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13 May 1999: 199 406 0 0 0 8 418 0.14048913E00 0 454 5 0 0 0 418 0.22753577E00 0 455 5 0 0 0 418 0.10838635E00 0 200 406 0 ... 13 0 0 0 204 0.13301892E-02 0 198 199 0 0 0 204 0.63208927E-03 0 200 200 0 0 0 204 0.10031293E-01 0 450 450

21 May 2012: histo/plot 1 . histo/plot 2 . histo/plot 3 . histo/plot 4 . c1 = new TCanvas("c1"," ",200,10,600,480);.

31 Jan 2008: Centre-of-mass energy adjustable from 200-500 GeV• upgradeable to 1 TeV (i.e. ... ee- qq 0.1 /Bunch Trainee- γγ X 200 /Bunch Train. 500 hits/BX in Vertex det.5 tracks/BX in TPC.

19 Apr 2007: Jet Transverse Energy [GeV]0 50 100 150 200 250 300 350.

28 Jun 2006: SCT contains 4088 “Modules”. 768 sensitive-strip diodes per side. (200 V).

12 Jan 2004: To set the scale on required level of understanding the systematics; statistical fluctuation on background in FD will be about 15-20% for a 200 kt-yr run.

4 Dec 2008: 0.095. 0.1. 0.105. 0.11. 0.115. 0.12. 0.125. 100 120 140 160 180 200.

7 Dec 2006: Look at jet energy resolution for Z uds events at• s = 200 GeV• s = 360 GeV. ... Use Mokka to generate Z uds events @ 200 GeV with differentECAL segmentation: 5x5, 10x10, 20x20 [mm2]. •

30 Mar 2005: cused by two neutrino horns with parabolic innerconductors. The horns are pulsed with a cur-rent of 200 kA which produces a toroidal magneticfield, B I/r, between the inner and ... Theprimary MINOS trigger algorithm is to requireactivity in at least 4

30 Jul 2007: 1 Widdecombe = 200 kg,but a little clumsy for particles, me= 3x10-31 kg.

28 Dec 2011: LED on delay(200); // wait for a second digitalWrite(13, LOW); // set the LED off delay(200); } } // wait for a second void pause() { digitalWrite(13, LOW); // set the LED off

20 Jul 2006: White. (9=) SU4 low mass point at limit of runII reach (isasugra 7.71: m0=200 geV, m12 = 160 geV, A0 = -400 geV, tan beta = 10, sgn(mu) = ). 100k Voss. (9=)

27 Feb 2006: At least, not very easily. In fact I could never get gtkam to work on my machine, and I couldn't understand how it worked, so instead I wrote a 200

3 Apr 2007: ILC : the machine Basic Machine Design Parameters. Centre-of-mass energy adjustable from 200-500 GeV• upgradeable to 1 TeV (i.e. ... ee- qq 0.1 /Bunch Trainee- γγ X 200 /Bunch Train. 500 hits/BX in Vertex det.5 tracks/BX in TPC.

4 Dec 2008: GeV)TLead Jet E50 100 150 200 250 300 350. [pb/. 5 G. ... of 200 GeV, the events are dominated by the higher multiplicity matrix elements, i.e.

9 Oct 2003: m_vertex_barcodes.end() ); } class vertex_iterator :! public std::forward_iteratorGenVertex,ptrdiff_t{ // Iterates over all vertices in this event public: vertex_iterator( --- 194,200 ---- m_vertex_barcodes.end() ); } class

10 Apr 2006: ee- qq 0.1 /Bunch Trainee- γγ X 200 /Bunch Train. 500 hits/BX in Vertex det.5 tracks/BX in TPC. •

9 Jan 2004: 5. 19. 22-Oct-02. 28. 13. 35. 11. 11. 6. 14. 200. ... 700. 620. 90. 510. 650. 2000. 550. 2000. 200. 200. 90.

28 Nov 2020: CALL HWWARN('HWANAL',ICODE,999). should become. CALL HWWARN('HWANAL',ICODE). IF (ICODE.LT.0.OR.(ICODE.GE.50.AND.ICODE.LT.200)) GOTO 999. An arithmetic IF statement has been

30 Jul 2007: 1x10-15 m apart : 200 N (equivalent weight of small child).

8 Jan 2021: 2 200 40 - 45Roast rabbit 1.5 Round 2 180 - 190 70 - 80Turkey breast 3 Turbo/Round 2 180 - 190 110 - 120Roast pork neck 2 - 3 Turbo/Round 2 180 - 190 ... Pizza 1 Turbo/Round 2 260 8 - 9Bread 1 Round 2 190 - 200 25 - 30Focaccia 1 Turbo/Round 2 180 - 190

8 Jan 2021: 2 200 40 - 45Roast rabbit 1.5 Round 2 180 - 190 70 - 80Turkey breast 3 Turbo/Round 2 180 - 190 110 - 120Roast pork neck 2 - 3 Turbo/Round 2 180 - 190 ... Pizza 1 Turbo/Round 2 260 8 - 9Bread 1 Round 2 190 - 200 25 - 30Focaccia 1 Turbo/Round 2 180 - 190

24 Oct 2011: 300. 250. 250. 200. 200. 150. 150. 100. 100. 50. 50.

16 Sep 2018: UEC125 125 335 260 140. UEC150 150 400 300 150. UEC200 200 400 300 150.

20 Sep 2011: Prospective summer students will therefore have to investigate other sources of maintenace, such as College funding, if they want to be paid the going rate of 200 pounds per week.

