Study of the Glass Press Molding Process

Total Page:16

File Type:pdf, Size:1020Kb

Study of the Glass Press Molding Process Study of the glass press molding process Diplomová práce Studijní program: N2301 – Mechanical Engineering Studijní obor: 2302T010 – Machines and Equipment Design Autor práce: Selma Kunosic Vedoucí práce: doc. Ing. Tomáš Vít, Ph.D. Liberec 2016 Study of the glass press molding process Diploma thesis Study programme: N2301 – Mechanical Engineering Study branch: 2302T010 – Machines and Equipment Design Author: Selma Kunosic Supervisor: doc. Ing. Tomáš Vít, Ph.D. Liberec 2016 TABLE OF CONTENTS 1. Introduction ..................................................................................................................................... 8 1.1. Glass versus plastics as lens materials .................................................................................... 9 1.2. Advantages and benefits ......................................................................................................... 9 2. Research objectives ....................................................................................................................... 11 3. Literature overview ....................................................................................................................... 12 4. About the process ......................................................................................................................... 14 4.1. Heating cycle ......................................................................................................................... 15 4.2. Soaking cycle ......................................................................................................................... 15 4.3. Pressing cycle......................................................................................................................... 15 4.4. Gradual cooling cycle............................................................................................................. 16 4.5. Rapid cooling cycle ................................................................................................................ 16 5. Fundamental of glass rheology ..................................................................................................... 17 5.1. Glass terminology .................................................................................................................. 17 5.2. Glass transition temperature and its significance ................................................................. 17 5.3. Viscoelasticity ........................................................................................................................ 19 5.4. Stress relaxation and creep ................................................................................................... 21 5.5. Structural relaxation .............................................................................................................. 23 5.6. Linearity and thermorheological simplicity ........................................................................... 26 6. Lens molding experiments ............................................................................................................ 28 6.1. Material of glass .................................................................................................................... 29 6.2. Molds and ring ....................................................................................................................... 31 6.3. Inserts .................................................................................................................................... 32 6.4. Experiment ............................................................................................................................ 33 6.5. Light white interferometry .................................................................................................... 36 7. Numerical simulation .................................................................................................................... 39 7.1. Inputs ..................................................................................................................................... 40 7.1.1. Materials ........................................................................................................................ 40 7.1.2. Boundary conditions...................................................................................................... 42 7.2. Cycles in simulation ............................................................................................................... 45 7.3. Results ................................................................................................................................... 47 7.4. Numerical simulation of molding of aspheric lens ................................................................ 50 7.4.1. Aspheric geometry ........................................................................................................ 50 7.4.2. Materials ........................................................................................................................ 51 7.4.3. Results ........................................................................................................................... 53 8. Conclusion and future work .......................................................................................................... 55 9. Literature ....................................................................................................................................... 56 1 LIST OF FIGURES Figure 4.1 Placing of raw glass gob/ blank material on the lower mold, (b) Heating of the glass and mold assembly to the molding temperature, (c) Pressing (molding) of the glass material between the mold halves and (d) Forced cooling of the lens and mold assembly to near room temperature and lens release ............................................................................................................................................ 14 Figure 5.1 Glass transition region .......................................................................................................... 18 Figure 5.2 Spring and dashpot ............................................................................................................... 19 Figure 5.3 Standard Maxwell linear model for viscoelasticity .............................................................. 20 Figure 5.4 Generalized Maxwell model for viscoelasticity .................................................................... 