{"id":10990,"date":"2025-09-25T15:34:18","date_gmt":"2025-09-25T13:34:18","guid":{"rendered":"https:\/\/deep-space-astronomy.ch\/?post_type=product&#038;p=10990"},"modified":"2025-11-18T17:37:00","modified_gmt":"2025-11-18T16:37:00","slug":"ritchey-chretien-ts-optics-gso-8","status":"publish","type":"product","link":"https:\/\/deep-space-astronomy.ch\/en\/product\/ritchey-chretien-ts-optics-gso-8\/","title":{"rendered":"Ritchey-Chr\u00e9tien TS-Optics GSO 8\u2033"},"content":{"rendered":"<h3 style=\"text-align: center;\">TS-Optics GSO 8\u2033 RC Pro 203\/1624 - The benchmark Ritchey-Chr\u00e9tien astrograph<\/h3>\n<p>Visit <strong>Ritchey-Chr\u00e9tien TS-Optics GSO 8\u2033 RC (203 mm, 1624 mm, f\/8)<\/strong> is designed for high-resolution astrophotography, but is also perfectly suited to visual observation. With its hyperbolic quartz mirrors (<em>fused silica<\/em>) with 94 % reflectivity and its ventilated open tube, it guarantees stable focus, bright images and fine stars across the entire field.<\/p>\n<h3>Highlights<\/h3>\n<ul>\n<li><strong>Genuine Ritchey-Chr\u00e9tien<\/strong> naturally corrected, coma-free field.<\/li>\n<li><strong>Quartz mirrors<\/strong> focus stability even at varying temperatures.<\/li>\n<li><strong>Reflectivity 94 %<\/strong> direct gain in brightness and contrast.<\/li>\n<li><strong>Open tube + ventilation<\/strong> rapid cooling, better contrast.<\/li>\n<li><strong>Generous backfocus (\u2248159 mm)<\/strong> ideal for correctors, gearboxes, OAGs and filter wheels.<\/li>\n<li><strong>No shifting<\/strong> : primary fixed, developed by <em>focuser Monorail 2\u2033<\/em>.<\/li>\n<li><strong>Two Vixen bars<\/strong> simple mounting of guidescope or piggyback camera.<\/li>\n<\/ul>\n<h3>Astrophotography<\/h3>\n<p>The 8\u2033 RC delivers <strong>sharper, brighter astrophotos<\/strong> than comparable SCT or Maksutov sensors. Without correctors, sensors up to <strong>APS-C<\/strong> are perfectly usable. For full format, an RC corrector is recommended. With the <strong>CCD47 reducer 0.67\u00d7<\/strong>the focal length increases from 1624 mm to \u22481088 mm and the f\/8 ratio to <strong>f\/5,36<\/strong>which means twice as fast installation times.<\/p>\n<h3>The Monorail 2\u2033 focuser<\/h3>\n<p>More rigid than a classic Crayford, the <strong>Monorail 2\u2033<\/strong> combines fluidity and stability: solid stainless steel slide, no tilt when locked, 360\u00b0 rotation for framing, 1:10 gear ratio for precise focusing, graduation for easy focus retrieval, motorization compatibility.<\/p>\n<h3>Why RC rather than SCT?<\/h3>\n<ul>\n<li><strong>No Schmidt blade<\/strong> less susceptible to fogging, maximum transmission (including IR).<\/li>\n<li><strong>Design-corrected field<\/strong> Fine stars in the center and on the edges.<\/li>\n<li><strong>No residual aberration<\/strong> no permanent corrector in the optical path.<\/li>\n<li><strong>No mirror shift<\/strong> : fixed primary \u2192 maximum stability in long exposure imaging.