E. Czerska, K. Wisniewski, E. Augustyn, C. Koepke, R. Lisiecki, M. Kępińska, M. Żelechower
{"title":"Erbium and ytterbium co-doped transparent oxyfluoride glass-ceramics optical fibers","authors":"E. Czerska, K. Wisniewski, E. Augustyn, C. Koepke, R. Lisiecki, M. Kępińska, M. Żelechower","doi":"10.1117/12.2271623","DOIUrl":"https://doi.org/10.1117/12.2271623","url":null,"abstract":"According to the earlier author’s papers, the erbium/ytterbium co-doped oxyfluoride glass-ceramics fibers should demonstrate better 1550 nm emission under 488/515/980 nm excitation (the erbium Er3+ ion transition 4I13/2→4I15/2) than corresponding glass fibers (the batch composition 48SiO211Al2O3-7Na2CO3-10CaO-10PbO-12PbF2- 1.5/0.6YbF3-0.5/0.2ErF3). Glass fibers provided as a core of standard multimode waveguide (the diameter of 62 μm) have been drawn with the mini-tower to the diameter between 50 μm and 80 μm, then annealed in the two-step regime (580°C/1h – nucleation of nano-crystals; 760oC/15/30 min – nano-crystals growth). This kind of heat treatment ensures the transparent glass-ceramics fibers with the microstructure of homogeneously distributed nano-crystals (lead, erbium and ytterbium enriched cubic fluorite-like crystals and hexagonal PbF2 crystals) embedded in a glassy host. Their transmission covers the range of 80-90% and seems to be sufficient with respect to their provided limited length (~2m). The luminescence intensity for glass-ceramics fibers at 1530 nm is higher than that of respective glass fibers and the lifetimes of the erbium ion excited state 4I13/2 are of the same order (~5 ms). In that context the glass-ceramics fibers discussed above seem to be promising candidates for cores of fiber lasers at the 1550 nm band.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"23 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123896096","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Simulation of partially coherent light propagation using parallel computing devices","authors":"Tiago E. C. Magalhães, J. Rebordão","doi":"10.1117/12.2272339","DOIUrl":"https://doi.org/10.1117/12.2272339","url":null,"abstract":"Light acquires or loses coherence and coherence is one of the few optical observables. Spectra can be derived from coherence functions and understanding any interferometric experiment is also relying upon coherence functions. Beyond the two limiting cases (full coherence or incoherence) the coherence of light is always partial and it changes with propagation. We have implemented a code to compute the propagation of partially coherent light from the source plane to the observation plane using parallel computing devices (PCDs). In this paper, we restrict the propagation in free space only. To this end, we used the Open Computing Language (OpenCL) and the open-source toolkit PyOpenCL, which gives access to OpenCL parallel computation through Python. To test our code, we chose two coherence source models: an incoherent source and a Gaussian Schell-model source. In the former case, we divided into two different source shapes: circular and rectangular. The results were compared to the theoretical values. Our implemented code allows one to choose between the PyOpenCL implementation and a standard one, i.e using the CPU only. To test the computation time for each implementation (PyOpenCL and standard), we used several computer systems with different CPUs and GPUs. We used powers of two for the dimensions of the cross-spectral density matrix (e.g. 324, 644) and a significant speed increase is observed in the PyOpenCL implementation when compared to the standard one. This can be an important tool for studying new source models.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"1 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124007309","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
M. Gomes, J. C. Costa, R. Alves, N. Silva, A. Guerreiro
{"title":"Development of a quantum particle in cell algorithm in GPU for solving Maxwell-Bloch equations","authors":"M. Gomes, J. C. Costa, R. Alves, N. Silva, A. Guerreiro","doi":"10.1117/12.2272052","DOIUrl":"https://doi.org/10.1117/12.2272052","url":null,"abstract":"In this paper we report on the development of a numerical solver for Vlasov equations based on heterogeneous supercomputing using GPGPUs. The solver adapts techniques from many-body simulation, namely the particlein-cell approach, to describe the interaction between the electromagnetic field and atomic gas whose internal state can be described by the multilevel Bloch equations. We also present the benchmark and performance analysis of the code. We investigate the interaction between two coherent light beams, as a case of study to demonstrate the validation of the code.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"659 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115122595","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
