{"id":77,"date":"2021-04-27T08:35:50","date_gmt":"2021-04-27T08:35:50","guid":{"rendered":"https:\/\/indico.inoe.ro\/?page_id=77"},"modified":"2026-03-16T21:27:16","modified_gmt":"2026-03-16T21:27:16","slug":"services","status":"publish","type":"page","link":"https:\/\/indico.inoe.ro\/index.php\/services\/","title":{"rendered":"Services"},"content":{"rendered":"\n<p class=\"has-text-align-center has-pale-cyan-blue-background-color has-background has-medium-font-size\"><strong>SERVICES<\/strong> of characterization and diagnosis <\/p>\n\n\n\n<p class=\"has-black-color has-text-color\"><a href=\"#laser-energy\" data-type=\"internal\" data-id=\"#laser-energy\">Laser energy\/power<\/a><\/p>\n\n\n\n<p class=\"has-black-color has-text-color\"><a href=\"#laser-beam\" data-type=\"internal\" data-id=\"#laser-beam\">Laser beam profile<\/a><\/p>\n\n\n\n<p class=\"has-black-color has-text-color\"><a href=\"#laser-pulse\" data-type=\"internal\" data-id=\"#laser-pulse\">Laser pulse width<\/a><\/p>\n\n\n\n<p class=\"has-black-color has-text-color\" id=\"spectral\"><a href=\"#ft-optical\" data-type=\"internal\" data-id=\"#ft-optical\">FT optical spectrum analysis<\/a><\/p>\n\n\n\n<p class=\"has-black-color has-text-color\"><a href=\"#polarization-state\" data-type=\"internal\" data-id=\"#polarization-state\">Polarization state analysis<\/a><\/p>\n\n\n\n<p class=\"has-black-color has-text-color\"><a href=\"#optical-components\" data-type=\"internal\" data-id=\"#optical-components\">Characterization of optical components<\/a> (focal length, angles of prisms, surface flatness, dimensional measurements )<\/p>\n\n\n\n<p class=\"has-black-color has-text-color\"><a href=\"#spectral-analysis\" data-type=\"internal\" data-id=\"#spectral-analysis\">Spectral analysis of materials<\/a> (filters transmission, thin films characterization)<\/p>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-cyan-bluish-gray-background-color has-background\"><strong>LIST OF INSTRUMENTS<\/strong><\/p>\n\n\n\n<figure class=\"wp-block-table\"><table><tbody><tr><td><strong>Crt. No.<\/strong><\/td><td><strong>Item<\/strong><\/td><td><strong>Manufacturer<\/strong><\/td><td><strong>Model<\/strong><\/td><td><strong>Status<\/strong><\/td><\/tr><tr><td>1<\/td><td>Video measurement microscope<\/td><td>Hoffmann<\/td><td>MM1-300\/6X GARANT<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>2<\/td><td>Laser Beam profiler<\/td><td>Ophir Photonics<\/td><td>NanoScan2<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>3<\/td><td>Electronic autocolimator<\/td><td>Moeller-Wedel Optical<\/td><td>Elcomat vario D 500T\/65<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>4<\/td><td>Interferometer and accessories<\/td><td>Moeller-Wedel Optical<\/td><td>Interferometer VI-direct 100 SL<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>5<\/td><td>Diopter telescope<\/td><td>Moeller-Wedel Optical<\/td><td>Diopter telescope \u00b15.0 dpt, 0.1 dpt div.<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>6<\/td><td>Dynameter<\/td><td>Moeller-Wedel Optical<\/td><td>Dynameter<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>7<\/td><td>Laser He-Ne CW 633nm<\/td><td>ThorLabs<\/td><td>Laser and accessories<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>8<\/td><td>Laser diodes CW &nbsp; 405, 532, 635, 859 and 1064 nm<\/td><td>ThorLabs<\/td><td>Laser and accessories<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>9<\/td><td>Laser UV 355nm CW<\/td><td>Roithner<\/td><td>Laser and accessories<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>10<\/td><td>Optical Spectrum Analyzer<\/td><td>ThorLabs<\/td><td>OSA 201, OSA 202<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>11<\/td><td>Polarization analyzing system<\/td><td>ThorLabs<\/td><td>PAX57VIS-T, PAN5710IR2<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>12<\/td><td>Ultrafast photodiode<\/td><td>Alphalas<\/td><td>UPD-200-UP<\/td><td><strong>New<\/strong><\/td><\/tr><tr><td>13<\/td><td>Oscilloscope<\/td><td>Tektronix<\/td><td>DPO7254<\/td><td>Exist.<\/td><\/tr><tr><td>14<\/td><td>Spectrophotometer<\/td><td>PerkinElmer<\/td><td>LAMBDA 1050 UV\/Vis\/NIR<\/td><td>Exist.<\/td><\/tr><tr><td>15<\/td><td>Ellipsometer<\/td><td>HORIBA<\/td><td>UVISEL ER AGAS<\/td><td>Exist.