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30 Mar 2011: 24. R (pT ) = exp. dΦRR (ΦB, ΦR). B (ΦB)θ (kT (ΦB, ΦR) pT ). B (ΦB) = B (ΦB) V (ΦB). R (ΦB, ΦR). i. ... 0.2. 0.3. 1 2 3 4. V Ciulli, Moriond, 24/03/11. {MEPS.

21 Sep 2021: m2ll•i = m2lli ei δ (24). and hence. Var[m2ll•. ]= Var. ... So only use in g_mean_mll2 and F_mean_mll2e_vec. 23 (event.mll2 - (Z_massZ_mass) config.safety_factor) :. 24 (event.mll2). 25 );. 13. 26 g_mean_mll2 =

11 Nov 2022: 1.34:. 1.33:. 1.32:. 1.31:. 1.30:. 1.29:. 1.28:. 1.27:. 1.26:. 1.25:. 1.24:. ... 0.27:. 0.26:. 0.25:. 0.24:. 0.23:. 0.22:. 0.21:. 0.20:. 0.19:. 0.18:. 0.17:.

3 May 2007: ILC software mtg., Paris 3/5/2007 Mark Thomson 24. Angular Dependence (NEW).

8 Oct 2009: Neutrino 6. Photon 2Z 1 2W 2 4. Higgs 1Total 4 90 24. ... 24. -1-0.5. 0 0.5. 1. 0 0.5 1 1.5 2 2.5 3 3.5.

16 Mar 2016: 16. Department 2012(2013 projection). HESA Russell Group (All UK)universities. Year 1 UG 24.5%BSci UG 16.7% 21.2% (21.2%)MaSt/MPhil UG 17.4%Research PG ... 24. “University” style. Bridging the gap!April 2014: Year 1 mock physics exam (funded by IoP).

31 Jul 2007: θ. Above. Below. ν. νµ. ν frombelow. 24. Neutrino OscillationsSuppose νµ and ντ are not fundamental particlesAssume they are mixtures of two fundamentalneutrino states, ν1 and ν2 of mass m1 and

24 Nov 2004: total 4 dr-xr-xr-x 4 root root 1 Jan 1 1970. drwxrwxrwt 21 root root 4096 Nov 24 01:44.

5 Apr 2006: PFA performance much more complex than α/E. Cambridge 5/4/06 Mark Thomson 24.

19 Apr 2007: 11 -50.76 31.35 35.3 69.5 4.95 14 W+ 24 195 12 11 19 20 50.36 -31.10 -35.0 104.5 78.64. ... 23 9.40 65.65 13.2 67.8 4.95 26 W- -24 195 24 23 32 33 -9.37 -65.43 -13.1 106.4 82.28.

10 Apr 2007: gaps between Tungsten increase effective RMoliere)• Lateral segmentation: 1cm2 matched to RMoliere• Longitudinal segmentation: 30 layers (24 X0, 0.9λhad)• Typical resolution: σE/E = 0.15/E(GeV). ... RAL Seminar, 7/2/2007 Mark Thomson 24. Particle

10 Sep 2009: 2N,. dabcdA dabcdA. NA=. N 2(N 2 36). 24,. dabcdF dabcdA. ... are available at present (see later). 24. Infrared Divergences. Even in high-energy, short-distance regime, long-distance aspects of QCD cannot be ignored.

8 Oct 2009: J. 24. MC4BSM3 Bryan Webber. Now add parton shower: result from showering after 0,1 emissions.But shower adds to 1 emission. ... 2. x10. log1. x10. Diff. PDF: 0.5(log. Figure 24: The distributions of x1,2 of the contributing parton distributions for the

6 Dec 2009: QCD Effects in Particle Searches Bonn 07/12/09. Theoretical Uncertainties. 24. σ [fb] LO (pdfs, αs) NLO (pdfs, αs) NNLO (pdfs, αs). ... 0-jets 3.4527%10% 2.883. 4%9% 2.707. 5%9%. 1-jet 1.75230%26% 1.280. 24%23% 1.165.

25 Oct 2023: r) 0er/a. with a 0.24 fmCorresponds to a rms charge radiusrrms 0.8 fm.Although suggestive, does not implyproton is composite!

9 Oct 2003: HepMC_Version1.24/HepMC/GenEvent.h Mon Jul 14 22:34:57 2003 --- HepMC_Version1.24_Factor/HepMC/OLD/GenEvent.h Tue Oct 7 17:47:17 2003 20,50 // subject

7 Dec 2006: gaps between Tungsten increase effective RMoliere)• Lateral segmentation: 1cm2 matched to RMoliere• Longitudinal segmentation: 30 layers (24 X0, 0.9λhad)• Typical resolution: σE/E = 0.15/E(GeV). ... ALCPG Seminar, Fermilab 8/12/2006 Mark Thomson

23 Nov 2005: 24 The Fourier representation of a Dirac field has the form.

30 Jul 2007: Made on 30-A. ug-2000 17:24:02 by konstant with D. AL. I_F1.Filenam. ... 24. Rµ• Compare ee- s s with ee- µµ-. e-. e+.

4 Sep 2013: with upper basket lowered 24 cm 29 cm. 19. Adding DetergentDetergents remove the dirt from dishes and cutlery. ... 24. Starting a Dishwashing Cycle1. Check that the spray arms can turn freely.2.