Engelhardsberg observatory

Comets By Designation (table is sortable)

info Nr. comet last observed thumbnail observations
  1 2P/Encke 08.09.2023

11
  2 4P/Faye 04.09.2021 6
  3 6P/d'Arrest 01.09.2021 3
  4 7P/Pons-Winnecke 15.04.2021 3
  5 8P/Tuttle 08.05.2021 1
  6 9P/Tempel 2016 6
  7 10P/Tempel 08.09.2021 5
  8 11P/Tempel-Swift-Linear 14.11.2020 1
9 12P/Pons-Brooks 07.03.2024 16
10 13P/Olbers 03.03.2024 4
  11 14P/Wolf 2017 1
  12 15P/Finlay 15.08.2021 6
  13 16P/Brooks 2014 1
  14 17P/Holmes 29.10.2021 6
  15 19P/Borrelly 20.03.2022 4
  16 21P/Giacobini-Zinner 18.09.2018 32
  17 22P/Kopff 25.07.2022 6
  18 24P/Schaumasse 22.02.2018 4
  19 28P/Neujmin 15.08.2021 1
  20 29P/Schwassmann-Wachmann 16.01.2024 14
  21 30P/Reinmuth 2017 2
  22 31P/Schwassmann-Wachmann 07.03.2019 1
  23 32P/Comas-Sola 30.12.2023 10
  24 33P/Daniel 2016 2
  25 36P/Whipple 28.08.2019 1
  26 37P/Forbes 20.08.2018 4
  27 38P/Stephan-Oterma 27.02.2019 6
  28 40P/Väisälä 2015 1
  29 41P/Tuttle-Giacobini-Kresak 2017 10
  30 43P/Wolf-Harrington 2016 2
  31 44P/Reinmuth 05.09.2022 2
  32 45P/Honda-Mrkos-Pajdusakova 2017 12
  33 46P/Wirtanen 07.03.2019 5
  34 47P/Ashbrook-Jackson 2017 4
  35 48P/Johnson 15.08.2018 5
  36 49P/Arend-Rigaux 29.03.2019 1
  37 50P/Arend 2015 1
  38 52P/Harrington/Abell 2014 3
  39 53P/van Biesbroeck 2016 4
  40 56P/Slaughter-Burnham 2016 4
  41 57P/du Toit-Neujmin-Delporte 2015 1
  42 59P/Kearns-Kwee 2017 1
  43 60P/Tsuchinshan 30.03.2019 2
  44 61P/Shajn-Schaldach 30.08.2022 3
  45 62P/Tsuchinshan 1 21.01.2024 6
  46 63P/Wild 2013 1
  47 64P/Swift-Gehrels 18.09.2018 12
  48 65P/Gunn 05.09.2018 3
  49 66P/du Toit 13.08.2018 1
  50 67P/Churyumov-Gerasimenko 02.03.2022 8
  51 68P/Klemola 26.08.2019 5
  52 70P/Kojima 23.03.2022 7
  53 71P/Clark 2017 2
  54 73P/Schwassmann-Wachmann 3 26.03.2022 5
  55 74P/Smirnova-Chernykh 06.04.2018 5
  56 76P/West-Kohoutek-Ikemura 04.12.2019 1
  57 77P/Longmore 2016 3
  58 78P/Gehrels 2 22.03.2020 7
  59 81P/Wild 19.01.2023 11
  60 84P/Giclas 2014 2
  61 87P/Bus 24.03.2020 2
  62 88P/Howell 26.05.2020 12
  63 89P/Russell 2016 1
  64 90P/Gehrels 1 2017 1
  65 91P/Rusell 11.04.2020 1
  66 93P/Lovas 1 2017 3
  67 94P/Russell 09.02.2023 2
  68 95P/Chiron 2016 3
  69 98P/Takamizawa 2013 2
  70 99P/Kowal 1 23.03.2022 3
  71 100P/Hartley 1 27.03.2022 2
  72 101P/Chernykh 30.11.2019 3
  73 102P/Shoemaker 2013 3
  74 103P/Hartley 2 05.09.2023 6
  75 104P/Kowal 2 26.03.2022 6
  76 105P/Singer Brewster 08.04.2018 2
  77 106P/Schuster 2014 1
  78 107P/Wilson-Harrington 07.08.2022 1
  79 108P/Ciffreo 28.02.2022 5
  80 110P/Hartley 26.03.2022 4
  81 112P/Urata-Niijima 19.04.2020 3
  82 114P/Wiseman-Skiff 22.03.2020 5