<\/td><\/tr><tr><td>16<\/td><td>Energy\/Powermeter<\/td><td>Gentec<\/td><td>SOLO PE<\/td><td>Exist.<\/td><\/tr><tr><td>17<\/td><td>Goniometer<\/td><td>Moeller-Wedel Optical<\/td><td>Goniometer II-VIS<\/td><td>Exist.<\/td><\/tr><tr><td>18<\/td><td>Focal length meas. device<\/td><td>Moeller-Wedel Optical<\/td><td>MELOS 530-3<\/td><td>Exist.<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"has-text-align-center has-vivid-green-cyan-background-color has-background\" id=\"laser-energy\"><strong>LASER ENERGY\/POWER <\/strong><\/p>\n\n\n\n<p>One of the most important characteristic of a laser source is its energy (for a pulsed laser) or its power (for a CW laser). Measurements can be done at high acquisition rates allowing thus an accurate determination of pulse-to-pulse energy fluctuation. All measured data are stored and processed to get statistics (average, standard deviation, RMS, maximum, minimum, peak-to-peak). Report contains also measurement uncertainty data.<\/p>\n\n\n\n<p><strong>Laser energy<\/strong> can be measured using a Gentec SOLO-PE Energy\/Powermeter together with the next measuring heads (QE 50 SP-MB and XLE4):<\/p>\n\n\n\n<figure class=\"wp-block-table\"><table><tbody><tr><td>Measuring head<\/td><td><strong>QE 50 SP-MB<\/strong><\/td><td><strong>XLE4<\/strong><\/td><\/tr><tr><td>Measured energy range<\/td><td>15 \u00b5J \u2013 75 J<\/td><td>100 nJ \u2013 4 mJ<\/td><\/tr><tr><td>Wavelength range<\/td><td>190 nm \u2013 20 \u00b5m<\/td><td>190 nm \u2013 2.5 \u00b5m<\/td><\/tr><tr><td>Sensor area<\/td><td>50 x 50 mm<\/td><td>\u00d8 4 mm<\/td><\/tr><tr><td>Rise time<\/td><td>&nbsp;<\/td><td>10 \u00b5s<\/td><\/tr><tr><td>Max. pulse width<\/td><td>225 \u00b5s<\/td><td>5 \u00b5s<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p><strong>Laser power<\/strong> can be measured using a Gentec SOLO-PE Energy\/Powermeter together with the next measuring heads (PH100-Si, PH20-Ge, UP12E, UP25N and UP55N):<\/p>\n\n\n\n<figure class=\"wp-block-table aligncenter\"><table><tbody><tr><td>Measuring head<\/td><td class=\"has-text-align-left\" data-align=\"left\"><strong>PH100-Si<\/strong><\/td><td><strong>PH20-Ge<\/strong><\/td><td><strong>UP12E<\/strong><\/td><td><strong>UP25N<\/strong><\/td><td><strong>UP55N<\/strong><\/td><\/tr><tr><td>Measured power range<\/td><td class=\"has-text-align-left\" data-align=\"left\">600 pW &#8211; 30 mW<\/td><td>2 nW &#8211; 30 mW<\/td><td>1 mW \u2013 70 W<\/td><td>3 mW &#8211; 300 W<\/td><td>5 mW &#8211; 400 W<\/td><\/tr><tr><td>Wavelength range<\/td><td class=\"has-text-align-left\" data-align=\"left\">300 nm &#8211; 1100 nm<\/td><td>800 nm &#8211; 1650 nm<\/td><td>190 nm &#8211; 11 \u00b5m<\/td><td>190 nm &#8211; 11 \u00b5m<\/td><td>190 nm &#8211; 11 \u00b5m<\/td><\/tr><tr><td>Sensor area<\/td><td class=\"has-text-align-left\" data-align=\"left\">\u00d8 11.28 mm<\/td><td>\u00d8 5 mm<\/td><td>\u00d8 12 mm<\/td><td>\u00d8 25 mm<\/td><td>\u00d8 55 mm<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/maestro-3.png\" alt=\"\" class=\"wp-image-196\" width=\"190\" height=\"187\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/maestro-3.png 277w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/maestro-3-12x12.png 12w\" sizes=\"(max-width: 190px) 100vw, 190px\" \/><\/figure><\/div>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-text-align-center has-vivid-green-cyan-background-color has-background\" id=\"laser-beam\"><strong>LASER BEAM PROFILE<\/strong><\/p>\n\n\n\n<p>A more precise diagnostic of a laser source requires an analysis of the laser beam profile. A laser beam profiler provides important information characterizing the laser, as the energy (pulsed lasers) or power (CW lasers) distribution in a cross section of the laser beam, the waist of the beam, its divergence and M<sup>2<\/sup> factor (that quantifies the beam quality of laser beams).<\/p>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/m2.jpg\" alt=\"\" class=\"wp-image-102\" width=\"260\" height=\"185\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/m2.jpg 402w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/m2-300x213.