Changeset 8613 for trunk/Dwarf/Documents
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- 06/27/07 15:38:59 (17 years ago)
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- trunk/Dwarf/Documents/ApplicationDFG
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trunk/Dwarf/Documents/ApplicationDFG/application.bib
r8607 r8613 2573 2573 adsnote = {Provided by the Smithsonian/NASA Astrophysics Data System} 2574 2574 } 2575 2576 @ARTICLE{Milagro:2007, 2577 author = {{Abdo}, A.~A. and others}, 2578 title = "{TeV Gamma-Ray Sources from a Survey of the Galactic Plane with Milagro}", 2579 journal = {ArXiv e-prints}, 2580 eprint = {0705.0707}, 2581 year = 2007, 2582 month = may, 2583 volume = 705, 2584 adsurl = {http://cdsads.u-strasbg.fr/abs/2007arXiv0705.0707A}, 2585 adsnote = {Provided by the Smithsonian/NASA Astrophysics Data System} 2586 } 2587 2588 @ARTICLE{Rieger:2000, 2589 author = {{Rieger}, F.~M. and {Mannheim}, K.}, 2590 title = "{Implications of a possible 23 day periodicity for binary black hole models in Mkn 501}", 2591 journal = {\aap}, 2592 eprint = {arXiv:astro-ph/0005478}, 2593 year = 2000, 2594 month = jul, 2595 volume = 359, 2596 pages = {948-952}, 2597 adsurl = {http://cdsads.u-strasbg.fr/abs/2000A%26A...359..948R}, 2598 adsnote = {Provided by the Smithsonian/NASA Astrophysics Data System} 2599 } 2600 2601 @INPROCEEDINGS{Rieger:2001, 2602 author = {{Rieger}, F.~M. and {Mannheim}, K.}, 2603 title = "{A Possible Black Hole Binary in Mkn 501}", 2604 booktitle = {American Institute of Physics Conference Series}, 2605 year = 2001, 2606 series = {American Institute of Physics Conference Series}, 2607 volume = 558, 2608 editor = {{Aharonian}, F.~A. and {V{\"o}lk}, H.~J.}, 2609 pages = {716-+}, 2610 adsurl = {http://cdsads.u-strasbg.fr/abs/2001AIPC..558..716R}, 2611 adsnote = {Provided by the Smithsonian/NASA Astrophysics Data System} 2612 } 2613 2614 @ARTICLE{Rieger:2003, 2615 author = {{Rieger}, F.~M. and {Mannheim}, K.}, 2616 title = "{On the central black hole mass in Mkn 501}", 2617 journal = {\aap}, 2618 eprint = {arXiv:astro-ph/0210326}, 2619 year = 2003, 2620 month = jan, 2621 volume = 397, 2622 pages = {121-125}, 2623 doi = {10.1051/0004-6361:20021482}, 2624 adsurl = {http://cdsads.u-strasbg.fr/abs/2003A%26A...397..121R}, 2625 adsnote = {Provided by the Smithsonian/NASA Astrophysics Data System} 2626 } -
trunk/Dwarf/Documents/ApplicationDFG/application.tex
r8610 r8613 3 3 \usepackage[round]{natbib} 4 4 5 \renewcommand{\familydefault}{\sfdefault}6 \usepackage{helvet}5 %\renewcommand{\familydefault}{\sfdefault} 6 %\usepackage{helvet} 7 7 8 8 \setlength{\parindent}{0pt} … … 140 140 % AUCH IN DEUTSCH BEIFGEN 141 141 We propose to set up an imaging air Cherenkov telescope with low-cost 142 but high performance design for robotic operation. The goal is to 143 achieve long-term monitoring of bright blazars which will unravel the 144 origin and nature of their variability (und den zugrunde liegen 145 Beschleunigungsmachanismen). The telescope design is based on a 146 technological upgrade of one of the former telescopes of the HEGRA 147 collaboration still located at the Observatorio Roque de los Muchachos 148 on the Canarian Island La Palma (Spain). With the upgrade an 149 improvement in senitivity by xx\% and a xx\% lower energy threshold 150 will be achieved. 151 142 but high performance design for robotic and remote operation. The goal 143 is to achieve long-term monitoring of bright blazars which will unravel 144 the origin and nature of their variability (und den zugrunde liegen 145 Beschleunigungsmachanismen der kosmischen Strahlung). The telescope 146 design is based on a technological upgrade of one of the former 147 telescopes of the HEGRA collaboration still located at the Observatorio 148 Roque de los Muchachos on the Canarian Island La Palma (Spain). With 149 the upgrade an improvement in senitivity by 25\%{\bf (?)