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  • ...d the error in the counts. Since the window is smaller, a constant fit was no long acceptable as the constant kept becoming negative and would yield a ne
    2 KB (211 words) - 15:39, 26 October 2017
  • <math>\leftarrow</math>'''NO DIFFERENCES'''
    2 KB (257 words) - 17:56, 14 December 2017
  • There is no 583 keV peak for the Nickel foil.
    2 KB (237 words) - 23:07, 14 June 2018
  • ...!Target!! Configuration !! Individual histos + rates !! Neutron Monitor !! no top bottom coin. !! other
    2 KB (306 words) - 02:34, 30 October 2017
  • This design is preliminary and subject to change. No BorAl shielding has been included.
    2 KB (299 words) - 16:38, 19 July 2021
  • ...rched for. If the crossing point is found, then a pulse is created, but if no crossing point is found, then the signal is rejected. For the purposes of t | Model No. || Endcap Size (mm) || CFG || Serial No. || Relative Eff @ 1.33 MeV (%)||FWHM @ 1.33 MeV || Ratio FW1M FWHM ||Rati
    8 KB (1,251 words) - 16:57, 26 March 2018
  • ...ring appears to be effective after 1st irradiation in > 680 nm region with no effect after 2nd irradiation. All lines show a sharp increase around 550 n ...ring appears to be effective after 1st irradiation in > 680 nm region with no effect after 2nd irradiation. All lines show a sharp increase around 550 n
    8 KB (1,156 words) - 19:06, 13 April 2018
  • physiTarget = new G4PVPlacement(0, // no rotation false, // no boolean operations
    10 KB (1,318 words) - 03:10, 4 April 2018
  • [[File:Soil No Irr 10 21 16 logplot.png|200px]]
    2 KB (269 words) - 17:52, 9 November 2017
  • No lead was included in the setup as it was not necessary. | 1 || Detector surrounded by BorAl at +1250V || 255 || No || 722 || 60000 || 0.0120 || 0.000448
    13 KB (1,461 words) - 18:46, 27 January 2022
  • physiTarget = new G4PVPlacement(0, // no rotation false, // no boolean operations
    11 KB (1,348 words) - 03:09, 4 April 2018
  • physiTarget = new G4PVPlacement(0, // no rotation false, // no boolean operations
    11 KB (1,347 words) - 03:08, 4 April 2018
  • ..., and if so, the opening angle between the two events is calculated. Since no information can be shared between the neutrons of different pulses, this di ...gles, the method of using uncorrelated neutron pairs from different pulses no longer works. While the neutrons from separate pulses are uncorrelated with
    7 KB (1,144 words) - 00:22, 24 January 2018
  • ...roughly equivalent to the low dose sloped divided by the high dose slope (no errors taken into account). ]]
    3 KB (467 words) - 19:53, 24 January 2018
  • ...unt applications. This crate supplies sixteen (16) slots for HV cards, but no keypad or LCD display. All control is via RS-232 or a local area network. T *If no interlock system exists, the interlock bnc connector must be capped. Otherw
    5 KB (823 words) - 20:19, 9 May 2022
  • * You can no longer use the Gd_In->Draw(); command, but instead have to use Gd_In.Draw()
    3 KB (556 words) - 18:06, 10 May 2022
  • ...ectors. For the generating particle, in this case the scattered electron, no hits are recorded, so the exact same trajectory cannot be reproduced.
    3 KB (460 words) - 20:13, 5 September 2018
  • #If there is no friction between the table cloth and the dishes, you can just pull on the t The total momentum of a system of a two particle with no external force is conserved.
    10 KB (1,649 words) - 00:15, 23 August 2021
  • ...l x_j} = \frac{\partial }{\partial x_j} \frac{1}{N} = 0 \Rightarrow</math> no Covariances : No! In reality there are systematic errors in every experiment so the best yo
    15 KB (2,338 words) - 20:05, 3 November 2017
  • logMsg("ERROR: NO data in ADC datascan = 0x%x\n",stat,0,0,0,0,0);
    3 KB (375 words) - 22:41, 11 May 2021

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