1,269 results on '"Skinner, G."'
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2. Sichuan's Population in the Nineteenth Century: Lessons from Disaggregated Data
- Author
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Skinner, G. William
- Published
- 2011
- Full Text
- View/download PDF
3. China's Fertility Transition through Regional Space: Using GIS and Census Data for a Spatial Analysis of Historical Demography
- Author
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Skinner, G. William (George William), Henderson, Mark, and Yuan, Jianhua
- Published
- 2000
4. An investigation of the clinical impact and therapeutic relevance of a DNA damage immune response (DDIR) signature in patients with advanced gastroesophageal adenocarcinoma
- Author
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Baxter, M.A., Spender, L.C., Cairns, D., Walsh, S., Oparka, R., Porter, R.J., Bray, S., Skinner, G., King, S., Turbitt, J., Collinson, D., Miedzybrodzka, Z.H., Jellema, G., Logan, G., Kennedy, R.D., Turkington, R.C., McLean, M.H., Swinson, D., Grabsch, H.I., Lord, S., Seymour, M.J., Hall, P.S., and Petty, R.D.
- Published
- 2024
- Full Text
- View/download PDF
5. The development of nuclear military strategy and Anglo-American relations, 1939-1958
- Author
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Skinner, G., Toye, R., and Thomas, M.
- Subjects
900 - Abstract
There was no special governmental partnership between Britain and America during the Second World War in atomic affairs. A recalibration is required that updates and amends the existing historiography in this respect. The wartime atomic relations of those countries were cooperative at the level of science and resources, but rarely that of the state. As soon as it became apparent that fission weaponry would be the main basis of future military power, America decided to gain exclusive control over the weapon. Britain could not replicate American resources and no assistance was offered to it by its conventional ally. America then created its own, closed, nuclear system and well before the 1946 Atomic Energy Act, the event which is typically seen by historians as the explanation of the fracturing of wartime atomic relations. Immediately after 1945 there was insufficient systemic force to create change in the consistent American policy of atomic monopoly. As fusion bombs introduced a new magnitude of risk, and as the nuclear world expanded and deepened, the systemic pressures grew. It was these pressures which forced America to review its security alignment. Science can hold a mirror to changing strategic relationships during the militarisation of nuclear affairs. From leadership during the inception phase, through to becoming one part of a multi-dimensional defence environment as technical progress accelerated, science reflected wider atomic developments in both Britain and America during the 1950s. It was the benefits resulting from its increasingly linked internal science-military structures, combined with the changing worldwide geopolitical forces of the late 1950's, which encouraged and constrained America to consider previously unthinkable external nuclear relationships. In 1958, America moved away from separatism in atomic affairs. It chose to create a nuclear state partnership with the nation that best reflected its new security orientation, and which had also reached a significant level of maturity in fusion weaponry. That country was Britain.
- Published
- 2019
6. Postoperative Outcomes Associated With Procedural Sedation Conducted by Physician and Nonphysician Anesthesia Providers: Findings From the Prospective, Observational African Surgical Outcomes Study
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van der Merwe, Freliza, Vickery, Nicola J., Kluyts, Hyla-Louise, Yang, Dongsheng, Han, Yanyan, Munlemvo, Dolly M., Ashebir, Daniel Z., Mbwele, Bernard, Forget, Patrice, Basenero, Apollo, Youssouf, Coulibaly, Antwi-Kusi, Akwasi, Ndonga, Andrew K., Ngumi, Zipporah W. W., Elkhogia, Abdulaziz, Omigbodun, Akinyinka O., Tumukunde, Janat, Madzimbamuto, Farai D., Gobin, Veekash, Mehyaoui, Ryad, Samateh, Ahmadou L., du Toit, Leon, Madiba, Thandinkosi E., Pearse, Rupert M., Biccard, Bruce M., Abadagan, H., Abbas, N., Abdelatif, A. I., Abdoulaye, T., Abd-rouf, A., Abduljalil, A., Abdulrahman, A., Abdurazig, S., Abokris, A., Abozaid, W., Abugassa, S. O. A., Abuhdema, F., Abujanah, S. A., Abusamra, R., Abushnaf, A., Abusnina, S. A., Abuzalout, T. S., Ackermann, H. M., Adamu, Y. B., Addanfour, A., Adeleke, D. M., Adigun, T. A., Adisa, A. O., Adjignon, S. V., Adu-Aryee, N. A., Afolabi, B. B., Agaba, A. F. X., Agaba, P. K. A., Aghadi, K., Agilla, H., Ahmed, B., Ahmed, El.-Z., Ahmed, Al.-J., Ahmed, M., Ahossi, R., Aji, S. A., Akanyun, S., Akhideno, I., Akhter, M., Akinyemi, O. A., Akkari, M., Akodjenou, J., al Shams, E. S., Alagbe-Briggs, O. T., Alakkari, E. A., Alalem, R. B., Alashhab, M., Alatise, O. I., Alatresh, A., Alayeb, M. S. I., Albakosh, B. A., Albert, F., Alberts, A. N. J. D., Aldarrat, A. D., Alfari, A., Alfetore, A., Algbali, M., Algddar, A., Algedar, H. A., Alghafoud, I. A., Alghazali, A., Alhajj, M., Alhendery, A., Alhoty, F. F. H., Ali, A., Ali, Y. A., Ali, A., Alioune, B. S., Alkassem, M. A., Alkchr, M. A., Alkesa, T. S., Alkilani, A., Alkobty, F., Allaye, T., Alleesaib, S. B. M., Alli, A., Allopi, K., Allorto, N. L., Almajbery, A., Almesmary, R., Almisslati, S. H. A., Almoraid, F., Alobeidi, H., Alomami, M. A., Alphonsus, C. S., Alqawi, O. A., Alraheem, A. A., Alsabri, S. A., Alsayed, A., Alsellabi, B., Al-Serksi, M., Alshareef, M. S. A., Altagazi, A. A., Aluvale, J. S., Alwahedi, H. W., Alzahra, E. A., Alzarouk, M. A., Al-Zubaidy, K., Amadou, M., Amadou, M., Amanor-Boadu, S. D., Amer, Al.-A., Amisi, B. T., Amuthenu, M. A., Anabah, T. W. A., Anani, F., Anderson, P. G. R., Andriamampionona, A. G. B., Andrianina, L., Anele, A., Angelin, R., Anjar, N., Antùnez, O., Anyanwu, L. J. C., Aribi, A. A., Arowolo, O. A., Arrey, O., Assefa, S. B., Assoum, G., Athanse, V., Athombo, J. S., Atiku, M., Atito-Narh, E., Atomabe, A., Attia, A., Aungraheeta, M., Aurélia, D. M. A., Ayandipo, O. O., Ayebale, A. E. T., Azzaidey, H. M. Z., Babajee, N. B., Badi, H. B., Badianga, E. K., Baghni, R. B., Bahta, M. T., Bai, M., Baitchu, Y., Baloyi, A. M., Bamuza, K. A., Bamuza, M. I., Bangure, L., Bankole, O. B., Barongo, M. L., Barow, M. M., Bashiya, L., Basson, C. H., Bechan, S., Belhaj, S., Ben Mansour, M. M., Benali, D., Benamour, A. S. B., Berhe, A., Bertie, J. D., Bester, J. J. A., Bester, M., Bezuidenhout, J. D., Bhagwan, K., Bhagwandass, D. R., Bhat, K. A. P., Bhuiyan, M. M. Z. U., Bigirimana, F., Bikuelo, C. J., Bilby, B. E., Bingidimi, S. S., Bischof, K. E., Bishop, D. G., Bitta, C., Bittaye, M., Biyase, T., Blake, C. A., Blignaut, E., Blignaut, F., Tanjong, B. N., Bogoslovskiy, A., Boloko, P. M., Boodhun, S. K. B., Bori, I., Boufas, F., Brand, M., Brouckaert, N. T., Bruwer, J. D., Buccimazza, I., Bula Bula, I. M., Bulamba, F., Businge, B. C., Bwambale, Y. B., Cacala, S. R. C., Cadersa, M. A., Cairns, C., Carlos, F., Casey, M. E., Castro, A. C., Chabayanzara, N. D., Chaibou, M. S., Chaibva, T. N. O., Chakafa, N. K., Chalo, C., Changfoot, C., Chari, M. C., Chelbi, L., Chibanda, J. T., Chifamba, H. N., Chikh, N., Chikumba, E., Chimberengwa, P., Chirengwa, J., Chitungo, F. M., Chiwanga, M. C., Chokoe, M. M., Chokwe, T. M., Chrirangi, B., Christian, M., Church, B., Cisekedi, J. C., Clegg-Lamptey, J. N., Cloete, E., Coltman, M., Conradie, W., Constance, N., Coulibaly, Y., Cronje, L., Da Silva, M. A., Daddy, H., Dahim, L., Daliri, D., Dambaki, M. S., Dasrath, A., Davids, J. G., Davies, G. L., De Lange, J. T., de Wet, J. B., Dedekind, B., Degaulle, M. A., Dehal, V., Deka, P. D., Delinikaytis, S., Desalu, I. S., Dewanou, H., Deye, M. B. M., Dhege, C., Diale, B. S. G., Dibwe, D. F., Diedericks, B. J. S., Dippenaar, J. M., Dippenaar, L., Diyoyo, M. P., Djessouho, E., Dlamini, S. N., Dodiyi-Manuel, A., Dokolwana, B. A., Domoyyeri, D. P., Drummond, L. W., du Plessis, D. E., du Plessis, W. M., du Preez, L. J., Dube, K., Dube, N. Z., Dullab, K. D., Duvenhage, R., Echem, R. C., Edaigbini, S. A., Egote, A. K., Ehouni, A., Ekwen, G., Ekwunife, N. C., El