} and a lower 150 energy threshold in the order of 350\,GeV{\bf (?)} will be achieved. 151 152 {\bf IceCube erw"ahnen?} 152 153 {\em Nicht gescheduled von anderen IACTs?} 153 154 %Beantragt \citeauthor{Chandrasekhar:1931} wird die F"orderung eines155 %Luft-Cherenkov-Teleskops f"ur Langzeitbeobachtungen von Gamma-Quellen156 %im Energiebereich zwischen 500 GeV und 50 TeV (DWARF=Dedicated157 %multiWavelength Astroparticle Research Facility). Mit DWARF sollen zwei158 %Aufgaben bei der Beobachtung erf"ullt werden:159 160 %1. weitgehend161 %automatisierte Langzeitbeobachtungen von bekannten hochenergetischen162 %Quellen. Solche Beobachtungen stehen nicht auf dem Programm der im163 %Betrieb befindlichen Generation von Cherenkov-Teleskopen 2.164 %Multiwavelenght-Kampangen mit Photon-Detektoren in unterschiedlichen165 %Energiebreichen, insbesondere auch mit dem Neutrino-Teleskop IceCube.166 %F"ur den Aufbau von DWARF soll die bestehende Infrastruktur auf dem167 %Roque de los Muchachos auf der kanarischen Insel La Palma genutzt168 %werden. Dort befindet sich der zur Zeit ungenutzte Mount des169 %ehemaligen ``HEGRA-Cherenkov-Teleskops 3'' sowie eine zur Plazierung170 %der Elektronik geeignete H"utte samt elektrischer Versorgung bei dem171 %Teleskop. Zur Minimierung von Peronalkosten soll das Teleskop nach der172 %Aufbauphase weitestgehend robotisch "uber das Internet / einen Link173 %"uber den ESA-Satelltien XYZ betrieben werden. Die mit DWARF174 %vorgenommenen Messungen dienen der Kl"arung der Frage nach der175 %zeitlichen Variabilit"at der Gamma-Emissionen von Aktiven Galaxien und176 %den zugrundeliegenden Beschelunigungsmechanismen der kosmsichen177 %Strahlung.\\178 154 179 155 {\em … … 198 174 \item Knapp und pr"azise in der unmittelbaren Beziehung zum Vorhaben 199 175 \item Als Begr"undung f"ur eigene Arbeit 200 \item in cl. einschl"agiger Arbeiten anderer Wissenschaftler176 \item inkl. einschl"agiger Arbeiten anderer Wissenschaftler 201 177 \item $\to$ Einordnung eigener Arbeit, welcher Beitrag zu welchen Fragen 202 178 \end{itemize} 203 179 } 180 181 {\bf Hier gibt es glaub ich drei Punkte: Physik, IACTs und gAPD} 204 182 205 183 \paragraph{Introduction:} Since the termination of the HEGRA … … 208 186 detecting tens of formerly unknown gamma ray sources and analyzing 209 187 their energy spectra and temporal behavior. This became possible by 210 lowering the energy threshold from 700 GeV to less than 100GeV and188 lowering the energy threshold from 700\,GeV to less than 100\,GeV and 211 189 increasing at the same time the sensitivity by a factor of five. 212 190 … … 237 215 a solid and complete data base for variability investigations. 238 216 239 {\bf Hier sollte ganz klar rauskommen warum man unbedingt ein 217 {\bf Hier sollte ganz klar rauskommen was der aktuelle Stand der 218 Forschung ist und wieso man um weiter zu kommen unbedingt ein 240 219 long-term monitoring IACT braucht} 241 220 242 {\bf Geigerm de APDs?}221 {\bf Geigermode APDs?} 243 222 244 223 \subsubsection{High energy gamma and neutrino sources} … … 251 230 decades. Additionally there are two diffuse regions within our galaxy 252 231 which have been detected by H.E.S.S.\cite{Aharonian:2006} and Milagro 253 {\bf ZITAT!!! } {\it Neues Millagro Papier mit "TeV Gamma-Ray Sources 254 from a Survex of the Galactic Plane with Milagro} 4+ Quellregionen: 255 "TeV Gamma-Ray Sources from a Survey of the Galactic Plane with 256 Milagro" Arxiv-Nr.: 0705.0707 The first source was discovered in the 257 year 19{\bf??} by the {\bf HEGRA} collaboration {\it (War das nicht wer 258 anders, die zu allererst den Crab sahen?...ZITAT?)}. In comparison to 232 \cite{Milagro:2007}. 233 %The first source was discovered in the 234 %year 19{\bf??} by the {\bf HEGRA} collaboration {\it (War das nicht wer 235 %anders, die zu allererst den Crab sahen?...ZITAT?)