{"title":"离子交换制备梯度折射率结构的应力诱导双折射","authors":"Todd H. Tomkinson, C. Saxer","doi":"10.1364/giois.1994.pd3","DOIUrl":null,"url":null,"abstract":"This paper examines an axial gradient-index (GRIN) glass sample produced by ion-exchange in the glass system:\n \n \n 0.704\n \n \n SiO\n \n 2\n \n +\n 0.044\n \n \n Al\n \n 2\n \n \n O\n 3\n \n +\n (\n 0.252\n −\n χ\n (\n z\n )\n )\n \n \n Na\n \n 2\n \n O\n +\n χ\n (\n z\n )\n \n \n Li\n \n 2\n \n O\n \n \n (where χ(z) represents the degree of exchange versus position, z), with the intention of determining χ(z) from a measurement of the index profile, n(z). Due to the ion-exchange conditions, the sample contains “frozen-in” stresses that strain the glass network, preventing it from obtaining its free expansion volume. The resulting volume change causes an additional birefringent index change. Therefore, when the index profile of the sample, n(z), is measured, it is necessary to take into account the sample’s birefringence to accurately determine the exchange profile, χ(z).\n The gradient’s index change, Δn(z), (where, Δn(z)=n(z)-nb, and nb is the base index), can be determined to accuracies reaching 0.03%. This paper shows that when frozen stresses are not taken into consideration, errors in determining χ(z) can reach 1.8%. However, it is shown that by also measuring the sample’s birefringence, determination of χ(z) may become more accurate.","PeriodicalId":203841,"journal":{"name":"Gradient Index Optical Systems","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Stress-Induced Birefringence in Gradient-Index Structures Fabricated by Ion-Exchange\",\"authors\":\"Todd H. Tomkinson, C. Saxer\",\"doi\":\"10.1364/giois.1994.pd3\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper examines an axial gradient-index (GRIN) glass sample produced by ion-exchange in the glass system:\\n \\n \\n 0.704\\n \\n \\n SiO\\n \\n 2\\n \\n +\\n 0.044\\n \\n \\n Al\\n \\n 2\\n \\n \\n O\\n 3\\n \\n +\\n (\\n 0.252\\n −\\n χ\\n (\\n z\\n )\\n )\\n \\n \\n Na\\n \\n 2\\n \\n O\\n +\\n χ\\n (\\n z\\n )\\n \\n \\n Li\\n \\n 2\\n \\n O\\n \\n \\n (where χ(z) represents the degree of exchange versus position, z), with the intention of determining χ(z) from a measurement of the index profile, n(z). Due to the ion-exchange conditions, the sample contains “frozen-in” stresses that strain the glass network, preventing it from obtaining its free expansion volume. The resulting volume change causes an additional birefringent index change. Therefore, when the index profile of the sample, n(z), is measured, it is necessary to take into account the sample’s birefringence to accurately determine the exchange profile, χ(z).\\n The gradient’s index change, Δn(z), (where, Δn(z)=n(z)-nb, and nb is the base index), can be determined to accuracies reaching 0.03%. This paper shows that when frozen stresses are not taken into consideration, errors in determining χ(z) can reach 1.8%. However, it is shown that by also measuring the sample’s birefringence, determination of χ(z) may become more accurate.\",\"PeriodicalId\":203841,\"journal\":{\"name\":\"Gradient Index Optical Systems\",\"volume\":\"10 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Gradient Index Optical Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/giois.1994.pd3\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Gradient Index Optical Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/giois.1994.pd3","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
本文研究了玻璃系统中离子交换产生的轴向梯度指数(GRIN)玻璃样品:0.704 sio2 + 0.044 Al 2o3 + (0.252 - χ(z)) Na 2o + χ(z) Li 2o(其中χ(z)表示交换程度与位置,z),目的是通过测量指数剖面n(z)来确定χ(z)。由于离子交换条件,样品含有“冻结”应力,使玻璃网络应变,阻止其获得自由膨胀体积。由此产生的体积变化引起额外的双折射率变化。因此,在测量样品的指数曲线n(z)时,必须考虑样品的双折射,才能准确地确定交换曲线χ(z)。梯度的指数变化Δn(z),(其中Δn(z)=n(z)-nb, nb为基指数)可以确定,精度达到0.03%。本文表明,在不考虑冻结应力的情况下,计算χ(z)的误差可达1.8%。然而,也表明,通过测量样品的双折射,可以更准确地确定χ(z)。
Stress-Induced Birefringence in Gradient-Index Structures Fabricated by Ion-Exchange
This paper examines an axial gradient-index (GRIN) glass sample produced by ion-exchange in the glass system:
0.704
SiO
2
+
0.044
Al
2
O
3
+
(
0.252
−
χ
(
z
)
)
Na
2
O
+
χ
(
z
)
Li
2
O
(where χ(z) represents the degree of exchange versus position, z), with the intention of determining χ(z) from a measurement of the index profile, n(z). Due to the ion-exchange conditions, the sample contains “frozen-in” stresses that strain the glass network, preventing it from obtaining its free expansion volume. The resulting volume change causes an additional birefringent index change. Therefore, when the index profile of the sample, n(z), is measured, it is necessary to take into account the sample’s birefringence to accurately determine the exchange profile, χ(z).
The gradient’s index change, Δn(z), (where, Δn(z)=n(z)-nb, and nb is the base index), can be determined to accuracies reaching 0.03%. This paper shows that when frozen stresses are not taken into consideration, errors in determining χ(z) can reach 1.8%. However, it is shown that by also measuring the sample’s birefringence, determination of χ(z) may become more accurate.