We present the latest development in multidisciplinary Third Pole research and associated recommendations regarding the unprecedented warming in the Third Pole’s past 2,000 years.
The Third Pole (TP) is the high-elevation area in Asia centered on the Tibetan Plateau and is home to around 1,000,000 km2 of glaciers, containing the largest volumes of ice outside the polar regions. The TP glaciers experience abrupt retreat under climate warming with westerly monsoon interaction (Yao et al. 2012b). More than 10 major rivers, including the Yangtze River, the Yellow River, and the Ganges River, originate from the TP, making it the “Water Tower of Asia.” However, the Water Tower of Asia is now in danger due to rapid warming (Immerzeel et al. 2012). Although the TP ecosystems are greening as a whole under climate warming, there is a clear north–south contrast (M. G. Shen et al. 2015b).
Climate over the TP is complex. It is primarily influenced by the interaction between the Asian monsoon and midlatitude westerlies and is highly sensitive to climate change, which can exert major control on the atmospheric circulation at the local and continental scales. Meteorological records reveal that the warming rate on the TP is twice of that observed globally over the past five decades (Chen et al. 2015). Reconstructions of temperature changes on the TP in the past 2,000 years have provided a historical context for the recent warming and for various mechanism studies of climate change, as well as for their linkages with human activity to be tested and thereby enable more accurate projections of future scenarios.
This article presents a mini review of the state of TP multidisciplinary research and associated recommendations motivated from the “International Workshop on Land Surface Multi-Spheres Processes of Tibetan Plateau and their Environmental and Climate Effects Assessment” held in Xining, China, in August 2016. This TP workshop was organized by the Third Pole Environment (TPE), Institute of Tibetan Plateau Research, Chinese Academy of Sciences (ITPCAS), and the University of California, Los Angeles (UCLA), with more than 230 participants from China, the United States, Japan, Nepal, the Netherlands, India, and six other countries. The American Geophysical Union (AGU), the National Natural Science Foundation of China (NSFC), the U.S. National Science Foundation (NSF), the Chinese Academy of Sciences, and 14 other organizations/agencies/institutions sponsored the workshop. The workshop brings together professionals from around the world in different disciplines to present the most up-to-date TP research, exchange ideas, and research findings to broaden understanding and bridge existing knowledge gaps in the TP scientific research (Yao and Xue 2016). The workshop presentations and discussions covered all major TP research areas and provided a base for this overview article.
This paper covers the following TP research subjects: paleo-environment on the TP; major characteristics of changing TP climate and environment, associated intensified hydrological cycles, glacial change, and other physical processes over the TP; the TP surface processes and its local and remote influence on the Asian monsoon; the TP ecosystem dynamics and its association with climate change and anthropogenic impact; the TP aerosols’ characteristics and their influence on the atmosphere and environment; and increased hazard risks on the TP.
TP TEMPERATURE CHANGE IN THE PAST 2,000 YEARS.
The stable oxygen isotope (δ18O) records in Tibetan ice cores are taken as proxies to represent the temperature on a long-term time scale (Thompson et al. 1997; X. Yang et al. 2014; Yao et al. 1996a,b, 1999, 2007). The δ18O and temperature relations have been studied over the globe and a linear relation between these two has been established. For instance, the slope of linear regression (0.69‰ °C–1) was spatially derived for mid- and high-northern-latitude coastal stations (Dansgaard 1964), and the slope (0.67‰ °C–1) was obtained for southern and western Greenland (Johnsen et al. 1989). Based on a quasi-decadal time series of δ18O in precipitation at Delingha on the northern TP (Yao et al. 1996b), a temporal slope of 0.66‰ °C–1 was obtained (Tian et al. 2003), which is very close to the ones derived in previous studies over other parts of the world. The discussion of temperature changes in the past 2,000 years in this section is mainly based on four δ18O in ice cores recovered from the TP, including the Guliya ice core in the northwest TP (35.3°N, 81.5°E), the Dunde ice core from the northeast TP (38.1°N, 96.4°E), the Puruogangri ice core in the central TP (33.9°N, 89.1°E), and the Dasuopu ice core in the southern TP (28.4°N, 85.7°E). The ice core collection started as early as the 1980s and still continues (e.g., Yao and Thompson 1992; Thompson et al. 2006). These four ice cores are the only ones that cover at least the past 2,000 years on the TP so far.