21 Figure 5.5 Stress relaxation vs. time...................................................................................................... 22 Figure 5.6 Creep vs. time ....................................................................................................................... 22 Figure 5.7 Phenomenon of structural relaxation a) Viscoelastic material subjected to a step change in temperature b) Corresponding response of a property like volume for e.g. with time when subjected to a step change in temperature ........................................................................................................... 24 Figure 5.8 Volume vs. temperature behavior for a viscoelastic material like glass .............................. 25 Figure 5.9 Thermo-rheological simple behavior ................................................................................... 26 Figure 6.1 Nanotech 140GPM ............................................................................................................... 28 Figure 6.2 Geometry of parts used in press molding ............................................................................ 29 Figure 6.3 Ring, guide and insert ........................................................................................................... 33 Figure 6.4 Molding setup ....................................................................................................................... 34 Figure 6.5 Process sheet showing the variation of mold temperature, position and molding force as a function of time during the experiment................................................................................................ 34 Figure 6.6 Different cycles in glass molding process ............................................................................. 35 Figure 6.7 Shape of the CuZnPb insert (coated with Al2O3) before molding......................................... 37 Figure 6.8 Shape of the CuZnPb insert (coated with Al2O3) after molding........................................... 37 Figure 6.9 Shape of the NiP coated stainless steel insert before molding ............................................ 37 Figure 6.10 Shape of the NiP coated stainless steel insert after molding ............................................. 38 Figure 6.11 Shape of the glass (CuZnPb side) after molding ................................................................. 38 Figure 6.12 Shape of the glass (NiP side) after molding ........................................................................ 38 Figure 7.1 Geometry of glass and molds modeled in MSC Marc .......................................................... 40 Figure 7.2 a) Fixed displacement in x-direction applied on lower mold b) Change in position applied on upper mold ....................................................................................................................................... 43 2 Figure 7.3 Boundary conditions applied on the geometry in the simulation a) Position of upper
Recommended publications
  • The American Ceramic Society 25Th International Congress On
    The American Ceramic Society 25th International Congress on Glass (ICG 2019) ABSTRACT BOOK June 9–14, 2019 Boston, Massachusetts USA Introduction This volume contains abstracts for over 900 presentations during the 2019 Conference on International Commission on Glass Meeting (ICG 2019) in Boston, Massachusetts. The abstracts are reproduced as submitted by authors, a format that provides for longer, more detailed descriptions of papers. The American Ceramic Society accepts no responsibility for the content or quality of the abstract content. Abstracts are arranged by day, then by symposium and session title. An Author Index appears at the back of this book. The Meeting Guide contains locations of sessions with times, titles and authors of papers, but not presentation abstracts. How to Use the Abstract Book Refer to the Table of Contents to determine page numbers on which specific session abstracts begin. At the beginning of each session are headings that list session title, location and session chair. Starting times for presentations and paper numbers precede each paper title. The Author Index lists each author and the page number on which their abstract can be found. Copyright © 2019 The American Ceramic Society (www.ceramics.org). All rights reserved. MEETING REGULATIONS The American Ceramic Society is a nonprofit scientific organization that facilitates whether in print, electronic or other media, including The American Ceramic Society’s the exchange of knowledge meetings and publication of papers for future reference. website. By participating in the conference, you grant The American Ceramic Society The Society owns and retains full right to control its publications and its meetings.
    [Show full text]
  • Technical Glasses
    Technical Glasses Physical and Technical Properties 2 SCHOTT is an international technology group with 130 years of ex­ perience in the areas of specialty glasses and materials and advanced technologies. With our high­quality products and intelligent solutions, we contribute to our customers’ success and make SCHOTT part of everyone’s life. For 130 years, SCHOTT has been shaping the future of glass technol­ ogy. The Otto Schott Research Center in Mainz is one of the world’s leading glass research institutions. With our development center in Duryea, Pennsylvania (USA), and technical support centers in Asia, North America and Europe, we are present in close proximity to our customers around the globe. 3 Foreword Apart from its application in optics, glass as a technical ma­ SCHOTT Technical Glasses offers pertinent information in terial has exerted a formative influence on the development concise form. It contains general information for the deter­ of important technological fields such as chemistry, pharma­ mination and evaluation of important glass properties and ceutics, automotive, optics, optoelectronics and information also informs about specific chemical and physical character­ technology. Traditional areas of technical application for istics and possible applications of the commercial technical glass, such as laboratory apparatuses, flat panel displays and glasses produced by SCHOTT. With this brochure, we hope light sources with their various requirements on chemical­ to assist scientists, engineers, and designers in making the physical properties, have led to the development of a great appropriate choice and make optimum use of SCHOTT variety of special glass types. Through new fields of appli­ products. cation, particularly in optoelectronics, this variety of glass types and their modes of application have been continually Users should keep in mind that the curves or sets of curves enhanced, and new forming processes have been devel­ shown in the diagrams are not based on precision measure­ oped.