26 Sep 2008: Ejj/GeV α(Ejj)100 < 27 %. < 38 %200. Typical di-jet energies at ILC (100-300 GeV) suggests jet energy resolution goal of.

27 Nov 2006: The second algorithm,. 16. 0. 100. 200. 300. 400. 0 5 10 15 20Nkt jet. ... 10. 10 2. 10 3. 10 4. 0 200 400 600 800 1000.

17 May 2016: 910. N. 0. 50. 100. 150. 200. 250. 300. 310. Figure: Overall D distribution for‘dimuon’ events. ... 910. N. 0. 50. 100. 150. 200. 250. 300. 310. before twistafter twist.

25 Oct 2023: Of the 16 possible helicity combinations only 4 are non-zero:. 200 / 563.

10 Feb 2024: E0 = 0.37aC. Z2. A1/30.26aSA2/3. e.g. 23892 U: maximum E0 200 MeV (aS = 18.0 MeV, aC = 0.72 MeV) 106 energy released in chemical reaction!

21 Sep 2007: 100-200 GeV jets! Caveat : work in progress, things will change. ... 200 GeV. MPV = 3.4 keV. σ = 0.8 keV. Geant4 energy of simulated hits.

24 Nov 2005: MH < 200 GeV. 37. Latest results from the LEP Electroweak Working Group:. ... 160. 180. 200. 10 10 2 10 3. mH [GeV]. mt [G.

19 Apr 2007: Rev. Lett. 84 (2000) 845. / GeV Z P0 20 40 60 80 100 120 140 160 180 200. ... pW. p1st jet. [ GeV ] Wp0 20 40 60 80 100 120 140 160 180 200. [

10 Jan 2004: Signals are 100 times smaller. 200 mV into 100 ohm  2 mV into 100 ohm.

22 May 2009: 0294 -38.7092 61.3615 0.000478589 15.4972 -48.6371 -39.5676 0.00222962 60.8014 6.07118 200.059 1.49707e-06 -40.4072 -3.29402 -147.908

30 May 2006: directEntries 2000000Mean -0.02588. RMS 17.87. -600 -400 -200 0 200 400 6001. ... directEntries 2000000Mean -0.02588. RMS 17.87. badEntries 2000000Mean 0.01601. RMS 7.586. -600 -400 -200 0 200 400 6001.

units;. and for the first 200 time units. The way in which the excess energy of the piston is gradually dissipated and the energy sloshes between the particles deserves hours of

27 Sep 2013: 0.8. 1.0S. 50 100 150 200 250N. 2.5. 3.0. 3.5. 4.0tscr.

31 Oct 2022: 36V/48V -- 200 --. Temperature Coefficient -- 0.05 -- %/. Minimum Load 0 -- -- %. Hold-up Time 230VAC -- 20 -- ms. Short Circuit Protection Recover time <3s after the short circuit disappear.

30 Mar 2021: GeV]1. χm(. 100 150 200 250 300 350 400 450 500. ) ... 120. 140. 160. 180. 200. 220. ) =. m(W. ). 1.

20 May 2023: RJ1P60. Operational voltage range 90 to 265VAC 200 to 550VAC 410 to 660VACBlocking voltage 650Vp 1200Vp 1200VpOperational frequency range 45 to 65Hz 45 to 65Hz 45 to 65HzOutput power 0 to

4 Jan 2013:  Emerging consensus on possible working point  200 kHz Level 1  20 µs latency. ... ATLAS Upgrade Week, Stanford, 29/3/2012 9 Mark Thomson. 50 20 L1 EM Rate 100 200 10 kHz.

29 Sep 2009: 1. 50 100 150 200 250 300 350 400. 0.6. 0.8. ... t. 2. 50 100 150 200 250 300. 0.6. 0.8. 1.

13 Oct 2009: 0.2 0.2 3.0σx/σy 240 / 4 mm 600 / 6 nm 200 / 2 nm 40 / 1 nm. ... 200,000 background hits per event! Also consider finite cluster size of background hits (10 pixels).

6 Oct 2022: 200,000 muons. The resulting data collection. phase, for a 1m square detector, would take. ... a) is a density map of. the sample. (b) shows the image with 200.

13 Apr 2010: The muon is 200 times more massive than the electron and about 10 times less massive than a single proton.

27 Jul 2011: 46.345850697 pmissx= -200.14895955 pmissy= 65.364481806 Kss= -12093.135843 Kcc= -1890.5383622 Kcs= -41898.349483 Ks= -43080.338357 Kc= -1910.2700728 K1= 0 A= 1859564684.7 B= 1039137029.4

8 May 2007: s = 91 GeV. s = 360 GeV s = 200 GeV. ... ECAL Transverse Granularity• Use Mokka to generate Z uds events @ 200 GeV with different.

19 Nov 2005: Forward IT (FIT)7 Si discs. TPC. 235 280. 210. 40. Inner radius: 40 cmOuter radius: 200 cmHalf-length : 235 cmReadout : 200 radial rings.

18 Jun 2004: The NuMI ν beam : III. protons. π+. • Horn pulsed with 200 kA • Toroidal Magnetic field B I/r between. ... Signal/Noise (cosmics) = 1/200,000Veto Shield helps : efficiency 97 %Have achieved rejection factor of 1:10,000,000!