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硅酸盐学报 1982年第1期 1-8页

作者： d.a.jefferson,温树林,j.m.thomas 英国剑桥大学物理化学系中国科学院上海硅酸盐研究所英国剑桥大学物理化学系

三种经过不同温度下热处理的热压氮化硅样品（含5wt％Y2O3和2wt％Al2O3添加物）,用X射线衍射、X射线微量分析和高分辨率电子显微镜进行了研究。结果表明在热处理后晶界区产生相变化。晶界玻璃相由于热处理而结晶化。

关键词：晶界玻璃相结晶化氮化硅四氮化三硅氮化物晶格像

(Ca,Sr)GeO3晶体中环-链结构的共生长

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化学学报 1983年第4期41卷 297-301页

作者：温树林 d.a.jefferson j.m.thomas 中国科学院上海硅酸盐研究所英国剑桥大学物理化学系英国剑桥大学物理化学系

通过（1-x）CaO+xSrO+GeO2→（Ca1-xSrx）GeO3的反应获得的产物经过淬火、退火形成晶态。用X射线衍射和分析电子显微镜进行研究,并用高分辨电子显微镜观察,由jEOLjEm200CX获得晶格象照片。研究结果指出:（Ca,Sr）GeO3晶体中存在环-链结... 详细信息

通过（1-x）CaO+xSrO+GeO2→（Ca1-xSrx）GeO3的反应获得的产物经过淬火、退火形成晶态。用X射线衍射和分析电子显微镜进行研究,并用高分辨电子显微镜观察,由jEOLjEm200CX获得晶格象照片。研究结果指出:（Ca,Sr）GeO3晶体中存在环-链结构的共生长,其共生长接触晶面为（100）SrGeO3/（101）CaGaO3·

关键词：链结构 Ca,Sr)GeO3 射线衍射晶格象电子衍射晶面面(晶体) 晶种链状结构晶粒颗粒硅灰石矽灰石链状硅酸盐矿物照片电子显微镜电镜 Sr 晶体

高分辨率电镜(HREm)对硅灰石中离子替换的研究

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矿物学报 1984年第1期 1-3+97页

作者：温树林,d.a.jefferson,j.m.thomas 中国科学院上海硅酸盐研究所英国剑桥大学物理化学系英国剑桥大学物理化学系

一、前言在材料化学中,一个很重要的问题是确定材料中加入多少量的别种离子或离子团以取代原来的离子,而不使原来的结构产生变化。这是寻找新材料的一个重要途径。目前,迅速发展的核能源中,一个迫切需要解决的重大研究课题是核废料处... 详细信息

一、前言在材料化学中,一个很重要的问题是确定材料中加入多少量的别种离子或离子团以取代原来的离子,而不使原来的结构产生变化。这是寻找新材料的一个重要途径。目前,迅速发展的核能源中,一个迫切需要解决的重大研究课题是核废料处理。而将核废料用固体反应引入一种稳定的矿物,如硅灰石,可能是解决这一课题的一个十分有希望的途径。以前的研究指出,Sr2+取代Ca2+可以使链状硅灰石（CaSiO3）(照片1a)成为环状的假硅灰石结构（照片1b）;锗取代硅氧四面体中的硅可以形成环-链结构的共生长。从几何因素上考虑,铝氧四面体[AlO4]和硅氧四面体[SiO4]大小相近。因此用[AlO4]

关键词：硅灰石照片 HREm 晶格象矽灰石链状硅酸盐矿物中离子电子衍射多面体四面体

CaO-SrO-SiO2-GeO2系统中环链结构转换的研究

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科学通报 1984年第20期29卷 1247-1250页

作者：温树林,d.a.jefferson,j.m.thomas 中国科学院上海硅酸盐研究所英国剑桥大学物理化学系英国剑桥大学物理化学系

前言偏硅酸钙有硅灰石和假硅灰石两种结构,其中硅灰石为链状结构,假硅灰石为环状结构,转变温度为1250℃。当用Sr2+取代偏硅酸钙中的Ca2+时,产生环状结构,与温度没有关系。与此同时,用锗取代偏硅酸钙中的硅所生成的产物应如何呢?对硅... 详细信息