  83 115P/Maury 20.08.2020 3
  84 116P/Wild 26.03.2022 7
  85 117P/Helin-Roman-Alu 1 18.03.2020 4
  86 118P/Shoemaker-Levy 4 27.12.2022 4
  87 119P/Parker-Hartley 27.12.2022 5
  88 121P/Shoemaker-Holt 2 16.01.2024 1
  89 123P/West-Hartley 07.05.2019 6
  90 124P/Mrkos 15.03.2020 5
  91 125P/Spacewatch 2013 1
  92 126P/Iras 06.09.2023 2
  93 127P/Holm-Olmstead 24.08.2022 1
  94 128P/Shoemaker-Holt 1 2016 1
  95 129P/Shoemaker-Levy 14.08.2018 4
  96 130P/McNaught-Hughes 13.08.2018 2
  97 131P/Mueller 05.09.2018 1
  98 132P/Helin-Roman-Alu 2 06.09.2021 3
  99 133P/Elst-Pizzaro 02.09.2019 1
  100 134P/Kowal-Vavrova 2014 6
  101 136P/Mueller 2016 1
  102 137P/Shoemaker-Levy 14.08.2018 4
  103 139P/Vaisala-Oterma 2017 2
  104 141P/Machholz 07.03.2021 2
  105 143P/Kowal-Mrkos 08.04.2018 1
  106 144P/Kushida 28.01.2024 6
  107 145P/Shoemaker-Levy 2017 1
  108 146P/Shoemaker-LINEAR 2016 1
  109 149P/Mueller 29.03.2019 1
  110 150P/LONEOS 09.01.2024 3
  111 152P/Helin-Lawrence 13.04.2021 1
  112 154P/Brewington 2014 8
  113 155P/Shoemaker 15.03.2020 2
  114 156P/Russell-LINEAR 07.03.2021 3
  115 157P/Tritton 06.09.2022 2
  116 158P/Kowal-LINEAR 2013 1
  117 159P/LONEOS 2017 1
  118 160P/LINEAR 21.01.2020 2
  119 162P/Siding Spring 2016 1
  120 164P/Christensen 27.02.2019 1
  121 170P/Christensen 2014 2
  122 171P/Spahr 18.09.2018 1
  123 172P/Yeung 2016 1
  124 173P/Mueller 28.12.2019 2
  125 174P/Echeclus 2016 2
  126 176P/LINEAR 2016 1
  127 178P/Hug-Bell 2014 3
  128 180P/NEAT 2016 2
  129 183P/Korlevic-Juric 06.04.2018 1
  130 184P/Lovas 2013 1
  131 185P/Petriew 06.04.2018 2
  132 187P/LINEAR 19.04.2018 1
  133 188P/LINEAR-Mueller 2017 2
  134 191P/McNaught 2014 1
  135 193P/LINEAR-NEAT 12.09.2021 4
  136 194P/Kowal 2016 1
  137 199P/Shoemaker 03.04.2022 1
  138 200P/Larsen 02.08.2018 1
  139 201P/LONEOS 2015 2
  140 202P/Scotti 03.12.2023 1
  141 203P/Korlevic 30.11.2019 2
  142 204P/LINEAR-NEAT 18.01.2023 3
  143 205P/Giacobini 2015 1
144 207P/NEAT 07.03.2024 2
  145 208P/McMillan 2016 1
  146 209P/LINEAR 2014 8
  147 210P/Christensen 25.04.2020 6
  148 211P/Hill 21.02.2023 3
  149 213P/Van Ness 2017 1
150 216P/LINEAR 07.03.2024 1
  151 217P/LINEAR 2017 2
  152 218P/LINEAR 2015 2
  153 219P/LINEAR 2016 2
  154 221P/LINEAR 2015 1
  155 223P/Skiff 11.09.2018 2
  156 226P/Pigott-LINEAR-Kowalski 09.01.2024 4
157 227P/Catalina-LINEAR 03.03.2024 2
  158 228P/LINEAR 01.01.2020 1
  159 230P/LINEAR 2015 1
  160 231P/LINEAR 31.03.2019 2
  161 235P/LINEAR 04.04.2018 1
  162 236P/LINEAR 2017 2
  163 237P/LINEAR 04.09.2023 2
  164 238P/Read 2016 1
  165 239P/LINEAR 06.04.2019 1
  166 240P/NEAT 27.02.2019 1
  167 243P/NEAT 06.08.2018 1