Hensheri, M., Elfaghi, I. E., Elfagieh, M. A., Elfallah, S., Elfiky, M., Elgelany, S., Elghallal, A. M., Elghandouri, M. G., Elghazal, Z. S., Elghobashy, A. M., Elharati, F. T., Elkhwildi, R. M., Ellis, S., Elmadani, L., Elmadany, H. B., Elmehdawi, H., Elmgadmi, A., Eloi, H., Elrafifi, D., Elsaadi, G., Elsaity, R. B., Elshikhy, A., Eltaguri, M., Elwerfelli, A., Elyasir, I. E., Elzoway, A. Z., Elzufri, A. M., Enendu, E. O., Enicker, B. C., Enwerem, E. O., Esayas, R., Eshtiwi, M., Eshwehdi, A. A., Esterhuizen, J. L., Esterhuizen, T. M., Etuk, E. B., Eurayet, O., Eyelade, O. R., Fanjandrainy, R. F., Fanou, L., Farina, Z., Fawzy, M., Feituri, A., Fernandes, N. L., Ford, L. M., François, T., Freeman, T., Freeman, Y. B. M., Gacii, V. M., Gadi, B., Gagara, M., Gakenia, A., Gallou, P. D., Gama, G. G. N., Gamal, M. G., Gandy, Y. G., Ganesh, A., Gangaly, D., Garcia, M., Gatheru, A. P., Gaya, S. S. D., Gbéhadé, O., Gerbel, G., Ghnain, A., Gigabhoy, R., Giles, D. G., Girmaye, G. T., Gitau, S., Githae, B., Gitta, S., Goga, R., Gomati, A. A. G., Gonzalez, M. E., Gopall, J., Gordon, C. S., Gorelyk, O., Gova, M., Govender, K., Govender, P., Govender, S., Govindasamy, V., Green-Harris, J. T. K., Greenwood, M. B., Grey-Johnson, S. V., Grobbelaar, M., Groenewald, M. A., Grünewald, K. K., Guegni, A., Guenane, M., Gueye, S., Guezo, M., Gunguwo, T., Gweder, M. G., Gwila, M., Habimana, L., Hadecon, R., Hadia, E., Hamadi, L., Hammouda, M., Hampton, M. I., Hanta, R., Hardcastle, T. C., Hariniaina, J. A., Hariparsad, S., Harissou, A. H., Harrichandparsad, R., Hasan, S. H. A., Hashmi, H. B., Hayes, M. P., Hdud, A., Hebli, S. H., Heerah, H. M. S. N., Hersi, S., Hery, A. H., Hewitt-Smith, A., Hlako, T. C., Hodges, S. C. H., Hodgson, R. E., Hokoma, M., Holder, H., Holford, E. B., Horugavye, E., Houston, C., Hove, M., Hugo, D., Human, C. M., Hurri, H., Huwidi, O., Ibrahim, A. I., Ibrahim, T., Idowu, O. K., Igaga, I. E., Igenge, J., Ihezie, O., Ikandi, K., Ike, I. A. R., Ikuku, J. J. N., Ilbarasi, M. N., Ilunga, I. B. B., Ilunga, J. P. M., Imbangu, N. A. V., Imessaoudene, Z., Imposo, D. H., Iraya, A. M., Isaacs, M., Isiguzo, M., Issoufou, A., Izquirdo, P., Jaber, A., Jaganath, U. V., Jallow, C. S., Jamabo, S., Jamal, Z. S., Janneh, L., Jannetjies, M. J., Jasim, I., Jaworska, M. A. J., Jay Narain, S., Jermi, K., Jimoh, R., Jithoo, S., Johnson, M., Joomye, S., Judicael, R. M., Judicaël, M., Juwid, A., Jwambi, L. P., Kabango, R., Kabangu, J. K., Kabatoro, D. K., Kabongo, A. N., Kabongo, K., Kabongo, L. T., Kabongo, M. D., Kady, N., Kafu, S., Kaggya, M., Kaholongo, B. N. K., Kairuki, P. C. K., Kakololo, S. I., Kakudji, K., Kalisa, A., Kalisa, R., Kalufwelu, M. R., Kalume, S., Kamanda, R. J., Kangili, M. K., Kanoun, Kapesa, H., Kapp, P., Karanja, J. K., Karar, M., Kariuki, K., Kaseke, K., Kashuupulwa, P. N. K., Kasongo, K. J. P., Kassa, S. K., Kateregga, G. K., Kathrada, M. I. S., Katompwa, P. M., Katsukunya, L., Kavuma, Khalfallah, K. A. M., Khamajeet, A., Khetrish, Kibandwa, S. B., Kibochi, W., Kilembe, A. M., Kintu, A. K., Kipng’etich, B., Kiprop, B., Kissoon, V. M. K., Kisten, T. K., Kiwanuka, J. K., Knox, M. E. K., Koledale, A. K., Koller, V. L., Kolotsi, M. A., Kongolo, M., Konwuoh, N. D., Koperski, W. J., Koraz, M. Y. K., Kornilov, A. A., Koto, M. Z., Kransingh, S., Krick, D., Kruger, S., Kruse, C., Kuhn, W., Kuhn, W. P., Kukembila, A. M., Kule, K. L., Kumar, M., Kusel, B. S., Kusweje, V. K., Kuteesa, K. J., Kutor, Y. Y., Labib, M. A., Laksari, M., Lanos, F., Lawal, T. A., Le Manach, Y., Lee, C., Lekoloane, R. M., Lelo, S. N., Lerutla, B., Lerutla, M. T., Levin, A. I., Likongo, T. B., Limbajee, M. L., Linyama, D. M., Lionnet, C., Liwani, M. M., Loots, E., Lopez, A. G., Lubamba, C. L. C., Lumbala, K. F., Lumbamba, A. J. M., Lumona, John, Lushima, R. F., Luthuli, L., Luweesi, H. L., Lyimo, T. S. K., Maakamedi, H. M., Mabaso, B. M., Mabina, M., Maboya, M. E., Macharia, I., Macheka, A. M., Machowski, A. Z., Madsen, A. S. M., Madzivhe, L. J., Mafafo, S. C., Maghrabi, M., Mahamane, D. D., Maharaj, A., Maharaj, A., Maharaj, A. D., Mahmud, M. R., Mahoko, M., Mahomedy, N. A., Mahomva, O., Mahureva, T. M., Maila, R. K., Maimane, D. M., Maimbo, M., Maina, S. N., Maiwald, D. A., Maiyalagan, M. D., Majola, N., Makgofa, N., Makhanya, V., Makhaye, W. P., Makhlouf, N. M., Makhoba, S., Makopa, E. K., Makori, O., Makupe, A. M., Makwela, M. A., Malefo, M. E., Malongwe, S. M., Maluleke, D. M., Maluleke, M. R., Mamadou, K. T., Mamaleka, M. P., Mampangula, Y., Mamy, R. M., Mananjara, M. N. R., Mandarry, M. T. M., Mangoo, D. M., Manirimbere, C., Manneh, A., Mansour, A., Mansour, I., Manvinder, M., Manyere, D. V., Manzini, V. T., Manzombi, J. K., Mapanda, P. M., Marais, L. C., Maranga, O., Maritz, J. P. B., Mariwa, F. K., Masela, R. S., Mashamba, M. M., Mashava, D. M., Mashile, M. V., Mashoko, E., Masia, O. R., Masipa, J. N., Masiyambiri, A. T. M., Matenchi, M. W., Mathangani, W., Mathe, R. C., Matola, C. Y., Matondo, P. M., Matos-Puig, R., Matoug, F. F. H., Matubatuba, J. T., Mavesere, H. P., Mavhungu, R., Maweni, S., Mawire, C. J. M., Mawisa, T., Mayeza, S., Mbadi, R., Mbayabu, M., Mbewe, N., Mbombo, W. D., Mbuyi, T., Mbuyi, W. M. S., Mbuyisa, M. W., Menkiti, I. D., Mesarieki, L. V. M., Metali, A., Mewanou, S., Mgonja, L., Mgoqo, N., Mhatu, S., Mhlari, T. M., Miima, S., Milod, I. M., Minani, P., Mitema, F., Mlotshwa, A., Mmasi, J. E., Mniki, T., Mofikoya, B. O., Mogale, J. O., Mohamed, A., Mohamed, A., Mohamed, A., Mohamed, S., Mohamed, S., Mohamed, T. S., Mohamed, A., Mohamed, A., Mohamed, A. M., Mohamed, P., Mohammed, I., Mohammed, F. A. M., Mohammed, M., Mohammed, N. M., Mohlala, M. P., Mokretar, R., Molokoane, F. M., Mongwe, K. N., Montenegro, L., Montwedi, O. D., Moodie, Q. K., Moopanar, M., Morapedi, M., Morulana, T. G., Moses, V. L., Mossy, P., Mostafa, H., Motilall, S. R., Motloutsi, S. P., Moussa, K., Moutari, M., Moyo, O. M., Mphephu, P. E., Mrara, B., Msadabwe, C., Mtongwe, V. M., Mubeya, F. K., Muchiri, K., Mugambi, J., Muguti, G. I. M., Muhammad, A. B., Mukama, I. F., Mukenga, M. M., Mukinda, F. K., Mukuna, P. M., Mungherera, A. R. W., Munyaradzi, T. W., Munyika, A. A., Muriithi, J. M., Muroonga, M. P., Murray, R., Mushangwe, V. K., Mushaninga, M., Musiba, V. E. M., Musowoya, J. M., Mutahi, S., Mutasiigwa, M. G. H., Mutizira, G., Muturi, A., Muzenda, T., Mvwala, K. R., Mvwama, N. M., Mwale, A., Mwaluka, C. N., Mwamba, J. D., Mwanga, H. A. M., Mwangi, C. M., Mwansa, S., Mwenda, V., Mwepu, I. M., Mwiti, T. M., Mzezewa, S. Z., Nabela, L., Nabukenya, M. T. N., Nabulindo, S. M., Naicker, K., Naidoo, D., Naidoo, L., Naidoo, L. C., Naidoo, N., Naidoo, R., Naidoo, R. D., Naidoo, S., Naidoo, T. D., Naidu, T. K., Najat, N. Z., Najm, Y., Nakandungile, F., Nakangombe, P., Namata, C. N., Namegabe, E. S., Nansook, A., Nansubuga, N. P., Nantulu, C., Nascimento, R., Naude, G. T., Nchimunya, H., Ndaie, M. A., Ndarukwa, P. N., Ndasi, H., Ndayisaba, G., Ndegwa, D., Ndikumana, R., Ndung’u, C., Neil, M. C., Nel, M. S., Neluheni, E. V., Nesengani, D. S., Nesengani, N. T., Netshimboni, L. E., Ngalala, A. M., Ngari, B. M., Ngari, N. B. M., Ngatia, E., Ngcobo, G. K., Ngcobo, T. S., Ngorora, D., Ngouane, D., Ngugi, K., Nibe, Z., Ninise, E., Niyondiko, J. C., Njenga, P. W., Njenga, M. N., Njoroge, M., Njoroge, S., Njuguna, W., Njuki, P. N., Nkesha, T., Nkuebe, T. N., Nkuliyingoma, N. P., Nkunjana, M., Nkwabi, E., Nkwine, R. N., Nnaji, C., Notoane, I., Nsalamba, S., Ntlhe, L. M., Ntoto, C., Ntueba, B., Nyassi, M. T., Nyatela-Akinrinmade, Z., Nyawanda, H. O., Nyokabi, N. N., Nziene, V. N., Obadiah, S., Ochieng, O. J. P., Odia, P. K., Oduor, O. E. O., Ogboli-Nwasor, E. O., Ogendo, S. W. O., Ogunbode, O., Ogundiran, T. O., Ogutu, O., Ojewola, R. W., Ojujo, M., Ojuka, D. O., Okelo, O. S., Okiya, S., Okonu, N., Olang, P. R., Omoding, S., Omoshoro-Jones, J., Onyango, R., Onyegbule, A., Orjiako, O., Osazuwa, M. O., Oscar, K., Osinaike, B. B., Osinowo, A. O., Othin, O. M., Otman, F. F. H., Otokwala, J., Ouanes, F., Oumar, O., Ousseini, A. O., Padayachee, S., Pahlana, S. M., Pansegrouw, J., Paruk, F. P., Patel, M. B., Patel, U., Patience, A. P., Pembe, J. D., Pengemale, G. N., Perez, N., Perez, M. F. A., Peter, A. M., Phaff, M., Pheeha, R. M., Pienaar, B. H., Pillay, V., Pilusa, K. A., Pochana, M. P., Polishchuk, O., Porrill, O. S., Post, E. F., Prosper, A., Pupyshev, M., Rabemazava, A., Rabiou, M. S., Rademan, L., Rademeyer, M., Raherison, R. A. R., Rajah, F. R., Rajcoomar, M. S. R., Rakhda, Z., Rakotoarijaona, A. H. R., Rakotoarisoa, A. H. N., Rakotoarison, S. R., Rakotoarison, R. R., Ramadan, L., Ramananasoa, M. L. R., Rambau, M., Ramchurn, T. P. R., Ramilson, H. E., Ramjee, R. J., Ramnarain, H., Ramos, R., Rampai, T. J., Ramphal, S. R., Ramsamy, T., Ramuntshi, R., Randolph, R., Randriambololona, D. M. A., Ras, W. A. P., Rasolondraibe, R. A. F., Rasolonjatovo, J. D. L. C., Rautenbach, R. M., Ray, S., Rayne, S. R., Razanakoto, F. A. R., Reddy, S. R., Reed, A. R., Rian, J. R., Rija, F. R., Rink, B., Robelie, A. T., Roberts, C. A., Rocher, A. G. L., Rocher, S., Rodseth, R. N., Rois, I., Rois, W., Rokhsi, S., Roos, J., Rorke, N. F., Roura, H., Rousseau, F. J., Rousseau, N., Royas, L., Roytowski, D., Rungan, D., Rwehumbiza, S. S. R., Ryabchiy, B. B., Ryndine, V., Saaiman, C. R., Sabwa, H. K., Sadat, S., Saed, S. S., Salaheddin, E., Salaou, H., Saleh, M., Salisu-Kabara, H. M., Sama, H. D., Samateh, A. L., Sam-Awortwi, W., Jnr, Samuel, N., Sanduku, D. K., Sani, C. M., Sanyang, L. N., Sarah, H. N., Sarkin-Pawa, A., Sathiram, R., Saurombe, T., Schutte, H., Sebei, M. P., Sedekounou, M. D., Segooa, M. P., Semenya, E. M., Semo, B. O., Sendagire, C. S., Senoga, S. A., Senusi, F. S., Serdyn, T., Seshibe, M. D., Shah, G. B., Shamamba, R., Shambare, C. S., Shangase, T. N., Shanin, S. H., Shefren, I. E., Sheshe, A. A., Shittu, O. B., Shkirban, A. S., Sholadoye, T., Shubba, A., Sigcu, N., Sihope, S. E., Sikazwe, D. S., Sikombe, B. S., Simaga