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15 Dec 2008: Introduce abstract concept of a field – the strength and direction of the force felt by a test body is uniquely defined at every point in space.

4 Dec 2008: To illustrate this procedure, we have used the test case with n = 2. ... temperature. We have applied this technique to our test case with four extra dimensions. –

4 Dec 2008: t decay, SUSY in future) directly from AMEGIC++• Works very well, further thorough tests required.• More to come (EvtGen,. )? ... With IS and FS showers running:– Can start to test Drell–Yan and jets in pp collisions. –

4 Dec 2008: Our supersymmetric test points, Monte Carlo event generator and detector. simulation are described in section 3. ... In fig. 6 we present the statistical separation expected for our test points (S5.

4 Dec 2008: ξ p. ZEUSH1. DIS:BESTASSOMARK IITPCCELLOAMYALEPHDELPHIL3OPAL. ee:. MLLA QCD fitwithout coherence. Energy-dependence of the peak position ξp tests suppression of hadron production at small.

4 Dec 2008: many models. We apply this technique to a test case with four extra dimensions and, using. ... Figure 7 shows. such a measurement for the test case with n = 2 which gives 〈QLept〉 = 0.1266 0.002and thus 〈QBH〉 = 0.654 0.008 using the expected

4 Dec 2008: states. Corrections up to O(α3S) are known. Comparisons with data provide test of QCD matrixelements, through shape of distribution, and measurement of αS, from overall rate.

4 Dec 2008: Highly non-trivial test (of both computations) for shapes and rates! MTWW =. (ET ll /ET )2 (pT ll /pT )2 where ET ll =. p2T ll m. 2ll. and /ET. /p2T m2ll

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23 Oct 2008: SctRodDaq. CGL. The ASICs are called “ABCD”s. Where the tests come in. ... Where the tests come in. A “ROD” (Read Out D). A Rod Crate:.