  168 244P/Scotti 2014 1
  169 245P/WISE 14.08.2018 2
  170 246P/NEAT 16.04.2020 8
  171 247P/LINEAR 27.02.2019 1
  172 249P/LINEAR 14.04.2020 4
  173 250P/Larson 21.02.2018 1
  174 252P/LINEAR 2016 3
  175 257P/Catalina 2013 4
  176 260P/McNaught 26.10.2019 7
  177 261P/Larson 03.09.2019 3
  178 263P/Gibbs 15.03.2023 3
  179 266P/Christensen 22.03.2020 4
  180 269P/Jedicke 2015 3
  181 270P/Gehrels 2014 1
  182 273P/Pons-Gambart 2013 1
  183 274P/Tombaugh-Tenagra 27.02.2022 1
  184 277P/LINEAR 14.11.2020 3
  185 278P/McNaught 19.04.2020 2
  186 279P/La Sagra 2016 1
  187 282P 04.04.2021 1
  188 284P/McNaught 02.09.2021 3
  189 285P/LINEAR 01.09.2022 8
  190 286P/Christensen 29.08.2022 3
  191 287P/Christensen 07.09.2023 1
  192 288P 2016 1
  193 289P/Blanpain 21.01.2020 3
  194 290P/Jager 2014 5
  195 291P/NEAT 2013 2
  196 292P/Li 2013 1
  197 293P/Spacewatch 2014 2
  198 294P/LINEAR 2014 1
  199 296P/Garradd 2014 2
  200 297P/Beshore 2014 2
  201 299P/Catalina-PANSTARRS 2016 1
  202 302P/Lemmon-PANSTARRS 2016 1
  203 303P/NEAT 2014 1
  204 304P/Ory 21.08.2020 1
  205 305P/Skiff 2014 2
  206 307P/LINEAR 2014 1
  207 312P/NEAT 21.08.2020 1
  208 314P/Montani 2015 1
  209 315P/LONEOS 2017 5
  210 318P/McNaught-Hartley 2015 1
  211 325P/Yang-Gao 02.07.2022 2
  212 327P/Van Ness 06.09.2022 5
  213 328P/LONEOS-Tucker 2015 1
  214 329P/LINEAR-Catalina 2015 1
  215 330P/Catalina 2016 1
  216 332P/Ikeya-Murakami 2016 2
  217 333P/LINEAR 2016 2
  218 334P/NEAT 20.05.2018 1
  219 337P/WISE 01.07.2022 2
  220 338P/McNaught 2016 1
  221 340P/Boattini 2016 1
  222 341P/Gibbs 2016 1
  223 343P/NEAT-LONEOS 2016 2
  224 344P/Read 2016 1
  225 345P/LINEAR 2016 1
  226 346P/Catalina 2016 1
  227 347P/PANSTARRS 05.09.2023 2
  228 349P/Lemmon 2017 1
  229 352P/Skiff 2017 2
  230 355P/LINEAR-NEAT 2017 2
  231 356P/WISE 2017 1
  232 360P/WISE 2017 1
  233 361P/Spacewatch 2017 2
  234 362P/(457175) 2017 1
  235 364P/PANSTARRS 27.03.2023 6
  236 365P/LINEAR 04.04.2018 1
  237 366P/LINEAR 07.04.2018 1
  238 368P/NEAT 15.09.2018 3
  239 369P/Hill 12.09.2018 1
  240 370P/NEAT 18.09.2018 1
  241 371P/LINEAR-Skiff 12.09.2018 1
  242 373P/Rinner 06.04.2019 1
  243 375P/Hill 31.03.2019 2
  244 376P/Loneos 30.04.2019 3
  245 377P/Scotti 23.03.2020 1
  246 378P/McNaught 30.08.2022 1
  247 379P/Spacewatch 23.04.2019 2
  248 380P/PANSTARRS 30.04.2019 1
  249 382P/Larson 07.08.2022 2
  250 384P/Kowalski 28.12.2019 3
  251 385P/Hill 30.11.2019 1
  252 390P/Gibbs 21.01.2020 2
  253 392P/LINEAR 30.11.2019 1
  254 395P/Catalina-NEAT 14.11.2022 4
  255 397P/Lemmon 21.08.2020 1
  256 398P/Boattini 07.03.2021 3
  257 399P/PANSTARRS 2013 1
  258 402P/LINEAR 28.02.2022 2
