{"id":164,"date":"2014-11-12T23:47:24","date_gmt":"2014-11-13T09:47:24","guid":{"rendered":"http:\/\/www.eaobservatory.org\/jcmt\/?page_id=164"},"modified":"2026-01-29T10:02:44","modified_gmt":"2026-01-29T20:02:44","slug":"harp","status":"publish","type":"page","link":"https:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/harp\/","title":{"rendered":"350 GHz band: HARP"},"content":{"rendered":"<p><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2015\/01\/harp1_lowres.png\"><img loading=\"lazy\" class=\"alignnone size-full wp-image-887\" style=\"margin: 10px; float: right;\" src=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2015\/01\/harp1_lowres.png\" alt=\"harp1_lowres\" width=\"392\" height=\"524\" srcset=\"https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2015\/01\/harp1_lowres.png 392w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2015\/01\/harp1_lowres-224x300.png 224w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2015\/01\/harp1_lowres-112x150.png 112w\" sizes=\"(max-width: 392px) 100vw, 392px\" \/><\/a><\/p>\n<p style=\"text-align: left;\">HARP (Heterodyne Array Receiver Program) is a <a href=\"http:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/dual-and-single-sideband\/\">Single Sideband<\/a> (SSB) array receiver with 16 SIS mixers. HARP can be tuned between 325 and 375 GHz and has a instantaneous bandwidth of ~2 GHz and an Intermediate Frequency (IF) of 5 GHz. The unwanted sideband is terminated on a 20 K load inside the Dewar. The mixers are called receptors and arranged in a 4&#215;4 configuration. The different receptors are separated by 30&#8243; and named H00, H01 &#8230; H15. HARP was designed and built by <a href=\"http:\/\/www.mrao.cam.ac.uk\/\">University of Cambridge<\/a> in collaboration with different other groups.<\/p>\n<p style=\"text-align: left;\">The half power beam width of each receptor is approximately 14 arcsec. One of the four center receptors is used for <a href=\"http:\/\/www.eaobservatory.org\/jcmt\/observing\/pointing\/\">pointing and focus<\/a> observations and for pointed observations. This is called the tracking receptor, currently it is H05.<\/p>\n<p style=\"text-align: left;\">At 345GHz the <a href=\"http:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/calibration\/harp-planets\/\">main beam efficiency<\/a> \u03b7<sub>mb<\/sub> for HARP is 0.64 and \u03b7<sub>fss<\/sub> (measured on the Moon in 2006) is 0.77. In April 2015 this efficiency was 0.75.<br \/>\nThe aperture efficiency \u03b7<sub>a<\/sub> for HARP is 0.52.<\/p>\n<p style=\"text-align: left;\">Together with the spectrometer <a href=\"http:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/acsis\/\">ACSIS<\/a>, HARP is designed to rapidly map large areas. The telescope is scanning in a raster pattern and spectra are read out at a high enough rate to avoid smearing the map. By using the short integration times made available by ACSIS, a map can be done quickly. Combining maps obtained by <a href=\"http:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/observing-modes\/harp-rasters\/\">scanning<\/a> in different ways improves the map uniformity in sensitivity and calibration. It is thus preferable to make several fast maps than one slow one.<\/p>\n<p>Note that <a href=\"https:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/calibration\/strong-continuum-het\/\">special considerations must be taken into account when observing targets with a strong continuum<\/a> such as the moon, the Sun, or planetary atmospheres.<\/p>\n<p style=\"text-align: left;\">Detailed information about this receiver is given by <a href=\"http:\/\/cdsads.u-strasbg.fr\/abs\/2009MNRAS.399.1026B\">Buckle, J.V., Hills, R.E., Smith, H., et al., 2009, MNRAS 399, 1026<\/a>.<\/p>\n<p style=\"text-align: left;\">The figure below shows the atmospheric transmission for the tuning range of HARP for <a href=\"http:\/\/www.eaobservatory.org\/jcmt\/observing\/weather\/\">weather bands 1 to 4<\/a>, taken from <a href=\"http:\/\/cdsads.u-strasbg.fr\/abs\/2009MNRAS.399.1026B\">Buckle et al.<\/a>. The frequencies of some frequently observed molecular transitions are indicated.<\/p>\n<p style=\"text-align: left;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2015\/01\/harp_transmission_buckle.gif\"><img class=\"alignnone size-full wp-image-959\" src=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2015\/01\/harp_transmission_buckle.gif\" alt=\"harp_transmission_buckle\" width=\"350\" \/><\/a><\/p>\n<p>The figure below shows the receiver temperature T<sub>rx<\/sub> of the tracking receptor H05 of HARP as a function of sky frequency for observations made in 2014. Observations made in the Lower Side Band (LSB) are indicated in purple; observations made in the Upper Side Band (USB) in blue. The drawn line gives the median T<sub>rx<\/sub> values which are used in the heterodyne time estimator (HITEC).<\/p>\n<p><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/HARP_H05_avg_trx_vs_freq.png\"><img loading=\"lazy\" class=\"alignnone size-full wp-image-452\" src=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/HARP_H05_avg_trx_vs_freq.png\" alt=\"HARP_H05_avg_trx_vs_freq\" width=\"413\" height=\"413\" srcset=\"https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/HARP_H05_avg_trx_vs_freq.png 413w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/HARP_H05_avg_trx_vs_freq-150x150.png 150w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/HARP_H05_avg_trx_vs_freq-300x300.png 300w\" sizes=\"(max-width: 413px) 100vw, 413px\" \/><\/a><\/p>\n<p>The following table below gives links to figures with the receiver temperature T<sub>rx<\/sub> as a function of sky frequency for 14 of the working receptors from data obtained in 2014, as well as the average T<sub>rx<\/sub> at 345.796GHz.