R. Martínez-Herrero, D. Maluenda, G. Piquero, Juan Carlos G. de Sande, M. Santarsiero, F. Gori
{"title":"Partially polarized pseudo-Schell model sources","authors":"R. Martínez-Herrero, D. Maluenda, G. Piquero, Juan Carlos G. de Sande, M. Santarsiero, F. Gori","doi":"10.1117/12.2272154","DOIUrl":"https://doi.org/10.1117/12.2272154","url":null,"abstract":"In this work a new type of partially polarized and partially coherent sources is proposed. The coherence characteristics of these sources are dependent on the difference of the radial distances from the source center of the two points to be compared. The coherence is perfect for points located on the same circle centered on the source center and decreases for points that belongs to different concentric circles. The maximum attainable coherence is related to the degree of polarization of the source. Coherence and polarization characteristics of this kind of fields at the source plane and upon free space propagation are analyzed in detail for a simple case. For the particular presented example, a partially polarized and partially coherent field is obtained, whose polarization properties are invariant in propagation.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"5 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115588961","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
M. Ghafoor, Y. Sgibnev, D. Marasanov, N. Nikonorov
{"title":"Energy transfer between silver clusters and europium Eu3+ ions in photo-thermo-refractive glasses","authors":"M. Ghafoor, Y. Sgibnev, D. Marasanov, N. Nikonorov","doi":"10.1117/12.2271688","DOIUrl":"https://doi.org/10.1117/12.2271688","url":null,"abstract":"Photo-thermo-refractive glass is a promising material because it combines the properties of several monofunctional materials in it. These glasses can be doped with rare earth ions and can then be used for many practical applications. But the major problem is the low absorption coefficient. So, a lot of research has been done to grow silver nanoclusters and nanoparticles for improving the spectroscopic properties of rare-earth ions. In this study we present a way to transfer energy from silver clusters to Eu3+ ions in the PTR glass. These results can be used for developing warm white LEDs and down converters for solar cells.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"8 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124969308","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Finite element model for the simulation of laser activated micro- and nano-scale drug delivery systems","authors":"Henrique Vilhena, J. Coelho, J. Rebordão","doi":"10.1117/12.2272721","DOIUrl":"https://doi.org/10.1117/12.2272721","url":null,"abstract":"This paper describes a flexible model that can be used to simulate laser-based photoactivation of drug delivery systems. It considers Gaussian beams for the excitation while the heat diffusion equation is solved by use of the finite element method. As an example, a typical liposome geometry in the focal volume of a laser beam is simulated and the results are compared with experimental data obtained in the literature, showing a good agreement. The model has potential in the design of drug delivery systems as it can be a starting point for the development of new kinds of micro- and nano-scale drug delivery systems.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"13 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123655682","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
P. Palevičius, M. Ragulskis, G. Janusas, A. Palevičius
{"title":"Image encryption scheme based on computer generated holography and time-averaged moiré","authors":"P. Palevičius, M. Ragulskis, G. Janusas, A. Palevičius","doi":"10.1117/12.2272126","DOIUrl":"https://doi.org/10.1117/12.2272126","url":null,"abstract":"A technique of computational image encryption and optical decryption based on computer generated holography and time-averaged moir´e is investigated in this paper. Dynamic visual cryptography (a visual cryptography scheme based on time-averaging geometric moir´e), Gerchberg–Saxton algorithm and 3D microstructure manufacturing techniques are used to construct the optical scheme. The secret is embedded into a cover image by using a stochastic moir´e grating and can be visually decoded by a naked eye. The secret is revealed if the amplitude of harmonic oscillations in the Fourier plane corresponds to an accurately preselected value. The process of the production of 3D microstructure is described in details. Computer generated holography is used in the design step and electron beam lithography is exploited for physical 3D patterning. The phase data of a complex 3D microstructure is obtained by Gerchberg-Saxton algorithm and is used to produce a computer generated hologram. Physical implementation of microstructure is performed by using a single layer polymethyl methacrylate as a basis for 3D microstructure. Numerical simulations demonstrate efficient applicability of this technique.