{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"采用中频感应熔炼方法制备Ni-5at％W合金锭,经锻造和热轧后,<span style=\"color:red\">再</span>冷轧到50 m长,厚度为60 μm的带材.随后在800～1200℃进行再结晶<span style=\"color:red\">退火</span>处理.在兼顾“高织构”和“浅<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>”要求下,得出1100℃/0.5h是Ni5W合金基带最佳的<span style=\"color:red\">退火</span>工艺.根据X射线衍射(XRD)和电子背散射衍射技术(EBSD)结果,在1100℃/0.5 h时该Ni5W合金基带的再结晶立方织构含量达到98.9％(≤10°),且晶粒尺寸均匀.<span style=\"color:red\">退火</span>后的Ni5W合金基带扫描半高宽(FWHM)值和孪<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>含量接近德国Dresden公司商业化Ni5W合金基带的水平.","authors":[{"authorName":"王毅","id":"05cc11b9-6660-4e2c-bbd9-74f2b55b65b7","originalAuthorName":"王毅"},{"authorName":"索红莉","id":"4a51eca4-114a-4097-b90a-cc8088edd5ad","originalAuthorName":"索红莉"},{"authorName":"马麟","id":"91e1f81d-0afb-4b2c-8685-7cf2d8d8963c","originalAuthorName":"马麟"},{"authorName":"王建宏","id":"712324d8-c5f5-4267-8d2a-77115b22f381","originalAuthorName":"王建宏"},{"authorName":"李孟晓","id":"bdf8d52a-9367-476a-af60-9d64e8c510be","originalAuthorName":"李孟晓"},{"authorName":"孟易辰","id":"1bd8ce76-e97e-423b-9e23-caa9075d3f62","originalAuthorName":"孟易辰"},{"authorName":"刘敏","id":"0540a0d1-b2b4-433c-829e-8ba2be48f695","originalAuthorName":"刘敏"}],"doi":"","fpage":"2590","id":"45194e57-12cb-4ebe-a2fd-dc9f7a8e9bd9","issue":"12","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"3b137305-bde1-4481-83a8-f7f4269d62bf","keyword":"<span style=\"color:red\">再</span><span style=\"color:red\">晶</span><span style=\"color:red\">界</span><span style=\"color:red\">退火</span>","originalKeyword":"再晶界退火"},{"id":"34ba6e53-8a19-4eb7-9a7e-b29a36fb8c20","keyword":"立方织构","originalKeyword":"立方织构"},{"id":"4f393683-2ff1-4409-b0ea-a1b3215592d3","keyword":"<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>","originalKeyword":"晶界"},{"id":"23c3f879-3fc8-4996-98dc-067188ff9bd7","keyword":"涂层导体","originalKeyword":"涂层导体"}],"language":"zh","publisherId":"xyjsclygc201312034","title":"再结晶<span style=\"color:red\">退火</span>工艺对Ni5W合金长带织构的影响","volume":"42","year":"2013"},{"abstractinfo":"利用电子背散射衍射技术,研究了Fe-25Mn-2.5Si-2Al孪品诱发塑性钢(TWIP钢)冷轧变形后<span style=\"color:red\">退火</span>再结晶微观组织的<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征、晶粒取向差和织构,分析了不同<span style=\"color:red\">退火</span>温度对<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征和织构的影响.结果表明:随着<span style=\"color:red\">退火</span>温度的升高,TWIP钢中∑1CSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>含量减少,∑3CSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>含量增加;α-取向线密度呈下降的趋势,β-取向线密度总体上升;G{011}＜100＞取向强度呈下降趋势,而B{011}＜211＞、S{123}＜634＞、Cu{112}＜111＞等取向强度呈上升趋势.","authors":[{"authorName":"苏钰","id":"dd297894-ae0f-4924-9d3e-765d1f46ef8a","originalAuthorName":"苏钰"},{"authorName":"李麟","id":"c6228922-072d-4471-9c12-8b80dd37f349","originalAuthorName":"李麟"},{"authorName":"何慎","id":"e1aec695-8a1a-40a2-b5b6-d59655ba30e2","originalAuthorName":"何慎"},{"authorName":"符仁钰","id":"ae424476-d3d3-403b-9a3e-93e0631bc9f8","originalAuthorName":"符仁钰"},{"authorName":"赵中华","id":"77cb8457-46d9-4d21-85e0-7b39300cc9f4","originalAuthorName