the thermosphere at 400 km and its potential connection to El-Nino Southern Oscillation (ENSO) and stratospheric Quasi-Biennial Oscillation (QBO). Wavelet analysis reveals two major modes of the thermosphere inter-annual oscillation, with the slower mode having an average period of ~64 months and the faster mode of ~28 months. The slower mode bears high coherence with the ENSO during 1982–2012, while the faster mode is found to vary coherently with the QBO around 1972, 1982 and 2002. Further examination reveals that the coherence between QBO and the faster mode is significantly influenced by their common coherent variation with the solar flux, while high coherence between the slower mode and ENSO is much less contaminated. Therefore, we conclude that the 28-month periodicity in thermospheric density may be caused by both QBO and solar radiation, whereas the 64-month periodicity possibly arises mainly from ENSO processes, with little/small contribution from solar radiation.


The thermosphere is the upper part of the Earth’s atmosphere, occupying the region between about 100–600 km altitude. This region is not only important for satellite operations because of air drag, but also scientifically important for vertical coupling between the upper and lower atmosphere because of its high sensitivity to both solar forcing and lower atmosphere forcing. The thermosphere is known to respond closely to solar forcing at various timescales ranging from the solar cycle to a few minutes during solar flares (e.g., Liu et al. 2005, 2007). In recent years, the thermosphere has also been found to be sensitive to meteorological forcing from the lower atmosphere. For instance, it responds to the non-migrating tidal forcing due to the land–sea distribution and forms a wave-4 structure in the zonal distribution of neutral density and wind (Liu et al. 2009; Häusler et al. 2007). It also responds globally to stratosphere sudden warming (SSW) events with semi-diurnal perturbations in the thermosphere temperature and a zonal mean cooling (Liu et al. 2011, 2014). Furthermore, the thermosphere shows a long-term cooling trend, in response to the increase of CO2 in the atmosphere during the twentieth-century global warming (Emmert et al. 2010). The agents which teleconnect the lower and upper atmosphere in these cases are atmospheric tides for the former two and CO2 infrared radiative cooling for the latter.

In the lower atmosphere, there are two distinct phenomena which occur periodically. One is the El-Nino Southern Oscillation (ENSO), and the other is the Quasi-Biennial Oscillation (QBO). ENSO refers to periodic variations in the sea surface temperatures over the tropical eastern Pacific Ocean. It has two phases, with the warming phase called El-Nino and cooling phase called La-Nina. ENSO occurs on average every \(\sim\)5 years, but varies considerably between 2–7 years (see, e.g., Wang and Picaut 2004). QBO refers to the quasi-periodic oscillation of the equatorial zonal wind in the tropical stratosphere with a mean period of about 28 months, ranging between 20 and 36 months (see, e.g., Baldwin 2001).

There have been reports on the effects of these oscillating meteorological phenomena on the ionosphere. For instance, ionospheric foF2 at two stations was found to highly correlate with ENSO (Pedatella and Forbes 2009). The equatorial electrojet and ionospheric foF2, hmF2 were found to oscillate at periods around 26–27 months, which was attributed to the influence of the stratospheric QBO (Olsen 1994; Kane 1995). Since the thermosphere is closely coupled to the ionosphere, it is interesting to examine whether the thermosphere bears imprints of ENSO and QBO as well. This study explores such a possibility by using a long time series of thermosphere density observations.


Since ENSO occurs only once every couple of years, we need a sufficiently long dataset to be able to examine possible ENSO signatures in the thermosphere. For this purpose, the thermospheric density dataset first introduced by Emmert (2009) and later extended to 2012 is employed. This dataset provides daily globally averaged thermospheric density obtained from orbital decay measurements of about 5000 satellites during the period of 1967–2012. Note that the temporal resolution of the data is 3–6 days, due to a 3- to 6-day smoothing procedure in the density retrieval (Emmert 2009). Density values are given at three different heights of 250, 400 and 550 km. For our analysis, we calculate monthly averaged values using only data under quiet geomagnetic conditions (daily average Kp\(<2^{+}\)).

To examine the thermosphere density perturbation possibly related to ENSO and QBO, we take density residuals by subtracting the NRLMSISE-00 model values from the measurements. By doing so, we remove density variations due to local time, season, solar cycle, and geomagnetic activity effects. Figure 1a shows the observed and model values. They are very close to each other, demonstrating NRLMSISE-00’s ability in capturing most solar and seasonal driven variabilities in the globally averaged thermospheric density. The residual (\(\Delta \rho\)) at 400 km is shown in Fig. 1b. To focus on inter-annual oscillations, a 12-month running mean is applied before subsequent analysis (thick curve in Fig. 1b). Although the model does not take into account lower atmosphere forcing like CO2 or stratospheric sudden warmings, it is not a big problem for our analysis here as their effects hardly enter the timescales we are interested in this study, which is between about 2–7 years.
Fig. 1