<\/li>\n<\/ul>\n<h3>Technical specifications<\/h3>\n<table border=\"1\" cellspacing=\"0\" cellpadding=\"6\">\n<tbody>\n<tr>\n<td><strong>Optical design<\/strong><\/td>\n<td>Ritchey-Chr\u00e9tien (hyperbolic mirrors)<\/td>\n<\/tr>\n<tr>\n<td><strong>Opening<\/strong><\/td>\n<td>203 mm (8\u2033)<\/td>\n<\/tr>\n<tr>\n<td><strong>Focal length<\/strong><\/td>\n<td>1624 mm<\/td>\n<\/tr>\n<tr>\n<td><strong>Ratio f\/<\/strong><\/td>\n<td>f\/8 (\u2248 f\/5.36 with reducer 0.67\u00d7)<\/td>\n<\/tr>\n<tr>\n<td><strong>Theoretical resolution<\/strong><\/td>\n<td>0,58\u2033<\/td>\n<\/tr>\n<tr>\n<td><strong>Mirrors<\/strong><\/td>\n<td>Quartz, reflectivity 94 %<\/td>\n<\/tr>\n<tr>\n<td><strong>Backfocus<\/strong><\/td>\n<td>\u2248254 mm from back of tube \/ 159 mm from 2\u2033 runner<\/td>\n<\/tr>\n<tr>\n<td><strong>Secondary obstruction<\/strong><\/td>\n<td>85 mm<\/td>\n<\/tr>\n<tr>\n<td><strong>Focuser<\/strong><\/td>\n<td>2\u2033 double-speed monorail + 1.25\u2033 adapter<\/td>\n<\/tr>\n<tr>\n<td><strong>Connection thread<\/strong><\/td>\n<td>M90\u00d71<\/td>\n<\/tr>\n<tr>\n<td><strong>Dovetail<\/strong><\/td>\n<td>2 x 395 mm Vixen bars (GP)<\/td>\n<\/tr>\n<tr>\n<td><strong>Tube diameter<\/strong><\/td>\n<td>230 mm<\/td>\n<\/tr>\n<tr>\n<td><strong>Tube length<\/strong><\/td>\n<td>580 mm (with focuser)<\/td>\n<\/tr>\n<tr>\n<td><strong>Weight<\/strong><\/td>\n<td>\u22488.25 kg (+0.5 kg extension rings)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<h3>In the box<\/h3>\n<ul>\n<li>RC 8\u2033 f\/8 telescope (203\/1624)<\/li>\n<li>Focuser Monorail 2\u2033 (with 1.25\u2033 adapter)<\/li>\n<li>Two Vixen-style dovetail bars (GP)<\/li>\n<li>M90 extension rings<\/li>\n<li>Protective cap<\/li>\n<\/ul>\n<h3>In a nutshell<\/h3>\n<p>Visit <strong>TS-Optics GSO 8\u2033 RC Pro<\/strong> is a high-end, affordable solution for astrophotographers looking for a stable, bright, full-field corrected instrument. With its optional accessories (corrector, reducer, OAG, filter wheel), it can easily be upgraded to advanced, high-quality setups.<\/p>","protected":false},"excerpt":{"rendered":"<p>TS-Optics GSO 8&Prime; RC Pro 203\/1624 \u2013 L\u2019astrographe Ritchey-Chr\u00e9tien de r\u00e9f\u00e9rence Le Ritchey-Chr\u00e9tien TS-Optics GSO 8&Prime;\u00a0RC (203 mm, 1624 mm, f\/8) est con\u00e7u pour l\u2019astrophotographie haute r\u00e9solution, mais reste parfaitement adapt\u00e9 \u00e0 l\u2019observation visuelle. Avec ses miroirs hyperboliques en quartz (fused silica) \u00e0 94 % de r\u00e9flectivit\u00e9 et son tube ouvert ventil\u00e9, il garantit une [&hellip;]<\/p>\n","protected":false},"featured_media":10992,"comment_status":"open","ping_status":"closed","template":"","meta":[],"product_brand":[842],"product_cat":[392,750],"product_tag":[],"class_list":{"0":"post-10990","1":"product","2":"type-product","3":"status-publish","4":"has-post-thumbnail","6":"product_brand-ts-optics","7":"product_cat-telescopes_reflecteurs","8":"product_cat-ritchey-chretien","10":"first","11":"on_supplier","12":"taxable","13":"shipping-taxable","14":"purchasable","15":"product-type-simple"},"_links":{"self":[{"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/product\/10990","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/product"}],"about":[{"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/types\/product"}],"replies":[{"embeddable":true,"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/comments?post=10990"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/media\/10992"}],"wp:attachment":[{"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/media?parent=10990"}],"wp:term":[{"taxonomy":"product_brand","embeddable":true,"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/product_brand?post=10990"},{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/product_cat?post=10990"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/deep-space-astronomy.ch\/en\/wp-json\/wp\/v2\/product_tag?post=10990"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}