  259 404P/Bressi 17.12.2023 2
  260 405P/Lemmon 14.11.2020 2
  261 407P/PANSTARRS-Fuls 14.04.2020 3
  262 408P/Novichonok-Gerke 03.09.2021 2
  263 409P/LONEOS-Hill 04.04.2021 2
  264 413P/Larson 04.04.2021 2
  265 415P/Tenagra 08.04.2021 1
  266 418P/LINEAR 08.04.2021 1
  267 425P/Kowalski 07.09.2021 1
  268 433P/(248370) 15.08.2021 2
  269 440P/Kobayashi 26.03.2022 3
  270 442P/McNaught 02.09.2022 2
  271 445P/Lemmon-PANSTARRS 01.09.2022 2
  272 446P/McNaught 06.08.2022 1
  273 452P/Sheppard-Jewitt 21.02.2023 1
  274 453P/WISE-Lemmon 17.03.2023 1
  275 465P/Hill 15.08.2023 1
  276 466P/PANSTARRS 07.09.2023 1
  277 471P/2010 YK3 03.12.2023 3
  278 472P/NEAT-LINEAR 09.01.2024 1
279 473P/NEAT 07.03.2024 5
280 475P/Spacewatch-LINEAR 08.03.2024 1
281 479P/Elenin 07.03.2024 4
282 P/2014 VF40 (PANSTARRS) 09.03.2024 1
  283 6478 Gault (comet like asteroid) 30.03.2019 1
  284 C/1975 V1 (West) 1976 1
  285 C/2006 S3 (Loneos) 2015 6
  286 C/2006 W3 (Christensen) 2009 1
  287 C/2007 Q3 (SidingSpring) 2010 1
  288 C/2008 S3 (Boattini) 2014 2
  289 C/2009 F4 (McNaught) 2014 1
  290 C/2009 K5 (McNaught) 2010 1
  291 C/2010 S1 (LINEAR) 2014 7
  292 C/2010 U3 (Boattini) 27.02.2019 3
  293 C/2011 J2 (LINEAR) 2015 13
  294 C/2011 KP36 (Spacewatch) 2016 5
  295 C/2011 L4 (PANSTARRS) 2014 13
  296 C/2011 R1 (McNaught) 2013 4
  297 C/2012 A1 (PANSTARRS) 2013 1
  298 C/2012 A2 (Linear) 2013 2
  299 P/2012 B1 (PANSTARRS) 2014 1
  300 P/2012 F2 (PANSTARRS) 2013 1
  301 C/2012 F3 (PANSTARRS) 2015 3
  302 C/2012 F6 (Lemmon) 2014 9
  303 C/2012 J1 (Catalina) 2014 3
  304 C/2012 K1 (PANSTARRS) 2014 17
  305 C/2012 K6 (McNaught) 2014 5
  306 C/2012 K8 (Lemmon) 2014 3
  307 C/2012 LP26 (Palomar) 2016 4
  308 C/2012 S1 (ISON) 2013 2
  309 C/2012 S3 (PANSTARRS) 2013 4
  310 C/2012 S4 (PANSTARRS) 2013 1
  311 C/2012 U1 (PANSTARRS) 2013 1
  312 C/2012 X1 (LINEAR) 2014 6
  313 C/2013 A1 (Siding Spring) 2015 2
  314 C/2013 C2 (Tenagra) 2014 2
  315 C/2013 E1 (McNaught) 2014 1
  316 C/2013 E2 (Iwamoto) 2013 2
  317 C/2013 F2 (Catalina) 2014 2
  318 C/2013 F3 (McNaught) 2013 1
  319 C/2013 G1 (Kowalski) 2014 1
  320 C/2013 G3 (PANSTARRS) 2014 3
  321 C/2013 G5 (Catalina) 2013 1
  322 C/2013 G8(PANSTARRS) 2014 1
  323 C/2013 G9(Tenagra) 2014 1
  324 C/2013 H1(La Sagra) 2013 1
  325 C/2013 H2(Boattini) 2014 1
  326 P/2013 J2 (McNaught) 2013 5
  327 C/2013 P2 (PANSTARRS) 2014 1
  328 C/2013 P3 (Palomar) 2014 1
  329 C/2013 P4 (PANSTARRS) 2014 1
  330 C/2013 R1 (Lovejoy) 2014 11
  331 P/2013 R3 (Catalina-PANSTARRS) 2013 2
  332 P/2013 T2 (Schwartz) 2013 1
  333 C/2013 TW5 2015 4
  334 C/2013 U1 (Catalina) 2013 1
  335 C/2013 U2 (Holvorcem) 2015 3
  336 C/2013 UQ4 (Catalina) 2014 9