前言偏硅酸钙有硅灰石和假硅灰石两种结构,其中硅灰石为链状结构,假硅灰石为环状结构,转变温度为1250℃。当用Sr2+取代偏硅酸钙中的Ca2+时,产生环状结构,与温度没有关系。与此同时,用锗取代偏硅酸钙中的硅所生成的产物应如何呢?对硅进行全部取代生成的锗酸钙肯定是链状结构,与温度没有关系。但如果进行局部取代,并进一步对阴阳离子同时取

关键词：链状环结构类型离子半径比假硅灰石阳离子正离子环链硅氧四面体 SrO 链状结构环状结构 CaO-SrO-SiO2-GeO2 晶格象

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环-链结构共生长

自然杂志 1982年第5期 396-397页

作者：温树林,d.a.jefferson,j.m.thomas 中国科学院上海硅酸盐研究所英国剑桥大学物理化学系英国剑桥大学物理化学系

硅灰石（CaSiO3）呈链状结构,属三斜晶系,但在1250°时发生相变,成为环状结构;对称性也由三斜变到假六方。

关键词：链结构链状结构环状结构

THE TRANSITION BETWEEN CHAIN ANd RING STRUCTURES IN THE SYSTEm OF CaO-SrO-SiO_2-GeO_2

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Chinese Science Bulletin 1985年第4期30卷 471-474页

作者：温树林 d.a.jefferson j.m.thomas Shanghai Institute of Ceramics Academia Sinica department of Physical Chemistry University of Cambrdge U. K. department of Physical Chemistry University of Cambrdge U. K.? INTRODUCTION Calcium metasilicate possesses two kinds of structures namely wollastonite and pseudowollastonite. Wollastonite has chain structure but pseudowollastonite ring structure. The transition temperature between the two is 1250°C.

Ⅰ. INTROdUCTION Calcium metasilicate possesses two kinds of structures, namely, wollastonite and pseudowollastonite. Wollastonite has chain structure, but pseudowollastonite ring structure. The transition temperature... 详细信息

关键词： Radius corner hough appearance powerful partially annealing 刃刀 struc figure

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硅锗酸钙多型体晶格象的观察

电子显微学报 1983年第1期 5-7页

作者：温树林 jefferson,d.A thomas,j.m 中国科学院上海硅酸盐研究所英国剑桥大学物理化学系英国剑桥大学物理化学系

硅灰石（CaSiO3）是链状硅酸盐。本工作发现,用锗局部取代硅所形成的硅锗酸钙,只要取代量X≤0.2,其结构与硅灰石完全相同。但形成的多型体无序程度较高。样品由氧化钙、二氧化锗和二氧化硅在1500℃反应制得。在制备过程中,配料按照关系m... 详细信息

硅灰石（CaSiO3）是链状硅酸盐。本工作发现,用锗局部取代硅所形成的硅锗酸钙,只要取代量X≤0.2,其结构与硅灰石完全相同。但形成的多型体无序程度较高。样品由氧化钙、二氧化锗和二氧化硅在1500℃反应制得。在制备过程中,配料按照关系mSi+mGe=mCa进行。式中mSi,mGe和mCa分别代表SiO2,GeO和CaO的克分子数。由此取代量为:X=mGe/mGe+mSi。对制得的Ca(Si1-xGex)O3晶体进行X—射线衍射和电子衍射,均证明其结构与硅灰石相同。样品用jEOL200CX高分辨电子显微镜进行了观察并获得晶格象照片。晶格象指出Ca(Si0.8Ge0.2O3具有硅灰石结构。晶格象还显示单斜和三斜两种多型体交替分布的情形。其无序分布程度较高。

关键词：晶格象晶体硅灰石矽灰石链状硅酸盐矿物电子衍射环状结构堆积顺序高分辨率电子显微镜 CaO 硅氧四面体链状结构单斜多型体照片

STCF conceptual design report (Volume 1): Physics & detector

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Frontiers of physics 2024年第1期19卷 1-154页