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/m2-16x12.jpg 16w\" sizes=\"(max-width: 260px) 100vw, 260px\" \/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/M22.jpg\" alt=\"\" class=\"wp-image-101\" width=\"233\" height=\"186\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/M22.jpg 484w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/M22-300x240.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/M22-16x12.jpg 16w\" sizes=\"(max-width: 233px) 100vw, 233px\" \/><\/figure><\/div>\n\n\n\n<figure class=\"wp-block-image size-large is-resized is-style-rounded\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ophir.png\" alt=\"\" class=\"wp-image-103\" width=\"295\" height=\"210\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ophir.png 396w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ophir-300x214.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ophir-16x12.png 16w\" sizes=\"(max-width: 295px) 100vw, 295px\" \/><\/figure>\n\n\n\n<p>These measurements can be done using one of the next three heads (NS2-Si\/9\/5-PRO, NS2-Ge\/9\/5-PRO and NS2-Pyro\/9\/5-PRO), depending on the required wavelength:<\/p>\n\n\n\n<ul><li><strong>Ophir NS2-Si\/9\/5-PRO<\/strong>: NanoScan2 Si Detector 9 mm aperture 5\u03bcm slits. High-resolution head featuring Si detector, 63.5 mm diameter head with rotation mount, 9 mm entrance aperture, and matched pair of 5 \u03bcm wide slits. Use for wavelengths from 190 nm to 1 \u03bcm.<\/li><li><strong>Ophir NS2-Ge\/9\/5-PRO<\/strong>: NanoScan2 Ge Detector 9 mm Aperture 5 \u03bcm slits. High-resolution head featuring Germanium detector, 63.5mm diameter head with rotation mount, 9 mm entrance aperture, and matched pair of 5 \u03bcm wide slits. Use for wavelengths from 700 nm to 1.8 \u03bcm.<strong><\/strong><\/li><li><strong>Ophir NS2-Pyro\/9\/5-PRO<\/strong>: NanoScan2 Pyro Detector 9 mm Aperture 5.0 \u03bcm slits. High-resolution head featuring pyroelectric detector, 63.5 mm diameter head with rotation mount, 9 mm entrance aperture, and matched pair of 5 \u03bcm wide slits. Use for wavelengths from 190 nm to 100 \u03bcm.<\/li><\/ul>\n\n\n\n<p>M<sup>2<\/sup> measurements require the use of <strong>Ophir RAL-FXT<\/strong> (Rayleigh fixture for manual M<sup>2<\/sup>) and <strong>Ophir COL-FXT 250<\/strong> (250 mm FL collimation \ufb01xture).<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-2.png\" alt=\"\" class=\"wp-image-106\" width=\"301\" height=\"156\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-2.png 234w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-2-16x8.png 16w\" sizes=\"(max-width: 301px) 100vw, 301px\" \/><\/figure><\/div>\n\n\n\n<p class=\"has-text-align-center has-vivid-green-cyan-background-color has-background\" id=\"laser-pulse\"><strong>LASER PULSE WIDTH<\/strong><\/p>\n\n\n\n<p>Temporal behavior of the pulsed lasers is characterized by the pulse width (duration). Because the commercially available lasers have pulse widths of few ns, the pulse width measurement requires both a wide band oscilloscope and an ultrafast photodiode. As oscilloscope we use a Tektronix DPO7254, with a 2.5 GHz band and a rise time of 150 ps. The ultrafast photodiode is UPD-200-UP from Alphalas:<\/p>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Osciloscop.jpg\" alt=\"\" class=\"wp-image-111\" width=\"198\" height=\"162\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Osciloscop.jpg 302w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Osciloscop-300x245.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Osciloscop-16x12.jpg 16w\" sizes=\"(max-width: 198px) 100vw, 198px\" \/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"alignleft size-large\"><img decoding=\"async\" loading=\"lazy\" width=\"298\" height=\"88\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/photo.jpg\" alt=\"\" class=\"wp-image-112\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/photo.jpg 298w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/photo-16x5.jpg 16w\" sizes=\"(max-width: 298px) 100vw, 298px\" \/><\/figure><\/div>\n\n\n\n<figure class=\"wp-block-image size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/oscilo-tab.jpg\" alt=\"\" class=\"wp-image-114\" width=\"258\" height=\"113\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/oscilo-tab.jpg 509w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/oscilo-tab-300x133.