A test for the first moment sum rule in the two-dimensional one-component plasma

A test for the first moment sum rule in the two-dimensional one-component plasma

15 January 1981 CHEMICAL PHYSICS LETTERS Volume 85, number 3 COhfWENT A TEST FOR THE FIRST MOMENT SUM RULE IN THE TWO-DIMENSIONAL ONE-COMPONENT PLA...

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15 January 1981

CHEMICAL PHYSICS LETTERS

Volume 85, number 3

COhfWENT A TEST FOR THE FIRST MOMENT SUM RULE IN THE TWO-DIMENSIONAL ONE-COMPONENT PLASMA L BLUhl* Dcparrmcrrr

of P~I_ISICS Umersrf_v of P~rrrro RICO RIO hedras.

Puerto RICO 00931,

USA

Jlld

D HENDERSON * IRJI Rcscarch Lahoraror_l . San Rrccwrd

29 Scptcmber

198

Jose Cahfonrra

95193.

US-1

I

The recent cuct solution oi lhc one-component two-dunenslonal mhomogencous conswent wth the sum rule for the iis. moment oi the polr correlation funcllon

III J rcant fld

conununtcat~un

[ I ] WCdcrtvcd n suni rule for the

pair

correlation

plasma by Jmcovm IS shown to be

function

of an electrolyte

near a

ch.rrged tntcrf.rcc

Thus sum rule. which IS tn contrJdtcIton to the ones dcrtved by Gruber et al of long-raugcd corrcldttons m the mhomogcneous regton nc.rr the flat interface. aP,(=I -

1

aE

171. and so tmpltes the extstcncc 1s

,,I =Pp,(‘I),~

e,J&

-

:l)P,(=&(l

2) %

wltcrc p,(zt)

IS tllc smglct densrty 01 tome spcctes

I at 3 dtstancc zl from the charged wall. E

clcctnc

P = I/knT

fxtor.

kld.

corrclatton For

IS

the Boltzntann

thermal

e,

IS

IS the

ektcrnal

the electrtc charge of tons]. and Ir,,(1.2)

appltcd

IS the pair

Functton

IIIC

~nl~o~~~ogcncous

tltng bxhground.

one-component

plasma tn two dtmenstons (with

w1t11 bulk density pb = I/a.

a logartthmic

interactton)

on a neutral-

and plasma coupltng constant

r=flez=z_

(3

13111~sfound that

ktncovic:

p(z)

satdies

eucrly

(3) whcrc o qs = -oe

IS

the surface chxge

m electron

umts. or

(4

= E/2x.

wnh qs IIIC surface charge per umt area and a(r) l

Supported ta part by NST Cnnt

374

No CHE80-01969

ts the error function,

CHEMICAL PHYSICS LETTERS

Volume 85. number 3

The parr correlatron

function

IS January 1981

IS

PT(l.7_)=P(Z&(Z2)II(l.2)

= ev[-(zt

- z2)21(41n3)

Constdcr now 111~M-t-hand

(6) stdc of (I )

P= j= dz2 r P~(I.~_)(:~ -=l)d_v2 -Em 0

=_-

:3[

(=2 - =I)

e\p[-(z2

(7)

- z1)2]

dz2_[r,z,,

eap{--f7 - 7_-“2(=t +=d”} x _<,I2 R(I - 1 +@(r2)

cxp(-[rt

- 2”2(zt

- c,p[_7’,q,.7(,, dt2 / _a2

I + aqf,)

+ =2)1’3

dr,

_ r,), d,,, _

w

But _Y ClPl

_= so Ill31

Y,,,(t,- _

- tz)j d_v2= 7%6(t1 -

- ‘a)

(9)

(10)

Exchangmg _f

-is-l12

the order m the mtcgratton. c-S2

and usmg

&=1+@(t).

(I I)

--I we get exp(-

P=e[I lntegrattng

p=_l

+ .I’?- [ I + +(t)](t

- 3”rz,)}

dr

_

+*(t)]”

by parts

112 exp[--2(an

() L

H 2n

+ zt)2]

1 + @(-21/2,,)

whtch satisfies eq. (1). one [2],

tz + Z3/‘z,) Ic_t2

I ap =_-AZ___. 4s aa

the sum rule of Blum et al

e ap

(13)

2 aE

[ 11. We therefore

conclude

that thts sum rule. and not the cariter

Is correct. 375

Volume

85

numbs

CHEMICAL

3

We thank. Professors B Jancovtc~, J.L. Lebowttz

PHYSICS

15 January 1981

LE-ITERS

and hi S. Wcrthetm

for very useful comments.

References [ 11 L Ulum. D Henderson, J L Lebowtz, Ch Grubcr and Ph A blxtm, J. Chcm [2] Ch Grubcr J L Lcboalrrand Ph A Martm. J Chem Phys. 75 (1981) 94-I [ 3 1 B Jancovw J Phys 0’~s) 42 (198 1) L223. prwatc commumalion

Phys ,

to be

pubhshed.

ERRATUM

W L Faust, L S Goldberg,

B B Cratg and R G W~ss, Ttme-resohed

emtsston from short-pulse

tton tnschantsms.

Chem

fragmentatton

Phys

Letters

Cz Swan

of CO- ekldence for two Cz forma-

83 (1981)

7-65

in the process of pubhcatton. the cttatton of authors and affiltattons was modtfied front the form presented m the ongmal manuscrtpt The correct cttatton to be restored IS

B B CRAIG Nod

* Dzpartrtret~r

316

*. W L FAUST,

Rcseorclr Loborarory

L S GOLDBERG

IVash:r~gro~r.DC 10375

and R G WEISS * US-I

of ChenrrsrryGcorgerowrz U~II ersrr), I~tdmg~orr.DC

XlOS7.

USA