作者： m.Achasov X.C.Ai L.P.An R.Aliberti Q.An X.Z.Bai Y.Bai O.Bakina A.Barnyakov V.Blinov V.Bobrovnikov d.Bodrov A.Bogomyagkov A.Bondar I.Boyko Z.H.Bu F.m.Cai H.Cai j.j.Cao Q.H.Cao X.Cao Z.Cao Q.Chang K.T.Chao d.Y.Chen H.Chen H.X.Chen j.F.Chen K.Chen L.L.Chen P.Chen S.L.Chen S.m.Chen S.Chen S.P.Chen W.Chen X.Chen X.F.Chen X.R.Chen Y.Chen Y.Q.Chen H.Y.Cheng j.Cheng S.Cheng T.G.Cheng j.P.dai L.Y.dai X.C.dai d.dedovich A.denig I.denisenko j.m.dias d.Z.ding L.Y.dong W.H.dong V.druzhinin d.S.du Y.j.du Z.G.du L.m.duan d.Epifanov Y.L.Fan S.S.Fang Z.j.Fang G.Fedotovich C.Q.Feng X.Feng Y.T.Feng j.L.Fu j.Gao Y.N.Gao P.S.Ge C.Q.Geng L.S.Geng A.Gilman L.Gong T.Gong B.Gou W.Gradl j.L.Gu A.Guevara L.C.Gui A.Q.Guo F.K.Guo j.C.Guo j.Guo Y.P.Guo Z.H.Guo A.Guskov K.L.Han L.Han m.Han X.Q.Hao j.B.He S.Q.He X.G.He Y.L.He Z.B.He Z.X.Heng B.L.Hou T.j.Hou Y.R.Hou C.Y.Hu H.m.Hu K.Hu R.j.Hu W.H.Hu X.H.Hu Y.C.Hu j.Hua G.S.Huang j.S.Huang m.Huang Q.Y.Huang W.Q.Huang X.T.Huang X.j.Huang Y.B.Huang Y.S.Huang N.Hüsken V.Ivanov Q.P.ji j.j.jia S.jia Z.K.jia H.B.jiang j.jiang S.Z.jiang j.B.jiao Z.jiao H.j.jing X.L.Kang X.S.Kang B.C.Ke m.Kenzie A.Khoukaz I.Koop E.Kravchenko A.Kuzmin Y.Lei E.Levichev C.H.Li C.Li d.Y.Li F.Li G.Li G.Li H.B.Li H.Li H.N.Li H.j.Li H.L.Li j.m.Li j.Li L.Li L.Li L.Y.Li N.Li P.R.Li R.H.Li S.Li T.Li W.j.Li X.Li X.H.Li X.Q.Li X.H.Li Y.Li Y.Y.Li Z.j.Li H.Liang j.H.Liang Y.T.Liang G.R.Liao L.Z.Liao Y.Liao C.X.Lin d.X.Lin X.S.Lin B.j.Liu C.W.Liu d.Liu F.Liu G.m.Liu H.B.Liu j.Liu j.j.Liu j.B.Liu K.Liu K.Y.Liu K.Liu L.Liu Q.Liu S.B.Liu T.Liu X.Liu Y.W.Liu Y.Liu Y.L.Liu Z.Q.Liu Z.Y.Liu Z.W.Liu I.Logashenko Y.Long C.G.Lu j.X.Lu N.Lu Q.F.Lü Y.Lu Y.Lu Z.Lu P.Lukin F.j.Luo T.Luo X.F.Luo Y.H.Luo H.j.Lyu X.R.Lyu j.P.ma P.ma Y.ma Y.m.ma F.maas S.malde d.matvienko Z.X.meng R.mitchell A.Nefediev Y.Nefedov S.L.Olsen Q.Ouyang P.Pakhlov G.Pakhlova X.Pan Y.Pan E.Passemar Y.P.Pei H.P.Peng L.Peng X.Y.Peng X.j.Peng K.Peters S.Pivovarov E.Pyata B.B.Qi Y.Q.Qi W.B.Qian Y.Qian C.F.Qiao j.j.Qin j.j.Qin L.Q.Qin X.S.Qin T.L.Qiu j.Rademacker C.F.Redmer H.Y.Sang Anhui University Hefei 230039China Beihang University Beijing 100191China Budker Institute of Nuclear Physics Novosibirsk 630090Russia CAS Key Laboratory of Theoretical Physics Institute of Theoretical PhysicsChinese Academy of SciencesBeijing 100190China Cavendish Laboratory University of CambridgeJJ Thomson AveCambridge CB30HEUnited Kingdom Central China Normal University Wuhan 430079China Central South University Changsha 410083China China University of Geosciences Wuhan 430074China China University of mining and Technology Xuzhou 221116China École Polytechnique Fédérale de Lausanne(EPFL) LausanneSwitzerland Fudan University Shanghai 200433China Goethe University Frankfurt D-60325 Frankfurt am MainGermany Guangxi Normal University Guilin 541004China Guangxi Uninversity Nanning 530004China Hangzhou Institute for Advanced Study UCASHangzhou 310024China Hebei Normal University Shijiazhuang 050024China Hebei University Baoding 071002China Hefei University of Technology Hefei 230601China Helmholtz Institute mainz Staudinger Weg 18D-55099 MainzGermany Henan Normal University Xinxiang 453007China Henan University Kaifeng 475004China High Energy Physics Center Chung-Ang UniversitySeoul 06974Korea Higher School of Economy 11 Pokrovsky Bulvar Moscow 109028Russia Huangshan University Huangshan 245000China Hubei University of Automotive Technology Shiyan 442002China Hunan Normal University Changsha 410081China Hunan University of Science and Technology Xiangtan 411201China Hunan University Changsha 410082China Indiana University BloomingtonIndiana 47405USA Inner mongolia University Hohhot 010021China Institute of Advanced Science Facilities Shenzhen 518107China Institute of High Energy Physics Chinese Academy of SciencesBeijing 100049China Institute of modern Physics Chinese Academy of SciencesLanzhou 730000China Institute of Physics Academia SinicaTaipeiTaiwan 11529China Institute of Theoretical Physics Chinese Academy of SciencesBeijing 100190China jilin University Changch

