不同热盐环流平均强度下北大西洋气候响应的差异

基于美国大气研究中心的CCSM3（Community Climate System Model version3）模式,对淡水扰动试验中不同热盐环流（thermohline circulation,THC）平均强度下,北大西洋气候响应的差异进行研究。结果表明：1）在不同平均强度下,北大西洋海洋、大气要素的气候态差异显著。相对于高平均强度,在低平均强度下,北大西洋地区海表温度（sea surface temperature,SST）、海表盐度（sea surface salinity,SSS）、海表密度（sea surface density,SSD）、表面气温（surface air temperature）异常减弱,最大负异常位于GIN（Greenland sea--Iceland sea--Norwegiansea）海域;海平面气压（sealev—elpressure,SLP）异常升高,相应于北大西洋海域降温,表现为异常冷性高压的响应特征;海冰分布区域向南扩大;北大西洋西部热带海域降水减少,导致热带辐合带（intertropical convergence zone,ITCZ）南移。2）在不同THC平均强度下,SST、SSS和SSD年际异常最显著的区域不同;在高平均强度下,最显著区域位于GIN海域,而在低平均强度下则位于拉布拉多海海域。3）在高平均强度下,北大西洋SST主导变率模态的变率极大区域位于GIN海,而在低平均强度下该极大区域不存在;北大西洋SLP的主导变率模态表现为类NAO型,但在高平均强度下,类NAO型表现得更明显。     

北极涛动与北大西洋涛动的低频变化特征

本文主要利用小波分析方法研究北极涛动(AO)和北大西洋涛动(NAO)的低频变化和周期特征。结果表明:AO在1965年以前有准两年周期振荡,1975年后转为准8 a周期和准16 a周期;NAO也存在相似的周期转变,但其准8 a周期出现在60年代末到1976年前后,并且没有明显的准16 a周期;AO和NAO准8 a周期的交叉小波能谱在1975年前后达到极大值,这与北半球气候突变时间基本吻合。另外,AO和NAO模态的北大西洋中心在1975年后表现出不同程度的东移,AO中心移到地中海地区,且太平洋中心明显增强,使其纬向对称的环形模态较突变前更显著。     

Nino海区SSTA的时频结构特征

根据1950～2003年Nino海区SSTA资料，采用小波变换方法分析了SST变化的多尺度结构及其强度变化。结果表明，Nino海区的SSTA序列表现为多层次相互嵌套的时频结构，存在着2～7a、8～20a和30a以上时间尺度的变化，经检验显著变化周期为2～7a，10a以上和1a以下的周期信号较弱。冷暖事件的能量主要集中在2～7a的尺度上，以准4a尺度的周期振荡最为显著。同一事件在不同海区的频率结构也不相同，1970年以后各尺度上冷暖事件的强度明显增大，有向低频发展的趋势。     

北大西洋年际变率的海气耦合模式模拟Ⅰ：局地海气相互作用

检验了一个全球海气耦合模式对北大西洋年际气候变率的模拟,讨论了导致这种年际变率型的物理机制,并分析了其对年代际变率的可能影响。北大西洋冬季SST的主导变率模态,在经向上表现为三核型,自北而南出现“- -”的带状距平型;最大距平中心位于副极地大洋、中纬度大洋的西部以及热带海域,耦合模式较为真实地再现了这一特征。与三核型SST异常相对应的大气环流型表现为北大西洋涛动,具有显著的正压结构。上述异常型主要发生在年际尺度,具有3—4年的谱峰;在次年代际尺度上,也存在谱峰。分析表明,模式中三核型SST异常的产生,主要来自大气的强迫,NAO增强,中纬度大洋上的西风减弱,海洋感热和潜热通量损失减少,中纬度大洋得到的净热通量增加,导致SST出现正距平;在包括Labrador海在内的副极地大洋,NAO增强、冰岛低压加深,气旋性环流增强,来自高纬度的冷空气吹过洋面,海气温差加大,大洋的感热通量损失增加,SST降低。热带地区东风的增强,也是导致那里SST降低的重要机制。三核型SST异常对大气的反馈作用较弱,文中没有证据表明它能够影响到北大西洋地区的年代际气候变率。     