  337 C/2013 US10 (Catalina) 2016 10
  338 C/2013 V1 (Boattini) 2014 8
  339 C/2013 V2 (Borisov) 2015 6
  340 C/2013 V3 (Nevski) 2014 3
  341 C/2013 V4 (Catalina) 2016 9
  342 C/2013 V5 (Oukaimeden) 2014 5
  343 P/2013 W1 (PANSTARRS) 2013 1
  344 C/2013 X1 (PANSTARRS) 2015 5
  345 C/2013 Y2 (PANSTARRS) 2014 1
  346 P/2014 A2 (Hill) 2014 1
  347 C/2014 A4 (SONEAR) 2016 7
  348 C/2014 AA52 (Catalina) 2014 1
  349 C/2014 B1 (Schwartz) 08.04.2018 4
  350 C/2014 C3 (NEOWISE) 2014 2
  351 P/2014 D2 (Catalina-PANSTARRS) 2014 2
  352 C/2014 E2 (Jacques) 2014 12
  353 C/2014 F1 (Hill) 2014 1
  354 C/2014 F2 (Tenagra) 2015 2
  355 C/2014 G3 (PANSTARRS) 2014 1
  356 C/2014 H1 (Christensen) 2014 1
  357 P/2014 L2 (NEOWISE) 2014 4
  358 P/2014 L3 (Hill) 2014 2
  359 C/2014 M3 (Catalina) 2014 1
  360 P/2014 M4 (PANSTARRS) 2014 1
  361 P/2014 MG4 (Spacewatch-PANSTARRS) 2014 1
  362 C/2014 N3 (NEOWISE) 2015 5
  363 C/2014 OE4 (PANSTARRS) 12.07.2018 6
  364 C/2014 Q1 (PANSTARRS) 2014 2
  365 C/2014 Q2 (Lovejoy) 2016 16
  366 C/2014 Q3 (Borisov) 2014 6
  367 C/2014 R1 (Borisov) 2015 1
  368 C/2014 R3 (PANSTARRS) 18.05.2018 3
  369 C/2014 R4 (Gibbs) 2014 1
  370 C/2014 S2 (PANSTARRS) 2016 11
  371 C/2014 W2 (PANSTARRS) 2016 8
  372 C/2014 W9 (PANSTARRS) 2015 1
  373 C/2014 W11 (PANSTARRS) 2015 2
  374 P/2014 X1 (Elenin) 2015 3
  375 C/2014 Y1 (PANSTARRS) 2015 3
  376 C/2015 C1 (TOTAS-GIBBS) 2015 2
  377 C/2015 C2 (SWAN) 2015 2
  378 C/2015 D3 (PANSTARRS) 2015 1
  379 C/2015 ER61 (PANSTARRS) 2017 4
  380 C/2015 F2 (Polonia) 2015 1
  381 C/2015 F3 (SWAN) 2015 2
  382 C/2015 F4 (Jacques) 2015 2
  383 C/2015 F5 (SWAN-Xingming) 2015 3
  384 C/2015 G2 (MASTER) 2015 1
  385 C/2015 GX (PANSTARRS) 2015 1
  386 C/2015 H2 (PANSTARRS) 11.09.2018 1
  387 C/2015 K1 (MASTER) 2015 1
  388 C/2015 LC2 (PANSTARRS) 2016 1
  389 C/2015 M3 (PANSTARRS) 2015 1
  390 C/2015 O1 (PANSTARRS) 01.07.2018 7
  391 C/2015 T2 (PANSTARRS) 2017 1
  392 C/2015 T4 (PANSTARRS) 2015 1
  393 P/2015 TP200 (LINEAR) 2016 2
  394 C/2015 V1 (PANSTARRS) 2017 4
  395 C/2015 V2 (Johnson) 2017 21
  396 C/2015 V3 (PANSTARRS) 2015 1
  397 C/2015 VL62 (Lemmon-Yeung-PanSTARRS ) 2017 6
  398 C/2015 W1 (Gibbs) 2016 1
  399 P/2015 W2 (Catalina) 2015 1
  400 C/2015 WZ (PANSTARRS) 2016 3
  401 C/2015 X4 (Elenin) 2015 1
  402 C/2015 X7 (ATLAS) 2017 3
  403 C/2015 X8 (NEOWISE) 2015 1
  404 C/2015 XY1 (Lemmon) 06.02.2018 2
  405 C/2015 Y1 (LINEAR) 2016 1
  406 C/2015 YG1 (NEOWISE) 2016 1
  407 C/2016 A1 (PANSTARRS) 06.04.2018 4
  408 C/2016 A8 (LINEAR) 2016 5
  409 P/2016 BA14 (PANSTARRS) 2016 1
  410 C/2016 B1 (NEOWISE) 2017 1
  411 C/2016 C1 (PANSTARRS) 2016 1
  412 P/2016 G1 (PANSTARRS) 2016 1