Abdoul, K., Simo, W. A. G., Singata, K., Singh, A. S., Singh, S., Singh, U., Sinoamadi, V., Sipuka, N., Sithole, N. L. M., Sitima, S., Skinner, D. L., Skinner, G. C., Smith, O. I., Smits, C. A. G., Sofia, M. S. I., Sogoba, G., Sohoub, A., Sookun, S. S., Sosinska, O., Souhe, R., Souley, G., Souleymane, T., Spicer, J. M., Spijkerman, S., Steinhaus, H., Steyn, A., Steyn, G., Steyn, H. C., Stoltenkamp, H. L., Stroyer, S., Swaleh, A., Swayeb, E., Szpytko, A. J., Taiwo, N. A., Tarhuni, A., Tarloff, D., Tchaou, B., Tchegnonsi, C., Tchoupa, M., Teeka, M. O., Thakoor, B., Theunissen, M. M., Thomas, B. P., Thomas, M. B., Thotharam, A., Tobiko, O., Torborg, A. M., Tshisekedi, S. M., Tshisola, S. K., Tshitangano, R., Tshivhula, F., Tshuma, H. T., Tun, M., Udo, I. A., Uhuebor, D. I., Umeh, K. U., Usenbo, A. O., Uwiteyimbabazi, Jd. D., Van der Merwe, D. J., van der Walt, J. E., van Dyk, D., Van Dyk, J. G., van Niekerk, J. J. S., van Wyk, S., van Zyl, H. A., Veerasamy, B., Venter, P. J., Vermeulen, A. J., Villarreal, R., Visser, J., Visser, L., Voigt, M., von Rahden, R. P., Wafa, A., Wafula, A., Wambugu, P. K., Waryoba, P., Waweru, E. N., Weideman, M., Wise, R. D., Wynne, E. E., Yahya, A. I., Yahya, A. A., Yahya, R., Yakubu, Y., Yanga, J. J., Yangazov, Y. M., Yousef, O., Yousef, G., Yunus, A. A., Yusuf, A. S., Zeiton, A. Z., Zentuti, H. Z., Zepharine, H., Zerihun, A. B., Zhou, S., Zidan, A., Zié, S. Z., Zinyemba, C. Z., Zo, A., Zomahoun, L., Zoobei, N. Z., Zoumenou, E., and Zubia, N. Z.
- Published
- 2021
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7. Towards a standardized framework for AI-assisted, image-based monitoring of nocturnal insects
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Roy, D. B., Alison, J., August, T. A., Bélisle, M., Bjerge, K., Bowden, J. J., Bunsen, M. J., Cunha, F., Geissmann, Q., Goldmann, K., Gomez-Segura, A., Jain, A., Huijbers, C. (Chantal), Larrivée, M., Lawson, J. L., Mann, H. M., Mazerolle, M. J., McFarland, K. P., Pasi, L., Peters, S., Pinoy, N., Rolnick, D., Skinner, G. L., Strickson, O. T., Svenning, A., Teagle, S., Høye, T. T., Roy, D. B., Alison, J., August, T. A., Bélisle, M., Bjerge, K., Bowden, J. J., Bunsen, M. J., Cunha, F., Geissmann, Q., Goldmann, K., Gomez-Segura, A., Jain, A., Huijbers, C. (Chantal), Larrivée, M., Lawson, J. L., Mann, H. M., Mazerolle, M. J., McFarland, K. P., Pasi, L., Peters, S., Pinoy, N., Rolnick, D., Skinner, G. L., Strickson, O. T., Svenning, A., Teagle, S., and Høye, T. T.
- Abstract
Automated sensors have potential to standardize and expand the monitoring of insects across the globe. As one of the most scalable and fastest developing sensor technologies, we describe a framework for automated, image-based monitoring of nocturnal insects—from sensor development and field deployment to workflows for data processing and publishing. Sensors comprise a light to attract insects, a camera for collecting images and a computer for scheduling, data storage and processing. Metadata is important to describe sampling schedules that balance the capture of relevant ecological information against power and data storage limitations. Large data volumes of images from automated systems necessitate scalable and effective data processing. We describe computer vision approaches for the detection, tracking and classification of insects, including models built from existing aggregations of labelled insect images. Data from automated camera systems necessitate approaches that account for inherent biases. We advocate models that explicitly correct for bias in species occurrence or abundance estimates resulting from the imperfect detection of species or individuals present during sampling occasions. We propose ten priorities towards a step-change in automated monitoring of nocturnal insects, a vital task in the face of rapid biodiversity loss from global threats. This article is part of the theme issue ‘Towards a toolkit for global insect biodiversity monitoring’.
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- 2024
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8. Science enabled by high precision inertial formation flying
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Skinner, G. K., Dennis, B. R., Krizmanic, J. F., and Kontar, E. P.
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
The capability of maintaining two satellites in precise relative position, stable in a celestial coordinate system, would enable major advances in a number of scientific disciplines and with a variety of types of instrumentation. The common requirement is for formation flying of two spacecraft with the direction of their vector separation in inertial coordinates precisely controlled and accurately determined as a function of time. We consider here the scientific goals that could be achieved with such technology and review some of the proposals that have been made for specific missions. Types of instrumentation that will benefit from the development of this type of formation flying include 1) imaging systems, in which an optical element on one spacecraft forms a distant image recorded by a detector array on the other spacecraft, including telescopes capable of very high angular resolution; 2) systems in which the front spacecraft of a pair carries an occulting disk, allowing very high dynamic range observations of the solar corona and exoplanets; 3) interferometers, another class of instrument that aims at very high angular resolution and which, though usually requiring more than two spacecraft, demands very much the same developments., Comment: To be published in "Int. J. Space Science and Engineering". This is a revised and expanded version of a paper presented at the "5th International Conference on Spacecraft Formation Flying Missions and Technologies(SFFMT)", Munich, May 2013
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- 2013
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9. The 70 Month Swift-BAT All-Sky Hard X-Ray Survey
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Baumgartner, W. H., Tueller, J., Markwardt, C. B., Skinner, G. K., Barthelmy, S., Mushotzky, R. F., Evans, P., and Gehrels, N.
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Astrophysics - High Energy Astrophysical Phenomena - Abstract
We present the catalog of sources detected in 70 months of observations of the BAT hard X-ray detector on the Swift gamma-ray burst observatory. The Swift-BAT 70 month survey has detected 1171 hard X-ray sources (more than twice as many sources as the previous 22 month survey) in the 14-195 keV band down to a significance level of 4.8 sigma, associated with 1210 counterparts. The 70 month Swift-BAT survey is the most sensitive and uniform hard X-ray all-sky survey and reaches a flux level of 1.03e-11 ergs/sec/cm2 over 50% of the sky and 1.34e-11 ergs/sec/cm2 over 90% of the sky. The majority of new sources in the 70 month survey continue to be AGN, with over 700 in the 70 month survey catalog. As part of this new edition of the Swift-BAT catalog, we also make available 8-channel spectra and monthly-sampled lightcurves for each object detected in the survey at the Swift-BAT 70 month website., Comment: Submitted to ApJS on 16 Nov 2012. 23 pages, 15 figures. The Swift-BAT 70-month Survey public website can be found at http://swift.gsfc.nasa.gov/docs/swift/results/bs70mon/
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- 2012
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10. Very High Resolution Solar X-ray Imaging Using Diffractive Optics
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Dennis, B. R., Skinner, G. K., Li, M. J., and Shih, A. Y.