冬季北太平洋优势气候模态的转移

采用EOF分解和小波分析,并引入相似度,分析冬季北太平洋的两个主要气候模态,即太平洋年代际振荡（PDO）模态与北太平洋涡旋振荡（NPGO）模态,及其结构特征随时间的演变。结果表明：1988/1989年的气候转移后,冬季海温距平（SSTA）优势模态为NPGO模态的年份越来越多,这种优势气候模态的转移现象表现出准18 a的年代际周期;SSTA与NPGO模态相似度的20年滑动平均在20世纪80年代中后期之后超过了SSTA与PDO模态的相应值,这表明此后SSTA的优势模态发生了转移,由PDO型转换为NPGO型;对典型时间段SSTA的合成分析显示,其优势模态由1988年前的PDO型转变为之后的NPGO型。     

HHT新技术及其对ENSO的诊断

年际及年代际时间变率是当代气候研究的重要问题之一。通过对近百年Nino3区月平均海面温度（SST）资料做HHT多时间尺度分析，结果表明：SST的变化包含了7个不同时间尺度的准周期振荡和一个世纪尺度的气候态，SST的主周期发生了一次显著的变化：1891-1943年主周期是准2a，1944-2002年的主周期是3～4a；分析不同模态对ENSO事件的作用表明：3～4a和6～8a分量决定了ENSO事件发生，具有相位锁定的作用，而其余尺度上的分量起着振幅和持续时间的调制作用；近百年来，冷、暖气候态变化对ENSO的冷、暖事件的影响并不显著；一些研究认为的1977年以来的“暖态有利于ENSO暖事件发生”的主要原因是：准18～20a、40a和平均气候态三个时间尺度振荡的共同作用在1977-2002年期间呈强暖相位的缘故。自20世纪90年代末期，这三个尺度的共同作用在暖相位的振幅显著的减弱，对ENSO暖事件的影响可能会减小，这在ENSO的预报中应该引起注意。     

北大西洋海表面温度锋与大西洋风暴路径及大气大尺度异常的关系研究

运用NCEP、Had ISST再分析资料,北大西洋涛动(NAO)月指数序列,探讨了海表面温度(SST)锋的时空变化特征,揭示了北大西洋SST锋的主要气候变率及其与北大西洋风暴轴和大气大尺度环流异常的关系。研究表明,剔除季节循环后的SST锋显示其最主要变率为锋区的向南/北摆动,其对应的风暴轴发生相应的西南/东北移动,并同时在北大西洋上空对应一个跨海盆的位势高度负/正异常。这种环流异常可引起高纬度海平面气压(SLP)的反气旋/气旋式环流,这有利于增强海表面风对大洋副极地环流的负/正涡度异常输入,进一步减弱/加强了高纬度上层冷水向SST锋区的输送。北大西洋SST锋的另一主要模态为锋区在南北方向的分支和合并。当SST锋异常在40°N~45°N以单支形式加强时,对流层位势高度场和SLP南北梯度增大,对应NAO正位相,此时风暴轴也为单支型;同时SLP异常场促使冰岛附近具有气旋式风应力异常,亚速尔地区具有反气旋式风应力异常,导致副极地环流和副热带环流均加强,增加高纬度冷水和低纬度暖水在锋区的输入,从而进一步增强40°N~45°N附近的SST锋区。当SST锋异常在40°N~45°N纬带南北发生分支时,风暴轴也同时出现北强南弱的南北分支,此时对应了负位相NAO,来自北南的冷暖水输送减弱,SST锋也发生减弱分支。此外,位于大洋内区的SST锋东端也存在一个偶极子型的模态,尽管其解释方差相对较小,但仍与偏东北的NAO型具有显著相关。谱分析表明,北大西洋SST锋与风暴轴具有1~3年和年代际共振,与中高纬大尺度环流也存在周期1~3年的共变信号,其中准一年共变信号体现了SST锋和NAO之间的对应关系。进一步诊断分析表明,SST锋上空的近表层大气斜压性和经向温度梯度随着SST锋的增强而增强,经向热通量的向北输送导致涡动有效位能的增加;海洋的非绝热加热产生更强的垂直热量通量,这有利于涡动有效位能释放成为涡动动能,从而表现为该区域的风暴轴加强,并进一步影响风暴轴中的天气尺度扰动与下游大尺度环流异常的相互作用过程。     