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/oscilo-tab-16x7.jpg 16w\" sizes=\"(max-width: 258px) 100vw, 258px\" \/><\/figure>\n\n\n\n<p><\/p>\n\n\n\n<p>All measured data are stored and processed to get statistics (average, standard deviation). Report contains also measurement uncertainty data.<\/p>\n\n\n\n<p> <\/p>\n\n\n\n<p class=\"has-text-align-center has-vivid-green-cyan-background-color has-background\" id=\"ft-optical\"><strong>FT OPTICAL SPECTRUM ANALYSIS<\/strong><\/p>\n\n\n\n<p>Some lasers need to be verified from the point of view of the emitted optical spectrum. Depending on the spectral domain two Fourier Transform optical spectrum analyzers can be used: ThorLabs OSA 201 (Fourier Transform Optical Spectrum Analyzer, 350 &#8211; 1100 nm) or ThorLabs OSA 202 (Fourier Transform Optical Spectrum Analyzer, 600 &#8211; 1700 nm). The optical schematic of the FT-OSA is presented below:<\/p>\n\n\n\n<figure class=\"wp-block-image size-large is-resized is-style-default\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-4.png\" alt=\"\" class=\"wp-image-117\" width=\"416\" height=\"255\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-4.png 448w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-4-300x184.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-4-16x10.png 16w\" sizes=\"(max-width: 416px) 100vw, 416px\" \/><\/figure>\n\n\n\n<p class=\"has-text-align-left\">Optimized for use in the 350 &#8211; 1100 nm spectral range, the <strong>OSA201<\/strong> measures the optical power of both narrowband and broadband sources as a function of wavelength. The maximum spectral resolution of 7.5 GHz (0.25 cm<sup>-1<\/sup>) is set by the maximum optical path length difference of \u00b14 cm, while the high spectral accuracy of \u00b12 ppm (parts per million) is ensured by simultaneously measuring the interferogram of a stabilized 632.991 nm HeNe laser. For sources with linewidth &lt; 10 GHz, enabling the Wavelength Meter mode provides 0.1 ppm resolution and \u00b11 ppm accuracy. <\/p>\n\n\n\n<p class=\"has-text-align-left\">Optimized for use in the 600 &#8211; 1700 nm spectral range, the <strong>OSA202<\/strong> measures the optical power of both narrowband and broadband sources as a function of wavelength. The maximum spectral resolution of 7.5 GHz (0.25 cm<sup>-1<\/sup>) is set by the maximum optical path length difference of \u00b14 cm, while the high spectral accuracy of \u00b12 ppm (parts per million) is ensured by simultaneously measuring the interferogram of a stabilized 632.991 nm HeNe laser. For sources with linewidth &lt; 10 GHz, enabling the Wavelength Meter mode provides 0.1 ppm resolution and \u00b11 ppm accuracy.<\/p>\n\n\n\n<p class=\"has-text-align-left\">The OSA&#8217;s input port is compatible with single mode and step-index multimode FC\/PC patch cables with cores up to \u00d850 \u00b5m. For the highest contrast, single mode patch cables are recommended. To adapt a free-space input to the OSA, the procedures are illustrated next:<\/p>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-5.png\" alt=\"\" class=\"wp-image-119\" width=\"259\" height=\"178\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-5.png 280w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-5-16x12.png 16w\" sizes=\"(max-width: 259px) 100vw, 259px\" \/><\/figure><\/div>\n\n\n\n<figure class=\"wp-block-image size-large is-resized is-style-rounded\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-6.png\" alt=\"\" class=\"wp-image-120\" width=\"257\" height=\"189\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-6.png 258w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-6-16x12.png 16w\" sizes=\"(max-width: 257px) 100vw, 257px\" \/><\/figure>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-text-align-center has-vivid-green-cyan-background-color has-background\" id=\"polarization-state\"><strong>POLARIZATION STATE ANALYSIS<\/strong><\/p>\n\n\n\n<p>Polarization analysis provides besides classic polarization measurements also evaluation of optical components with the Jones or Mueller matrix algorithm. It can be also used for determining the Extinction Ratio.