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21 Nov 2014: addr_h_NTC_Tnom = 20;// byte const unsigned int addr_h_NTC_B = 24;// u_int: 2B const unsigned int addr_u_NTC_T_Lo = 40;// float: 4B const unsigned int ... chars lcd.setCursor(20,0); lcd.print(HnSamples, DEC); lcd.setCursor(21,0); lcd.print(", ");

1 May 2014: 24. ( ). ( (. )). Using our definition of momentum this becomes:. ( (. )).

2 Jun 2014: between 1.8 and3.7 GeV, the precision in (24) is significantly improved com-pared to the HLMNT result, which relies on experimentaldata in that domain.12. ... md mu) = 2.35(8)(24) MeV in [104] was obtained assumingϵ = 0.7(5) [1] and ϵm = ϵπ0 = ϵK0 =

13 Sep 2014: ghazi@noc.rutgers.edu 1994-08-24) if (test -f /.attbin/uname) /dev/null 2&1 ; then PATH=$PATH:/.attbin ; export PATH fi UNAME_MACHINE=(uname -m) 2/dev/null ||

12 Sep 2014: 13.3 Hint: The expression for P(νe νe) can be obtained from equation (13.24)by making the replacing in the sub-scripts µ e. ... 13)(24) : m13 = (84.8 9.3) GeV and m24 = (82.6 5.9) GeV.

20 Nov 2014: Note that this operator violatesthe individual and total lepton numbers; moreover, it gives masses to neutrinos after EWSB(exercise 24), just as we observe.

1 May 2014: orthonormal. The resulting states are shown in Equation 24 and have eigenvalues under the Free. ... 24). (25). This completes the necessary theory required by the simulator for non-interacting systems.

1 May 2014: Illustration 24: Oscilloscope trace showing closely matched arrival times of AB and C after the introduction of a delay to C. ... 5 See “Investigating the 'missing' efficiency” on page 24. 23. Illustration 35: Efficiency of final product as a

1 May 2014: end for. 24. 1 Introduction. 2 Theory & control approach. 2.1 Unicycle dynamics.

1 May 2014: Approximately, the accidentals rate is proportional to the product of the dark current and pulse width so the accidentals ratio for H6780 to H7826 to H8443 to XP3240 is 1 : 24 :