我国西南地区干湿季降水的主模态分析

利用我国西南地区26个台站降水资料,通过经验正交函数（EOF）分解的方法,分析了1980～2009年该地区干季（10～4月）和湿季（5～9月）降水的主模态。我国西南地区干季降水的时空变化存在两种主模态,它们分别可以解释总方差的22.4%和15.6%。第1主模态为全区一致型,具有准两年周期振荡的年际变化特征;第2主模态为东南—西北反向型,从20世纪90年代中期至21世纪初呈现2～3年的变化周期。我国西南地区湿季降水的时空变化存在三种主模态,它们分别可以解释总方差的17.1%,13.8%和11.1%。第1主模态为全区一致型,20世纪90年代初期具有较强的2～4年周期;第2主模态为经向偶极子型分布,并具有显著的4年周期;第3主模态为纬向偶极子型分布,具有2～4年的年际变化信号。进一步利用NCEP/NCAR再分析资料以及美国国家海洋和大气管理局（NOAA）的海表面温度（SST）资料,通过合成分析和回归分析的方法探讨了与干湿季降水各主模态对应的大尺度大气环流和海温状况。我国西南地区干季降水第1主模态与北极涛动（AO）有明显的正相关关系,对应的大气环流和海温状况表现为高纬北冰洋与中纬度地区上空高度场的反向异常分布,北大西洋和北太平洋海温低纬与中高纬的偶极子型异常分布;第2主模态与中高纬欧亚大陆上空高度场经向偶极子型异常分布有关,中纬度北太平洋的海温异常与该模态具有紧密的联系。我国西南地区湿季降水第1主模态与北大西洋涛动（NAO）显著负相关,对应的大气环流和海温状况表现为北大西洋上,高纬度与中纬度地区上空高度场的偶极子型异常分布,海温从低纬到中高纬的三极子型异常分布;第2主模态受欧亚大陆上空高度场经向三极子型异常分布影响,并与北太平洋海温异常的一致型分布有关;第3主模态可能与El Ni?o Modoki有关,同时受到南亚高压的影响,赤道太平洋海温的纬向三极子型异常分布对该模态具有一定的潜在预报意义。     

1953～2017年黄河源区气温变化的多尺度特征

基于黄河源区8个站点的年平均气温序列,利用集合经验模态分解（Ensemble Empirical Mode Decomposition,EEMD）方法,揭示了以玛多站为代表的黄河源区1953~2017年气温演变的多时间尺度特征,探讨不同时间尺度上的周期振荡对气温变化总体特征的影响程度,分析了黄河源区不同时间尺度的气温变化与海温指数,尤其是与北大西洋多年代际振荡（Atlantic Multidecadal Oscillation,AMO）间的关系。结果表明:（1）1953年以来黄河源区玛多站年平均气温以0.31 ℃/10 a的变化率表现为明显的增暖趋势,20世纪80年代后期开始转暖,尤其是进入20世纪90年代后期变暖更加明显。（2）1953~2017年,黄河源区年平均气温呈现3 a、6 a、11 a、25 a、64 a及65 a以上时间尺度的准周期变化,其中以准3 a和65 a以上时间尺度的振荡最显著,准3 a的年际振荡在21世纪以前振幅较大,而进入21世纪后年际振荡振幅减弱,65 a以上时间尺度的年代际振荡振幅明显加大。（3）1998年气候显著变暖以前,以准3 a周期为代表的年际振荡在气温演变过程中占据主导地位,1998年气候显著变暖以后,65 a以上时间尺度周期振荡的贡献率增加近5倍,与准3 a周期振荡的贡献相当。（4）气温与Nino3.4指数和PDO（Pacific Decadal Oscillation）指数的同期相关均不显著,但当气温领先PDO指数22 a时正相关最大且显著,不同于PDO指数,气温原始序列及其3个年代际尺度分量滞后AMO指数3~7 a或二者同期时相关性最高,这就意味着AMO对黄河源区气温具有显著影响。（5）AMO的正暖位相对应着包括中国的整个东亚地区偏暖,黄河源区只是受影响区域的一部分,20世纪60年代至90年代初期AMO的负冷位相期、20世纪90年代中后期至今AMO的正暖位相与黄河源区气温距平序列的负距平、正距平相对应,气温在65 a以上时间尺度的变化与AMO指数相关性更高,可见,AMO是影响黄河源区气温变化的一个重要的气候振荡,这种影响主要表现在年代际时间尺度上。     