}. 236 In comparison to 259 237 x-ray measurments, which are able to scan the entire sky for sources 260 and thus have 238 and thus have cataloged more than {\bf 1000 ???} sources, this number 261 239 appears to be quite small. One reason for this is the small field of 262 240 view of imaging air cherenkov telesopes (IACTs), another reason the … … 264 242 extragalactic background light (EBL). Due to this small statistic at 265 243 the moment it is of particular importance that instruments with high 266 sensitivity concentrate on the analysisof new objects in the TeV sky244 sensitivity concentrate on the observation of new objects in the TeV sky 267 245 and not on the quantitative, permanent observation of already known 268 sources. Even when a source was observed over a longer period of time 269 this does mean {\bf less than three month ???? {\it Viel l"anger sind 270 die Quellen am St"uck doch gar nicht sichtbar, oder? Sinnvoller w"are 271 es wom"oglich die wenigen Beobachtungsstunden in diesen X Monaten 272 hervorzuheben.}} But one has to take into account that during this time 273 also periods of bad weather and times with strong moon light can 274 significantly reduce observation time. Furthermore one has to consider 275 that the sources are visible in the sky only for a few hours each night. 246 sources. 247 % BRAUCHT MAN DEN FOLGENDEN ABSATZ WIRKLICH 248 %Even when a source was observed over a longer period of time 249 %this does mean {\bf less than three month ???? {\it Viel l"anger sind 250 %die Quellen am St"uck doch gar nicht sichtbar, oder? Sinnvoller w"are 251 %es wom"oglich die wenigen Beobachtungsstunden in diesen X Monaten 252 %hervorzuheben.}} But one has to take into account that during this time 253 %also periods of bad weather and times with strong moon light can 254 %significantly reduce observation time. Furthermore one has to consider 255 %that the sources are visible in the sky only for a few hours each night. 256 257 %{\bf Ist die Aufz"ahlung nich total "ubertrieben? Ist es f"ur unseren 258 %Antrag wirklich interessant welchem Typ die detektierten AGN angeh"oren 259 %und wie sie hei"sen?} 276 260 277 261 The so far observed galactic objects are microqasars and supernova 278 262 remnands (SNR). The identified extragalactic sources are active 279 galactic nuclei (AGN). The objects are listed in table~\ref{dummy} {\bf 280 TESHIMAS VORTRAG IN MADISON}. The AGN are 13 BLLacs and one FR-I 263 galactic nuclei (AGN). 264 %NOETIG??? The objects are listed in table~\ref{dummy} {\bf 265 %TESHIMAS VORTRAG IN MADISON}. 266 The AGN are 13 BLLacs and one FR-I 281 267 galaxy, M87. So High-peaked BL Lacertae objects are the prime source 282 population for studies with Cherenkov telescopes. 268 population for studies with Cherenkov telescopes. It is obvious that 283 269 monitoring observations of strong blazars are orthogonal to the mission 284 270 of the larger Cherenkov telescopes with their discovery potential for 285 271 new sources (luminosity function, redshift distribution). 272 {\bf Das hatten wir oben eigtnlich schonmal} 286 273 287 274 In case of hadronic particle acceleration within the TeV emitters, the 288 TeVsignal may arise from $\pi^0$-decays. These neutral pions are decay289 products of ofdelta resonances, which are formed in proton-photon290 interactions. An ther decay channel of the delta resonance leads to the275 signal may arise from $\pi^0$-decays. These neutral pions are decay 276 products of delta resonances, which are formed in proton-photon 277 interactions. Another decay channel of the delta resonance leads to the 291 278 production of charged pions and thus to neutrino production, coincident 292 with the TeV photons mentioned before. Therefrom TeV sources are always279 with the TeV photons. Therefrom TeV sources are always 293 280 interesting objects for investigations with high energy neutrino 294 281 telescopes. … … 453 440 expected from galaxy merger models.