    [Show full text]
  • Crystallization Kinetics of Chalcogenide Glasses
    2 Crystallization Kinetics of Chalcogenide Glasses Abhay Kumar Singh Department of Physics, Banaras Hindu University, Varanasi, India 1. Introduction 1.1 Background of chalcogenides Chalcogenide glasses are disordered non crystalline materials which have pronounced tendency their atoms to link together to form link chain. Chalcogenide glasses can be obtained by mixing the chalcogen elements, viz, S, Se and Te with elements of the periodic table such as Ga, In, Si, Ge, Sn, As, Sb and Bi, Ag, Cd, Zn etc. In these glasses, short-range inter-atomic forces are predominantly covalent: strong in magnitude and highly directional, whereas weak van der Waals' forces contribute significantly to the medium-range order. The atomic bonding structure is, in general more rigid than that of organic polymers and more flexible than that of oxide glasses. Accordingly, the glass-transition temperatures and elastic properties lay in between those of these materials. Some metallic element containing chalcogenide glasses behave as (super) ionic conductors. These glasses also behave as semiconductors or, more strictly, they are a kind of amorphous semi-conductors with band gap energies of 1±3eV (Fritzsche, 1971). Commonly, chalcogenide glasses have much lower mechanical strength and thermal stability as compared to existing oxide glasses, but they have higher thermal expansion, refractive index, larger range of infrared transparency and higher order of optical non-linearity. It is difficult to define with accuracy when mankind first fabricated its own glass but sources demonstrate that it discovered 10,000 years back in time. It is also difficult to point in time, when the field of chalcogenide glasses started.
    [Show full text]
  • Unraveling the Crystallization Kinetics of Supercooled Liquid Gete By
    Article pubs.acs.org/crystal Unraveling the Crystallization Kinetics of Supercooled Liquid GeTe by Ultrafast Calorimetry † ‡ § ‡ † § ‡ † † Yimin Chen, , , Guoxiang Wang, Lijian Song, , Xiang Shen,*, Junqiang Wang,*, Juntao Huo, ‡ † ‡ ‡ ‡ Rongping Wang, Tiefeng Xu, , Shixun Dai, and Qiuhua Nie † Key Laboratory of Magnetic Materials and Devices & Zhejiang Province Key Laboratory of Magnetic Materials and Application Technology, Ningbo Institute of Materials Technology & Engineering, Chinese of Sciences, Ningbo, 315201, China ‡ Laboratory of Infrared Material and Devices & Key Laboratory of Photoelectric Materials and Devices of Zhejiang Province, Advanced Technology Research Institute, Ningbo, 315211, China § University of Chinese Academy of Sciences, Beijing, 100049, China *S Supporting Information ABSTRACT: Crystallization kinetics of phase change materials (PCMs) at high temperatures is of key importance for the extreme speed of data writing and erasing. In this work, the crystallization behavior of one of the typical PCMs, GeTe, has been studied using ultrafast differential scanning calorimetry (DSC) at high heating rates up to 4 × 104 Ks−1. A strong non-Arrhenius temperature-dependent viscosity has been observed. We considered two viscosity models for estimating the crystal growth kinetics ffi coe cient (Ukin). The results showed that the MYEGA model was more suitable to describe the temperature-dependent viscosity and the crystal growth kinetics for supercooled liquid GeTe. The glass transition temperature (Tg) and fragility m were estimated to be 432.1 K and 130.7, respectively. The temperature-dependent crystal growth rates, which were extrapolated by the MYEGA model, were in line with the experimental results that were measured by in situ transmission electron microscopy at a given temperature. The crystal growth rate reached a maximum of 3.5 m s−1 at 790 K.
    [Show full text]
  • Hybrid Polymer Photonic Crystal Fiber with Integrated Chalcogenide Glass Nanofilms
    View metadata,Downloaded citation and from similar orbit.dtu.dk papers on:at core.ac.uk Dec 20, 2017 brought to you by CORE provided by Online Research Database In Technology Hybrid polymer photonic crystal fiber with integrated chalcogenide glass nanofilms Markos, Christos; Kubat, Irnis; Bang, Ole Published in: Scientific Reports Link to article, DOI: 10.1038/srep06057 Publication date: 2014 Document Version Publisher's PDF, also known as Version of record Link back to DTU Orbit Citation (APA): Markos, C., Kubat, I., & Bang, O. (2014). Hybrid polymer photonic crystal fiber with integrated chalcogenide glass nanofilms. Scientific Reports, 4. DOI: 10.1038/srep06057 General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. • Users may download and print one copy of any publication from the public portal for the purpose of private study or research. • You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. OPEN Hybrid polymer photonic crystal fiber SUBJECT AREAS: with integrated chalcogenide glass POLYMERS NONLINEAR OPTICS nanofilms Christos Markos, Irnis Kubat & Ole Bang Received 10 March 2014 DTU Fotonik, Department of Photonics Engineering, Technical University of Denmark, DK-2800 Kgs.