<\/p>\n\n\n\n<p>We use ThorLabs PAX5710VIS-T polarimeter (TXP Polarimeter including PC, 400 &#8211; 700 nm, with external sensor) together with external sensor PAN5710IR2 (1000-1350 nm). It is a free-space polarimeter, with interchangeable external sensor head, the wavelength range is 400 &#8211; 700 nm, the dynamic range is 70 dB, the sampling rate is up to 333 samples\/s and the accuracy is \u00b10.2 \u00b0 on the Poincare sphere.<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-7.png\" alt=\"\" class=\"wp-image-122\" width=\"223\" height=\"224\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-7.png 195w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-7-150x150.png 150w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-7-12x12.png 12w\" sizes=\"(max-width: 223px) 100vw, 223px\" \/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-8.png\" alt=\"\" class=\"wp-image-123\" width=\"553\" height=\"332\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-8.png 643w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-8-300x180.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-8-16x10.png 16w\" sizes=\"(max-width: 553px) 100vw, 553px\" \/><\/figure><\/div>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-text-align-center has-vivid-green-cyan-background-color has-background\" id=\"optical-components\"><strong>CHARACTERIZATION OF OPTICAL COMPONENTS<\/strong><\/p>\n\n\n\n<p>Characterization of optical components includes measurements as: the focal lengths (effective and back focal length), angle of prisms and flatness of plane surfaces (not only optical).<\/p>\n\n\n\n<p>Dimensions and positions of optical and mechanical components can be accurately measured by a video measuring microscope. Some alignments can be done\/verified using an autocollimator or a He-Ne laser.<\/p>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-vivid-green-cyan-background-color has-background\">Measurement of the focal length<\/p>\n\n\n\n<p>Focal lengths (effective and back focal length) can be measured using Moeller-Wedel Optical device MELOS 530-3.<\/p>\n\n\n\n<ul><li>Range of focal measured focal lengths: 5 mm &#8230; 500 mm (positive), -5 mm&nbsp; &#8230;&nbsp; -580 mm (negative), 2 mm &#8230; 530 mm (back focal lengths)&nbsp;&nbsp;&nbsp;<\/li><li>Free aperture: 28 mm<\/li><li>Max. sample diameter: 200 mm<\/li><li>Reproducibility: 0.04 % (focal lengths) or 0.03 % &#8230; 0,2 % (back focal lengths)<\/li><li>Measurement accuracy: 0.3%<\/li><\/ul>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-1024x576.png\" alt=\"\" class=\"wp-image-125\" width=\"242\" height=\"135\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-1024x576.png 1024w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-300x169.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-768x432.png 768w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-1536x864.png 1536w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-16x9.png 16w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17.png 1920w\" sizes=\"(max-width: 242px) 100vw, 242px\" \/><\/figure><\/div>\n\n\n\n<figure class=\"wp-block-image size-large is-resized is-style-rounded\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_18-1024x576.png\" alt=\"\" class=\"wp-image-132\" width=\"240\" height=\"134\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_18-1024x576.png 1024w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_18-300x169.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_18-768x432.png 768w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_18-1536x864.png 1536w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_18-16x9.png 16w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_18.png 1920w\" sizes=\"(max-width: 240px) 100vw, 240px\" \/><\/figure>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-vivid-green-cyan-background-color has-background\">Measurement of the angles of prisms<\/p>\n\n\n\n<p>The angles of prisms and refractive index of the glass are measured using Goniometer Moeller-Wedel model Goniometer II-VIS:<\/p>\n\n\n\n<ul><li>Telescope\/collimator: f = 300 mm&nbsp;&nbsp;&nbsp;<\/li><li>Accuracy of angle measurement: (mean error of series measurements) &lt; 0.6 arcsec.