":"赵中华"}],"doi":"","fpage":"71","id":"a325bcdd-2d6c-4361-b15f-665bb47daac9","issue":"7","journal":{"abbrevTitle":"CLRCLXB","coverImgSrc":"journal/img/cover/CLRCLXB.jpg","id":"15","issnPpub":"1009-6264","publisherId":"CLRCLXB","title":"材料热处理学报"},"keywords":[{"id":"5c0874f6-3e31-47e4-b3ce-5d6fe67e0d89","keyword":"TWIP钢","originalKeyword":"TWIP钢"},{"id":"92faa154-5f86-43d1-a3e2-a31b5a4201a9","keyword":"<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征","originalKeyword":"晶界特征"},{"id":"c8e87489-ab08-4645-a168-ee5e2d50706f","keyword":"织构","originalKeyword":"织构"}],"language":"zh","publisherId":"jsrclxb201007015","title":"TWIP钢<span style=\"color:red\">退火</span>织构与<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征","volume":"31","year":"2010"},{"abstractinfo":"<FONT face=Verdana>不同La施主掺杂浓度的BaTiO<SUB>3</SUB>陶瓷在H<SUB>2</SUB>/Ar的还原气氛下烧结后, 再在氧分压P <SUB>O2</SUB>=260Pa的气氛(Ar和O<SUB>2</SUB>的混合气体)下进行氧化, 通过氧流量计检测还原样品在<span style=\"color:red\">再</span>氧化过程的吸氧行为; 用TEM分析样品氧化后显微结构的变化, 测定了在不同最高氧化温度下氧化样品的PTCR效应以及复阻抗图谱. 结果表明: 氧流量计在升温阶段检测到三个不同行为的吸氧峰,峰I(起始温度～250℃)为氧空位的填充过程; 峰II(起始温度～800℃)和峰III(起始温度～1250℃)为还原相的氧化过程, 具体来说, 峰II是通过<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>扩散提供氧使靠近<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>附近的区域被氧化; 而峰III是由晶格扩散过程控制, 氧化过程从<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>逐渐向晶粒内部区域扩展, 并伴随着富Ti的Ba<SUB>6</SUB>Ti<SUB>17</SUB>O<SUB>40</SUB>相的沉淀. 在还原相向氧化相的转变过程中, 于<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>处形成了两个具有<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>势垒的电结构单元而使陶瓷呈现强PTCR效应. </FONT>","authors":[{"authorName":"蒲永平","id":"8a59b577-479b-4505-b4dc-6f6f5810a2f3","originalAuthorName":"蒲永平"},{"authorName":"陈寿田","id":"f25d0444-c42e-49ca-b478-9e36ee32c243","originalAuthorName":"陈寿田"},{"authorName":"LANGHAMMERHT","id":"d6ffda87-7031-44d2-9881-29e3ecc658dc","originalAuthorName":"LANGHAMMERHT"},{"authorName":"MAKOVECD","id":"092b06d9-fda5-40fc-9c6d-88d6c9b4f553","originalAuthorName":"MAKOVECD"}],"categoryName":"|","doi":"10.3724/SP.J.1077.2006.00919","fpage":"919","id":"975ea3c1-d68e-4593-a5e8-7367ab0dd703","issue":"4","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"a061a6d0-a0d2-4318-9a22-9830ced6113c","keyword":"掺杂的La钛酸钡陶瓷","originalKeyword":"掺杂的La钛酸钡陶瓷"},{"id":"63c9ffc2-39e8-4d56-81d3-9d2e7a035835","keyword":" grain boundary reoxidation","originalKeyword":" grain boundary reoxidation"},{"id":"25d47bc5-a923-4094-84c4-a6af24be636a","keyword":" positive temperature coefficient resistance effect","originalKeyword":" positive temperature coefficient resistance effect"}],"language":"zh","publisherId":"1000-324X_2006_4_5","title":"Ba<SUB>1-x</SUB>La<SUB>x</SUB>TiO<SUB>3</SUB>陶瓷的<span style=\"color:red\">晶</span><span style=\"color:red\">界</span><span style=\"color:red\">再</span>氧化机理研究","volume":"21","year":"2006"},{"abstractinfo":"不同La施主掺杂浓度的BaTiO3陶瓷在H2/Ar的还原气氛下烧结后,再在氧分压Po2=260Pa的气氛(Ar和O2的混合气体)下进行氧化,通过氧流量计检测还原样品在<span style=\"color:red\">再</span>氧化过程的吸氧行为;用TEM分析样品氧化后显微结构的变化,测定了在不同最高氧化温度下氧化样品的PTCR效应以及复阻抗图谱.