\\ \textbf{the search for signatures of 454 441 binary black hole systems from orbital modulation of VHE gamma ray 455 emission}\\ 456 \textbf{\item Rieger, Mannheim; Implications of a possible 23 day periodocit for binary black hole models in Mkn 501 457 \item Rieger, Mannheim; A possible black hole binary in Mkn 501 442 emission} \cite{Rieger:2000, Rieger:2001}\\ 443 \item {\bf Wird das nicht ein bisschen viel Rieger? 458 444 \item Rieger; Periodic variability and binary black hole systems in blazars 459 445 \item Rieger; Supermassive binary black holes among cosmic gamma-ray sources … … 518 504 studied with hybrid MHD and particle-in-cell methods. 519 505 520 \item {The black hole mass and accretion rate will be determined from506 \item The black hole mass and accretion rate will be determined from 521 507 the emission models. Estimates of the black hole mass from emission 522 508 models, a possible orbital modulation, and the Magorrian relation 523 509 (relating the black hole mass with the stellar bulge mass of the host 524 galaxy) will be compared. 525 \textbf{\item Rieger, Mannheim; On the central black hole mass in Mkn 501}} 510 galaxy) will be compared. \cite{Rieger:2003} {\bf eigentlich ist das 511 nicht mehr die Stelle mit Zitaten sondern die wo wir sagen, dass 512 wir das Know-how - in Form von Frank - haben.} 526 513 527 514 \item \textbf{To achieve a maximal database for these studies the … … 629 616 single pixel will be in the order of 600 EURO. 630 617 631 If development of G-APDs (QE$\ge$50$\%$) will be fast enough,618 If development of geigermode APDs (QE$\ge$50$\%$) will be fast enough, 632 619 respectively the price low enough, and their long term stability is 633 620 proven well in time, their usage will be considered. … … 636 623 (see figure \ref{camCT3}). With a special coating (wavelength shifter) 637 624 its quantum efficiency might be improved by ~8$\%$\cite{Paneque:2004}. 638 \textbf{8\% sind f ür flat-window-pmts angegeben...nach den Zeichnungen639 in z.B. German Hermanns Diss. sind sie aber nicht v öllig flach...demnach640 k önnten wir wohl 19\% zitieren.}625 \textbf{8\% sind f"ur flat-window-pmts angegeben... nach den Zeichnungen 626 in z.B. German Hermanns Diss. sind sie aber nicht v"ollig flach...demnach 627 k"onnten wir wohl 19\% zitieren.} 641 628 \textbf{Figure?} 642 629 … … 655 642 CT3 system. 656 643 657 For this setup the camera holding has to be redesigned. (1500 EURO?)644 For this setup the camera holding has to be redesigned. (1500\,Eur?) 658 645 659 646 An electric and optical shielding of the individual PMs is planned. … … 692 679 and processed by the W"urzburg Datacenter (current online capacity 693 680 $>$20\,TB, offline capacity $>$30\,TB, $>$16\,CPUs). To archive the data 694 safely 25 tapes (LTO3 with 400\,GB each, $\sim$1000\,E URO) and a SATA695 disk-array ($\sim$4000 EURO) will be bought.681 safely 25 tapes (LTO3 with 400\,GB each, $\sim$1000\,Eur) and a SATA 682 disk-array ($\sim$4000\,Eur) will be bought. 696 683 697 684 \paragraph{On-site computing:} 698 685 For on-site computing less than three standard PCs are needed 699 ($\sim$8.000 EURO). This includes readout and storage, preprocessing,686 ($\sim$8.000\,Eur). This includes readout and storage, preprocessing, 700 687 and telescope control. For safety reasons a firewall is mandatory. For 701 688 local storage and backup two RAID\,5 SATA disk arrays with less than one 702 Terabyte capacity each will fulfill the requirement ($\sim$4.000 EURO).689 Terabyte capacity each will fulfill the requirement ($\sim$4.000\,Eur). 