  413 C/2016 KA (Catalina) 2016 1
  414 C/2016 K1 (LINEAR) 2016 2
  415 C/2016 M1 (PANSTARRS) 21.05.2018 13
  416 C/2016 N4 (Master) 20.05.2018 5
  417 C/2016 N6 (PANSTARRS) 18.04.2018 8
  418 P/2016 P2 (PANSTARRS) 2016 1
  419 C/2016 Q2 (PANSTARRS) 31.05.2021 2
  420 C/2016 Q4 (Kowalski) 2016 1
  421 C/2016 R2 (PANSTARRS) 02.07.2019 11
  422 C/2016 T1 (Matheny) 2016 1
  423 C/2016 T2 (Matheny) 2016 2
  424 C/2016 T3 (PANSTARRS) 06.02.2018 2
  425 C/2016 U1 (NEOWISE) 2016 2
  426 C/2016 VZ18 (PANSTARRS) 2017 5
  427 C/2016 X1 (Lemmon) 2016 1
  428 C/2017 AB5 (PANSTARRS) 06.02.2018 1
  429 C/2017 D2 (Barros) 2017 1
  430 C/2017 D3 (ATLAS) 19.02.2018 1
  431 C/2017 E3 (PANSTARRS) 18.04.2018 2
  432 C/2017 E4 (Lovejoy) 2017 1
  433 C/2017 K2 (PANSTARRS) 18.12.2023 37
  434 C/2017 K4 (ATLAS) 16.07.2018 2
  435 C/2017 K6 (Jacques) 19.02.2018 1
  436 C/2017 M4 (ATLAS) 05.08.2018 7
  437 C/2017 M5 (TOTAS) 14.08.2018 3
  438 C/2017 O1 (ASASSN) 06.04.2018 6
  439 C/2017 S3 (PANSTARRS) 03.08.2018 15
  440 P/2017 S5 (ATLAS) 2017 1
  441 C/2017 S6 (Catalina) 2017 1
  442 C/2017 S7 (Lemmon) 2017 1
  443 C/2017 T1 (Heinze) 2017 2
  444 C/2017 T2 (PANSTARRS) 26.05.2020 24
  445 C/2017 T3 (ATLAS) 2017 1
  446 C/2017 U7 (PANSTARRS) 01.09.2021 2
  447 C/2017 W2 (Leonard) 06.02.2018 1
  448 P/2017 W3 (Gibbs) 08.04.2018 1
  449 C/2018 A1 (PANSTARRS) 06.02.2018 1
  450 C/2018 A3 (ATLAS) 23.08.2019 2
  451 C/2018 A6 (Gibbs) 04.04.2018 2
  452 C/2018 B1 (Lemmon) 03.03.2018 1
  453 P/2018 C1 (Lemmon-Read) 18.02.2018 1
  454 C/2018 C2 (Lemmon) 08.04.2018 1
  455 C/2018 DO4 (Lemmon) 27.10.2019 1
  456 C/2018 EF9 (Lemmon) 20.05.2018 1
  457 C/2018 F1 (Grauer) 07.04.2018 1
  458 C/2018 F4 (PANSTARRS) 18.04.2018 1
  459 P/2018 H2 (PANSTARRS) 02.06.2018 1
  460 C/2018 K1 (Weiland) 20.06.2018 1
  461 C/2018 KJ3 (Lemmon) 14.08.2018 1
  462 C/2018 L2 (ATLAS) 04.12.2018 2
  463 P/2018 L4 (PANSTARRS) 03.07.2018 1
  464 P/2018 L5 (Leonard) 18.07.2018 1
  465 C/2018 M1 (Catalina) 13.07.2018 1
  466 C/2018 N1 (NEOWISE) 08.09.2018 3
  467 C/2018 N2 (ASASSN) 30.11.2019 8
  468 P/2018 P3 (PANSTARRS) 11.09.2018 1
  469 P/2018 P4 (PANSTARRS) 04.09.2018 1
  470 C/2018 P5 (PANSTARRS) 08.09.2018 1
  471 C/2018 R3 (Lemmon) 07.04.2019 1
  472 C/2018 U1 (Lemmon) 08.05.2021 6
  473 C/2018 V1 (Machholz-Fujikawa-Iwamoto) 04.12.2018 1
  474 C/2018 W2 (Africano) 03.09.2019 11
  475 C/2018 X2 (Fitzsimmons) 07.03.2019 1
  476 C/2018 Y1 (Iwamoto) 30.04.2019 5
  477 P/2019 A2 (ATLAS) 29.03.2019 1
  478 C/2019 B1 (Africano) 07.03.2019 1
  479 P/2019 B2 (Groeller) 07.03.2019 1
  480 C/2019 C1 (ATLAS) 22.03.2020 2
  481 C/2019 D1 (Flewelling) 05.07.2019 6
  482 C/2019 F1 (ATLAS-Africano) 19.04.2020 4