<\/p>\n<table style=\"width: 33.2071%;\" width=\"674\">\n<tbody>\n<tr>\n<td style=\"width: 13.674%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h12.png\">H12<\/a><br \/>\n160K<\/td>\n<td style=\"width: 12.7793%;\">H13<\/td>\n<td style=\"width: 14.3972%;\">H14*<\/td>\n<td style=\"width: 15.2901%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h15.png\">H15<\/a><br \/>\n175K<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 13.674%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h11.png\">H11<\/a><br \/>\n170K<\/td>\n<td style=\"width: 12.7793%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h10.png\">H10<\/a><br \/>\n152K<\/td>\n<td style=\"width: 14.3972%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h09.png\">H09<\/a><br \/>\n105K<\/td>\n<td style=\"width: 15.2901%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h08.png\">H08<\/a><br \/>\n143K<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 13.674%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h04.png\">H04<\/a><br \/>\n118K<\/td>\n<td style=\"width: 12.7793%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h05.png\">H05<\/a><br \/>\n110K<\/td>\n<td style=\"width: 14.3972%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h06.png\">H06<\/a><br \/>\n182K<\/td>\n<td style=\"width: 15.2901%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h07.png\">H07<\/a><br \/>\n112K<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 13.674%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h03.png\">H03<\/a><br \/>\n185K<\/td>\n<td style=\"width: 12.7793%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h02.png\">H02<\/a><br \/>\n125K<\/td>\n<td style=\"width: 14.3972%;\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h01.png\">H01<\/a><br \/>\n148K<\/td>\n<td style=\"width: 15.2901%;\"><em><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2014\/11\/harp_trx_h00.png\">H00*<\/a><\/em><br \/>\n<em>127K*<br \/>\n<\/em><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>*H00, H02, H14 and H15 are not currently operational (January 2026). H13 and H14 were not operational in 2014 when the data for the table was obtained..<\/p>\n<p>HARP is located in the right Nasmyth focus of the JCMT. The orientation of the array on the sky is determined by the <a href=\"http:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/harp\/k-mirror\/\">K-mirror<\/a>. The software determines which of the four possible K-mirror angles (with the array in a N-S\/E-W, or user specified direction) allows the longest tracking time.<\/p>\n<h3>Important Notes\/Current status<\/h3>\n<ul>\n<li>H05 is used as the pointing receptor.<\/li>\n<li>12 of the 16 receptors (detectors) are operational: H00, H02, H14 and H15 are not operational (Jan 2026).<\/li>\n<\/ul>\n<p><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/03\/harp_footprint_post2019.jpg\"><img loading=\"lazy\" class=\"size-medium wp-image-11805 aligncenter\" src=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/03\/harp_footprint_post2019-251x300.jpg\" alt=\"\" width=\"251\" height=\"300\" srcset=\"https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/03\/harp_footprint_post2019-251x300.jpg 251w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/03\/harp_footprint_post2019-856x1024.jpg 856w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/03\/harp_footprint_post2019-768x919.jpg 768w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/03\/harp_footprint_post2019-125x150.jpg 125w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/03\/harp_footprint_post2019.jpg 1192w\" sizes=\"(max-width: 251px) 100vw, 251px\" \/><\/a><\/p>\n<ul>\n<li><span class=\"comment\">Receptor H04 and H13 have bad baselines at and below 330 GHz<\/span><\/li>\n<li>PIs with projects involving jiggle maps on extended sources may wish to review the central pointings and\/or K-mirror orientations in their MSBs. The image below is a recent observation for a graphical example of the relative positions of the nonfunctional receptors (rotated 90 degrees anticlockwise to the table above).<\/li>\n<\/ul>\n<p><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023.jpg\"><img loading=\"lazy\" class=\"size-medium wp-image-12901 aligncenter\" src=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023-300x297.jpg\" alt=\"\" width=\"300\" height=\"297\" srcset=\"https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023-300x297.jpg 300w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023-1024x1012.jpg 1024w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023-150x148.jpg 150w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023-768x759.jpg 768w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023-1536x1519.jpg 1536w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2023\/07\/HARP-footprint-2023.jpg 1588w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<ul>\n<li>Sensitivity variations creating striping &#8211; worst at 13CO\/C18O<\/li>\n<li>HARP data can be affected by <a href=\"https:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/ozone-lines\/\">ozone lines<\/a><\/li>\n<\/ul>\n<p style=\"text-align: right;\">&#8211; page updated 20230707<\/p>\n","protected":false},"excerpt":{"rendered":"<p>HARP (Heterodyne Array Receiver Program) is a Single Sideband (SSB) array receiver with 16 SIS mixers. HARP can be tuned between 325 and 375 GHz and has a instantaneous bandwidth of ~2 GHz and an Intermediate Frequency (IF) of 5 GHz. The unwanted sideband is terminated on a 20 K\u2026 <a class=\"continue-reading-link\" href=\"https:\/\/www.eaobservatory.org\/jcmt\/instrumentation\/heterodyne\/harp\/\">Continue reading<\/a><\/p>\n","protected":false},"author":3,"featured_media":0,"parent":162,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/164"}],"collection":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/comments?post=164"}],"version-history":[{"count":76,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/164\/revisions"}],"predecessor-version":[{"id":13483,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/164\/revisions\/13483"}],"up":[{"embeddable":true,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/162"}],"wp:attachment":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/media?parent=164"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}