Over the past 2,000 years, δ18O in the Guliya ice core record has increased (Fig. 1a), although with fluctuations. The record can be divided into seven cold periods and eight warm periods, and toward the present the temperature shows greater warmth in the warm periods and less cold in the cold ones, with the warmest period occurring in the twentieth century. The Little Ice Age (LIA) in the TP was represented by three cold events in the sixteenth, seventeenth, and nineteenth centuries. However, the LIA is not the coldest period in the past 2,000 years (Yao et al. 1996a,b).

Ice core and tree-ring climate records in the TP (red = warm climate; blue = cold climate). (a) 10-yr averages of δ18O in the past 2,000 years recorded in the Guliya, Dunde, Puruogangri, and Dasuopu ice cores. (b) Temperature change curve in the past 2,000 years in the TP reconstructed from the four ice cores. (c) Temperature change curve in the past 2,000 years in the TP reconstructed from tree rings. The z score in the figure refers to the normalized anomalies, which consider both mean and standard deviation
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1

Ice core and tree-ring climate records in the TP (red = warm climate; blue = cold climate). (a) 10-yr averages of δ18O in the past 2,000 years recorded in the Guliya, Dunde, Puruogangri, and Dasuopu ice cores. (b) Temperature change curve in the past 2,000 years in the TP reconstructed from the four ice cores. (c) Temperature change curve in the past 2,000 years in the TP reconstructed from tree rings. The z score in the figure refers to the normalized anomalies, which consider both mean and standard deviation
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
Ice core and tree-ring climate records in the TP (red = warm climate; blue = cold climate). (a) 10-yr averages of δ18O in the past 2,000 years recorded in the Guliya, Dunde, Puruogangri, and Dasuopu ice cores. (b) Temperature change curve in the past 2,000 years in the TP reconstructed from the four ice cores. (c) Temperature change curve in the past 2,000 years in the TP reconstructed from tree rings. The z score in the figure refers to the normalized anomalies, which consider both mean and standard deviation
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
The δ18O record for the Dunde ice core (Fig. 1a) shows overall decreasing temperature trends with fluctuation starting in the fifth century and culminating to the coldest climate in the tenth century, followed by a warming to the relative warmth of the thirteenth century. The LIA started in AD 1400 and contained three cold periods in the fifteenth, seventeenth, and nineteenth centuries (Yao and Thompson 1992), culminating in the warm twentieth century.
In the Puruogangri ice core, the δ18O record (Fig. 1a) illustrates a temperature transition from frequent and intense cooling to obvious warming around AD 1000. The twelfth to thirteenth centuries were a period of minor warming, and the nineteenth century was cold. This record indicates little about the Medieval Warm Period (MWP), and the LIA is not clearly expressed in this ice core record, but the twentieth century warming is significant (Thompson et al. 2006).
Temperature anomalies recorded by δ18O in the Dasuopu ice core (Fig. 1a) show cool periods between AD 0 and 700 and between AD 1000 and 1840, although, like Puruogangri, the MWP is poorly expressed. Temperatures dropped to the lowest levels at the beginning of the nineteenth century, marking the LIA in this region, and as in the other ice core records the warming trend was very clear during the twentieth century (Yao et al. 2002).
After examining the δ18O records in the four ice cores, a comprehensive temperature proxy curve can be delineated (Fig. 1b) that shows an overall warming trend during the past 2,000 years. The climate remained stable with little fluctuation until AD 1600, followed by three significant cold periods in the seventeenth, eighteenth, and late nineteenth centuries. Rapid warming began in the 1960s, culminating in the highest levels of the past two millennia in the last 30 years.