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Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Solar and Stellar Astrophysics - Abstract
This paper describes the development of X-ray diffractive optics for imaging solar flares with better than 0.1 arcsec angular resolution. X-ray images with this resolution of the \geq10 MK plasma in solar active regions and solar flares would allow the cross-sectional area of magnetic loops to be resolved and the coronal flare energy release region itself to be probed. The objective of this work is to obtain X-ray images in the iron-line complex at 6.7 keV observed during solar flares with an angular resolution as fine as 0.1 arcsec - over an order of magnitude finer than is now possible. This line emission is from highly ionized iron atoms, primarily Fe xxv, in the hottest flare plasma at temperatures in excess of \approx10 MK. It provides information on the flare morphology, the iron abundance, and the distribution of the hot plasma. Studying how this plasma is heated to such high temperatures in such short times during solar flares is of critical importance in understanding these powerful transient events, one of the major objectives of solar physics. We describe the design, fabrication, and testing of phase zone plate X-ray lenses with focal lengths of \approx100 m at these energies that would be capable of achieving these objectives. We show how such lenses could be included on a two-spacecraft formation-flying mission with the lenses on the spacecraft closest to the Sun and an X-ray imaging array on the second spacecraft in the focal plane \approx100 m away. High resolution X-ray images could be obtained when the two spacecraft are aligned with the region of interest on the Sun. Requirements and constraints for the control of the two spacecraft are discussed together with the overall feasibility of such a formation-flying mission.
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- 2012
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11. The Proposed High Energy Telescope (HET) for EXIST
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Hong, J., Grindlay, J., Allen, B., Skinner, G., Barthelmy, S., Gehrels, N., Garson, A., Krawczynski, H., Cook, W., Harrison, F., Natalucci, L., Ubertini, P., and team, the EXIST/HET
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
The hard X-ray sky now being studied by INTEGRAL and Swift and soon by NuSTAR is rich with energetic phenomena and highly variable non-thermal phenomena on a broad range of timescales. The High Energy Telescope (HET) on the proposed Energetic X-ray Imaging Survey Telescope (EXIST) mission will repeatedly survey the full sky for rare and luminous hard X-ray phenomena at unprecedented sensitivities. It will detect and localize (<20", at 5 sigma threshold) X-ray sources quickly for immediate followup identification by two other onboard telescopes - the Soft X-ray imager (SXI) and Optical/Infrared Telescope (IRT). The large array (4.5 m^2) of imaging (0.6 mm pixel) CZT detectors in the HET, a coded-aperture telescope, will provide unprecedented high sensitivity (~0.06 mCrab Full Sky in a 2 year continuous scanning survey) in the 5 - 600 keV band. The large field of view (90 deg x 70 deg) and zenith scanning with alternating-orbital nodding motion planned for the first 2 years of the mission will enable nearly continuous monitoring of the full sky. A 3y followup pointed mission phase provides deep UV-Optical-IR-Soft X-ray and Hard X-ray imaging and spectroscopy for thousands of sources discovered in the Survey. We review the HET design concept and report the recent progress of the CZT detector development, which is underway through a series of balloon-borne wide-field hard X-ray telescope experiments, ProtoEXIST. We carried out a successful flight of the first generation of fine pixel large area CZT detectors (ProtoEXIST1) on Oct 9, 2009. We also summarize our future plan (ProtoEXIST2 & 3) for the technology development needed for the HET., Comment: 10 pages, 13 figures, 2 tables, SPIE Conference "Astronomical Telescopes and Instrumentation 2010"; to appear in Proceedings SPIE (2010)
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- 2010
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12. DUAL Gamma-Ray Mission
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Boggs, S., Wunderer, C., von Ballmoos, P., Takahashi, T., Gehrels, N., Tueller, J., Baring, M., Beacom, J., Diehl, R., Greiner, J., Grove, E., Hartmann, D., Hernanz, M., Jean, P., Johnson, N., Kanbach, G., Kippen, M., Knödlseder, J., Leising, M., Madejski, G., McConnell, M., Milne, P., Motohide, K., Nakazawa, K., Oberlack, U., Phlips, B., Ryan, J., Skinner, G., Starrfield, S., Tajima, H., Wulf, E., Zoglauer, A., and Zych, A.
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
Gamma-ray astronomy presents an extraordinary scientific potential for the study of the most powerful sources and the most violent events in the Universe. In order to take full advantage of this potential, the next generation of instrumentation for this domain will have to achieve an improvement in sensitivity over present technologies of at least an order of magnitude. The DUAL mission concept takes up this challenge in two complementary ways: a very long observation of the entire sky, combined with a large collection area for simultaneous observations of Type Ia SNe. While the Wide-Field Compton Telescope (WCT) accumulates data from the full gamma-ray sky (0.1-10 MeV) over the entire mission lifetime, the Laue-Lens Telescope (LLT) focuses on 56Co emission from SNe Ia (0.8-0.9 MeV), collecting gamma-rays from its large area crystal lens onto the WCT. Two separated spacecraft flying in formation will maintain the DUAL payloads at the lens' focal distance., Comment: White paper for US National Academy of Sciences Decadal Survey "Astro2010"
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- 2010
13. Imaging and burst location with the EXIST high-energy telescope
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Skinner, G. K., Barthelmy, S. D., Finger, M. H., Hong, J., Jernigan, G. G., Sturner, S. J., Allen, B. T., and Grindlay, J. E.
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
The primary instrument of the proposed EXIST mission is a coded mask high energy telescope (the HET), that must have a wide field of view and extremely good sensitivity. It will be crucial to minimize systematic errors so that even for very long total integration times the imaging performance is close to the statistical photon limit. There is also a requirement to be able to reconstruct images on-board in near real time in order to detect and localize gamma-ray bursts. This must be done while the spacecraft is scanning the sky. The scanning provides all-sky coverage and is key to reducing systematic errors. The on-board computational problem is made even more challenging for EXIST by the very large number of detector pixels. Numerous alternative designs for the HET have been evaluated. The baseline concept adopted depends on a unique coded mask with two spatial scales. Monte Carlo simulations and analytic analysis techniques have been used to demonstrate the capabilities of the design and of the proposed two-step burst localization procedure.
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- 2010
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14. Soccer matches as experiments: how often does the 'best' team win?
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Skinner, G. K. and Freeman, G. H.
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Physics - Physics and Society ,Physics - Data Analysis, Statistics and Probability ,Statistics - Applications - Abstract
Models in which the number of goals scored by a team in a soccer match follow a Poisson distribution, or a closely related one, have been widely discussed. We here consider a soccer match as an experiment to assess which of two teams is superior and examine the probability that the outcome of the experiment (match) truly represents the relative abilities of the two teams. Given a final score, it is possible by using a Bayesian approach to quantify the probability that it was or was not the case that 'the best team won'. For typical scores, the probability of a misleading result is significant. Modifying the rules of the game to increase the typical number of goals scored would improve the situation, but a level of confidence that would normally be regarded as satisfactory could not be obtained unless the character of the game was radically changed., Comment: Contact the corresponding author in case of difficulty in accessing the published paper
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- 2009
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15. The High Energy Telescope on EXIST
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Hong, J., Grindlay, J. E., Allen, B., Barthelmy, S. D., Skinner, G. K., Gehrels, N., and Group, the EXIST HET Working
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
The Energetic X-ray Imaging Survey Telescope (EXIST) is a proposed next generation multi-wavelength survey mission. The primary instrument is a High Energy telescope (HET) that conducts the deepest survey for Gamma-ray Bursts (GRBs), obscured-accreting and dormant Supermassive Black Holes and Transients of all varieties for immediate followup studies by the two secondary instruments: a Soft X-ray Imager (SXI) and an Optical/Infrared Telescope (IRT). EXIST will explore the early Universe using high redshift GRBs as cosmic probes and survey black holes on all scales. The HET is a coded aperture telescope employing a large array of imaging CZT detectors (4.5 m^2, 0.6 mm pixel) and a hybrid Tungsten mask. We review the current HET concept which follows an intensive design revision by the HET imaging working group and the recent engineering studies in the Instrument and Mission Design Lab at the Goddard Space Flight Center. The HET will locate GRBs and transients quickly (<10-30 sec) and accurately (< 20") for rapid (< 1-3 min) onboard followup soft X-ray and optical/IR (0.3-2.2 micron) imaging and spectroscopy. The broad energy band (5-600 keV) and the wide field of view (~90 deg x 70 deg at 10% coding fraction) are optimal for capturing GRBs, obscured AGNs and rare transients. The continuous scan of the entire sky every 3 hours will establish a finely-sampled long-term history of many X-ray sources, opening up new possibilities for variability studies., Comment: 10 pages, 6 figures, 3 tables, SPIE conference proceedings (UV, X-ray, and Gamma-Ray Space Instrumentation for Astronomy XVI, 7435-9)
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- 2009
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16. The main-sequence rotation-colour relation in the Coma Berenices open cluster
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Cameron, A. Collier, Davidson, V. A., Hebb, L., Skinner, G., Anderson, D. R., Christian, D. J., Clarkson, W. I., Enoch, B., Irwin, J., Joshi, Y., Haswell, C. A., Hellier, C., Horne, K. D., Kane, S. R., Lister, T. A., Maxted, P. F. L., Norton, A. J., Parley, N., Pollacco, D., Ryans, R., Scholz, A., Skillen, I., Smalley, B., Street, R. A., West, R. G., Wilson, D. M., and Wheatley, P. J.
- Subjects
Astrophysics - Solar and Stellar Astrophysics - Abstract
We present the results of a photometric survey of rotation rates in the Coma Berenices (Melotte 111) open cluster, using data obtained as part of the SuperWASP exoplanetary transit-search programme. The goal of the Coma survey was to measure precise rotation periods for main-sequence F, G and K dwarfs in this intermediate-age (~600 Myr) cluster, and to determine the extent to which magnetic braking has caused the stellar spin periods to converge. We find a tight, almost linear relationship between rotation period and J-K colour with a root-mean square scatter of only 2 percent. The relation is similar to that seen among F, G and K stars in the Hyades. Such strong convergence can only be explained if angular momentum is not at present being transferred from a reservoir in the deep stellar interiors to the surface layers. We conclude that the coupling timescale for angular momentum transport from a rapidly-spinning radiative core to the outer convective zone must be substantially shorter than the cluster age, and that from the age of Coma onward, stars rotate effectively as solid bodies. The existence of a tight relationship between stellar mass and rotation period at a given age supports the use of stellar rotation period as an age indicator in F, G and K stars of Hyades age and older. We demonstrate that individual stellar ages can be determined within the Coma population with an internal precision of order 9 percent (RMS), using a standard magnetic braking law in which rotation period increases with the square root of stellar age. We find that a slight modification to the magnetic-braking power law, P proportional to t^0.56, yields rotational and asteroseismological ages in good agreement for the Sun and other stars of solar age for which p-mode studies and photometric rotation periods have been published., Comment: 14 pages, 10 figures, accepted for publication in MNRAS
- Published
- 2009
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17. X-ray interferometry with transmissive beam combiners for ultra-high angular resolution astronomy
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Skinner, G. K. and Krizmanic, J. F.