CMIP5模式对AMO与PDO模拟评估及未来预估

利用1880—2009年海表温度(Sea Surface Temperature, SST)观测资料以及耦合模式比较计划第五阶段(Coupled Model Intercomparison Project phase 5,CMIP5)中4种情景(piControl、historical、RCP2.6、RCP4.5)下的模拟资料,通过资料对比,评估了CMIP5模式对两个最为重要年代际尺度模态——北大西洋年代际振荡(Atlantic Multidecadal Oscillation, AMO)和太平洋年代际振荡(Pacific Decadal Oscillation, PDO)的模拟性能,并分析了在不同增暖情景下,这两个海洋年代际模态的变化特征。结果表明:在historical和piControl情景下,多模式集合可以再现北太平洋、东太平洋和北大西洋海表温度的年代际变化中心,但模拟的AMO和PDO模态的振幅都偏弱,特别是PDO模态在东太平洋强度的再现能力较弱。与观测资料相比,在historical情景下对AMO和PDO时空特征模拟较好的模式有:CESM1-CAM5、FGOALS-g2、GISS-E2-H-CC、MIROC5和NorESM1-ME,多模式集合则有更好的模拟效果。在不同增暖情景下,AMO与PDO的空间特征基本一致且振幅差随增暖变化不明显,但是伴随全球增暖加强,两模态都呈现方差贡献减小的特征,尤其AMO模态。     

Influence of Low-frequency Solar Forcing on the East Asian Winter Monsoon Based on HadCM3 and Observations

In this study, we investigate the influence of low-frequency solar forcing on the East Asian winter monsoon(EAWM)by analyzing a four-member ensemble of 600-year simulations performed with Had CM3(Hadley Centre Coupled Model,version 3). We find that the EAWM is strengthened when total solar irradiance(TSI) increases on the multidecadal time scale. The model results indicate that positive TSI anomalies can result in the weakening of Atlantic meridional overturning circulation, causing negative sea surface temperature(SST) anomalies in the North Atlantic. Especially for the subtropical North Atlantic, the negative SST anomalies can excite an anomalous Rossby wave train that moves from the subtropical North Atlantic to the Greenland Sea and finally to Siberia. In this process, the positive sea-ice feedback over the Greenland Sea further enhances the Rossby wave. The wave train can reach the Siberian region, and strengthen the Siberian high. As a result, low-level East Asian winter circulation is strengthened and the surface air temperature in East Asia decreases. Overall,when solar forcing is stronger on the multidecadal time scale, the EAWM is typically stronger than normal. Finally, a similar linkage can be observed between the EAWM and solar forcing during the period 1850–1970.     

A 1,000-year ice core record of interannual to multidecadal variations in atmospheric circulation over the North Atlantic

Interannual to multidecadal modes in ocean/atmosphere dynamics in the North Atlantic region have been identified using sea salt aerosol proxy records from northern Greenland ice cores over the last 1,000 years. Sea salt concentrations show a consistent relationship with anomalies in the meridional pressure gradient over the North Atlantic region over all considered time scales. These pressure anomalies are connected to shifts in storm tracks, leading to lower pressure and higher storm activity, hence, higher sea salt export over the Greenland ice sheet. Two modes of long-term variability with a period of 10.4 years and 62 years could be identified. The latter is connected to long-term changes in sea surface temperature (SST) as documented by a high correlation of North Atlantic SST with our sea salt record over the last 150 years. Long-term reconstruction of these modes shows that the 10.4-year cycle has been a phenomenon persistent over the last millennium while the 62-year cycle has been mainly active after 1700. Accordingly, the longer-term persistence of this multidecadal variability in sea salt points also to significant variations in SST over the last 300 years.     