Tree-ring records are also regarded as temperature proxies. The reconstruction of tree-ring width at the Dulan upper forest limit on the east TP covers the past 2,000 years and is compared with ice core records (Y. Liu et al. 2009). The annually resolved time series of temperature anomalies during the past 2,000 years (Fig. 1c) show a slow temperature decrease from the early first century to AD 350 characterized by strong interannual and decadal variability. Temperature anomalies exhibit drastic fluctuations afterward. However, because of limited sample density, substantial changes between the years AD 784 and 989 cannot be confirmed. Several cold periods occurred between the sixteenth and eighteenth centuries, representing the LIA in this region. Just as in the ice core records, the late-twentieth-century warming trend is significant. Overall, the records of temperature changes retrieved from tree rings are consistent with those from ice cores over the northeast TP.
Records of temperature variations from ice core and tree-ring records are consistent over the past 2,000 years. From the third to the fifth century, the temperature was relatively low and was followed by moderate warming from the fifth to the mid-twelfth century. Warming continued from the mid-twelfth century to the late fourteenth century and was followed by the LIA cold climate from the fifteenth to the late nineteenth century. In both types of proxy records, the accelerating warming (Fig. 1) since the beginning of the twentieth century on the TP is unprecedented in the last 2,000 years (Yao et al. 2007; Thompson 2017; Thompson et al. 2018).
It should be pointed out that the TP proxy data are not only useful for paleoclimate analyses, but also have the potential to provide valuable information for the paleo models’ cross validation over the TP region; the designs of such paleo model intercomparison experiments have been reported recently (e.g., Kageyama et al. 2018; Jungclaus et al. 2017).
RECENT RAPID ATMOSPHERIC WARMING ON THE TP.
The climate on the TP is characterized by low air temperatures, high diurnal temperature range (DTR), and low seasonal temperature variations (Xie and Zhu 2013). The annual mean temperature across the TP is generally below 0°C and decreases from east to west (Frauenfeld et al. 2005). The TP has undergone significant warming during the recent decades (Liu and Chen 2000; Zhou and Zhang 2005; Wang et al. 2008; Zhang and Zhou 2009; Guo and Wang 2012; Chen et al. 2013; Zhu et al. 2013; Song et al. 2014; Cai et al. 2017). The warming in this region started in the early 1950s, much earlier than in the Northern Hemisphere (NH), which started in the mid-1970s (Liu and Chen 2000; Niu et al. 2004). From 1955 to 1996 the warming rate was 0.16°C decade–1, substantially higher than that of the NH (0.054 K decade–1) and of the northern midlatitudes during the same period (Liu and Chen 2000; Oku et al. 2006; Duan and Xiao 2015). A sudden jump in the warming occurred during the mid-1980s (Niu et al. 2004). The most dramatic temperature increase occurred during the 1990s (Gao et al. 2015), with a rate of 0.25°C decade–1 from 1998 to 2013 (Duan and Xiao 2015), which is in contrast to the cooling trend in the rest of China. Figure 2 shows the variations in the annual mean temperature record, averaged over 91 stations on the TP, during the period from 1970 to 2014, which is compared with that averaged using the Climatic Research Unit gridded data (Jones et al. 2012) for the continent in the NH high-latitudinal (to the north of 60°N) region. During the period from 1970 to 2014, the warming rate of the annual mean temperature based on the average of 91 stations on the TP was 0.35°C decade–1, slightly lower than the warming rate (0.48°C decade–1) over the continent in the NH high-latitudinal region using the Climatic Research Unit (CRU) gridded data. The published record showed that the Antarctic decadal temperature trend during 1957–2006 was 0.12°C decade–1 (Steig et al. 2009). The data indicate the TP had a significantly stronger warming compared with those over the NH and northern midlatitude. The TP warming rate was slightly less than the one in the NH high-latitude area, but it was higher than the published Antarctic records (Steig et al. 2009; Bromwich et al. 2013). The strongest warming occurred in the winter months (Du et al. 2004; Liu and Chen 2000; Chen et al. 2006), about twice as much as the annual mean (Liu and Chen 2000). The magnitude of climate warming increases from south to north; the most significant warming was found in the northern part of the TP (e.g., Yang et al. 2011; Chen et al. 2013; You et al. 2016).

(top) Time series of annual mean maximum, mean, and minimum air temperature anomalies, and diurnal temperature range over the TP region and NH high-latitude (60°–90°N) region, respectively, and (bottom) elevation dependence of winter mean air temperature over the TP during the period 1970–2014. The TP temperature data are from 91 in situ stations derived by China Meteorological Administration, while those for the NH high latitudes are derived from CRU 4.0. The anomaly is calculated based on the 1971–2000 climatology.