- Subjects
Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
Interferometry provides one of the possible routes to ultra-high angular resolution for X-ray and gamma-ray astronomy. Sub-micro-arc-second angular resolution, necessary to achieve objectives such as imaging the regions around the event horizon of a super-massive black hole at the center of an active galaxy, can be achieved if beams from parts of the incoming wavefront separated by 100s of meters can be stably and accurately brought together at small angles. One way of achieving this is by using grazing incidence mirrors. We here investigate an alternative approach in which the beams are recombined by optical elements working in transmission. It is shown that the use of diffractive elements is a particularly attractive option. We report experimental results from a simple 2-beam interferometer using a low-cost commercially available profiled film as the diffractive elements. A rotationally symmetric filled (or mostly filled) aperture variant of such an interferometer, equivalent to an X-ray axicon, is shown to offer a much wider bandpass than either a Phase Fresnel Lens (PFL) or a PFL with a refractive lens in an achromatic pair. Simulations of an example system are presented., Comment: To be published in "Experimental Astronomy"
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- 2009
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18. The 22-Month Swift-BAT All-Sky Hard X-ray Survey
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Tueller, J., Baumgartner, W. H., Markwardt, C. B., Skinner, G. K., Mushotzky, R. F., Ajello, M., Barthelmy, S., Beardmore, A., Brandt, W. N., Burrows, D., Chincarini, G., Campana, S., Cummings, J., Cusumano, G., Evans, P., Fenimore, E., Gehrels, N., Godet, O., Grupe, D., Holland, S., Kennea, J., Krimm, H. A., Koss, M., Moretti, A., Mukai, K., Osborne, J. P., Okajima, T., Pagani, C., Page, K., Palmer, D., Parsons, A., Schneider, D. P., Sakamoto, T., Sambruna, R., Sato, G., Stamatikos, M., Stroh, M., Ukwatta, T. N., and Winter, L.
- Subjects
Astrophysics - High Energy Astrophysical Phenomena ,Astrophysics - Cosmology and Extragalactic Astrophysics - Abstract
We present the catalog of sources detected in the first 22 months of data from the hard X-ray survey (14--195 keV) conducted with the BAT coded mask imager on the \swift satellite. The catalog contains 461 sources detected above the 4.8 sigma level with BAT. High angular resolution X-ray data for every source from Swift XRT or archival data have allowed associations to be made with known counterparts in other wavelength bands for over 97% of the detections, including the discovery of ~30 galaxies previously unknown as AGN and several new Galactic sources. A total of 266 of the sources are associated with Seyfert galaxies (median redshift z ~ 0.03) or blazars, with the majority of the remaining sources associated with X-ray binaries in our Galaxy. This ongoing survey is the first uniform all sky hard X-ray survey since HEAO-1 in 1977. Since the publication of the 9-month BAT survey we have increased the number of energy channels from 4 to 8 and have substantially increased the number of sources with accurate average spectra. The BAT 22-month catalog is the product of the most sensitive all-sky survey in the hard X-ray band, with a detection sensitivity (4.8 sigma) of 2.2e-11 erg/cm2/s (1 mCrab) over most of the sky in the 14--195 keV band., Comment: Accepted by the Astrophysical Journal Supplement Series. 27 pages. This version was accepted by the journal and includes changes to the text and figures in response to the referee's comments. The main data table remains substantially the same as the previous version
- Published
- 2009
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19. Super-Orbital Variability in Hard X-rays
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Farrell, S. A., Barret, D., and Skinner, G. K.
- Subjects
Astrophysics - Abstract
We present the results of a study with the \emph{Swift} Burst Alert Telescope in the 14 -- 195 keV range of the long-term variability of 5 low mass X-ray binaries with reported or suspected super-orbital periods -- 4U 1636-536, 4U 1820-303, 4U 1916-053, Cyg X-2 and Sco X-1. No significant persistent periodic modulation was detected around the previously reported periods in the 4U 1916-053, Cyg X-2 or Sco X-1 light curves. The $\sim$170 d period of 4U 1820-303 was detected up to 24 keV, consistent with variable accretion due to the previously proposed triple system model. The $\sim$46 d period in 4U 1636-536 was detected up to 100 keV, with the modulation in the low and high energy bands found to be phase shifted by $\sim180^\circ$ with respect to each other. This phase shift, when taken together with the near-coincident onset of the $\sim$46 d modulation and the low/hard X-ray state, leads us to speculate that the modulation could herald transient jet formation., Comment: 19 pages, 16 figures, 3 tables, accepted for publication in MNRAS
- Published
- 2008
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20. Swift Observations of Shock Evolution in RS Ophiuchi
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Bode, M. F., Osborne, J. P., Page, K. L., Beardmore, A. P., O'Brien, T. J., Ness, J. -U., Starrfield, S., Skinner, G. K., Darnley, M. J., Drake, J. J., Evans, A., Eyres, S. P. S., Krautter, J., and Schwarz, G.
- Subjects
Astrophysics - Abstract
Our \textit{Swift} observations of RS Oph form an unprecedented X-ray dataset to undertake investigations of both the central source and the interaction of the outburst ejecta with the circumstellar environment. Over the first month, the XRT data are dominated by emission from rapidly evolving shocks. We discuss the differences in derived parameters from those found for \textit{RXTE} at early times and the evolution of the X-ray emission to much later times. It is apparent that at late times several emission components are present. We find no strong evidence of the proposed shock break-out in our data., Comment: 5 pages, 3 figures, to appear in ASP conference proceedings Volume 401 "RS Ophiuchi (2006) and the recurrent nova phenomenon"
- Published
- 2008
21. R&D progress on second-generation crystals for Laue lens applications
- Author
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Barrière, N., von Ballmoos, P., Bastie, P., Courtois, P., Abrosimov, N. V., Andersen, K., Buslaps, T., Camus, T., Halloin, H., Jentschel, M., Knodlseder, J., Roudil, G., Serre, D., and Skinner, G.
- Subjects
Astrophysics - Abstract
The concept of a gamma-ray telescope based on a Laue lens offers the possibility to increase the sensitivity by more than an order of magnitude with respect to existing instruments. Laue lenses have been developed by our collaboration for several years : the main achievement of this R&D program was the CLAIRE lens prototype. Since then, the endeavour has been oriented towards the development of efficient diffracting elements (crystal slabs), the aim being to step from a technological Laue lens to a scientifically exploitable lens. The latest mission concept featuring a gamma-ray lens is the European Gamma-Ray Imager (GRI) which intends to make use of the Laue lens to cover energies from 200 keV to 1300 keV. Investigations of two promising materials, low mosaicity copper and gradient concentration silicon-germanium are presented in this paper. The measurements have been performed during three runs on beamline ID15A of the European Synchrotron Radiation Facility, and on the GAMS 4 instrument of the Institute Laue-Langevin (both in Grenoble, France) using highly monochromatic beam of energy close to 500 keV. Despite it was not perfectly homogeneous, the presented copper crystal exhibits peak reflectivity of 25% in accordance with theoretical predictions, and a mosaicity around 26 arcsec, the ideal range for the realization of a Laue lens such as GRI. Silicon-germanium featuring a constant gradient have been measured for the very first time at 500 keV. Two samples showed a quite homogeneous reflectivity reaching 26%, which is far from the 48% already observed in experimental crystals but a very encouraging beginning. This results have been used to estimate the performance of the GRI Laue lens design.
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- 2008
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22. Detectability of gamma-ray emission from classical novae with Swift/BAT
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Senziani, F., Skinner, G. K., Jean, P., and Hernanz, M.
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Astrophysics - Abstract
Classical novae are expected to emit gamma rays during their explosions. The most important contribution to the early gamma-ray emission comes from the annihilation with electrons of the positrons generated by the decay of 13N and 18F. The photons are expected to be down-scattered to a few tens of keV, and the emission is predicted to occur some days before the visual discovery and to last ~2 days. Despite a number of attempts, no positive detections of such emission have been made, due to lack of sensitivity and of sky coverage. Because of its huge field of view, good sensitivity, and well-adapted energy band, Swift/BAT offers a new opportunity for such searches. BAT data can be retrospectively used to search for prompt gamma-ray emission from the direction of novae after their optical discovery. We have estimated the expected success rate for the detection with BAT of gamma rays from classical novae using a Monte Carlo approach. Searches were performed for emission from novae occurring since the launch of Swift. Using the actual observing program during the first 2.3 years of BAT operations as an example, and sensitivity achieved, we estimate the expected rate of detection of classical novae with BAT as ~0.2-0.5/yr, implying that several should be seen within a 10 yr mission. The search for emission in the directions of the 24 classical novae discovered since the Swift launch yielded no positive results, but none of these was known to be close enough for this to be a surprise. Detections of a recurrent nova (RS Oph) and a nearby dwarf nova (V455 And) demonstrate the efficacy of the technique. The absence of detections is consistent with the expectations from the Monte Carlo simulations, but the long-term prospects are encouraging given an anticipated Swift operating lifetime of ~10 years., Comment: 10 pages, 6 figures. Accepted for publication in A&A
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- 2008
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23. Mortality of the immature stages of the cabbage root fly
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Finch, S., primary and Skinner, G., additional
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- 2020
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24. Emergence of cabbage root flies from puparia collected throughout northern Europe
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Finch, S., primary, Bromand, B., additional, Brunel, E., additional, Bues, M., additional, Collier, R.H., additional, Dunne, R., additional, Foster, G., additional, Freuler, J., additional, Hommes, M., additional, Van Keymeulen, M., additional, Mowat, D.J., additional, Pelerents, C., additional, Skinner, G., additional, Städler, E., additional, and Theunissen, J., additional
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- 2020
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25. Field and laboratory studies on the behaviour of the carrot fly, Psila rosae
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Skinner, G., primary and Finch, S., additional
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- 2020
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26. Oilseed rape crops as a source of cabbage root fly infestations for cruciferous vegetable crops
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Skinner, G., primary and Finch, S., additional
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- 2020
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27. Swift BAT Survey of AGN
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Tueller, J., Mushotzky, R. F., Barthelmy, S., Cannizzo, J. K., Gehrels, N., Markwardt, C. B., Skinner, G. K., and Winter, L. M.
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Astrophysics - Abstract
We present the results of the analysis of the first 9 months of data of the Swift BAT survey of AGN in the 14-195 keV band. Using archival X-ray data or follow-up Swift XRT observations, we have identified 129 (103 AGN) of 130 objects detected at |b|> 15 deg and with significance >4.8 sigma. One source remains unidentified. These same X-ray data have allowed measurement of the X-ray properties of the objects. We fit a power law to the log N - log S distribution, and find the slope to be 1.42+/-0.14. Characterizing the differential luminosity function data as a broken power law, we find a break luminosity log L_*(erg/s) = 43.85+/-0.26, a low luminosity power law slope a=0.84^{+0.16}_{-0.22}, and a high luminosity power law slope b=2.55^{+0.43}_{-0.30}, similar to the values that have been reported based on INTEGRAL data. We obtain a mean photon index 1.98 in the 14-195 keV band, with an rms spread of 0.27. Integration of our luminosity function gives a local volume density of AGN above 10^{41} erg/s of 2.4x10^{-3}/Mpc^3, which is about 10% of the total luminous local galaxy density above M_*=-19.75. We have obtained X-ray spectra from the literature and from Swift XRT follow-up observations. These show that the distribution of log n_H is essentially flat from n_H=10^{20}/cm^{2} to 10^{24}/cm^2, with 50% of the objects having column densities of less than 10^{22}/cm^{2}. BAT Seyfert galaxies have a median redshift of 0.03, a maximum log luminosity of 45.1, and approximately half have log n_H > 22., Comment: 15 pages, 15 figures, 2 tables; to appear in the Astrophysical Journal, July 10, 2008, v. 681
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- 2007
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28. EXIST's Gamma-Ray Burst Sensitivity
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Band, D. L., Grindlay, J. E., Hong, J., Fishman, G., Hartmann, D. H., Garson III, A., Krawczynski, H., Barthelmy, S., Gehrels, N., and Skinner, G.