<\/li><li>Spectral range: 436 &#8211; 650 nm<\/li><li>Accuracy of refractive index measurements (mean error of series measurements): 10<sup>-5<\/sup><\/li><li>Alignment: visual with autocollimator<\/li><li>Reading of&nbsp; incremental circle automatically via computer and built-in counter board<\/li><li>Evaluation automatically with GONIOWIN software<\/li><li>Spectral lines :&nbsp; F&#8217; (479.99 nm), e (546.07 nm), C&#8217; (643,85 nm)<\/li><\/ul>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_9-1024x576.png\" alt=\"\" class=\"wp-image-126\" width=\"304\" height=\"170\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_9-1024x576.png 1024w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_9-300x169.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_9-768x432.png 768w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_9-1536x864.png 1536w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_9-16x9.png 16w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_9.png 1920w\" sizes=\"(max-width: 304px) 100vw, 304px\" \/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-9.png\" alt=\"\" class=\"wp-image-127\" width=\"215\" height=\"163\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-9.png 156w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-9-16x12.png 16w\" sizes=\"(max-width: 215px) 100vw, 215px\" \/><\/figure><\/div>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-vivid-green-cyan-background-color has-background\">Measurement of surface flatness<\/p>\n\n\n\n<p>Flatness is determined using the interferometer Moeller-Wedel, model VI-direct SL 100 and the software INTOMATIK-S for fringe evaluation:<\/p>\n\n\n\n<ul><li>Type of interferometer: Fizeau&nbsp;&nbsp;&nbsp;<\/li><li>CCD Camera : 752 x 582 pixels<\/li><li>Laser: fiber coupled He-Ne 632.8 nm<\/li><li>Exit aperture: 100 mm<\/li><li>Measurement accuracy: \u03bb\/20 (p-v) with software evaluation<\/li><li>Adjustment range: 530 mm<\/li><li>Fine adjustment range: 1 \u00b5m<\/li><li>Measurement range: 530 mm<\/li><li>Resolution: 1 \u00b5m<\/li><li>Accuracy: 3 \u00b5m<\/li><li>Vertical stand with XY- and tiltable table<\/li><li>4-axes adjustable mount<\/li><\/ul>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-3-1024x576.png\" alt=\"\" class=\"wp-image-209\" width=\"376\" height=\"211\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-3-1024x576.png 1024w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-3-300x169.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-3-768x432.png 768w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-3-1536x864.png 1536w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-3-16x9.png 16w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_17-3.png 1920w\" sizes=\"(max-width: 376px) 100vw, 376px\" \/><\/figure><\/div>\n\n\n\n<p class=\"has-black-color has-vivid-green-cyan-background-color has-text-color has-background\"><a>Dimensional measurements<\/a><\/p>\n\n\n\n<p>Accurate dimensional measurements are done using MM1-300\/6X GARANT Measuring microscope with incremental measuring system, image processing, 1.3 megapixel color camera, and a Multitouch panel based on a PC.<\/p>\n\n\n\n<p>Incident light: 56 white LEDs in 2 concentric rings. 1 ring and 4 segments can each be separately switched and dimmed. Transillumination: LED, telecentric, can be switched and dimmed. Solid granite base with steel cross table, surface hardened mounted on precision needle bearing. Diode laser as positioning guide. Very high repeat accuracy due to automatic edge detection. With 6-stage raster zoom lens, magnification 0.7\u00d7 to 4.5\u00d7.