结果表明:氧流量计在升温阶段检测到三个不同行为的吸氧峰,峰Ⅰ(起始温度～250℃)为氧空位的填充过程;峰Ⅱ(起始温度～800℃)和峰Ⅲ(起始温度～1250℃)为还原相的氧化过程,具体来说,峰Ⅱ是通过<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>扩散提供氧使靠近<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>附近的区域被氧化;而峰Ⅲ是由晶格扩散过程控制,氧化过程从<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>逐渐向晶粒内部区域扩展,并伴随着富Ti的Ba6Ti17O40相的沉淀.在还原相向氧化相的转变过程中,于<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>处形成了两个具有<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>势垒的电结构单元而使陶瓷呈现强PTCR效应.","authors":[{"authorName":"蒲永平","id":"cb903043-8a8d-4625-a39e-cb33645fcb7f","originalAuthorName":"蒲永平"},{"authorName":"陈寿田","id":"a1c18eed-7ccf-408f-8044-974bf80d5535","originalAuthorName":"陈寿田"},{"authorName":"LANGHAMMER H. T","id":"a8cafc3d-16fd-4521-98e3-4f5df206c5b1","originalAuthorName":"LANGHAMMER H. T"},{"authorName":"MAKOVEC D","id":"698c8f26-22c5-46e7-829c-85f0f9045c93","originalAuthorName":"MAKOVEC D"}],"doi":"10.3321/j.issn:1000-324X.2006.04.026","fpage":"919","id":"63118fdc-a591-4470-b3b2-e1513c5db53e","issue":"4","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"b6d7f9c3-39d0-4c9e-926c-bbd02083adc2","keyword":"掺杂的La钛酸钡陶瓷","originalKeyword":"掺杂的La钛酸钡陶瓷"},{"id":"aabd4728-bd73-45f2-9223-75bf1fc590b2","keyword":"<span style=\"color:red\">晶</span><span style=\"color:red\">界</span><span style=\"color:red\">再</span>氧化","originalKeyword":"晶界再氧化"},{"id":"b5bdd31e-5812-47d2-b900-c884549dea7a","keyword":"正温度系数电阻效应","originalKeyword":"正温度系数电阻效应"}],"language":"zh","publisherId":"wjclxb200604026","title":"Ba1-xLaxTiO3陶瓷的<span style=\"color:red\">晶</span><span style=\"color:red\">界</span><span style=\"color:red\">再</span>氧化机理研究","volume":"21","year":"2006"},{"abstractinfo":"采用背散射电子衍射(EBSD和透射电镜(TEM)研究了纯铜大变形异步累积叠轧与再结晶过程中的低重合位置点阵(ΣCSL)<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>演化过程.研究表明:纯铜在600℃长时间均匀化<span style=\"color:red\">退火</span>时,形成大量较长的平直共格Σ3<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>,并作为大角度<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>阻碍晶粒的异常长大;在随后的大变形异步累积叠轧中,随着晶粒转动,形变组织的形成,低ΣCSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>的逐渐减少;再结晶<span style=\"color:red\">退火</span>中形成大量超细孪<span style=\"color:red\">晶</span>,同时形成大量Σ3特殊<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>,并与高ΣCSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>反应,形成大量低ΣCSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>,Σ1小角度<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>迅速增多,阻断一般大角度<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>网络,表明Σ3<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>的反应是大变形+<span style=\"color:red\">退火</span>纯铜<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布(GBCD)的优化机制.","authors":[{"authorName":"周蕾","id":"46ceee16-7d87-427d-820b-aed560b9dc2d","originalAuthorName":"周蕾"},{"authorName":"史庆南","id":"f48d26d7-d575-434d-b930-a76e552dd0d5","originalAuthorName":"史庆南"},{"authorName":"蔡晓兰","id":"4ada6a3d-fa6a-4c21-80cc-66b17b40d8ac","originalAuthorName":"蔡晓兰"},{"authorName":"王军丽","id":"2cb68b41-b2f6-4a23-87b6-81f3ca2a84cc","originalAuthorName":"王军丽"}],"doi":"10.13289/j.issn.1009-6264.2017-0001","fpage":"25","id":"96772af9-0b93-413f-a6b4-bc806858c5da","issue":"6","journal":{"abbrevTitle":"CLRCLXB","coverImgSrc":"journal/img/cover/CLRCLXB.jpg","id":"15","issnPpub":"1009-6264","publisherId":"CLRCLXB","title":"材料热处理学报"},"keywords":[{"id":"1e02dc8a-3842-4f64-8742-06daf4e474f0","keyword":"铜","originalKeyword":"铜"},{"id":"5527177b-54e9-47aa-b708-55e9074fffae","keyword":"异步累积叠轧","originalKeyword":"异步累积叠轧"},{"id":"3c8c172b-ed8b-4058-af55-d175c8e2b1c8","keyword":"再结晶","originalKeyword":"再结晶"},{"id":"877ce6e7-3552-47db-ae94-6222bcfe8d1a","keyword":"重合位置点阵","originalKeyword":"重合位置点阵"},{"id":"692444c3-5d5a-4d1f-a3c0-2a1877d1f465","keyword":"<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布","originalKeyword":"晶界特征分布"}],"language":"zh","publisherId":"jsrclxb201706004","title":"大变形<span style=\"color:red\">退火</span>超细<span style=\"color:red\">晶</span>铜中的<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布","volume":"38","year":"2017"},{"abstractinfo":"Hastelloy C-276合金经小变形量冷轧后进行1100℃不同时间的<span style=\"color:red\">退火</span>处理.采用EBSD技术对∑3和∑9<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例进行统计,同时采用五参数法对∑3和∑9<span style=\"color:red\">晶</span>界面分布进行分析.结果表明,∑3<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>随着<span style=\"color:red\">退火</span>时间的延长更加接近于标准重合点阵<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>取向,而其<span style=\"color:red\">晶</span>界面更加接近于低能量的{111}<span style=\"color:red\">晶</span>界面.这一结果符合<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>“微调”机制.∑9<span style=\"color:red\">晶</span>界面分布则越来越集中在[110]<span style=\"color:red\">晶</span>带.而偏差较大的∑9<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例增加,是由于非共格∑3比例的增加导致的.","authors":[{"authorName":"张晓宇","id":"2bb339fc-3b01-4ae0-8b6c-6788253503b5","originalAuthorName":"张晓宇"},{"authorName":"李德富","id":"0d782c71-5ad4-4ce8-b288-446ba0164d63","originalAuthorName":"李德富"},{"authorName":"郭胜利","id":"941a308f-7cfc-43fd-85ac-470efcf5daf6","originalAuthorName":"郭胜利"},{"authorName":"赵宪明","id":"1a64234c-f12d-41bd-a270-41821f6c6716","originalAuthorName":"赵宪明"}],"doi":"","fpage":"2253","id":"d88613a9-3566-4cf6-9e66-3fb8c34f266f","issue":"9","journal":{"abbrevTitle":"XYJS","coverImgSrc":"journal/img/cover/XYJS.jpg","id":"67","issnPpub":"0258-7076","publisherId":"XYJS","title":"稀有金属"},"keywords":[{"id":"da80538b-0fe2-4c45-a50a-da416aa02289","keyword":"Hastelloy C-276合金","originalKeyword":"Hastelloy C-276合金"},{"id":"dd70ca9f-1c8e-4000-91d0-7d811bbccd63","keyword":"∑3和∑9<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>","originalKeyword":"∑3和∑9晶界"},{"id":"a33eb3c4-87b5-427d-a319-ec4686144690","keyword":"<span style=\"color:red\">晶</span>界面分布","originalKeyword":"晶界面分布"},{"id":"cf2b6037-20f9-4bc4-81e4-2ca056249fcc","keyword":"EBSD","originalKeyword":"EBSD"}],"language":"zh","publisherId":"xyjsclygc201609010","title":"Hastelloy C-276合金∑3<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>和∑9<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>随着<span style=\"color:red\">退火</span>时间的演变规律","volume":"45","year":"2016"},{"abstractinfo":"利用背散射电子衍射(EBSD)及透射电子显微镜(TEM)技术研究TA15合金不同温度<span style=\"color:red\">退火</span>后<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>取向差变化情况.