    [Show full text]
  • Measurement of Crystal Growth Velocity in a Melt-Quenched Phase-Change Material
    ARTICLE Received 26 Mar 2013 | Accepted 29 Jul 2013 | Published 29 Aug 2013 DOI: 10.1038/ncomms3371 OPEN Measurement of crystal growth velocity in a melt-quenched phase-change material Martin Salinga1, Egidio Carria1, Andreas Kaldenbach1, Manuel Bornho¨fft2, Julia Benke1, Joachim Mayer2 & Matthias Wuttig1 Phase-change materials are the basis for next-generation memory devices and reconfigurable electronics, but fundamental understanding of the unconventional kinetics of their phase transitions has been hindered by challenges in the experimental quantification. Here we obtain deeper understanding based on the temperature dependence of the crystal growth velocity of the phase-change material AgInSbTe, as derived from laser-based time-resolved reflectivity measurements. We observe a strict Arrhenius behaviour for the growth velocity over eight orders of magnitude (from B10 nm s À 1 to B1msÀ 1). This can be attributed to the formation of a glass at elevated temperatures because of rapid quenching of the melt. Further, the temperature dependence of the viscosity is derived, which reveals that the supercooled liquid phase must have an extremely high fragility (4100). Finally, the new experimental evidence leads to an interpretation, which comprehensively explains existing data from various different experiments reported in literature. 1 I. Physikalisches Institut (IA) and JARA-FIT, RWTH Aachen University, Sommerfeldstrae 14, 52074 Aachen, Germany. 2 Gemeinschaftslabor fu¨r Elektronenmikroskopie, RWTH Aachen University, Ahornstrae 55, 52074 Aachen, Germany. Correspondence and requests for materials should be addressed to M.S. (email: [email protected]). NATURE COMMUNICATIONS | 4:2371 | DOI: 10.1038/ncomms3371 | www.nature.com/naturecommunications 1 & 2013 Macmillan Publishers Limited.
    [Show full text]
  • Ultrafast-Laser-Inscribed 3D Integrated Photonics: Challenges and Emerging Applications
    Nanophotonics 2015; 4:332–352 Review Article Open Access S. Gross* and M. J. Withford Ultrafast-laser-inscribed 3D integrated photonics: challenges and emerging applications DOI 10.1515/nanoph-2015-0020 ing methods used to create photonic chips are relatively Received July 7, 2015; accepted July 30, 2015 immature, and the common approach is to adapt the pla- nar (2D) lithography methods originally developed for sil- Abstract: Since the discovery that tightly focused fem- icon microelectronics. Unfortunately, this is akin to push- tosecond laser pulses can induce a highly localised and ing a square peg into a round hole because photons, the permanent refractive index modification in a large num- elementary particle of light, have many degrees of free- ber of transparent dielectrics, the technique of ultrafast dom, in contrast to electrons which have few. For exam- laser inscription has received great attention from a wide ple, a stream of electrons can be characterised in terms range of applications. In particular, the capability to create of current and voltage. A stream of photons, on the other three-dimensional optical waveguide circuits has opened hand, can exhibit different traits based on velocity and up new opportunities for integrated photonics that would brightness, the optical equivalent to current and voltage as not have been possible with traditional planar fabrication well as wavelength, polarisation, spatial mode and orbital techniques because it enables full access to the many de- angular momentum. These additional features reflect the grees of freedom in a photon. This paper reviews the basic three dimensionality of light, features that cannot be fully techniques and technological challenges of 3D integrated exploited with planar circuitry.