703 690 The data will be transmitted as soon as possible after data taking via 704 691 Internet to the W"urzburg Datacenter. … … 730 717 An uninterruptible power-supply unit (UPS) with 5-10\,kW will be 731 718 installed to protect the equipment against power cuts and ensure a safe 732 telescope position at the time of sun-rise. ($<$2000 EURO)719 telescope position at the time of sun-rise. ($<$2000\,Eur) 733 720 734 721 \paragraph{Mirrors:} … … 748 735 the old glass mirrors (8.5\,m$^2$) is possible with high purity aluminum 749 736 and quartz coating. (Both cases: 30 mirrors, 10k, offer by L-Tec 750 $\lesssim$500 EURO / mirror *30 mirrors = 15.000 EUROwithout transfer)737 $\lesssim$500\,Eur/mirror * 30\,mirrors = 15.000\,Eur without transfer) 751 738 752 739 \textbf{In both cases the mirrors can be coated with the same high … … 764 751 For a 3.5\,m \textbf{4\,m} diameter mirror the delay between an isochronous parabolic 765 752 mirror and a spherical mirror at the edge is in the order of\textbf{well below} 1ns (see 766 figure/appendix). For a sampling rate in the order of 1\,GHz a mirror767 mounting with a parabolic shape is \textbf{not}needed. Since their small size the768 individual mirrors can still\textbf{also}have a spherical shape.753 figure/appendix). For a sampling rate in the order of 2\,GHz a mirror 754 mounting with a parabolic shape is not needed. Since their small size the 755 individual mirrors can have a spherical shape. 769 756 770 757 \paragraph{Telescope calibration:} … … 776 763 guide stars on the camera surface and ensures a pointing accuracy well 777 764 below the pixel diameter. Therefore a high sensitive low-cost video 778 camera, as already in operation for MAGIC I and II, (300 EUROcamera,779 300 EURO optics, 300 EUROhousing) will be installed.765 camera, as already in operation for MAGIC I and II, (300\,Eur camera, 766 300\,Eur optics, 300\,Eur housing) will be installed. 780 767 781 768 PM Gain: For the calibration of the PM gain a calibration system as 782 used for the MAGIC telescope is build. (2.000 EURO)769 used for the MAGIC telescope is build. (2.000\,Eur) 783 770 784 771 Summarizing, the expenses for the telescope are dominated by the camera 785 772 and DAQ. The financial volume for the complete hardware inclusive 786 transport amounts roughly 400.000 EURO.773 transport amounts roughly 400.000\,Eur. 787 774 788 775 \textbf{Future extensions:} The known duty cycle of 10\% 789 ($\sim$1000 h/year) for a Cherenkov telescope operated at La Palma776 ($\sim$1000\,h/year) for a Cherenkov telescope operated at La Palma 790 777 limits the time-coverage of the observations. Therefore we propose a 791 778 worldwide network of ($<$10) small scale Cherenkov telescopes to be … … 799 786 telescope, also builds by MERO, and has a diameter in the order of 800 787 eight meters. Including support (concrete foundation, railways, etc) 801 the costs are below 100.000 EURO788 the costs are below 100.000\,Eur. 802 789 \textbf{The intended future use of a camera built of G-APDs will by their 803 790 highly improved QE (50\% instead of 20\%) increase the sensitivity by a factor … … 1256 1243 %\section{References} 1257 1244 1258 %\bibliographystyle{alpha}1259 1245 \newpage 1260 1246 %(Referenzen aus unseren Gruppen sind mit einem Stern gekennzeichnet *) 1261 1247 (References of our groups are marked by an asterix *) 1262 1248 \bibliography{application} 1263 %This in the bibtex style, is ok. 1264 \bibliographystyle{plain} 1265 References will be added in the final version. 1266 %\begin{thebibliography}{99} 1267 %\bibitem{andreas_05} *M.~Ackermann et al., ''On the selection of AGN neutrino 1268 % source candidates $\ldots$'', submitted to {\app} 1269 1270 1271 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 1272 %\end{thebibliography} 1249 \bibliographystyle{plainnat} 1250 %\bibliographystyle{alpha} 1251 %\bibliographystyle{plain} 1273 1252 1274 1253 \end{document}
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