结果表明,800 ℃<span style=\"color:red\">退火</span>处理有少量小角<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>转化为大角<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>;<span style=\"color:red\">退火</span>温度提高到950 ℃,大角<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>分数大幅度增加;小角<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>转化为大角<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>的平均激活能为151.4 kJ/mol,等于α钛的自扩散激活能,说明了小角<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>向大角<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>转变是由钛原子的自扩散控制;TEM观察结果表明,800 ℃<span style=\"color:red\">退火</span>处理后亚<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>变为具有六方网络的位错网络,950 ℃<span style=\"color:red\">退火</span>处理则得到大量的等轴<span style=\"color:red\">晶</span>.","authors":[{"authorName":"刘勇","id":"3a112138-7ecb-4f8a-974c-63b09c21d04d","originalAuthorName":"刘勇"},{"authorName":"朱景川","id":"dfeed702-39e4-48e8-8f84-b9601d21985f","originalAuthorName":"朱景川"},{"authorName":"王洋","id":"e6afad5b-fa60-4c21-be0d-7015a3bc2893","originalAuthorName":"王洋"}],"doi":"","fpage":"1390","id":"15ab130a-f159-4c92-b13e-69a90b8abd59","issue":"8","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"731f3bbe-fbd7-4570-a0f1-125c0ba1a2f4","keyword":"TA15合金","originalKeyword":"TA15合金"},{"id":"65b5e59a-0855-4fb2-a12c-33e314e24167","keyword":"<span style=\"color:red\">退火</span>处理","originalKeyword":"退火处理"},{"id":"cf8e0aea-39ff-45a7-8a85-636963565f5e","keyword":"<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>取向差","originalKeyword":"晶界取向差"}],"language":"zh","publisherId":"xyjsclygc200908017","title":"<span style=\"color:red\">退火</span>处理对TA15合金<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>取向差演化特性的影响","volume":"38","year":"2009"},{"abstractinfo":"Hastelloy C-276合金经1150℃+30 min固溶处理后,进行不同变形量的冷轧高温<span style=\"color:red\">退火</span>处理.采用电子背散射(EBSD)技术对<span style=\"color:red\">退火</span>后的<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布和<span style=\"color:red\">晶</span>界面分布进行表征.结果表明,在<span style=\"color:red\">退火</span>过程中,∑1小角度<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例减小,变形存储能释放,<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>发生迁移,促进了<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>相互作用,从而导致∑9和∑27<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例增加.与此同时,晶粒发生异常长大并促进了特殊<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>的形成,产生的特殊<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>阻断了大角度<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>的连通性.合金经变形高温<span style=\"color:red\">退火</span>之后,∑3<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>分布在{111｝<span style=\"color:red\">晶</span>界面扭转<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>,∑9<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>分布在[110]<span style=\"color:red\">晶</span>带倾斜<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>.