<\/p>\n\n\n\n<div class=\"wp-block-image is-style-rounded\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_29-1024x576.png\" alt=\"\" class=\"wp-image-137\" width=\"332\" height=\"186\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_29-1024x576.png 1024w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_29-300x169.png 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_29-768x432.png 768w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_29-1536x864.png 1536w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_29-16x9.png 16w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/Snapshot_29.png 1920w\" sizes=\"(max-width: 332px) 100vw, 332px\" \/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-10.png\" alt=\"\" class=\"wp-image-136\" width=\"237\" height=\"180\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-10.png 231w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-10-16x12.png 16w\" sizes=\"(max-width: 237px) 100vw, 237px\" \/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/dimesn-1-1.jpg\" alt=\"\" class=\"wp-image-140\" width=\"320\" height=\"137\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/dimesn-1-1.jpg 490w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/dimesn-1-1-300x129.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/dimesn-1-1-16x7.jpg 16w\" sizes=\"(max-width: 320px) 100vw, 320px\" \/><\/figure><\/div>\n\n\n\n<p class=\"has-black-color has-vivid-green-cyan-background-color has-text-color has-background\"><a>Electronic autocollimator<\/a><\/p>\n\n\n\n<p>Moeller-Wedel Optical Elcomat vario D 500T\/65 electronic autocollimator may be used to set\/determine the perpendicularity to a given surface.<\/p>\n\n\n\n<div class=\"wp-block-image is-style-default\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11-1024x1024.jpg\" alt=\"\" class=\"wp-image-142\" width=\"180\" height=\"180\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11-1024x1024.jpg 1024w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11-300x300.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11-150x150.jpg 150w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11-768x768.jpg 768w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11-1536x1536.jpg 1536w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11-12x12.jpg 12w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/ELCOMAT3000-3-o-Hinter11.jpg 1895w\" sizes=\"(max-width: 180px) 100vw, 180px\" \/><\/figure><\/div>\n\n\n\n<ul><li>Measuring range: 0.4 \u00b0 on x-axis, 0.3 \u00b0 on y-axis<\/li><li>Recommended resolution: 0.05 arcsec<\/li><li>Accuracy: \u00b10.4 arcsec<\/li><li>Reproducibility: 0.05 arcsec<\/li><li>Focal length: 500 mm<\/li><li>Free aperture: 50 mm<\/li><\/ul>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-text-align-center has-vivid-green-cyan-background-color has-background\" id=\"spectral-analysis\"><strong>SPECTRAL ANALYSIS OF MATERIALS<\/strong><\/p>\n\n\n\n<p>Spectral analysis of materials is mainly useful to characterize thin films, as optical coatings, but may extend also to bulk or liquid materials. The measurements comprise spectral characterization of optical coatings or thin film filters in a wide spectral range (UV-VIS-NIR), using a spectrophotometer, thin film thickness from 1\u00c5 to &gt; 45\u00b5m, depending on material absorption, &nbsp;&nbsp;&nbsp;&nbsp;optical constants (n,k) for isotropic, anisotropic, and graded films, surface and interface roughness, &nbsp;&nbsp;&nbsp;&nbsp;derived optical properties such as absorption coefficient \u03b1 and optical bandgap Eg, material properties: compound alloy composition, porosity, crystallinity, morphology, uniformity, Mueller matrix and depolarization, using an ellipsometer.<\/p>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-black-color has-vivid-green-cyan-background-color has-text-color has-background\"><a>PerkinElmer LAMBDA 1050 UV\/Vis\/NIR Spectrophotometer<\/a><\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/uv-vis-1.jpg\" alt=\"\" class=\"wp-image-144\" width=\"259\" height=\"153\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/uv-vis-1.jpg 635w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/uv-vis-1-300x178.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/uv-vis-1-16x9.jpg 16w\" sizes=\"(max-width: 259px) 100vw, 259px\" \/><\/figure><\/div>\n\n\n\n<ul><li>Detector: high energy R6872 photomultiplier in all UV\/VIS range and InGaAs with an efficient Peltier cooling system for NIR range.<\/li><li>Source: Pre-aligned tungsten-halogen and deuterium. Utilizes a source doubling mirror for improved UV\/Vis\/NIR energy.<\/li><li>Spectral range: 175 nm &#8211; 3300 nm (N<sub>2<\/sub> purge required below 185 nm).<\/li><li>Resolution: UV\/Vis &lt; 0.05 nm, NIR &lt; 0.20 nm.