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"35 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"121238877","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Phase contrast imaging of red blood cells using digital holographic interferometric microscope","authors":"Varun Kumar, G. Khan, C. Shakher","doi":"10.1117/12.2276335","DOIUrl":"https://doi.org/10.1117/12.2276335","url":null,"abstract":"In this paper, digital holographic interferometric microscope (DHIM) in conjunction with Fresnel reconstruction method is demonstrated for phase contrast imaging of red blood cells (RBCs). The advantage of using the DHIM is that the distortions due to aberrations in the optical system are avoided by the interferometric comparison of reconstructed phase with and without the object.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"150 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"121395163","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
C. García-Resúa, Hugo Pena-Verdeal, M. .. Giraldez, E. Yebra-Pimentel
{"title":"Clinical performance of an objective methodology to categorize tear film lipid layer patterns","authors":"C. García-Resúa, Hugo Pena-Verdeal, M. .. Giraldez, E. Yebra-Pimentel","doi":"10.1117/12.2271845","DOIUrl":"https://doi.org/10.1117/12.2271845","url":null,"abstract":"Purpose: To validate the performance of a new objective application designated iDEAS (Dry Eye Assessment System) to categorize different zones of lipid layer patterns (LLPs) in one image. Material and methods: Using the Tearscopeplus and a digital camera attached to a slit-lamp, 50 images were captured and analyzed by 4 experienced optometrists. In each image the observers outlined tear film zones that they clearly identified as a specific LLP. Further, the categorization made by the 4 optometrists (called observer 1, 2, 3 and 4) was compared with the automatic system included in iDEAS (5th observer). Results: In general, observer 3 classified worse than all observers (observers 1, 2, 4 and automatic application, Wilcoxon test, <0.05). The automatic system behaved similar to the remaining three observers (observer 1, 2 and 4) showing differences only for Open meshwork LLP when comparing with observer 4 (Wilcoxon test, p=0.02). For the remaining two observers (observer 1 and 2) there was not found statistical differences (Wilcoxon test, >0.05). Furthermore, we obtained a set of photographs per LLP category for which all optometrists showed agreement by using the new tool. After examining them, we detected the more characteristic features for each LLP to enhance the description of the patterns implemented by Guillon. Conclusions: The automatic application included in the iDEAS framework is able to provide zones similar to the annotations made by experienced optometrists. Thus, the manual process done by experts can be automated with the benefits of being unaffected by subjective factors.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"23 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"128493594","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Photo-induced ultrasound microscopy for photo-acoustic imaging of non-absorbing specimens","authors":"Elena Tcarenkova, S. Koho, P. Hänninen","doi":"10.1117/12.2276315","DOIUrl":"https://doi.org/10.1117/12.2276315","url":null,"abstract":"Photo-Acoustic Microscopy (PAM) has raised high interest in in-vivo imaging due to its ability to preserve the near-diffraction limited spatial resolution of optical microscopes, whilst extending the penetration depth to the mm-range. Another advantage of PAM is that it is a label-free technique – any substance that absorbs PAM excitation laser light can be viewed. However, not all sample structures desired to be observed absorb sufficiently to provide contrast for imaging. This work describes a novel imaging method that makes it possible to visualize optically transparent samples that lack intrinsic photo-acoustic contrast, without the addition of contrast agents. A thin, strongly light absorbing layer next to sample is used to generate a strong ultrasonic signal. This signal, when recorded from opposite side, contains ultrasonic transmission information of the sample and thus the method can be used to obtain an ultrasound transmission image on any PAM.","PeriodicalId":150522,"journal":{"name":"Applications of Optics and Photonics","volume":"47 7","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2017-08-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"133169562","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}