不同变形条件下,∑3<span style=\"color:red\">晶</span>界面与∑9<span style=\"color:red\">晶</span>界面分布演变规律不同,原因在于变形<span style=\"color:red\">退火</span>导致∑3<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例的不同和<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>之间的相互作用的结果.","authors":[{"authorName":"张晓宇","id":"8879e323-bc2f-4671-833c-1b6ed9dd592e","originalAuthorName":"张晓宇"},{"authorName":"李德富","id":"d8d0f7ca-edbd-46cd-aa24-31b21526fdc0","originalAuthorName":"李德富"},{"authorName":"郭胜利","id":"27bbcd6e-ff3d-44d3-99a4-43a0dfc31671","originalAuthorName":"郭胜利"},{"authorName":"赵宪明","id":"59ea31da-e847-4f42-b1f1-a1e585e1190d","originalAuthorName":"赵宪明"},{"authorName":"刘贤钙","id":"be0edaa7-9fa9-4301-a016-aad89465bba7","originalAuthorName":"刘贤钙"}],"doi":"","fpage":"1866","id":"734e3ccd-3eb5-4eb2-ad5f-136d182d622c","issue":"7","journal":{"abbrevTitle":"XYJS","coverImgSrc":"journal/img/cover/XYJS.jpg","id":"67","issnPpub":"0258-7076","publisherId":"XYJS","title":"稀有金属"},"keywords":[{"id":"50132801-04c9-4436-81f5-3ffb8a0c6cc2","keyword":"Hastelloy C-276","originalKeyword":"Hastelloy C-276"},{"id":"1407ceaf-74d8-400b-bc4c-8e3f33af0cb1","keyword":"<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布","originalKeyword":"晶界特征分布"},{"id":"33ae2982-4a37-42a8-a162-3be6628ecb3b","keyword":"<span style=\"color:red\">晶</span>界面分布","originalKeyword":"晶界面分布"},{"id":"a055cb90-d2e4-417f-a277-15f497753c7f","keyword":"形变热处理工艺","originalKeyword":"形变热处理工艺"}],"language":"zh","publisherId":"xyjsclygc201607043","title":"小变形高温<span style=\"color:red\">退火</span>对Hastelloy C-276合金<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布和<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>平面分布的影响","volume":"45","year":"2016"},{"abstractinfo":"用扫描电子显微镜(SEM)和电子背散射衍射(EBSD)技术研究了5%冷变形316不锈钢经1100℃不同时间<span style=\"color:red\">退火</span>样品的<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布(GBCD).结果表明:低ΣCSL(Σ≤29)<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例的提高是在再结晶过程中实现的.在<span style=\"color:red\">退火</span>40 min时再结晶完成,低ΣCSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例达到80%,其中Σ3<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例占总的低ΣCSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>80%左右,<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布得到优化;尺寸较大形状不规则的晶粒团簇(grain-clusters)形成,每个晶粒团簇内部存在大量孪<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>、多重孪<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>和特殊的三叉<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>节点.部分再结晶状态样品的显微组织特点和晶粒团簇内部孪<span style=\"color:red\">晶</span>链的分析表明再结晶过程中多重孪<span