    [Show full text]
  • Structure of Liquid Phase Change Material Aginsbte from Density Functional/ Molecular Dynamics Simulations J
    Structure of liquid phase change material AgInSbTe from density functional/ molecular dynamics simulations J. Akola, and R. O. Jones Citation: Appl. Phys. Lett. 94, 251905 (2009); View online: https://doi.org/10.1063/1.3157166 View Table of Contents: http://aip.scitation.org/toc/apl/94/25 Published by the American Institute of Physics Articles you may be interested in Nanoscale nuclei in phase change materials: Origin of different crystallization mechanisms of Ge2Sb2Te5 and AgInSbTe Journal of Applied Physics 115, 063506 (2014); 10.1063/1.4865295 Nucleation of films employed in phase-change media Journal of Applied Physics 99, 064907 (2006); 10.1063/1.2184428 Crystallization kinetics of sputter-deposited amorphous AgInSbTe films Journal of Applied Physics 90, 3816 (2001); 10.1063/1.1405141 Evidence for thermally assisted threshold switching behavior in nanoscale phase-change memory cells Journal of Applied Physics 119, 025704 (2016); 10.1063/1.4938532 Investigation of switching region in superlattice phase change memories AIP Advances 6, 105104 (2016); 10.1063/1.4964729 Low power phase change memory switching of ultra-thin In3Sb1Te2 nanowires Applied Physics Letters 109, 213103 (2016); 10.1063/1.4968510 APPLIED PHYSICS LETTERS 94, 251905 ͑2009͒ Structure of liquid phase change material AgInSbTe from density functional/molecular dynamics simulations ͒ J. Akola1,2,3 and R. O. Jones1,a 1Institut für Festkörperforschung, Forschungszentrum Jülich, D-52425 Jülich, Germany 2Nanoscience Center, Department of Physics, P.O. Box 35, FI-40014 University of Jyväskylä, Finland 3Department of Physics, Tampere University of Technology, P.O. Box 692, FI-33101 Tampere, Finland ͑Received 20 April 2009; accepted 28 May 2009; published online 23 June 2009͒ The liquid phase of the AgInSbTe phase change material Ag3.5In3.8Sb75.0Te17.7 has been studied using molecular dynamics/density functional simulations.
    [Show full text]
  • Investigation of Index of Refraction Changes in Chalcogenide Glasses During Molding Processes
    Investigation of index of refraction changes in chalcogenide glasses during molding processes. Jacklyn Novak1, Ray Pini1, William V. Moreshead1, Erik Stover2, Alan Symmons1 1LightPath Technologies, Inc., 2603 Challenger Tech Ct, Ste 100, Orlando, FL, USA 32826 2M3 Measurement Solutions, Inc., 2048 Aldergrove Ave, Suite D, Escondido, CA 92029 ABSTRACT Precision glass molding has a well-documented effect of a decrease in the index of refraction of the glass during the molding process. This index drop has such significant value that optical designs for molded lenses must take into account the index drop to accurately determine the optical performance of the final lens. Widespread adoption of chalcogenide glasses for molded infrared optics has raised a series of questions as to the behavior of these glasses under molding conditions. This paper will investigate the index of refraction changes in two different chalcogenide glasses and determine if these changes are significant enough for optical designers to consider in their designs. Keywords: Precision glass molding, chalcogenide glass, refractive index, infrared 1. INTRODUCTION Until recently, the only materials used for infrared optics were salts and crystals such as germanium or zinc selenide. These materials require expensive processing techniques and the materials themselves also have a high cost. Chalcogenide glasses (ChGs) were invented to meet the increasing demand for low-cost infrared optics. Examples of ChGs include Ge28Sb12Se60 and As40Se60. These materials are less expensive due to containing little to no germanium. Processing costs are also reduced because ChGs are moldable. Precision glass molding (PGM) is an alternative to traditional methods of producing high quality optical lenses.
    [Show full text]
  • Bespoke Photonic Devices Using Ultrafast Laser Driven Ion Migration in Glasses ⇑ T.T
    Progress in Materials Science 94 (2018) 68–113 Contents lists available at ScienceDirect Progress in Materials Science journal homepage: www.elsevier.com/locate/pmatsci Bespoke photonic devices using ultrafast laser driven ion migration in glasses ⇑ T.T. Fernandez a,1, M. Sakakura b,1, S.M. Eaton a, B. Sotillo a, , J. Siegel c, J. Solis c, Y. Shimotsuma d, K. Miura d a Istituto di Fotonica e Nanotecnologie-Consiglio Nazionale delle Ricerche (IFN-CNR), Milano, Italy b Optoelectronics Research Centre, University of Southampton, Southampton, United Kingdom c Laser Processing Group, Instituto de Optica, Consejo Superior de Investigaciones Científicas (IO,CSIC), Madrid, Spain d Department of Materials Chemistry, Kyoto University, Kyoto, Japan article info abstract Article history: This Review provides an exhaustive and detailed description of ion migration phenomena Received 16 August 2016 which occur inside transparent dielectric media due to the interaction with intense ultra- Accepted 20 December 2017 short pulses. The paper differentiates various processes underlying the ion migration influ- Available online 29 December 2017 enced by simultaneous heat accumulation and diffusion. The femtosecond laser induced temperature distribution, the major driving force of ions in dielectrics, is described in detail. Keywords: This discussion is based on three meticulous analysis methods including the thermal modi- Femtosecond laser micromachining fication of transparent dielectrics at various ambient temperatures, numerical simulations Ion-migration and comparison with direct observation of the light-matter interaction and micro-Raman Scanning electron microscope Glass spectroscopy. The ion migration phenomena studied have been triggered in four different Waveguides configurations: at low repetition and high repetition rates, and observations perpendicular Photonic devices and parallel to the laser irradiation direction.