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1

(top) Time series of annual mean maximum, mean, and minimum air temperature anomalies, and diurnal temperature range over the TP region and NH high-latitude (60°–90°N) region, respectively, and (bottom) elevation dependence of winter mean air temperature over the TP during the period 1970–2014. The TP temperature data are from 91 in situ stations derived by China Meteorological Administration, while those for the NH high latitudes are derived from CRU 4.0. The anomaly is calculated based on the 1971–2000 climatology.
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
(top) Time series of annual mean maximum, mean, and minimum air temperature anomalies, and diurnal temperature range over the TP region and NH high-latitude (60°–90°N) region, respectively, and (bottom) elevation dependence of winter mean air temperature over the TP during the period 1970–2014. The TP temperature data are from 91 in situ stations derived by China Meteorological Administration, while those for the NH high latitudes are derived from CRU 4.0. The anomaly is calculated based on the 1971–2000 climatology.
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
Similar to mean air temperature, both minimum and maximum temperatures (Tmin and Tmax, respectively) exhibited significant warming trends (0.45° and 0.26°C decade–1, respectively) from 1961 to 2005 (Duan et al. 2006; Duan and Wu 2006; You et al. 2008). In particular, during the period 1970–2014, Tmin and Tmax reached 0.42° and 0.34°C decade–1, only slightly less than the warming rates of Tmin (0.55°C decade–1) and Tmax (0.43°C decade–1) for the NH high latitudes, respectively (Fig. 2). Due to greater warming in Tmin than in Tmax, the DTR decreased noticeably: −0.19°C decade–1 during 1979–2012 (Yang and Ren 2017) and −0.08°C decade–1 during 1970–2014 (Fig. 2), respectively. Studies found that the changes in radiative processes were mainly responsible for the decreased DTR (e.g., Yang and Ren 2017). The increased low cloud cover tended to induce radiative cooling during daytime and warming during the night (Yang and Ren 2017; Duan and Xiao 2015).
There is growing evidence of elevation-dependent warming (EDW; Pepin et al. 2015; Thompson et al. 2018), or amplified warming rate with elevation (X. P. Li et al. 2017), over and around the TP (Fig. 2). This phenomenon is especially pronounced during winter and fall, as indicated by in situ observation data from stations below 5,000 m above mean sea level (MSL; Yan and Liu 2014). The Moderate Resolution Imaging Spectroradiometer (MODIS) data suggest that EDW may not occur above 5,000 m MSL (Qin et al. 2009). Mean minimum temperatures also show that EDW occurs on an annual basis (Yan and Liu 2014; X. D. Liu et al. 2009). Such tendencies have manifested mainly since the 1990s (Fig. 2) and may continue in the future, especially during the winter and spring seasons (X. D. Liu et al. 2009).
As a consequence of the greenhouse effect, the TP is warming faster than the global average. Studies also suggest that increased absorbed energy through the snow–albedo feedback (Liu and Chen 2000) and cloud–radiation interactions (Duan and Xiao 2015) may also contribute to this rapid warming over the TP. Decreased snow cover increases the absorption of solar shortwave radiation, which then enhances atmospheric warming (Rangwala et al. 2010). Meanwhile, less cloud cover results in more downward solar radiation, which ultimately causes surface warming (Zhang et al. 2008; Kuang and Jiao 2016). In addition, changes in surface water vapors, atmospheric circulation, and land uses are all likely contributors to the warming, especially for winter warming on the TP (Cui and Graf 2009; Rangwala et al. 2009). Moreover, effects of snow–albedo feedbacks and solar radiations are also responsible for the warming, especially the EDW, in the TP (Zhang et al. 2003; Chen et al. 2003). The current snow line is expected to retreat to higher elevations under the overall climate warming. The surface absorbs more incoming solar radiation as the snow line retreats upslope, which then causes enhanced warming at that elevation. The warming leads to more snow melting and snow-line ascension, forming a positive feedback.
