{"id":12122,"date":"2023-11-25T12:09:06","date_gmt":"2023-11-25T11:09:06","guid":{"rendered":"https:\/\/www.bramjacobse.nl\/wordpress\/?p=12122"},"modified":"2023-11-25T12:17:10","modified_gmt":"2023-11-25T11:17:10","slug":"a-semiconductor-laser-for-information-read-out-cql10","status":"publish","type":"post","link":"https:\/\/www.bramjacobse.nl\/wordpress\/?p=12122","title":{"rendered":"A semiconductor laser for information read-out &#8211; CQL10"},"content":{"rendered":"<h4><strong><i>A semiconductor laser for information read-out <\/i><\/strong><\/h4>\n<h4><strong><i><span style=\"color: #3366ff;\"><a style=\"color: #3366ff;\" href=\"https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/PTechReview-39-1980-037-1.pdf\">PTechReview-39-1980-037<\/a><\/span><\/i><\/strong><\/h4>\n<p><i>J. C. J. Finek, H. J. M. van der Laak and J. T. Schrama<\/i><\/p>\n<p><i>Semiconductor lasers only became efficient lasers when they were made in theform of &#8216;double<\/i><\/p>\n<p><i>heteroj unctions&#8217;: an active layer in which the laser radiation is produced, between two layers of<\/i><\/p>\n<p><i>another composition. In the first lasers of this type the active layer consisted of GaAs. The laser<\/i><\/p>\n<p><i>radiation from this m\u00e0terial has a wavelength of about 890 nm. Since then the development of<\/i><\/p>\n<p><i>semiconductor lasers has moved simultaneously in two opposing directions. On the one hand<\/i><\/p>\n<p><i>there is a clear needfor laser radiation at longer wavelengthsfor optical communication by glass<\/i><\/p>\n<p><i>fibres, since Rayleigh scattering in the fibres is lower at these longer wavelengths. On the other<\/i><\/p>\n<p><i>hand there is a need for semiconductor lasers that produce radiation at shorter wavelengths for<\/i><\/p>\n<p><i>applications in which the radiated power is concentrated in the smallest possible area. This<\/i><\/p>\n<p><i>article describes a laserof this shorter- wavelength type that Philips isputting on the market. The<\/i><\/p>\n<p><i>wavelength of the emitted radiation is 780 nm.<\/i><\/p>\n<p>&nbsp;<\/p>\n<p><strong><i>Introduction<\/i><\/strong><\/p>\n<p><i>The information on a &#8216;VLP&#8217; disc is recorded in a <\/i><i>spiral track 25 km long, with a pitch of 1.66 urn and<\/i><\/p>\n<p><i>consisting of pits 0.6 urn wide and 0.12 urn deep. This <\/i><i>form of information storage also has its attractions<\/i><\/p>\n<p><i>for applications such as audio discs and data filing, <\/i><i>mainly because it can provide a very high information<\/i><\/p>\n<p><i>density &#8211; of the order of one bit per um&#8221;, Philips are <\/i><i>active in the development of such systems (&#8216;Compact<\/i><\/p>\n<p><i>Disc&#8217;; &#8216;DOR&#8217; <\/i><i>= <\/i><i>Digital Optical Recording). <\/i><i>The information stored in this way is read out by<\/i><\/p>\n<p><i>scanning the track of pits with an optical system; a <\/i><i>photodiode converts the intensity variations of the reflected<\/i><\/p>\n<p><i>light into an electrical signal <\/i><i>(fig. 1): <\/i><i>The <\/i><i>requirements imposed on the light source <\/i><i>(L) <\/i><i>for this<\/i><\/p>\n<p><i>system can only be met by lasers: the radiation must <\/i><i>have a radiation density of about 2500 W per cm<\/i><i>2 <\/i><i>per<\/i><\/p>\n<p><i>steradian for a detected signal with an acceptable <\/i><i>signal-to-noise ratio to be generated by the variations<\/i><\/p>\n<p><i>in reflection from an area of about 1 <\/i><i>Ilm<\/i><i>2 <\/i><i>[11. <\/i><i>The <\/i><i>light source in the &#8216;VLP&#8217; system is at present a <\/i><i>helium-neon laser <\/i><i>[21<\/i><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-12121\" src=\"https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser.jpg\" alt=\"\" width=\"1280\" height=\"701\" srcset=\"https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser.jpg 1280w, https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser-300x164.jpg 300w, https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser-800x438.jpg 800w, https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser-768x421.jpg 768w, https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser-720x394.jpg 720w, https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser-520x285.jpg 520w, https:\/\/www.bramjacobse.nl\/wordpress\/wp-content\/uploads\/2023\/11\/CQL10_Laser-320x175.jpg 320w\" sizes=\"auto, (max-width: 1280px) 100vw, 1280px\" \/><\/p>\n","protected":false},"excerpt":{"rendered":"<p>A semiconductor laser for information read-out PTechReview-39-1980-037 J. C. J. Finek, H. J. M. van der Laak and J. T. Schrama Semiconductor lasers only became efficient lasers when they were made in theform of&#46;&#46;&#46;<\/p>\n","protected":false},"author":1,"featured_media":12121,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[121],"tags":[],"class_list":["post-12122","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-philips"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.5 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>A semiconductor laser for information read-out - CQL10 - Bram Jacobse<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.bramjacobse.nl\/wordpress\/?p=12122\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"A semiconductor laser for information read-out - CQL10 - Bram Jacobse\" \/>\n<meta property=\"og:description\" content=\"A semiconductor laser for information read-out PTechReview-39-1980-037 J. 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