  483 C/2019 F2 (ATLAS) 23.04.2019 1
  484 C/2019 H1 (NEOWISE) 08.05.2019 1
  485 C/2019 J2 (Palomar) 30.06.2019 2
  486 C/2019 J3 (ATLAS) 02.07.2019 1
  487 C/2019 K4 (Ye) 23.08.2019 4
  488 C/2019 K5 (Young) 28.12.2019 3
  489 A/2019 K6 16.04.2020 1
  490 C/2019 K7 (Smith) 15.04.2021 5
  491 C/2019 K8 (ATLAS) 31.08.2019 2
  492 C/2019 L1 (PANSTARRS) 01.08.2019 1
  493 C/2019 L2 (NEOWISE) 29.06.2019 1
  494 C/2019 L3 (ATLAS) 20.03.2022 16
  495 P/2019 LD2 (ATLAS) 07.09.2021 1
  496 P/2019 LM4 (Palomar) 18.05.2020 2
  497 P/2019 M2 (ATLAS) 01.08.2019 1
  498 C/2019 M3 (ATLAS) 31.07.2019 1
  499 C/2019 N1 (ATLAS) 15.05.2020 6
500 C/2019 O2 (PANSTARRS) 09.03.2024 1
  501 C/2019 O3 (Palomar) 29.08.2022 5
  502 2I/2019 Q4 (Borisov) 31.10.2019 1
  503 C/2019 S4 (Lemmon) 01.04.2020 1
  504 C/2019 T2 (Lemmon) 21.08.2020 2
  505 C/2019 T3 (ATLAS) 02.09.2022 8
  506 C/2019 T4 (ATLAS) 28.03.2023 3
  507 P/2019 T6 (PANSTARRS) 30.11.2019 1
  508 C/2019 U5 (PANSTARRS) 27.03.2023 11
  509 C/2019 U6 (Lemmon) 05.11.2020 6
  510 C/2019 V1 (Borisov) 30.11.2019 1
  511 P/2019 X1 (Pruyne) 16.01.2020 1
  512 C/2019 Y1 (ATLAS) 18.05.2020 22
  513 C/2019 Y4 (ATLAS) 15.05.2020 22
  514 C/2020 A2 (Iwamoto) 19.03.2020 3
  515 C/2020 B3 (Rankin) 22.03.2020 1
  516 C/2020 F2 (ATLAS) 22.02.2023 3
  517 C/2020 F3 (NEOWISE) 20.08.2020 7
  518 C/2020 F5 (NEOWISE) 24.08.2022 2
  519 C/2020 F8 (ATLAS) 19.05.2020 1
  520 P/2020 G1 (PIMENTEL) 19.04.2020 1
  521 C/2020 H2 (Pruyne) 11.05.2020 1
  522 C/2020 H3 (Wierzchos) 19.05.2020 1
  523 C/2020 H6 (ATLAS) 02.06.2022 7
  524 C/2020 H7 (Lemmon) 28.05.2020 1
  525 C/2020 H8 (PANSTARRS) 27.05.2020 1
  526 C/2020 J1 (ATLAS) 07.03.2022 3
  527 C/2020 K1 (PANSTARRS) 02.09.2022 12
  528 C/2020 K3 (Leonard) 18.06.2020 1
  529 C/2020 K7 (PANSTARRS) 21.07.2020 1
  530 C/2020 K8 (Catalina-ATLAS) 19.06.2020 1
  531 P/2020 K9 (Lemmon-PANSTARRS) 20.08.2020 1
  532 C/2020 M3 (ATLAS) 14.11.2020 1
  533 C/2020 M5 (ATLAS) 22.03.2022 5
  534 C/2020 N1 (PANSTARRS) 06.11.2020 2
  535 C/2020 O2 (Amaral) 08.08.2021 1
  536 C/2020 P3 (ATLAS) 07.03.2021 2
  537 C/2020 PV6 (PANSTARRS) 01.09.2021 3
  538 C/2020 R2 (PANSTARRS) 05.09.2021 1
  539 C/2020 R4 (ATLAS) 30.05.2021 6
  540 C/2020 R7 (ATLAS) 27.02.2023 1
  541 C/2020 S3 (Erasmus) 14.08.2021 1
  542 C/2020 S4 (PANSTARRS) 18.01.2023 4
  543 P/2020 S6 (Leonard) 14.11.2020 1
  544 C/2020 S8 (Lemmon) 08.05.2021 5
  545 C/2020 T2 (Palomar) 30.05.2021 8
  546 P/2020 U2 (PANSTARRS) 07.03.2021 1
  547 C/2020 U4 (PANSTARRS) 14.11.2022 4
  548 C/2020 U5 (PANSTARRS) 21.08.2022 3
  549 C/2020 V2 (ZTF) 24.08.2023 14
  550 P/2020 V4 (Rankin) 19.02.2022 1
  551 P/2020 WJ5 (Lemmon) 21.03.2023 1