The superτ-charm facility(STCF)is an electron–positron collider proposed by the Chinese particle physics *** is designed to operate in a center-of-mass energy range from 2 to 7 GeV with a peak luminosity of 0.5×10^(35) cm^(–2)·s^(–1) or *** STCF will produce a data sample about a factor of 100 larger than that of the presentτ-charm factory—the BEPCII,providing a unique platform for exploring the asymmetry of matter-antimatter(charge-parity violation),in-depth studies of the internal structure of hadrons and the nature of non-perturbative strong interactions,as well as searching for exotic hadrons and physics beyond the Standard *** STCF project in China is under development with an extensive R&d *** document presents the physics opportunities at the STCF,describes conceptual designs of the STCF detector system,and discusses future plans for detector R&d and physics case studies.

关键词： electron–positron collider tau-charm region high luminosity STCF detector conceptual design

Changes in otolaryngology application requirements and match outcomes:Are we doing any better?

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World journal of Otorhinolaryngology-Head and Neck Surgery 2023年第2期9卷 144-152页

作者： Emma de Ravin Ariel S.Frost Neal R.Godse Amber d.Shaffer Noel jabbour Barry m.Schaitkin jason Newman Leila j.mady department of Otorhinolaryngology-Head and Neck Surgery University of Pennsylvania Health SystemPhiladelphiaPennsylvaniaUSA Head and Neck Institute Cleveland ClinicClevelandOhioUSA division of Pediatric Otolaryngology Children's Hospital of Pittsburgh of UPMCPittsburghPennsylvaniaUSA department of Otolaryngology University of Pittsburgh Medical CenterPittsburghPennsylvaniaUSA department of Otolaryngology-Head and NeckSurgery Medical Universityof South CarolinaCharlestonSouth CarolinaUSA mUSC Hollings Cancer Center CharlestonSouthCarolinaUSA department of Otolaryngology-Head and Neck Surgery Thomas Jefferson UniversityPhiladelphiaPennsylvaniaUSA Cancer Risk and Control Program of Excellence Sidney Kimmel Cancer CenterPhiladelphiaPennsylvaniaUSA