Time series during 1967–2012. a The observed (black line) and NRLMSISE-00 modeled (green line) values of the global mean thermospheric density at 400 km altitude. b The density residual (thin line) and its yearly running mean (thick line). c Nino3 index and its yearly running mean. d QBO and its yearly running mean

ENSO is represented by the commonly used Nino3 index provided by the Japanese Meteorological Agency ( This index is calculated from the sea surface temperature anomaly in eastern Pacific region of \(5^\circ\)N–\(5^\circ\)S, \(90^\circ\)W–\(150^\circ\)W. Stratospheric QBO is represented by the zonal wind at 30-hPa pressure level provided by the Frei University Berlin ( Both Nino3 and QBO indices come as monthly values (Fig. 1c, d). Similar to the thermospheric density residual, we apply a 12-month running mean to suppress fluctuations below one year.

The solar flux is also used, particularly in the later part of the study. The proxy \(P10.7=(f10.7+f10.7A)/2\) is chosen to represent the solar flux, since it is shown to be more suitable than f10.7 as a linear indicator for the solar EUV radiation (e.g., Richards et al. 1994; Liu et al. 2006). Here f10.7A is the centered 81-day average of the f10.7 values. Monthly averaged values are used to be consistent with the temporal resolution of ENSO and QBO indices.

Results and discussion

The data series of density residual, Nino3, and QBO obtained above are subjected to various spectrum analyses to reveal the characteristics of their inter-annual oscillations. Since results at 250 km are rather similar to that at 400 km, we present the results at 400 km altitude to avoid repetition. Results at 550 km are discussed afterward.

We first apply simple Fourier spectrum analysis using the Lomb–Scargle method (Lomb 1976; Scargle 1982) to bring out the overall (in contrast to wavelet) periodicities in these datasets. Periodograms in Fig. 2 show that the density residual at 400 km bears a distinct peak around 62 months and two broad peaks at \(\sim\)78 and \(\sim\)105 months (Fig. 2a). Nino3 exhibits two isolated peaks around 43 and 62 months (Fig. 2b), while the QBO shows a prominent peak at \(\sim\)28 months (Fig. 2c). These periodicities in the Nino3 and QBO are consistent with known values. The P10.7 index shows no significant peak below 100 months.
Fig. 2

The Lomb–Scargle periodogram of a the density residual at 400 km altitude; b Nino3 index; c QBO index; d P10.7 index. Dash lines indicate 95 % significance level

Since Fourier analysis yields only a time mean spectrum of a data series, we perform wavelet analysis to reveal more accurate information on the periodicities and their temporal evolution. As illustrated in Fig. 3a, the density residual experiences oscillations in several periodicity bands. The band of low periodicity is centered around 28 months with a range of 20–36 months. These oscillations likely produced the two minor peaks between 20 and 40 months in the mean spectrum shown in Fig. 2a. Because these oscillations occur only intermittently around 1972, 1982, 1992 and 2002, when averaged over the entire period, the spectral peak drops below the 95 % significance level as seen in Fig. 2a. On the other hand, these intermittent occurrences indicate that this oscillation is likely regulated by solar cycle. This point is further confirmed later. Two higher periodicities centered around 52 and 88 months occur during 1975–1990 and converge to one centered around \(\sim\)64 months after 1990. Meanwhile, Nino3 exhibits a broad peak around 42 months before 1972 (Fig. 3b). It bifurcated to two separate peaks after 1972, with one remaining around 42 months and another one shifting from \(\sim\)52 months around 1987 to \(\sim\)64 months during 1997–2010. The QBO exhibits the known periodicity around 28 months, with a range of 24–36 months (Fig. 3c). The solar flux index P10.7 shows only one peak with greater than 95 % significance, which is around 128 months, roughly corresponding to the solar cycle.
Fig. 3

The wavelet power spectrum of a the density residual at 400 km altitude; b Nino3 index; c QBO index; d P10.7 during 1967–2012. The thick contour encloses regions of greater than 95 % significance level

To further examine how coherently these oscillations vary with each other, wavelet coherence analysis is carried out. The result shown in Fig. 4 (top panel) reveals a high coherence over 0.9 between Nino3 and the density residual at the periodicity centered around 64 months with a range of 56–78 months. The phase shift is indicated by the arrows, being persistently around \(\sim\)60°. This means that ENSO leads the density oscillation by \(\sim\)60°, which corresponds to about 10 months for a periodicity of 64 months. Note that the Nino3 index represents variations in the sea surface temperature, and it takes about 5 months for these changes in the ocean to transfer to the tropical troposphere (Trenberth et al. 2002). The bottom panel of Fig. 4 reveals high coherence between the density and QBO around 1972, 1982 and 2002.
Fig. 4

The wavelet coherence between the density residual at 400 km altitude and Nino3 index (upper) and between the density residual and QBO index (bottom). Thick contours enclose regions of greater than 95 % significance level. The arrows indicate the relative phase relationship between the time series, right in-phase; left anti-phase; down Nino3/QBO leading \(\Delta \rho\) by 90\(^\circ\); up \(\Delta \rho\) leading Nino3/QBO by 90\(^\circ\)