style=\"color:red\">晶</span>的发展是提高316不锈钢低ΣCSL<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>比例的关键.","authors":[{"authorName":"王坤","id":"77746fc2-f425-419d-848d-bd513ace1c36","originalAuthorName":"王坤"},{"authorName":"陈文觉","id":"a6975175-a156-4a8f-b7a1-7f17e10a9991","originalAuthorName":"陈文觉"},{"authorName":"夏爽","id":"8302869d-dd1f-45fa-aa03-09a00a7408b7","originalAuthorName":"夏爽"},{"authorName":"周邦新","id":"6bc90d88-6e99-49fd-8910-8c81112d91da","originalAuthorName":"周邦新"}],"doi":"10.3969/j.issn.1001-7208.2009.05.003","fpage":"13","id":"25ea4a9e-40c6-4383-b195-cd76d77329bd","issue":"5","journal":{"abbrevTitle":"SHJS","coverImgSrc":"journal/img/cover/SHJS.jpg","id":"59","issnPpub":"1001-7208","publisherId":"SHJS","title":"上海金属"},"keywords":[{"id":"0521a026-da89-4695-8fa6-5ee11c45f724","keyword":"316不锈钢","originalKeyword":"316不锈钢"},{"id":"5460a60f-3cbe-4d46-9b32-ee2d4ae45c21","keyword":"再结晶<span style=\"color:red\">退火</span>","originalKeyword":"再结晶退火"},{"id":"e2a3637e-55dc-4a70-a77a-e7082d227a50","keyword":"<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布","originalKeyword":"晶界特征分布"},{"id":"565dd503-de54-47c3-9460-b6015941b36d","keyword":"晶粒团簇","originalKeyword":"晶粒团簇"}],"language":"zh","publisherId":"shjs200905003","title":"高温<span style=\"color:red\">退火</span>过程中316不锈钢<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布的演化","volume":"31","year":"2009"},{"abstractinfo":"采用电子背散射衍射（EBSD）技术研究了经290℃固溶处理以及经固溶处理后在100℃～200℃预时效处理的Pb-0.05%Ca-1.5%Sn-0.026%Al (质量分数)合金再经形变<span style=\"color:red\">退火</span>后的<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布(GBCD)。结果表明：固溶处理后直接进行形变<span style=\"color:red\">退火</span>的合金样品中出现了较多的特殊<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>，∑3和（∑9+∑27）<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>的比例分别达到49.6%和7.2%，并且特殊<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>能较好地打断一般大角度<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>网络的连通性。相反，固溶处理后先进行预时效处理，然后再进行形变<span style=\"color:red\">退火</span>的合金样品中形成了较少的特殊<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>，∑3和（∑9+∑27）<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>的比例分别低于35.9%和2.5%，特殊<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>几乎不能打断一般大角度<span style=\"color:red\">晶</span><span style=\"color:red\">界</span>网络的连通性。","authors":[{"authorName":"张欣","id":"9b8fe534-03fb-42b2-b68b-c04006ceacae","originalAuthorName":"张欣"},{"authorName":"王卫国","id":"45317cf9-72dd-4da4-8f49-9876b60dadff","originalAuthorName":"王卫国"},{"authorName":"郭红","id":"591f26eb-6f72-41b7-ae49-03602ac752e0","originalAuthorName":"郭红"},{"authorName":"姜英","id":"a322d31a-2bf3-43a2-ab16-6cec49b242ed","originalAuthorName":"姜英"}],"categoryName":"|","doi":"","fpage":"454","id":"7586161d-dc84-4fab-a6b8-b1de3d5723bf","issue":"5","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"e6bd9605-89f4-49a4-adbf-747118d9c26e","keyword":"Pb合金","originalKeyword":"Pb合金"},{"id":"c10e26c3-411c-43a6-9f21-89dd48105bd3","keyword":"\ngrain boundary character\ndistribution (GBCD)","originalKeyword":"\ngrain boundary character\ndistribution (GBCD)"},{"id":"331d7bfd-c351-4a64-9518-9fee47acb372","keyword":"\ncold rolling and annealing","originalKeyword":"\ncold rolling and annealing"}],"language":"zh","publisherId":"0412-1961_2007_5_2","title":"固溶和预时效Pb合金冷轧<span style=\"color:red\">退火</span><span style=\"color:red\">晶</span><span style=\"color:red\">界</span>特征分布","volume":"43","year":"2007"}],"totalpage":3086,"totalrecord":30852}