The accelerated climate warming on the TP has caused significant glacier retreat, snowmelt, permafrost degradation, vegetation change, and increased climate aridity, which will be discussed in the next section and in the “Impact on ecosystem” section (Cheng and Wu 2007; Piao et al. 2010; Yao et al. 2012a; Guo and Wang 2013; Immerzeel et al. 2010; K. Yang et al. 2014; Gao et al. 2015; Xu and Liu 2007). Despite the significant progress in understanding the warming TP environment, scientists have identified several issues that need further investigation. Current evidence for rapid warming and significant EDW phenomenon generally come from in situ data below 5,000 m MSL. However, how the air temperatures did, and will, change above 5,000 m MSL is still unknown due to lack of in situ observations, as these regions are largely covered by glaciers and snow. Furthermore, model projections have suggested more obvious warming on the TP in the twenty-first century compared with the rest of China (Xu et al. 2003). Under the Special Report on Emissions Scenarios (SRES) A1B scenario, a 4°C warming is likely to occur over the TP within the next 100 years (Meehl et al. 2007). The mechanisms driving the rise of future temperature have not been comprehensively investigated. It is imperative to investigate both how air temperatures change in regions of higher elevation and the driving mechanisms for future warming. The warming and its altitudinal dependence have great implications for TP water resources and environmental changes.
RECENT INTENSIVE CRYOSPHERIC MELT AND HYDROSPHERIC RESPONSES.
Climate warming brought remarkable changes to the cryosphere on the TP, including glacier retreat and variations in snow amount and cover, as well as increase in temperature, degradation of permafrost, and thickening of the active layer (Kang et al. 2010a ; Bibi et al. 2018). Yao et al. (2012b) conducted a comprehensive and systematic assessment of the glacier status on the TP and its surrounding regions. They investigated the retreat rate of 82 glaciers, the area reduction of 7,090, and mass balance changes in 15 glaciers. They concluded that the glaciers were experiencing extraordinary shrinkage, as shown by the reduction in glacial length and area, and negative mass balance. The most intensive shrinkage occurred in the Himalayas (excluding the Karakorum). The shrinkage was not homogeneous across the TP: it generally decreased from the Himalayas to the continental interior and was least pronounced in the eastern Pamir (Fig. 3a).

(a) Observed changes in glacier (m yr–1; from Yao et al. 2012b), (b) simulated changes in active layer thickness during 1981–2010 (m decade–1; from Guo and Wang 2013), (c) observed changes in lake areas during 1976–2010 (from Lei et al. 2014), and (d) runoff change based on hydrological station data (modified from Cuo et al. 2014).
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1

(a) Observed changes in glacier (m yr–1; from Yao et al. 2012b), (b) simulated changes in active layer thickness during 1981–2010 (m decade–1; from Guo and Wang 2013), (c) observed changes in lake areas during 1976–2010 (from Lei et al. 2014), and (d) runoff change based on hydrological station data (modified from Cuo et al. 2014).
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
(a) Observed changes in glacier (m yr–1; from Yao et al. 2012b), (b) simulated changes in active layer thickness during 1981–2010 (m decade–1; from Guo and Wang 2013), (c) observed changes in lake areas during 1976–2010 (from Lei et al. 2014), and (d) runoff change based on hydrological station data (modified from Cuo et al. 2014).
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
Snow-covered days and snow depth also show great changes, though with regional and periodical differences. Both numbers decreased in the north and northwest regions, while they increased in the southwest edge and the southeast part of the TP from 2000 to 2014 (Huang et al. 2016). Overall, in situ observations and multisensor satellite data (Qin et al. 2006) show a small increasing trend in snow cover over the TP between 1951 and 1997, and a slight decreasing trend was identified between 1997 and 2012, mostly through the use of satellite images (S. S. Shen et al. 2015). Newer methods are expected to be able to directly measure the snow depth (Dozier et al. 2016). Using the observed temperature and precipitation with other meteorological forcing and a land surface model, the increase in the area-mean active layer thickness by 0.15 m decade–1 in 1981–2010 was simulated (Guo and Wang 2013). Figure 3b shows a nearly homogeneous increase in the active layer thickness over TP. Long-term soil temperature measurements indicated that the lower altitudinal limit of permafrost moved up by 25 m in the north of the TP during the 1980s, 1990s, and 2000s and between 50 and 80 m in the south of the TP during the 1990s and 2000s (Cheng and Wu 2007). The permafrost area and the soil freeze depth have generally decreased in the TP during the 1980s, 1990s, 2000s, and 2010s, as supported by both observational data and numerical simulation results (Guo and Wang 2013; Peng et al. 2017). Another study showed the thickness of seasonally frozen ground in the TP decreased by 0.05–0.22 m from 1967 to 1997, and the permafrost temperature increased by 0.2°–0.5°C from the 1970s to the 1990s over most of the TP (Zhao et al. 2004).