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Astrophysics - Abstract
We use semi-analytic techniques to evaluate the burst sensitivity of designs for the EXIST hard X-ray survey mission. Applying these techniques to the mission design proposed for the Beyond Einstein program, we find that with its very large field-of-view and faint gamma-ray burst detection threshold, EXIST will detect and localize approximately two bursts per day, a large fraction of which may be at high redshift. We estimate that EXIST's maximum sensitivity will be ~4 times greater than that of Swift's Burst Alert Telescope. Bursts will be localized to better than 40 arcsec at threshold, with a burst position as good as a few arcsec for strong bursts. EXIST's combination of three different detector systems will provide spectra from 3 keV to more than 10 MeV. Thus, EXIST will enable a major leap in the understanding of bursts, their evolution, environment, and utility as cosmological probes., Comment: 25 pages, 10 figures, accepted by ApJ
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- 2007
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29. The sky distribution of 511 keV positron annihilation line emission as measured with INTEGRAL/SPI
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Weidenspointner, G., Knoedlseder, J., Jean, P., Skinner, G. K., Roques, J. -P., Vedrenne, G., Milne, P., Teegarden, B. J., Diehl, R., Strong, A., Schanne, S., Cordier, B., and Winkler, C.
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Astrophysics - Abstract
The imaging spectrometer SPI on board ESA's INTEGRAL observatory provides us with an unprecedented view of positron annihilation in our Galaxy. The first sky maps in the 511 keV annihilation line and in the positronium continuum from SPI showed a puzzling concentration of annihilation radiation in the Galactic bulge region. By now, more than twice as many INTEGRAL observations are available, offering new clues to the origin of Galactic positrons. We present the current status of our analyses of this augmented data set. We now detect significant emission from outside the Galactic bulge region. The 511 keV line is clearly detected from the Galactic disk; in addition, there is a tantalizing hint at possible halo-like emission. The available data do not yet permit to discern whether the emission around the bulge region originates from a halo-like component or from a disk component that is very extended in latitude., Comment: to be published in the proceedings of the 6th INTEGRAL Workshop "The Obscured Universe" (3-7 July 2006, Moscow)
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- 2007
30. Effect of Ca on the Microstructure and Mechanical Properties in Mg Alloys
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Andritsos, E. I., Skinner, G. C. G., Paxton, A. T., Orlov, Dmytro, editor, Joshi, Vineet, editor, Solanki, Kiran N., editor, and Neelameggham, Neale R., editor
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- 2018
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31. VLTI/AMBER interferometric observations of the recurrent Nova RS Oph 5.5 days after outburst
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Chesneau, Olivier, Nardetto, N., Millour, F., Hummel, Ch., De Souza, A. Domiciano, Bonneau, D., Vannier, M., Rantakyro, F. T., Spang, A., Malbet, F., Mourard, D., Bode, M. F., O'brien, T. J., Skinner, G., Petrov, R., Stee, Ph., Tatulli, E., and Vakili, F.
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Astrophysics - Abstract
We report on interferometric AMBER/VLTI observations of the recurrent nova RS Oph five days after its outburst on 2006 Feb 12. Using three baselines from 44 to 86m, and a spectral resolution of 1500, we measured the extension of the emission in the K band continuum and in the BrG and HeI2.06 micron lines. The continuum visibilities were interpreted by fitting simple geometric models consisting of uniform and Gaussian ellipses, ring and binary models. The visibilities and differential phases in the BrG line were interpreted using skewed ring models aiming to perform a limited parametric reconstruction of the extension and kinematics of the line forming region. The limited uv coverage does not allow discrimination between filled models and rings. Binary models are discarded because the measured closure phase in the continuum is close to zero. The visibilities in the lines are at a low level compared to their nearby continuum, consistent with a more extended line forming region for HeI2.06 than BrG. The ellipse models for the continuum and for the lines are highly flattened and share the same position angle. Two radial velocity fields are apparent in the BrG line: a 'slow' expanding ring-like structure (v~1800km/s), and a 'fast' structure extended in the E-W direction (v~2500-3000km/s). These results confirm the basic fireball model, contrary to the conclusions of other interferometric observations conducted by Monnier et al. (2006)., Comment: Accepted in A&A
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- 2006
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32. Swift observations of the 2006 outburst of the recurrent nova RS Ophiuchi: I. Early X-ray emission from the shocked ejecta and red giant wind
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Bode, M. F., O'Brien, T. J., Osborne, J. P., Page, K. L., Senziani, F., Skinner, G. K., Starrfield, S., Ness, J-U., Drake, J. J., Schwarz, G., Beardmore, A. P., Darnley, M. J., Eyres, S. P. S., Evans, A., Gehrels, N., Goad, M. R., Jean, P., Krautter, J., and Novara, G.
- Subjects
Astrophysics - Abstract
RS Ophiuchi began its latest outburst on 2006 February 12. Previous outbursts have indicated that high velocity ejecta interact with a pre-existing red giant wind, setting up shock systems analogous to those seen in Supernova Remnants. However, in the previous outburst in 1985, X-ray observations did not commence until 55 days after the initial explosion. Here we report on Swift observations covering the first month of the 2006 outburst with the Burst Alert (BAT) and X-ray Telescope (XRT) instruments. RS Oph was clearly detected in the BAT 14-25 keV band from t=0 to $t\sim6$ days. XRT observationsfrom 0.3-10 keV, started at 3.17 days after outburst. The rapidly evolving XRT spectra clearly show the presence of both line and continuum emission which can be fitted by thermal emission from hot gas whose characteristic temperature, overlying absorbing column, $[N_H]_W$, and resulting unabsorbed total flux decline monotonically after the first few days. Derived shock velocities are in good agreement with those found from observations at other wavelengths. Similarly, $[N_H]_W$ is in accord with that expected from the red giant wind ahead of the forward shock. We confirm the basic models of the 1985 outburst and conclude that standard Phase I remnant evolution terminated by $t\sim10$ days and the remnant then rapidly evolved to display behaviour characteristic of Phase III. Around t=26 days however, a new, luminous and highly variable soft X-ray source began to appear whose origin will be explored in a subsequent paper., Comment: 20 pages, 4 figures (2 updated), accepted by ApJ
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- 2006
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33. Gamma Ray Fresnel lenses - why not?
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Skinner, G. K.
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Astrophysics - Abstract
Fresnel lenses offer the possibility of concentrating the flux of X-rays or gamma-rays flux falling on a geometric area of many square metres onto a focal point which need only be a millimetre or so in diameter (and which may even be very much smaller). They can do so with an efficiency that can approach 100%, and yet they are easily fabricated and have no special alignment requirements. Fresnel lenses can offer diffraction-limited angular resolution, even in a domain where that limit corresponds to less than a micro second of arc. Given all these highly desirable attributes, it is natural to ask why Fresnel gamma ray lenses are not already being used, or at least why there is not yet any mission that plans to use the technology. Possible reasons (apart from the obvious one that nobody thought of doing so) include the narrow bandwidth of simple Fresnel lenses, their very long focal length, and the problems of target finding. It is argued that none of these is a "show stopper" and that this technique should be seriously considered for nuclear astrophysics., Comment: Presented at "Gamma Wave 2005", Bonifacio, September 2005. To be published in "Experimental Astronomy"
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- 2006
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34. The sky distribution of positronium annihilation continuum emission measured with SPI/INTEGRAL
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Weidenspointner, G., Shrader, C. R., Knoedlseder, J., Jean, P., Lonjou, V., Guessoum, N., Diehl, R., Gillard, W., Harris, M. J., Skinner, G. K., von Ballmoos, P., Vedrenne, G., Roques, J. -P., Schanne, S., Sizun, P., Teegarden, B. J., Schoenfelder, V., and Winkler, C.
- Subjects
Astrophysics - Abstract
We present a measurement of the sky distribution of positronium (Ps) annihilation continuum emission obtained with the SPI spectrometer on board ESA's INTEGRAL observatory. The only sky region from which significant Ps continuum emission is detected is the Galactic bulge. The Ps continuum emission is circularly symmetric about the Galactic centre, with an extension of about 8 deg FWHM. Within measurement uncertainties, the sky distribution of the Ps continuum emission is consistent with that found by us for the 511 keV electron-positron annihilation line using SPI. Assuming that 511 keV line and Ps continuum emission follow the same spatial distribution, we derive a Ps fraction of 0.92 +/- 0.09. These results strengthen our conclusions regarding the origin of positrons in our Galaxy based on observations of the 511 keV line. In particular, they suggest that the main source of Galactic positrons is associated with an old stellar population, such as Type Ia supernovae, classical novae, or low-mass X-ray binaries. Light dark matter is a possible alternative source of positrons., Comment: accepted for publication by A&A
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- 2006
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35. The ECLAIRs micro-satellite mission for gamma-ray burst multi-wavelength observations
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Schanne, S., Atteia, J. -L., Barret, D., Basa, S., Boer, M., Casse, F., Cordier, B., Daigne, F., Klotz, A., Limousin, O., Manchanda, R., Mandrou, P., Mereghetti, S., Mochkovitch, R., Paltani, S., Paul, J., Petitjean, P., Pons, R., Ricker, G., and Skinner, G.
- Subjects
Astrophysics - Abstract
Gamma-ray bursts (GRB), at least those with a duration longer than a few seconds are the most energetic events in the Universe and occur at cosmological distances. The ECLAIRs micro-satellite, to be launched in 2009, will provide multi-wavelength observations of GRB, to study their astrophysics and to use them as cosmological probes. Furthermore in 2009 ECLAIRs is expected to be the only space borne instrument capable of providing a GRB trigger in near real-time with sufficient localization accuracy for GRB follow-up observations with the powerful ground based spectroscopic telescopes available by then. A "Phase A study" of the ECLAIRs project has recently been launched by the French Space Agency CNES, aiming at a detailed mission design and selection for flight in 2006. The ECLAIRs mission is based on a CNES micro-satellite of the "Myriade" family and dedicated ground-based optical telescopes. The satellite payload combines a 2 sr field-of-view coded aperture mask gamma-camera using 6400 CdTe pixels for GRB detection and localization with 10 arcmin precision in the 4 to 50 keV energy band, together with a soft X-ray camera for onboard position refinement to 1 arcmin. The ground-based optical robotic telescopes will detect the GRB prompt/early afterglow emission and localize the event to arcsec accuracy, for spectroscopic follow-up observations., Comment: 7 pages, 1 figure, proceedings of the conference "New Developments in Photodetection", Beaune (France), June 25005. Submitted to NIM-A (Elsevier Science)
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- 2006
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36. The Swift/BAT High Latitude Survey: First Results
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Markwardt, C. B., Tueller, J., Skinner, G. K., Gehrels, N., Barthelmy, S. D., and Mushotzky, R. F.
