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p1,p5,q1,q5), The base invariance test demands that these tt.,ro numbers be equal; i.e., that (7) Ut Us Us P(p ,p ,q Ut ,q )/P(p ,p ,q ,q ) — P(p it it isis ,p ,q ,q )/P(p ,p ,q ,q ). Our next test was first proposed by Laspeyres (1871,308), and has. come to be known as the strong identity if prices in the two periods under consideration remain constant, then even if the quantities change11...

www.nber.org/papers/w2713.pdf

Optimal Non-Preemptive Semi-Online Scheduling on

If OPT runs J1 with two more jobs, OPT ≥ p1 + p4 + p5 ≥ 1 SONL ≥ C 1 SONL. q (q ) We split the case where OPT runs J1 with exactly one other job in three subcases, based on which job is combined with J1 .

math.haifa.ac.il/lea/pfh.pdf

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www.logicalchess.com/hcc/reports/sco2003/open_gameframe0102.html

Modeling aggregated returns with

In this manner the transition matrix in Table 5.2 was constructed, where for simplicity, p1,1 = p and p2,2 = q . Table 5.2: Markov Chain Transition Probabilities for Two Aggregated Returns Next State St+1 = (1, 1) St+1 = (2, 0) p2 (1 − p)q p2 (1

p)2 (1 − q ) + q (1 − p)p From lines 2 to 5 we use the Markov property from the underlying log return model. Using this technique the transition matrix can be calculated.

www.stat.sfu.ca/content/dam/sfu/stat/alumnitheses/Singh-2006.pdf

NNLO predictions for event shapes and jet rates in electron-positron...

(1.1) where q1 and q2 are the momenta of the initial-state particles and 1/(8s) corresponds to the ux factor and the average over the spins of the initial state particles. The observable has to be infrared safe, in particular this implies that in single and double unresolved limits we must have ′ O4 ( p1 , ..., p4 , q1 , q2 ) → O3 ( p′ 1 , ..., p3 , q1 , q2 ) for single unresolved limits, for double unresolved limits.

pos.sissa.it/archive/conferences/092/051/RADCOR2009_051.pdf

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