Inland lakes over the TP have also responded to the rapid climate warming. There is a contrast in lake dynamics between the TP interior and the Himalayas region. Since the middle of the 1990s, major lakes in the central TP have expanded significantly both in area and depth, whereas many lakes along the marginal region of the south and east TP have shrunk (Fig. 3c; Lei et al. 2014; K. Yang et al. 2014; Sheng and Li 2011; Sheng 2014). Increased precipitation may mainly be responsible for lake expansion in the central TP along with a contribution due to enhanced meltwater from cryosphere (Lei et al. 2014; K. Yang et al. 2014). On the other hand, reduced precipitation caused lake shrinkage in the Himalayas (Lei et al. 2014). The Qinghai Lake, the largest lake in China, shows dramatic lake-level fluctuation: it experienced a dramatic 3-m reduction of the lake level during 1961–2000, and then an increase by 1 m since. It seems that the climate variability and change, as well as anthropogenic influence, all played a role in the fluctuation (X. Li and D. Yang 2018, unpublished manuscript).
Furthermore, the river discharge has also changed under the climate warming. Through the multiple influences of glacier, permafrost, lake, snow, and climate, the runoff at hydrological stations show different characteristics: some are increasing and others are decreasing (Fig. 3d). The combined effects of spatiotemporal variations of precipitation, evaporation, and meltwater led to decreased discharge in the southern and eastern TP and a slight increase in the central TP since the beginning of the 1980s (Yang et al. 2011; K. Yang et al. 2014). At the basin scale, streamflow was dominated by precipitation in the northern, eastern, and southeastern basins, while meltwater or groundwater also contributed to streamflow in the central and western basins (Cuo et al. 2014). In large part, streamflow and lake variations are the products of the multispherical interactions in the TP Earth system and are directly affected by climate warming (K. Yang et al. 2014; Yao et al. 2015).
Accurate monitoring of cryospheric and hydrospheric processes are essential for understanding the changing multispherical interactions on the TP and for predicting their regional responses to climate warming. The recent studies highlighted the importance of in situ observations, which are required to support the application of relevant research methods (e.g., remote sensing, hydrological modeling, and other physically based methods). During the 2000s, in addition to the glacial measurements over the TP (Yao et al. 2012b), some in situ observations with more physical variables have been established, such as soil moisture and temperature monitoring networks in Naqu and Pali (Chen et al. 2017), inflow and evaporation measurements at typical lakes (Zhou et al. 2013), and observations of snow and glacier melt runoff in glacier-fed basins (Zhang et al. 2016). However, there remain large ungauged areas over the western TP, where the climate and environmental conditions are quite harsh. We suggest that numerical modeling tools with coupled cryospheric and hydrospheric processes along with multispherical observational data (e.g., Wang et al. 2017) should be developed in order to better physically and comprehensively understand the mechanism of lake change and runoff variations over the TP.
INTERACTIONS BETWEEN TP SURFACE PROCESSES AND MONSOONS.
One of the most imperative topics for the TP atmospheric research under changing climate and environment conditions are atmospheric energy and water circulations associated with land–atmosphere interactions over the TP and its surrounding regions. The TP has been identified as a region with the strongest land–atmosphere interactions in the midlatitude areas (Xue et al. 2010, 2017). This section focuses on the land–atmosphere interaction under the present climate with relatively short time scales (subseasonal to interannual).