Impact of freshwater discharge from the Greenland ice sheet on North Atlantic climate variability

Using a coupled ocean–atmosphere general circulation model, we investigated the impact of Greenland ice sheet melting on North Atlantic climate variability. The positive-degree day (PDD) method was incorporated into the model to control continental ice melting (PDD run). Models with and without the PDD method produce a realistic pattern of North Atlantic sea surface temperature (SST) variability that fluctuates from decadal to multidecadal periods. However, the interdecadal variability in PDD run is significantly dominated in the longer time scale compared to that in the run without PDD method. The main oscillatory feature in these experiments likely resembles the density-driven oscillatory mode. A reduction in the ocean density over the subpolar Atlantic results in suppression of the Atlantic Meridional Overturning Circulation (AMOC), leading to a cold SST due to a weakening of northward heat transport. The decreased surface evaporation associated with the cold SST further reduces the ocean density and thus, simultaneously acts as a positive feedback mechanism. The southward meridional current associated with the suppressed AMOC causes a positive tendency in the ocean density through density advection, which accounts for the phase transition of this oscillatory mode. The Greenland ice melting process reduces the mean meridional current and meridional density gradient because of additional fresh water flux, which suppress the delayed negative feedback due to meridional density advection. As a result, the oscillation period becomes longer and the transition is more delayed.     

20世纪90年代以后华北初春低温增强和北大西洋海温关系

本文利用ECMWF再分析资料及Hadley中心提供的海温数据分析了20世纪90年代以后华北地区初春低温增强的原因,并通过数值模拟结果予以验证。结果表明,北大西洋“马蹄型”海温模态与影响我国华北地区的欧亚波列存在显著的相关关系。同时该海温模态与1997年以后北大西洋关键区垂直波作用通量有着较密切的相关关系,1997年以后北大西洋地区的500 hPa环流模态,整体呈现出东移南撤的趋势。1997年以后格陵兰岛东侧表面温度受异常热力强迫导致正值区增多,同时此处西风急流加大,有利于Rossby波向下游传播,导致其下游欧洲大陆地区形成暖脊。通过局地多尺度能量涡度分析法（Localized Multiscale Energy and Vorticity Analysis,简称MS-EVA）证明格陵兰岛东侧关键区表面温度的异常热力强迫作用与气压梯度力在对流层整层做正功,导致高层动能的增加并向外辐散,使得脊加强向北伸展。通过欧亚波列致使下游华北地区上空气旋式异常加强,促使亚洲极涡加强和稳定维持,华北地区温度下降剧烈,极端低温事件增多。最后通过CAM5.1模式模拟研究了北大西洋“马蹄型”海温模态对大气环流异常及华北地区极端低温的影响。模拟结果很好地验证了观测结果,进一步表明该海温模态可以通过激发出欧亚波列,影响欧亚大陆大气环流异常,进而导致我国华北地区气旋性加强和经向环流加大,极端低温事件增多。     

Decadal‐to‐interdecadal fluctuations of arctic sea‐ice cover and the atmospheric circulation during 1954–1994

Abstract

The relationship between the Arctic and subarctic sea‐ice concentration (SIC) anomalies, particularly those associated with the decadal‐scale Greenland and Labrador Seas “Ice and Salinity Anomalies (ISAs) “, and the overlying atmospheric circulation fluctuations is investigated using the singular value decomposition (SVD) and composite map analysis methods. The data analyzed are monthly SIC and sea level pressure (SLP) anomalies, which cover the northern hemisphere poleward of 45°N and extend over the 41‐year period 1954–1994.