Objectives:Otolaryngology-specific requirements were piloted to minimize applicant and program *** investigated the impact of introducing and then removing these requirements on match ***:2014-2021 National Resident matching Program?data were *** primary outcome was the impact of Otolaryngology Resident Talent Assessment(ORTA;prematch 2017,postmatch 2019)and Program-Specific Paragraph(PSP;implemented 2016,optional 2018)on applicant numbers and match *** survey analysis assessed candidate perceptions of PSP/***:Applicant numbers declined significantly during PSP/ORTA(18.9%;p=0.001).With the optional PSP and postmatch ORTA,applicant numbers increased significantly(39.0%;p=0.002).Examined individually,mandatory PSP was associated with a significant decline in applicants(p=0.007),whereas postmatch ORTA was associated with significant increases in applicants(p=0.010).ORTA and PSP negatively impacted the decision to apply to otolaryngology in 59.8%and 51.3%of applicants,***,match rate success improved significantly from 74.8%to 91.2%during PSP/ORTA(p=0.014),followed by a significant decline to 73.1%after PSP was made optional and ORTA moved to postmatch(p=0.002).Conclusions:ORTA and PSP correlated with decreased applicant numbers and increased match rate *** programs seek ways to remove barriers to applying to otolaryngology,the potential consequences of an increasing pool of unmatched candidates must also be considered.

关键词： academic success internship and residency medical students otolaryngology surveys and questionnaires

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Treg cells in pancreatic lymph nodes： the possible role in diabetogenesis and βcell regeneration in a TId model

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Cellular & molecular Immunology 2012年第6期9卷 455-463页

作者： Benjamin K Nti janet L markman Suzanne Bertera Alexis j Styche Robert j Lakomy Vladimir m Subbotin massimo Trucco Tatiana d Zorina Indiana University School of medicine Indianapolis IN USA Cedars-Sinai medical Center Los Angeles CA USA division of Irnmunogenetics Children's Hospital of Pittsburgh University of Pittsburgh School of Medicine Pittsburgh PA USA Independent investigator 602 Samuel dr. Madison Wl USA department of Bioscience Technologies Jefferson School of Health Professions Thomas Jefferson University Philadelphia PA USA

Previously, we established a model in which physiologically adequate function of the autologous β cells was recovered in non-obese diabetic （NOd） mice after the onset of hyperglycemia by rendering them hemopoietic chimera. These mice were termed antea-diabetic. In the current study, we addressed the role of T regulatory （Treg） cells in the mechanisms mediating the restoration of euglycemia in the antea-diabetic NOd model. The data generated in this study demonstrated that the numbers of Treg cells were decreased in unmanipulated NOd mice, with the most profound deficiency detected in the pancreatic lymph nodes （PLNs）. The impaired retention of the Treg cells in the PLNs correlated with the locally compromised profile of the chemokines involved in their trafficking, with the most prominent decrease observed in SdF-1. The amelioration of autoimmunity and restoration of euglycemia observed in the antea-diabetic mice was associated with restoration of the Treg cell population in the PLNs. These data indicate that the function of the SdF-1/CXCR4 axis and the retention of Treg cells in the PLNs have a potential role in diabetogenesis and in the amelioration of autoimmunity and β cell regeneration in the antea-diabetic model. We have demonstrated in the antea-diabetic mouse model that lifelong recovery of the β cells has a strong correlation with normalization of the Treg cell population in the PLNs. This finding offers new opportunities for testing the immunomodulatory regimens that promote accumulation of Treg cells in the PLNs as a therapeutic approach for type 1 diabetes （TId）.

关键词： β cell regeneration T regulatory cell trafficking type 1 diabetes