The TP has a unique planetary boundary layer (PBL). The PBL over the TP is about 9 km MSL, much higher than many other regions. Results from reanalyses and modeling studies have indicated that weak atmospheric stability and the resultant deep PBLs were associated with higher upper-level potential vorticity values, which corresponded to a more southerly jet position and higher wind speeds (X. L. Chen et al. 2016). The penetrating convection and deep PBL south of the plateau are quite important in bringing up water vapor and aerosols into the tropopause/lower stratosphere, which may change the atmospheric heat balance across Asia.
With the unique geographic and atmospheric structure, the TP surface processes play an important role in regional climate. The basic atmospheric and land thermal and dynamic characteristics over the TP, as well as their relationships with the Asian monsoon based on recently available datasets, are an important subject in TP research (e.g., Li et al. 2014a; Lin et al. 2016; Ma and Ma 2016; Ge et al. 2017). Radiosonde data and a land data assimilation system coupled with a mesoscale model show that the vertical profile of temperature in the premonsoon season as a whole was warming below 200 hPa and cooling above 200 hPa. However, there were also relative warming and cooling subperiods alternately during this premonsoon period showing opposite temperature profiles. Furthermore, the troposphere over the TP in the subwarming periods was divided into three vertical layers in terms of the major heating processes: sensible heat transport below 450 hPa, latent heat from 450 to 250 hPa, and horizontal advection above 250 hPa originating in the southwest of the plateau. The cooling subperiods also exhibit similar vertical structures of each heating component, but net heating was reversed because of the influence of synoptic-scale disturbances through horizontal advection (Tamura and Koike 2010; Seto et al. 2013).
The mesoscale convective systems (MCSs) over the TP are closely related with heavy rainfall (Li et al. 2011) and rainfall diurnal variation (Li et al. 2014b), and they affect the MCSs in the downstream region (L. Li et al. 2017). The relationship between MCSs and soil moisture/precipitation has been investigated using different satellite and reanalysis products (Fig. 4; Sugimoto and Ueno 2010; Ueno et al. 2016; Zeng et al. 2016). These studies found that the occurrences of MCSs in the eastern and central-southern TP occurred with and without precipitation, respectively, indicating different vertical structure of MCSs and land surface heating condition in these two regions. On the interannual scale, a weak Indian monsoon accompanied drier and wetter soil moisture over the central-southern TP and eastern and western TP, respectively, with more precipitation in the eastern TP. The main driver was due to the enhancement of west–east soil moisture contrasts as discussed in Ueno et al. (2016).

(top left) Monthly precipitation and (bottom left) soil moisture anomaly from the average over 2008–10 produced by the Coordinated Asia–European Long-Term Observing System of Qinghai–Tibet Plateau Hydro-Meteorological Processes and the Asian-Monsoon System with Ground Satellite Image Data and Numerical Simulations (CEOP-AEGIS) project data. (right) Occurrences of daytime (red) and nighttime (black) MCS in 30°–31°N identified by infrared data are plotted on the day of year (DOY)–longitude diagram with temperature of black body (Tbb; K) distribution.
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1

(top left) Monthly precipitation and (bottom left) soil moisture anomaly from the average over 2008–10 produced by the Coordinated Asia–European Long-Term Observing System of Qinghai–Tibet Plateau Hydro-Meteorological Processes and the Asian-Monsoon System with Ground Satellite Image Data and Numerical Simulations (CEOP-AEGIS) project data. (right) Occurrences of daytime (red) and nighttime (black) MCS in 30°–31°N identified by infrared data are plotted on the day of year (DOY)–longitude diagram with temperature of black body (Tbb; K) distribution.
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
(top left) Monthly precipitation and (bottom left) soil moisture anomaly from the average over 2008–10 produced by the Coordinated Asia–European Long-Term Observing System of Qinghai–Tibet Plateau Hydro-Meteorological Processes and the Asian-Monsoon System with Ground Satellite Image Data and Numerical Simulations (CEOP-AEGIS) project data. (right) Occurrences of daytime (red) and nighttime (black) MCS in 30°–31°N identified by infrared data are plotted on the day of year (DOY)–longitude diagram with temperature of black body (Tbb; K) distribution.
