Nucl ear
Physi cs B349 ( 1991) 635- 654
Nort h-Hol l and
C
C NGAND
SEMI - I NCLUSI VE CESSES
AT L®
. RGEx
S . CATANI ** and B .R. WEBBER
Car endi sh Labor at or y, Uni r er si t y of Cambri dge, Madi ngl ey
Road, Cambr i dge CB3 OH3, UK
G . MARC' HESI NI
Di part i ment o di Fi si ca, Uni r er si t à
di
Par ma,
I NFN, Gi zi ppo Col l egat o di Par ma, I t al y
Recei ved 22 June 1990
Usi ng t he QCD coher ent
br anchi ng al gori t hm, we comput e t he Deep I nel ast i c Scat t er i ng
and Drel l -Yan har d cr oss sect i ons in t he sem i - i ncl usi ve r egi on of l ar ge x .
The cal cul at i on is
done
to
next - t o- l eadi ng
l ogar i t hm ic accur acy in t he resummat i on of per t ur bat i ve QCD . We
compar e t he r esul t s with t he known anal yt i cal expr essi ans to t he s ame
accur acy
in t he
MS
subt r act i on s c heme . They coi nci de if one def i nes an i mpr ove- J br anchi ng al gor i t hm sui t abl e f or
Mont e Carl o si mul at i on, in whi ch t he t wo-l oop r unni ng coupl i ng const ant and
Al t ar el l i - Par i si
spl i t t i ng f unct i on ar e used. Ther ef or e such a si mul at i on can be used to measur e . 1j w s f r om t hese
sem i - i ncl usi ve cr oss sect i ons .
Mor eover
we show
t hat t he s ame r esul t s can al so be obt ai ned usi ng
t he usual one- l oop spl i t t i ng f unct i on, pr ovi ded t he scal e paramet er .1 Mc used in t he Mont e
Carl o si mul at i on is r el at ed
to
;1
Ms
by
a comput ed f act or : :1
mc
=
1
. 569 .1
Ms
( f or five f l avour s) .
1 . I nt r oduct i on
The per t ur bat i ve eval uat i on of physi cal quant i t i es in har d hadr oni c pr ocesses is
char act er i zed by t he pr esence of l ar ge doubl e l ogar i t hm i c cor r ect i ons [I], whi ch
ar e
due t o t he em i ssi on of bot h sof t and col l i near gl uons . In or der to comput e
physi cal
pr ocesses cor r ect l y it is necessar y to r esum t hese l ar ge cor r ect i ons t o al l
or der s in
t he QCD coupl i ng const ant « s .
Col l i near l ogar i t hm ic cont r i but i ons af f ect any har d pr ocess wi t h det ect ed
hadr ons
in t he i ni t i al or f i nal st at e
.
They can be r es ummed by usi ng r enor mal i zât i on
gr oup
t echni ques [ 2] and by def i ni ng hadr oni c st r uct ur e and f ragment at i on
f unct i ons .
Sof t l ogari t hms
ar e r el evant
in t he comput at i on of i nf r ar ed (I R) sensi t i ve
qu2^t i -
t i es
. These
can
be cl assi f i ed
i nt o t wo subcl asses accor di ng to whet her
f i nal - st at e
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