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Astrophysics - Abstract
We present preliminary results from the first 3 months of the Swift BAT high galactic latitude survey in the 14--195 keV band. The survey reaches a flux of \~10^{-11} erg/cm^2/s and has ~2.7' (90% confidence) positional uncertainties for the faintest sources. This represents the most sensitive survey to date in this energy band. These data confirm the conjectures that a high energy selected AGN sample would have very different properties from those selected in other bands and represent a `true' sample of the AGN population. We have identified 86% of the 66 high-latitude sources. 12 are galactic type sources and 44 can be identified with previously known AGN. All but 5 of the AGN have archival X-ray spectra, enabling the estimation of line of sight column densities and other spectral properties. Both of the z > 0.11 objects are Blazars. The median redshift of the others (excluding radio-loud objects) is 0.012. We find that the column density distribution of these AGN is bimodal with 64% of the non-blazar sources having column densities N_H >= 10^{22} cm$^{-2}$. None of the sources with log L_X > 43.5 show high column densities and very few of the lower L_X sources have low column densities. Based on these data, we expect the final BAT catalog to have >200 AGN and reach fluxes of less than ~10^{-11} erg/cm^2/s over the entire sky., Comment: Final version submitted to ApJ Letters; on-line only Table 1 is included in-full in the article text
- Published
- 2005
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37. Monte-Carlo simulations of the expected imaging performance of the EXIST high-energy telescope
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Vadawale, S. V., Hong, J., Grindlay, J. E., and Skinner, G.
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Astrophysics - Abstract
EXIST is being studied as the Black Hole Finder Probe, one of the 3 Einstein Probe missions under NASA's Beyond Einstein program. The major science goals for EXIST include highly sensitive full-sky hard X-ray survey in a very wide energy band of 5-600 keV. The scientific requirements of wide energy band (10-600 keV for the High Energy Telescope considered for EXIST) and large field of view (approximately 130 deg x 60 deg in the current design, incorporating an array of 18 contiguous very large area coded aperture telescopes) presents significant imaging challenges. The requirement of achieving high imaging sensitivity puts stringent limits on the uniformity and knowledge of systematics for the detector plane. In order to accomplish the ambitious scientific requirements of EXIST, it is necessary to implement many novel techniques. Here we present the initial results of our extensive Monte-Carlo simulations of coded mask imaging for EXIST to estimate the performance degradation due to various factors affecting the imaging such as the non-ideal detector plane and bright partially coded sources., Comment: 12 pages, 12 figures, 1 table, appears in SPIE 2005 proceedings (5900: Optics for EUV, X-ray, and Gamma-ray Astronomy II)
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- 2005
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38. The all-sky distribution of 511 keV electron-positron annihilation emission
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Knödlseder, J., Jean, P., Lonjou, V., Weidenspointner, G., Guessoum, N., Gillard, W., Skinner, G., von Ballmoos, P., Vedrenne, G., Roques, J. -P., Schanne, S., Teegarden, B., Schönfelder, V., and Winkler, C.
- Subjects
Astrophysics - Abstract
We present a map of 511 keV electron-positron annihilation emission, based on data accumulated with the SPI spectrometer aboard ESA's INTEGRAL gamma-ray observatory, that covers approximately 95% of the celestial sphere. 511 keV line emission is significantly detected towards the galactic bulge region and, at a very low level, from the galactic disk. The bulge emission is highly symmetric and is centred on the galactic centre with an extension of 8 deg. The emission is equally well described by models that represent the stellar bulge or halo populations. The disk morphology is only weakly constrained by the present data, being compatible with both the distribution of young and old stellar populations. The 511 keV line flux from the bulge and disk components is 1.05e-3 ph cm-2 s-1 and 0.7e-3 ph cm-2 s-1, respectively, corresponding to a bulge-to-disk flux ratio in the range 1-3. Assuming a positronium fraction of 0.93 this translates into annihilation rates of 1.5e43 s-1 and 3e42 s-1, respectively. The ratio of the bulge luminosity to that of the disk is in the range 3-9. We find no evidence for a point-like source in addition to the diffuse emission, down to a typical flux limit of 1e-4 ph cm-2 s-1. We also find no evidence for the positive latitude enhancement that has been reported from OSSE measurements; our 3 sigma upper flux limit for this feature is 1.5e-4 ph cm-2 s-1. The disk emission can be attributed to the beta+ decay of the radioactive species 26Al and 44Ti. The bulge emission arises from a different source which has only a weak or no disk component. We suggest that Type Ia supernovae and/or low-mass X-ray binaries are the prime candidates for the source of the galactic bulge positrons. Light dark matter annihilation could also explain the observed 511 keV bulge emission characteristics., Comment: accepted for publication in A&A
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- 2005
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39. SPI energy calibration
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Lonjou, V., Knodlseder, J., Roques, J. P., Skinner, G. K., von Ballmoos, P., Jean, P., Paul, P., Weidenspointner, G., Wunderer, C., and Schanne, S.
- Subjects
Astrophysics - Abstract
The status of the SPI energy calibration after the first year of INTEGRAL operations is reported. We have studied the gain variations and we have demonstrated that the most important parameter is the germanium detector temperature. This study permits us to determine the limits of our calibration method and the frequency of calibrations needed., Comment: 3 pages, 7 figures
- Published
- 2005
40. On the high coherence of kilo-Hz Quasi-Periodic Oscillations
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Barret, D., Kluzniak, W., Olive, J. F., Paltani, S., and Skinner, G. K.
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Astrophysics - Abstract
We have carried out a systematic study of the properties of the kilo-Hertz quasi-periodic oscillations (QPO) observed in the X-ray emission of the neutron star low-mass X-ray binary 4U1608-52, using archival data obtained with the Rossi X-ray Timing Explorer. We have investigated the quality factor, Q, of the oscillations (defined as the ratio of the frequency of the QPO peak to its full width at half maximum). In order to minimise the effect of long-term frequency drifts, power spectra were computed over the shortest times permitted by the data statistics. We show that the high Q of ~200 reported by Berger et al. (1996) for the lower frequency kilo-Hz QPO in one of their observations is by no means exceptional, as we observe a mean Q value in excess of 150 in 14 out of the 21 observations analysed and Q can remain above 200 for thousands of seconds. The frequency of the QPO varies over the wide range 560--890 Hz and we find a systematic trend for the coherence time of the QPO, estimated as tau=Q /(pi nu), to increase with the frequency, up to a maximum level at ~ 800 Hz, beyond which it appears to decrease, at frequencies where the QPO weakens. There is a more complex relationship between tau and the QPO root mean squared amplitude (RMS), in which positive and negative correlations can be found. A higher-frequency QPO, revealed by correcting for the frequency drift of the 560-890 Hz one, has a much lower Q (~10) which does not follow the same pattern. We discuss these results in the framework of competing QPO models and show that those involving clumps orbiting within or above the accretion disk are ruled out., Comment: Accepted for publication in MNRAS, 8 pages, 6 figures, 3 Tables
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- 2004
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41. Rapid variability of the kHz-QPO frequency in 4U1608-52
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Paltani, S., Barret, D., Olive, J. F., and Skinner, G. K.
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Astrophysics - Abstract
We investigate the variability of the QPO frequency in 4U1608-52 on very short time scales of a few seconds. We detect changes in frequency as fast as 0.5 Hz/s, which is more than ten times the fastest change reported for this object. Using a structure function analysis, we are able to detect variability on time scales as short as ~4 seconds. We do not detect any time asymmetry in the QPO-frequency history. These results have important consequences on the measurement of the QPO coherence., Comment: Proceedings of the Annual meeting of the French Astronomical Society (SF2A), in press, 4 pages, 4 figures
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- 2004
42. SPI observations of positron annihilation radiation from the 4th galactic quadrant: Spectroscopy
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Lonjou, V., Weidenspointner, G., Knodlseder, J., Jean, P., Allain, M., von Ballmoos, P., Harris, M. J., Roques, J. P., Skinner, G. K., Teegarden, B. J., Gehrels, N., Guessoum, N., Chapuis, C., Durouchoux, Ph., Cisana, E., and Valsesia, M.
- Subjects
Astrophysics - Abstract
The status of the analysis of the electron/positron annihilation radiation performed by INTEGRAL/SPI in the 4th GALACTIC QUADRANT is reported. We use data from the first two Galactic Center Deep Exposures (GCDE) and from the Galactic Plane Scans (GPS). The analysis presented here is focused on the spectroscopic aspects of the electron/positron annihilation radiation. Background substraction and model fitting methods are described, and the parameters of the 511 keV line (flux, energy, and width) are deduced., Comment: 4 pages, 5 figures, accepted for publication in the proceedings of the 5th INTEGRAL Workshop (held in Munich, 2004)
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- 2004
43. The ECLAIRs micro-satellite for multi-wavelength studies of gamma-ray burst prompt emission
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Schanne, S., Atteia, J. -L., Barret, D., Basa, S., Boer, M., Cordier, B., Daigne, F., Ealet, A., Goldoni, P., Klotz, A., Limousin, O., Mandrou, P., Mochkovitch, R., Paltani, S., Paul, J., Petitjean, P., Pons, R., and Skinner, G.