Citation: Bulletin of the American Meteorological Society 100, 3; 10.1175/BAMS-D-17-0057.1
Various studies have explored the mechanisms through which Tibetan land processes interact with the atmosphere. Based on a general circulation model (GCM) study with and without sensible or latent heat as well as associated diagnostic analysis, it was found that sensible heating from the land surface and latent heating from cloud convection in the entire atmospheric column during the summer could induce a prominent center of minimum absolute potential vorticity and anomalous potential vorticity forcing near the tropopause within the westerly flow. These effects enhanced the meridional circulation of the Asian summer monsoon and influenced circulation in the Northern Hemisphere (Wu et al. 2016; Y. M. Liu et al. 2013). Moreover, analysis of the results from the regional climate model (RCM) experiments with and without a diurnal cycle of solar radiation show that a diurnal variation in solar radiation increases the sensible heat flux at the ground and enhances the thermal low near the surface and the summertime anticyclonic circulation in the upper troposphere over the TP. This is because the daytime solar flux was much greater than the nighttime cooling over TP, which also enhanced the South Asian and East Asian summer precipitation (Hong et al. 2012). Furthermore, the TP’s topographic effects were also discussed (Ma et al. 2014; Song et al. 2010).
Application of the TP land condition for the subseasonal to seasonal (S2S) prediction, especially the extreme events, is an important subject for land–atmosphere interaction studies. Recurrent extreme climate events, such as droughts and floods, are important features of the East Asian monsoon, especially over the Yangtze River basin. Xue et al. (2016) demonstrated the important role of the spring surface and subsurface temperature anomalies over the northern Rocky Mountain areas on the late spring–summer droughts/floods in the U.S. southern plains and surrounding areas. Following that approach, observational data analyses and modeling studies have also suggested that the spring surface and subsurface temperature anomalies over the TP have significant effects on the summer drought/flood in the East Asian lowland plains. Its effect is probably more important than the well-known sea surface temperature effects (Xue et al. 2018). Due to the importance of the S2S prediction, a multimodel experiment under the Global Energy and Water Exchanges project (GEWEX) and TPE support will be conducted to further investigate this issue (Xue et al. 2019). In addition, the TP snow and atmosphere interaction has also been investigated (Seol and Hong 2009; Li et al. 2018; Xiao and Duan 2016).
To approach the next scientific issues of the TP and its future change, it is important to understand the causes and consequences of accelerated warming of the TP regions and make credible future projections for society. For this purpose, multimodel intercomparisons would be very desirable. Future studies need to consider different time scales, such as interannual variability with water resource changes for hazard mitigation and social impact, as well as global warming time scales with glacier/climate/ecosystem changes and paleo time scales. Observational data sharing and cross-cutting discussions with other research groups (e.g., stratosphere, glacier, water resource, ecosystems, aerosol) could be very beneficial. The 2016 Xining workshop provided a very good starting point.
IMPACT ON ECOSYSTEM.
There have been significant advances in our understanding of variability and changes in TP spring phenology, movement of tree line, vegetation greening, and vegetation feedback associated with the climate variability and warming over the TP. The recent developments in satellite observations and field measurements have greatly enhanced our ability to understand the response of the ecosystem under a changing climate (e.g., Xiao et al. 2016; Jia et al. 2015; Lettenmaier et al. 2015; Cai et al. 2015). Recent studies have pinpointed the crucial role of precipitation in affecting spring phenology. Figure 5 shows multisource satellite-based phenological observations, which indicate widespread phenological advancing trends in most TP regions, but there is spring phenological delay over the southwest TP mainly due to the recent decline in spring precipitation (Shen et al. 2014; M. G. Shen et al. 2015a). The role of precipitation is further confirmed by the 7-yr spring phenological observations in Kobresia meadows in the central TP, where leaf-unfolding dates of dominant sedge and grass species are synchronized with the arrival of the monsoon rainfall (C. L. Li et al. 2016). Meanwhile, in addition to a number of experiments conducted over the TP that have refreshed our common knowledge on the temperature responses of phenological events, it has also been found that, contrary to the finding from northern high latitudes (Piao et al. 2015), spring phenology over the TP is determined by nighttime temperature (Shen et al. 2016).