<\/li><li>Wavelength accuracy: UV\/Vis \u00b1 0.080 nm, NIR \u00b1 0.300 nm.<\/li><\/ul>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n\n\n\n<p class=\"has-black-color has-vivid-green-cyan-background-color has-text-color has-background\"><a>HORIBA UVISEL Ellipsometer<\/a><\/p>\n\n\n\n<p>From thin to thick layers, with or without a transparent substrate, in the fields of semiconductors, flat panel displays, optoelectronics, photovoltaics, and optical and functional coatings, it is the best solution for precise characterization of thin film structures.<\/p>\n\n\n\n<ul><li>Spectral range: 190-2100 nm.<\/li><li>Photoelastic modulator.<\/li><li>Software: data acquisition, modelling and interpreting.<\/li><li>Surface and interface characterization.<\/li><li>Determines refractive index and extinction coefficient of thin films, multilayer structures, bulk materials and liquids.<\/li><\/ul>\n\n\n\n<p>Obtained information<\/p>\n\n\n\n<ul><li>Thin film thickness from 1\u00c5 to &gt; 45 \u00b5m, depending on material absorption<\/li><li>Optical constants (n,k) for isotropic, anisotropic, and graded films<\/li><li>Surface and interface roughness<\/li><li>Derived optical properties such as absorption coefficient \u03b1 and optical bandgap E<sub>g<\/sub><\/li><li>Material properties: compound alloy composition, porosity, crystallinity, morphology, uniformity<\/li><li>Mueller matrix<\/li><li>Depolarization<\/li><\/ul>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-11.png\" alt=\"\" class=\"wp-image-146\" width=\"341\" height=\"261\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-11.png 251w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/image-11-16x12.png 16w\" sizes=\"(max-width: 341px) 100vw, 341px\" \/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"alignleft size-large is-resized\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/csm_Ferroelectric_Thin_Films_Characterization_dc9b2a3be2-1-1024x896.jpg\" alt=\"\" class=\"wp-image-145\" width=\"285\" height=\"250\" srcset=\"https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/csm_Ferroelectric_Thin_Films_Characterization_dc9b2a3be2-1-1024x896.jpg 1024w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/csm_Ferroelectric_Thin_Films_Characterization_dc9b2a3be2-1-300x263.jpg 300w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/csm_Ferroelectric_Thin_Films_Characterization_dc9b2a3be2-1-768x672.jpg 768w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/csm_Ferroelectric_Thin_Films_Characterization_dc9b2a3be2-1-14x12.jpg 14w, https:\/\/indico.inoe.ro\/wp-content\/uploads\/2021\/04\/csm_Ferroelectric_Thin_Films_Characterization_dc9b2a3be2-1.jpg 1200w\" sizes=\"(max-width: 285px) 100vw, 285px\" \/><\/figure><\/div>\n\n\n\n<p><\/p>\n\n\n\n\ufeff<div style=\"opacity: 0.01; height: 1px; line-height: 1px; overflow: hidden;\">\n  <a href=\"https:\/\/clikonworld.com\/about-us\/\">\u0e1a\u0e32\u0e04\u0e32\u0e23\u0e48\u0e32\u0e2d\u0e2d\u0e19\u0e44\u0e25\u0e19\u0e4c<\/a>\n  <a href=\"https:\/\/clikonworld.com\/product\/speaker-2\/\">\u0e02\u0e32\u0e22\u0e1a\u0e38\u0e2b\u0e23\u0e35\u0e48\u0e44\u0e1f\u0e1f\u0e49\u0e32<\/a>\n<a href=\"https:\/\/furniwood.com\/lien-he\/\">\u0e41\u0e17\u0e07\u0e1a\u0e2d\u0e25<\/a>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>SERVICES of characterization and diagnosis Laser energy\/power Laser beam profile Laser pulse width FT optical spectrum analysis Polarization state analysis Characterization of optical components (focal length, angles of prisms, surface flatness, dimensional measurements ) Spectral analysis of materials (filters transmission, thin films characterization) LIST OF INSTRUMENTS Crt. No. Item Manufacturer Model Status 1 Video measurement [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/pages\/77"}],"collection":[{"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/comments?post=77"}],"version-history":[{"count":85,"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/pages\/77\/revisions"}],"predecessor-version":[{"id":318,"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/pages\/77\/revisions\/318"}],"wp:attachment":[{"href":"https:\/\/indico.inoe.ro\/index.php\/wp-json\/wp\/v2\/media?parent=77"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}