The SVD₁ (first) mode of the coupled variability, which accounts for 57% of the square covariance, is for the most part an atmosphere‐to‐ice forcing mode characterized by the decadal timescale. The aforementioned ISA anomalies are clearly captured by this mode whose SIC anomalies are dominated by a strong dipole across Greenland. However, as part of the same mode, there is also a weaker SIC dipole in the northern North Pacific which has opposite‐signed anomalies in the Sea of Okhotsk and the Bering Sea. It is also shown that there exists a significant negative correlation between the decadal SIC variability in the Greenland‐Barents Seas region associated with this mode and the North Atlantic Oscillation, whose spectrum also exhibits a quasi‐decadal signal.

The SVD₂ mode accounts for 12% of the square covariance and shows no evidence of a dominant forcing field of either SIC or SLP. This SVD mode exhibits very low frequency (interdecadal) variability, and its co‐variability is mainly concentrated in the northern North Pacific. It appears to be a high‐latitude extension of the recently investigated interdecadal North Pacific Oscillation. The spatial structure of the second mode complements the case of the first SVD mode whose co‐variability mainly occurs in the northern North Atlantic.     

Tropical Atlantic Variability in a Coupled GCM

Summary:Tropical Atlantic Variability (TAV) is simulated in a coupled GCM. The TAV seems to be consistent with a dipole mode that involves both surface and subsurface oceanic dynamics. The poor correlation of the tropical North and South Atlantic SST is suggested to be distorted by the presence of a symmetric tropical Atlantic mode.     

Holocene climate variability as derived from alkenone sea surface temperature and coupled ocean-atmosphere model experiments

Holocene climate modes are identified by the statistical analysis of reconstructed sea surface temperatures (SSTs) from the tropical and North Atlantic regions. The leading mode of Holocene SST variability in the tropical region indicates a rapid warming from the early to mid Holocene followed by a relatively weak warming during the late Holocene. The dominant mode of the North Atlantic region SST captures the transition from relatively warm (cold) conditions in the eastern North Atlantic and the western Mediterranean Sea (the northern Red Sea) to relatively cold (warm) conditions in these regions from the early to late Holocene. This pattern of Holocene SST variability resembles the signature of the Arctic Oscillation/North Atlantic Oscillation (AO/NAO). The second mode of both tropical and North Atlantic regions captures a warming towards the mid Holocene and a subsequent cooling. The dominant modes of Holocene SST variability emphasize enhanced variability around 2300 and 1000 years. The leading mode of the coupled tropical-North Atlantic Holocene SST variability shows that an increase of tropical SST is accompanied by a decrease of SST in the eastern North Atlantic. An analogy with the instrumental period as well as the analysis of a long-term integration of a coupled ocean-atmosphere general circulation model suggest that the AO/NAO is one dominant mode of climate variability at millennial time scales.     

A 20-year coupled ocean-sea ice-atmosphere variability mode in the North Atlantic in an AOGCM

In order to understand potential predictability of the ocean and climate at the decadal time scales, it is crucial to improve our understanding of internal variability at this time scale. Here, we describe a 20-year mode of variability found in the North Atlantic in a 1,000-year pre-industrial simulation of the IPSL-CM5A-LR climate model. This mode involves the propagation of near-surface temperature and salinity anomalies along the southern branch of the subpolar gyre, leading to anomalous sea-ice melting in the Nordic Seas, which then forces sea-level pressure anomalies through anomalous surface atmospheric temperatures. The wind stress associated to this atmospheric structure influences the strength of the East Greenland Current across the Denmark Strait, which, in turn, induces near-surface temperature and salinity anomalies of opposite sign at the entrance of the Labrador Sea. This starts the second half of the cycle after approximatively 10 years. The time scale of the cycle is thus essentially set by advection of tracers along the southern branch of the subpolar gyre, and by the time needed for anomalous East Greenland Current to accumulate heat and freshwater anomalies at the entrance of the Labrador Sea. The Atlantic meridional overturning circulation (AMOC) does not play a dominant role in the mode that is confined in the subpolar North Atlantic, but it also has a 20-year preferred timescale. This is due to the influence of the propagating salinity anomalies on the oceanic deep convection. The existence of this preferred timescale has important implications in terms of potential predictability of the North Atlantic climate in the model, although its realism remains questionable and is discussed.