The high coherences obtained above are very encouraging. However, a concern arises as to how much these coherences are attributed simply to their common co-variation with the solar flux. For instance, the 64-month periodicity where the density has high coherence with ENSO is very close to the second harmonic of the 11-year solar cycle. To clarify whether there is any contamination due to this aspect, we carried out coherence analysis separately between the density residual and solar flux and between Nino3 index and the solar flux. Results in Fig. 5 reveal a coherence between the density and P10.7 around 64 months (top panel), but being mostly insignificant except for during periods before 1976 and around 1997. On the other hand, Nino3 index shows no significant coherence with P10.7 at periods between 50 and 80 months (middle panel). Therefore, these examinations indicate that the strong coherence between the density and Nino3 index is likely a true signature of the lower–upper atmosphere coupling during ENSO periods.
Fig. 5

The wavelet coherence between P10.7 index and the density residual at 400 km altitude (upper), between the P10.7 and Nino3 (middle), between the P10.7 and QBO. The thick contour encloses regions of greater than 95 % significance level

Similarly, we have examined possible solar contamination to the high \(\Delta \rho\)-QBO coherence around 28 months. As seen in Fig. 5 (upper panel), the density residual shows high coherence with P10.7 at periods of 16–32 months around 1972 and during most time of 1987–2012. At the same time, the QBO shows high coherence with P10.7 between 17 and 32 months around 1972, 1982, 1992, 2002 and 2012. Thus, it is difficult to tell whether the high coherence between the QBO and density residual (lower panel in Fig. 4) is a true coupling signature between the two or simply caused by their common coherence with the solar flux. In other words, we may say that the 28-month periodicity of the thermospheric density could be caused by both QBO and solar radiation.

Here we note that the QBO index is obtained from the wind velocities at the 30-hPa pressure level. Using winds at other pressure levels in the stratosphere will not significantly impact the coherence pattern shown in the lower panel of Fig. 4, except for producing a somewhat different phase shift (that is, the arrow direction may change). This is because the extension of the QBO-wind fields throughout the vertical domain of the stratosphere is not random, but rather organized with a continuous downward phase shift (Baldwin 2001).

Finally, we discuss the density variation at 550 km altitudes. Examination of Fig. 6b tells us that it has almost no coherence with the Nino3 index, indicating weakening of the ENSO effect in the topside thermosphere. On the other hand, it has high coherence with the QBO around 28 months. But similar to the situation at 400 km altitude, this high coherence is significantly affected by the density and QBO’s co-variation with solar flux as can be seen in Fig. 6d.
Fig. 6

a Wavelet power spectrum of the density residual at 550 km altitude. Wavelet coherence between Nino3 and the density residual (b), between QBO and the density residual (c), and between P10.7 index and the density residual (d). The thick contour encloses regions of greater than 95 % significance level


We examined the inter-annual variability of the thermospheric density residual and its potential link to ENSO and stratospheric QBO. The density residual is found to have high coherence with the QBO index at an average periodicity around 28 months at 250, 400 and 550 km altitude. However, their strong coherent variation with the solar flux makes difficult to tell whether there is a direct physical link between the density and the QBO. On the other hand, strong coherence between the density residual and the ENSO at an average period of \(\sim\)64 months at 250 and 400 km altitude exhibits little contamination by co-variation with solar flux and hence indicates a more likely physical connection between the ENSO and the upper thermosphere.

Possible physical mechanisms which can cause such a teleconnection between the troposphere and thermosphere can be envisaged based on the following reasoning. ENSO is known to affect global climate and weather conditions by primarily altering the precipitation patterns in the tropics. Since absorption of solar heating by water vapor is the major source for tidal generation, changes in precipitation patterns will change the global distribution of water vapor and hence lead to changes in atmospheric tides. Indeed, there have been many studies showing an increase in the diurnal tides amplitude during ENSO period from both observational (Gurubaran et al. 2005; Lieberman et al. 2007) and model simulations (Lieberman et al. 2007; Pedatella and Liu 2012, 2013). It is known that both migrating and non-migrating diurnal tides can propagate upward to the thermosphere and cause perturbations in the thermospheric density (Liu et al. 2009, 2014; Yamazaki and Richmond 2013). Based on this knowledge, it is not a far stretch to consider that tidal changes may create a ENSO fingerprint in the thermospheric density. In addition, if ENSO also modifies planetary and gravity waves, these waves can also be potential carrier of ENSO effect to the thermosphere. Dedicated model simulations would be required to examine these possible mechanisms.



I thank Dr. John Emmert for providing the thermospheric data and helpful comments. This work is supported by JSPS KAKENHI Grants 15K05301, 15H02135 and 15H03733.

Competing interests

The author declares that he has no competing interests.

Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (, which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Authors’ Affiliations

Department of Earth and Planetary Science, Kyushu University


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