- Subjects
Astrophysics - Abstract
The cosmological revolution of 1997 has established that (at least long duration) gamma-ray bursts (GRB) are among the most energetic events in the Universe and occur at cosmological distances. The ECLAIRs micro-satellite, to be launched in 2009, will provide multi-wavelength observations for astrophysical studies of GRB and for their possible use as cosmological probes. It is expected to be the only space borne GRB trigger available for ground based robotic telescopes operational at that time. This paper presents the ECLAIRs project and its status. An X/gamma-ray camera onboard ECLAIRs with a wide field of view of 2 sr, will detect ~100 GRB/yr in the 4-50 keV energy range, localize the GRB with a precision of ~10 arcmin on the sky, and transmit this information to the ground in near real-time, as a GRB trigger for ground based optical telescopes. Inspired by the INTEGRAL imager IBIS, it is based on a CdTe detection plane covering 1000 cm^2, placed 35 cm below a coded mask. An optical camera, sensitive to magnitude-15 stars, covering up to 1/4th of the X/gamma-ray camera's field of view, will observe the prompt emission and a possible precursor of ~10 GRB/yr in the visible-band. Used in a continuous acquisition mode at a rate of ~5 images/s dumped into an on-board memory, a GRB event sent by the X/gamma-ray camera triggers a seek-back in memory for the GRB optical precursor. The full X/gamma-ray and visible-band data of a GRB are sent to ground when a high data-rate telemetry ground receiver is reachable., Comment: 8 pages, 11 figures, IEEE NSS 2004 conference, submitted to IEEE Transact. Nucl. Sci
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- 2004
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44. INTEGRAL/SPI Limits on Electron-Positron Annihilation Radiation from the Galactic Plane
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Teegarden, B. J., Watanabe, K., Jean, P., Knodlseder, J., Lonjou, V., Roques, J. P., Skinner, G. K., von Ballmoos, P., Weidenspointner, G., Bazzano, A., Butt, Y. M., Decourchelle, A., Fabian, A. C., Goldwurm, A., Gudel, M., Hannikainen, D. C., Hartmann, D. H., Hornstrup, A., Lewin, W. H. G., Makishima, K., Malzac, A., Miller, J., Parmar, A. N., Reynolds, S. P, Rothschild, R. E., Tomsick, J. A., and Vink, J.
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Astrophysics - Abstract
The center of our Galaxy is a known strong source of electron-positron 511-keV annihilation radiation. Thus far, however, there have been no reliable detections of annihilation radiation outside of the central radian of our Galaxy. One of the primary objectives of the INTEGRAL (INTErnational Gamma-RAy Astrophysics Laboratory) mission, launched in Oct. 2002, is the detailed study of this radiation. The Spectrometer on INTEGRAL (SPI) is a high resolution coded-aperture gamma-ray telescope with an unprecedented combination of sensitivity, angular resolution and energy resolution. We report results from the first 10 months of observation. During this period a significant fraction of the observing time was spent in or near the Galactic Plane. No positive annihilation flux was detected outside of the central region (|l| > 40 deg) of our Galaxy. In this paper we describe the observations and data analysis methods and give limits on the 511-keV flux., Comment: Accepted for publication in the Astrophysical Journal. 13 pages, 3 figures
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- 2004
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45. The INTEGRAL View of the Galactic Nucleus
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Goldwurm, A., Belanger, G., Goldoni, P., Paul, J., Terrier, R., Falanga, M., Ubertini, P., Bazzano, A., Del Santo, M., Winkler, C., Parmar, A. N., Kuulkers, E., Ebisawa, K., Roques, J. P., Skinner, G., Lund, N., Melia, F., and Yusef-Zadeh, F.
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Astrophysics - Abstract
We present the preliminary results of the observational campaign performed in 2003 to study the Galactic Nucleus with INTEGRAL. The mosaicked images obtained with the IBIS/ISGRI coded aperture instrument in the energy range above 20 keV, give a yet unseen view of the high-energy sources of this region in hard X and gamma-rays, with an angular resolution of 12'. We report on the discovery of a source, IGR J17456-2901, compatible with the instrument's point spread function and coincident with the Galactic Nucleus Sgr A* to within 0.9'. The source is visible up to 60-80 keV with a 20-100 keV luminosity at 8 kpc of 3 x 10E35 erg/s. Although we cannot unequivocally associate the new INTEGRAL source to the Galactic Nucleus, this is the first report of significant hard X-ray emission from within the inner 10' of the Galaxy and a contribution from the galactic center supermassive black hole itself cannot be excluded. Here we discuss the results obtained and the perspectives for future observations of the Galactic Nucleus with INTEGRAL and other observatories, Comment: 6 pages, 4 figures. Proceedings of the 5th INTEGRAL Workshop 'The INTEGRAL Universe', Munich, 16-20 February 2004, to be published in ESA SP-552
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- 2004
46. SPI observations of positron annihilation radiation from the 4th galactic quadrant: sky distribution
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Weidenspointner, G., Lonjou, V., Knoedlseder, J., Jean, P., Allain, M., von Ballmoos, P., Harris, M. J., Skinner, G. K., Vedrenne, G., Teegarden, B. J., Gehrels, N., Guessoum, N., Schoenfelder, V., Chapuis, C., Durouchoux, Ph., Cisana, E., and Valsesia, M.
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Astrophysics - Abstract
During its first year in orbit the INTEGRAL observatory performed deep exposures of the Galactic Center region and scanning observations of the Galactic plane. We report on the status of our analysis of the positron annihilation radiation from the 4th Galactic quadrant with the spectrometer SPI, focusing on the sky distribution of the 511 keV line emission. The analysis methods are described; current constraints and limits on the Galactic bulge emission and the bulge-to-disk ratio are presented., Comment: 4 pages, 2 figures, accepted for publication in the proceedings of the 5th INTEGRAL workshop
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- 2004
47. The INTEGRAL/SPI response and the Crab observations
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Sizun, P., Shrader, C. R., Attie, D., Dubath, P., Schanne, S., Cordier, B., Sturner, S. J., Bouchet, L., Roques, J. -P., Skinner, G. K., and Connell, P.
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Astrophysics ,Physics - Instrumentation and Detectors - Abstract
The Crab region was observed several times by INTEGRAL for calibration purposes. This paper aims at underlining the systematic interactions between (i) observations of this reference source, (ii) in-flight calibration of the instrumental response and (iii) the development and validation of the analysis tools of the SPI spectrometer. It first describes the way the response is produced and how studies of the Crab spectrum lead to improvements and corrections in the initial response. Then, we present the tools which were developed to extract spectra from the SPI observation data and finally a Crab spectrum obtained with one of these methods, to show the agreement with previous experiments. We conclude with the work still ahead to understand residual uncertainties in the response., Comment: 4 pages, 4 figures, Proc. of the 5th INTEGRAL Workshop (Feb. 16-20 2004), to be published by ESA
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- 2004
48. SPI/INTEGRAL in-flight performance
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Roques, J. -P., Schanne, S., von Kienlin, A., Knödlseder, J., Briet, R., Bouchet, L., Paul, Ph., Boggs, S., Caraveo, P., Cassé, M., Cordier, B., Diehl, R., Durouchoux, P., Jean, P., Leleux, P., Lichti, G., Mandrou, P., Matteson, J., Sanchez, F., Schönfelder, V., Skinner, G., Strong, A., Teegarden, B., Vedrenne, G., von Ballmoos, P., and Wunderer, C.
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Astrophysics - Abstract
The SPI instrument has been launched on-board the INTEGRAL observatory on October 17, 2002. SPI is a spectrometer devoted to the sky observation in the 20 keV-8 MeV energy range using 19 germanium detectors. The performance of the cryogenic system is nominal and allows to cool the 19 kg of germanium down to 85 K with a comfortable margin. The energy resolution of the whole camera is 2.5 keV at 1.1 MeV. This resolution degrades with time due to particle irradiation in space. We show that the annealing process allows the recovery of the initial performance. The anticoincidence shield works as expected, with a low threshold at 75 keV, reducing the GeD background by a factor of 20. The digital front-end electronics system allows the perfect alignement in time of all the signals as well as the optimisation of the dead time (12%). We demonstrate that SPI is able to map regions as complex as the galactic plane. The obtained spectrum of the Crab nebula validates the present version of our response matrix. The 3 $\sigma$ sensitivity of the instrument at 1 MeV is 8 10$^{-7}$ph$\cdot$cm$^{-2}\cdot$s$^{-1}\cdot$keV$^{-1}$ for the continuum and 3 10$^{-5}$ph$\cdot$cm$^{-2}\cdot$s$^{-1}$ for narrow lines., Comment: 10 pages, 18 figures, accepted for publication in A&A (special INTEGRAL volume)
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- 2003
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49. Calibration of the Spectrometer aboard the INTEGRAL satellite
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Schanne, Stéphane, Cordier, B., Gros, M., Attié, D., Ballmoos, P. v., Bouchet, L., Carli, R., Connell, P., Diehl, R., Jean, P., Kiener, J., Kienlin, A. v., Knödlseder, J., Laurent, P., Lichti, G., Mandrou, P., Paul, J., Paul, P., Roques, J. -P., Sanchez, F., Schönfelder, V., Shrader, C., Skinner, G., Strong, A., Sturner, S., Tatischeff, V., Teegarden, B., Vedrenne, G., Weidenspointner, G., and Wunderer, C.
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Astrophysics - Abstract
SPI, the Spectrometer on board the ESA INTEGRAL satellite, to be launched in October 2002, will study the gamma-ray sky in the 20 keV to 8 MeV energy band with a spectral resolution of 2 keV for photons of 1 MeV, thanks to its 19 germanium detectors spanning an active area of 500 cm2. A coded mask imaging technique provides a 2 deg angular resolution. The 16 deg field of view is defined by an active BGO veto shield, furthermore used for background rejection. In April 2001 the flight model of SPI underwent a one-month calibration campaign at CEA in Bruy\`eres le Ch\^atel using low intensity radioactive sources and the CEA accelerator for homogeneity measurements and high intensity radioactive sources for imaging performance measurements. After integration of all scientific payloads (the spectrometer SPI, the imager IBIS and the monitors JEM-X and OMC) on the INTEGRAL satellite, a cross-calibration campaign has been performed at the ESA center in Noordwijk. A set of sources has been placed in the field of view of the different instruments in order to compare their performances and determine their mutual influence. Some of those sources had already been used in Bruy\`eres during the SPI standalone test. For the lowest energy band calibration an X-ray generator has been used. We report on the scientific goals of this calibration activity, and present the measurements performed as well as some preliminary results., Comment: 12 pages, 19 figures, Published in Proceedings of SPIE conference, 24-28 August 2002, Waikoloa, Hawaii, USA
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- 2003
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50. SPI/INTEGRAL observation of the Cygnus region
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Bouchet, L., Jourdain, E., Roques, J. -P., Mandrou, P., von Ballmoos, P., Boggs, S., Caraveo, P., Cassé, M., Cordier, B., Diehl, R., Durouchoux, P., von Kienlin, A., Knödlseder, J., Jean, P., Leleux, P., Lichti, G., Matteson, J., Sanchez, F., Schanne, S., Schönfelder, V., Skinner, G., Strong, A., Teegarden, B., Vedrenne, G., and Wunderer, C.
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Astrophysics - Abstract
We present the analysis of the first observations of the Cygnus region by the SPI spectrometer onboard the Integral Gamma Ray Observatory, encompassing ${\sim}$ 600 ks of data. Three sources namely Cyg X-1, Cyg X-3 and EXO 2030+375 were clearly detected. Our data illustrate the temporal variability of Cyg X-1 in the energy range from 20 keV to 300 keV. The spectral analysis shows a remarkable stability of the Cyg X-1 spectra when averaged over one day timescale. The other goal of these observations is SPI inflight calibration and performance verification. The latest objective has been achieved as demonstrated by the results presented in this paper., Comment: 6 pages, 10 figures, accepted for publication in A&A (special INTEGRAL volume)
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- 2003
- Full Text
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