Pairs in pp Collisions - inspire-hep

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Amherst, Massachusetts, 01003. D.C. Christian, G. Gutierrez, S.D. Holmes, and A.Wehmann. Fermi National Accelerator Laboratory,. Batavia, Illinois 60510.
a

Fermi National Accelerator

Laboratory

FERMILAB-Pub-92/67

Observation of Coulomb Effects in Production of n;+r, and K+ K- Pairs in pp Collisions at 27.5 GeV/c L.R. Wiencke, M.D. Church, E.E. Gottschalk, R.A. Hylton, B.C. Knapp, W. Sippach and B.J. Stern Columbia Univeristy, Neuis Laboratories, Irvington, New York 10533

E.P. Hartouni, D.A. Jensen, B. Klima, M.N. Kreisler, M.S.Z. Rabin, J.B. Strait, and J. Uribe Department

of Physics and Astronomy, Amherst,

University of Massachusetts, Massachusetts, 01003

D.C. Christian, G. Gutierrez, S.D. Holmes, and A.Wehmann Fermi National Accelerator Laboratory, Batavia, Illinois 60510

C. Avilez Institute

de Fisica, Uniuersidad de Guanajuato, Leon, Gto., Mexico

M. Forbush, F.R. Huson and J.T. White Depatiment

of Physics, Terns A & M University, College Staion, Texas 77843

October 1992 Submitted

0

to Physical

Operated by Universities

Review D

Research Association

Inc. under Contract No. DE-AC02-76CH03000

with me United States Department

of Energy

Disclaimer

This report was prepared as an account of work sponsored by an agency of the United States Gouernment. Neither the United States Government nor any agency thereof nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, ‘completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof: The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof:

To Be Published

in

Physical

Review

D (1992).

Ncvis RW 1477 UMHEP 392 FERMIlAB PUB 92/67

Observation of Coulomb Effects in Production of lt+n-, pn-, and K*K- Pairs in pp Collisions rt 27.5 GcVlc

l

L.R. Wicncke, M.D. Church(a), E.E. Gottschalk, R.A. HyIton(b). B.C. Knapp, W. Sippach, and B.J. Stern(c) University, Ncvis’ Laboratories. Irvington, New York 10533 USA

Columbia

E.P. Hartouni,

M.S.Z. Deparlmenl

D.A. Jensen(e), B. Klimata), M.N. Kreisler. Rabin, J.B. Straitfa), and J. Uribe

df Physics and Astronomy. Amherst, Massachusells

D. C. Christian,

G. Gutierrez. Fermilab,

Batavia,

University of Massachusetts. 01003 USA

S.D. Holmes,

and A. Wehmann

Illinois

USA

60510

C. Avilcz(c) Institute

de Fisica.

Univcrsidsd

M:+er&stie)),

de Guanajualo.

F.R. Huson.

Leon, Gto.. Mexico

and J.T. &hite

Department of Physics, Texas ABM Universily. College Station. Texas 77843 USA

*Funded

in part

PHY89-21320, Contracts CONACyT

by the National PHY90-14879;

No. DE-AC02-76CH03000, de Mexico.

Science

Foundation

the Department

under

of Energy

DE-ASOS-87ER40356;

Grants under and

Abstract In a study

of collisions

have

observed

pairs

when

frame

interaction

(PACS

enhanced

the relative

approaches

enhancement

of 27.5 GeVlc

ac.

agree

production velocity

as described

numbers:

13.85.Hd.

with

in liquid

of oppositely of the two

The scale

well

protons

hadrons

and velocity

the effect

by the Gamow

13.40.K~)

charged

dependence

we

hadron

in the pair

of the attractive factor.

hydrogen

of the Coulomb

ies~

The

electromagnetic

modify

observed

having

relative

interaction

phase

space

velocity,

fi*,

has long

for pairs

densities in their

been

rest frame

of order

effect

is described

by the Gamow

G(q)=ZItq/(e**nl-1).

where

q=a2tZ-2p/qq,

uis

l/m+

+

1 /m-).

Z+and

three-momentum

difference

qccu. R* is simply

q12u.

correction observation

used

reconstructed GeV/c

Gradient

protons

Six

drift

measured magnetic was

in liquid

charged field

GeV/c). hardware

of central

trajectories value

by time-of-flight counter

reconstruction

7.5 kG.

used

production.

Alternating-

a large

l.mm

aperture at high

particle

rates.

to 1..7.mm

in a non-uniform Direct

8

in interactions

interactions

distance

high

on average

produced

hodoscopes (n/K/p

We report

pair

at the BNL

complex

of metimuml-drift particle

foil(o).

containing

766(7)

direct

in x%-pair

in moderately

were

When

The first

and K+K-

hydrogen

Experiment

Cherenkov Track

that

I) to measure

c.hambers

provided

threshold

using

(Fig.

events

and q is the

as an unobservable

interaction

pn-,

mass

of the pair.

studies(s).

effects

This

factor,

charges,

on tantalum

for n+x-,

particles

Sy~nchrotron.

spectrometer

protons

300 million

charged

used

particles

ac(t-4).

reduced

frame

correlation

of Coulomb

pp collisions

We analyzed

has been

state Coulomb

70 GeV/c

the measurement

multiplicity

27.5

pair

of the final

production here

G(q)

in same sign

the

Z- are the particle in the rest

to

of charged

velocity-dependent

( l/u=

predicted

dipole identification

and by a 96-cell

thresholds

was performed

of 2.5/9.0/17.0 by a special

purpose

processor(8).

We investigate

the p’, dependence

quantities

are independent

that

of (+/-) of particle

pairs

at small

fi*

mass assignment.

of

We directly the

pair

measure momentum,

qL, the relative

momentum

and

asymmetry:

Y-(IPr-IP-I)/(IPr+lP-I)

momentum

where

For relativistic

momenta.

P+and

small

perpendicular

P’ are the particles’

opening

angle

to

lab

pairs,

Y=E+!b$ ( )I )I1 For small

a narrow

ql,

provides

a signature

We selected neither

particle

intersecting

assigned

softer

pairs

for the conversion

horizontal

candidates

counter with

as an e+(e-);

identified

as heavier

Fig.

to help

select

2 shows

a pion;

< 250 (MeV/c)2, and both

by at least

particles two

e+e- pairs

These pairs,

from

c+e- pairs

samples:

qx i

100

(J15-lOMeV/c 2 .-a 0 a 150 z Dti 100 E :

50 (J10-5 MeV/c 0 0.65 0.7 0.75

0.8

Y (Data)

0.65

~0.7

0.75

Y (Monte Carlo)

Fig. 4

0.8

Number 8

0

-

of Pairs -

IA0

Per

Y bin L

(1 bin = 0.02) cm0 M i.3

2,