    [Show full text]
  • Chalcogenide Glass Materials for Integrated Infrared Photonics
    Chalcogenide Glass Materials for Integrated Infrared Photonics by Vivek Singh B.S. Materials Science and Engineering Columbia University, 2009 Submitted to the Department of Materials Science and Engineering in Partial Fulfillment of the Requirements for the Degree of DOCTOR OF PHILOSOPHY at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY September 2015 © 2015 Massachusetts Institute of Technology. All rights reserved. Signature of Author:_________________________________________ Department of Materials Science and Engineering July 20, 2015 Certified by:_____________________________________________ Lionel C. Kimerling Thomas Lord Professor of Materials Science and Engineering Thesis Supervisor Certified by:_____________________________________________ Anuradha M. Agarwal Principal Research Scientist, Materials Processing Center Thesis Supervisor Accepted by:_____________________________________________ Donald Sadoway Chair, Departmental Committee on Graduate Students 2 Chalcogenide Glass Materials for Integrated Infrared Photonics by Vivek Singh Submitted to the Department of Materials Science and Engineering on July 20, 2015 in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy in Materials Science and Engineering Abstract Chalcogenide glasses (ChGs) are amorphous compounds containing the chalcogen elements (S, Se, Te) and exhibit wide infrared transparency windows. They are easy to synthesize in bulk and thin film forms and their compositional flexibility allows tuning of optical properties such as refractive index making them ideal for infrared photonics. We have studied the material attenuation in ChGs that arises due to the presence of impurities in the raw materials and established UV photolithography-based process flows that enable fabrication of chalcogenide glass waveguides and microresonators for near- and mid-IR wavelength ranges. Waveguides and optical resonators are key microphotonic elements for many on-chip applications such as telecommunications and chemical sensing.
    [Show full text]
  • Hybrid Polymer Photonic Crystal Fiber with Integrated
    OPEN Hybrid polymer photonic crystal fiber SUBJECT AREAS: with integrated chalcogenide glass POLYMERS NONLINEAR OPTICS nanofilms Christos Markos, Irnis Kubat & Ole Bang Received 10 March 2014 DTU Fotonik, Department of Photonics Engineering, Technical University of Denmark, DK-2800 Kgs. Lyngby, Denmark. Accepted 10 July 2014 The combination of chalcogenide glasses with polymer photonic crystal fibers (PCFs) is a difficult and Published challenging task due to their different thermo-mechanical material properties. Here we report the first 14 August 2014 experimental realization of a hybrid polymer-chalcogenide PCF with integrated As2S3 glass nanofilms at the inner surface of the air-channels of a poly-methyl-methacrylate (PMMA) PCF. The integrated high refractive index glass films introduce distinct antiresonant transmission bands in the 480–900 nm wavelength region. We demonstrate that the ultra-high Kerr nonlinearity of the chalcogenide glass makes Correspondence and the polymer PCF nonlinear and provides a possibility to shift the transmission band edges as much as 17 nm requests for materials by changing the intensity. The proposed fabrication technique constitutes a new highway towards all-fiber should be addressed to nonlinear tunable devices based on polymer PCFs, which at the moment is not possible with any other C.M. (chmar@fotonik. fabrication method. dtu.dk) he photonic crystal fiber (PCF) is an optical fiber in which the cladding is formed by a periodic array of micron sized holes running along the entire length of the fiber1. The hole-structure defines the fiber T properties and consequently PCFs have attracted a lot of scientific attention, since they offer unique design flexibility and provide an amazing degree of freedom for manipulation of their guiding properties.
    [Show full text]