  552 C/2020 Y2 (ATLAS) 20.04.2021 1
  553 C/2020 Y3 (ATLAS) 07.03.2021 1
  554 C/2021 A1 (Leonard) 30.05.2021 3
  555 C/2021 A2 (NEOWISE) 07.03.2021 1
  556 C/2021 A4 (NEOWISE) 06.03.2021 1
  557 C/2021 A9 (PANSTARRS) 27.03.2022 1
  558 C/2021 C1 (Rankin) 08.03.2021 1
  559 C/2021 C3 (Catalina) 08.03.2021 1
  560 C/2021 D1 (SWAN) 30.03.2021 2
  561 C/2021 D2 (ZTF) 23.02.2022 4
  562 C/2021 E3 (ZTF) 03.09.2021 2
  563 C/2021 F1 (Lemmon-PANSTARRS) 03.03.2022 2
  564 C/2021 K1 (ATLAS) 04.09.2021 1
  565 C/2021 L3 (Borisov) 09.03.2022 1
  566 P/2021 N2 (Fuls) 08.09.2021 2
  567 C/2021 O3 (PANSTARRS) 05.09.2021 3
  568 C/2021 P4 (PANSTARRS) 02.06.2022 7
  569 C/2021 Q3 (ATLAS) 01.09.2021 1
  570 C/2021 Q4 (FULS) 05.09.2022 3
  571 P/2021 Q5 (ATLAS) 08.09.2021 1
  572 C/2021 QM45 (PANSTARRS) 06.09.2022 2
  573 C/2021 S1 (ATLAS) 28.02.2022 2
574 C/2021 S3 (PANSTARRS) 09.03.2024 1
  575 C/2021 S4 (Tsuchinshan) 10.01.2024 3
  576 C/2021 T4 (Lemmon) 12.12.2022 3
  577 C/2021 U5 (Catalina) 26.03.2022 1
  578 P/2021 V2 (Fuls) 17.03.2023 1
  579 C/2021 X1 (Maury-Attard) 07.09.2023 2
  580 C/2021 Y1 (ATLAS) 17.12.2022 3
  581 C/2022 A2 (PANSTARRS) 14.08.2023 4
  582 C/2022 A3 (Lemmon-ATLAS) 19.01.2023 1
  583 P/2022 C2 (PANSTARRS) 22.03.2022 2
  584 P/2022 D1 (PANSTARRS) 27.03.2022 1
585 C/2022 E2 (ATLAS) 03.03.2024 5
  586 C/2022 E3 (ZTF) 09.02.2023 15
  587 C/2022 J2 (Bok) 17.12.2022 1
  588 C/2022 L1 (Catalina) 28.08.2022 4
  589 C/2022 L2 (ATLAS) 10.08.2023 3
  590 P/2022 L3 (ATLAS) 12.12.2022 6
  591 C/2022 N1 (Attard-Maury) 19.07.2022 1
  592 C/2022 P1 (NEOWISE) 03.09.2022 3
  593 P/2022 P2 (ZTF) 05.09.2022 1
  594 C/2022 P3 (ZTF) 08.02.2023 1
  595 C/2022 Q2 (ATLAS) 14.11.2022 1
  596 C/2022 QE78 (ATLAS) 07.12.2023 1
  597 C/2022 R3 (Leonard) 16.12.2022 2
  598 C/2022 S4 (Lemmon) 12.09.2023 2
  599 C/2022 U1 (Leonard) 17.12.2023 3
  600 C/2022 U2 (ATLAS) 09.02.2023 4
  601 C/2022 U3 (Bok) 03.12.2023 2
  602 C/2022 U4 (Bok) 27.03.2023 4
  603 C/2022 W2 (ATLAS) 08.02.2023 1
  604 C/2022 W3 (Leonard) 07.02.2023 1
  605 C/2023 A1 (Leonard) 26.02.2023 2
  606 C/2023 A3 (Tsuchinshan-ATLAS) 21.01.2024 2
  607 P/2023 B1 (PANSTARRS) 27.03.2023 3
  608 C/2023 E1 (ATLAS) 05.09.2023 5
  609 C/2023 H2 (Lemmon) 10.09.2023 2
610 C/2023 H5 (Lemmon) 08.03.2024 3
  611 C/2023 P1 (Nishimura) 09.09.2023 8
  612 C/2023 RN3 (ATLAS) 17.12.2023 1
  613 C/2023 S2 (ATLAS) 03.12.2023 1
  614 C/2023 T2 (Borisov) 10.01.2024 2
615 C/2023 V4 (Camarasa-Duszanowicz) 28.02.2024 1
  616 C/2023 X1 (Leonard) 18.12.2023 1
  617 C/2023 X4 (Hogan) 17.12.2023 1
618 C/2024 C1 (PANSTARRS) 08.03.2024 1
619 C/2024 C2 (PANSTARRS) 08.03.2024 2
620 C/2024 E1 (Wierzchos) 10.03.2024 2