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From: "zjwu" <zjwu@ns.ciac.jl.cn>
To: "help@gaussian.com" <help@gaussian.com>
CC: "chemistry@ccl.net" <chemistry@ccl.net>
Subject: Re: Re: CCL:CPCM TS location
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Date: Fri, 2 May 2003 8:26:57 +0800



This is a multi-part message in MIME format.

--=====002_Dragon120100783831_=====
Content-Type: text/plain;
      charset="GB2312"
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Dear Dr. Hess,

Do you know any publications containing cpcm ts structure=
 calculations? I do find some papers on local minima=
 optimizations using cpcm, but did not see any paper on=
 transition state calculation using cpcm model?

Any papers on this aspect are appreaciated.

Best wishes,

Zhijian Wu



Dear Dr. Zhijian Wu,
    You have performed the steps I'd recommend, i.e. using the=
 gas-phase  
Hessian or the Hessian from an Onsager calculation. Since these=
 options  
did not work, it might be necessary to calculate the CPCM=
 Hessian. You  
cannot do this with "opt=3D(ts,calcfc)" in G98, but you can perform=
 a  
two-step job in which the first step uses "freq" and the second=
 job  
step uses "opt=3D(ts,rcfc)". You might also consider performing an =
 
"opt=3Dqst3" calculation in which you use your Onsager model=
 optimized TS  
as the initial guess structure for the CPCM transition state.

Regards,
Jim Hess

On Thursday, April 24, 2003, at 01:13 AM, zjwu wrote:

>>  Dear Dr. Hess,
>> 
>>  ?/DIV> 
>> 
>>  I mean the job failing because the structure is not the TS=
 structure  
>>  anymore. The calculation may converge but goes to different=
 geometry  
>>  which I did not want. I have tried to read force constants at=
 cpcm  
>>  calculation from either gas phase frequency calculation or=
 Onsager  
>>  frequency calculation (these frequencies are obtained based=
 on the  
>>  optimized geometry) (calculation using Onsager model works=
 well for  
>>  the TS calculation).=A0In addition, I also tried=
 opt=3D(ts,calcfc), but as  
>>  you know,=A0calcfc does not exist for=A0cpcm.=A0It seems g03 is=
 possible to  
>>  calculate fc at cpcm level.
>> 
>>  ?/DIV> 
>> 
>>  Hope I have made myself clear.
>> 
>>  ?/DIV> 
>> 
>>  Thank you very much for your answer.
>> 
>>  ?/DIV> 
>> 
>>  Best regards,
>> 
>>  ?/DIV> 
>> 
>>  Zhijian Wu
>> 
>>  ?/DIV> 
>> 
>> 
>> 
<< image.tiff> 
>> 
>>  Dear=A0Dr.=A0Zhijian=A0Wu,
>> =
 =A0=A0=A0=A0Is=A0this=A0job=A0failing=A0because=A0it=A0runs=A0out=A0of=A0optimization=A0cycl=
es?=A0I'd 
>>  ?/DIV> 
>> =
 need=A0to=A0know=A0more=A0details=A0about=A0what=A0is=A0going=A0wrong=A0before=A0I=A0mak=
e?/DIV> 
>> =
 detailed=A0suggestions,=A0but=A0one=A0possible=A0way=A0to=A0improve=A0this=A0calcu=
lation?/DIV> 
>> =
 is=A0to=A0calculate=A0the=A0force=A0constants=A0in=A0the=A0solution=A0phase,=A0then=A0=
use?/DIV> 
>> =
 these=A0force=A0constants=A0to=A0start=A0the=A0transition=A0state=A0search..=A0Usu=
ally=A0the 
>>  ?/DIV> 
>> =
 gas-phase=A0Hessian=A0is=A0a=A0good=A0enough=A0approximation,=A0but=A0in=A0some=A0ca=
ses?/DIV> 
>> =
 where=A0the=A0gas-phase=A0and=A0solution-phase=A0potential=A0energy=A0surfaces=
=A0are?/DIV> 
>> =
 different=A0enough,=A0explicitly=A0calculating=A0the=A0second=A0derivatives=A0=
in=A0the?/DIV> 
>> =
 solution=A0phase=A0can=A0be=A0helpful.=A0Incidentally,=A0if=A0you=A0are=A0using=A0G9=
8,=A0the?/DIV> 
>> =
 CPCM=A0second=A0derivatives=A0will=A0be=A0performed=A0by=A0numerical=A0different=
iation?/DIV> 
>> =
 of=A0the=A0analytic=A0gradients=A0and=A0if=A0you=A0are=A0using=A0G03,=A0the=A0second?/=
DIV> 
>>  derivatives=A0will=A0be=A0calculated=A0analytically.
>>  ?/DIV> 
>>  Regards,
>>  Jim=A0Hess
>>  ?/DIV> 
>>  ++++++++++++++++++++++++++
>>  James=A0Hess,=A0Ph.D.
>>  Customer=A0Support=A0Scientist
>>  Gaussian,=A0Inc.
>>  e-mail:=A0help@gaussian.com
>>  ++++++++++++++++++++++++++
>>  ?/DIV> 
>>  ?/DIV> 
>>  On=A0Tuesday,=A0April?2,?003,=A0at?8:29=A0PM,=A0zjwu=A0wrote:
>>  ?/DIV> 
>>  > >  =A0Dear=A0members,
>>  > > 
>>  > >  ?/DIV> 
>>  > > 
>>  > > =
 =A0I=A0am=A0trying=A0to=A0locate=A0the=A0transition=A0state=A0using=A0cpcm=A0model.=A0Th=
e?/DIV> 
>>  > > =
 =A0initial=A0structure=A0is=A0from=A0gas=A0phase=A0optimized=A0transition=A0struct=
ure?/DIV> 
>>  > >   
>> =
 ?with=A0correct=A0vibrational=A0mode).=A0The=A0optimization=A0at=A0cpcm=A0level=A0=
fails?/DIV> 
>>  > >  =A0by=A0the=A0following=A0keywords
>>  > > 
>>  > >  ?/DIV> 
>>  > > 
>>  > >   
>> =
 ?b3lyp/6-31g(d,p)=A0opt=3D(ts,=A0readfc,=A0noeigen)=A0scrf=3D(cpcm,solvent=3Dw=
ater)
>>  > > 
>>  > >  ?/DIV> 
>>  > > 
>>  > > =
 =A0Do=A0anybody=A0has=A0experience=A0in=A0cpcm=A0transition=A0structure=A0calculat=
ion?
>>  > > 
>>  > >  ?/DIV> 
>>  > > 
>>  > >  =A0Thanks=A0a=A0lot.
>>  > > 
>>  > >  ?/DIV> 
>>  > > 
>>  > >  =A0Best=A0regards,
>>  > > 
>>  > >  ?/DIV> 
>>  > > 
>>  > >  =A0Zhijian=A0Wu
>>  > > 
Dear Dr. Zhijian Wu,

   You have performed the steps I'd recommend, i.e. using the
gas-phase Hessian or the Hessian from an Onsager calculation.=
 Since
these options did not work, it might be necessary to calculate=
 the
CPCM Hessian. You cannot do this with "opt=3D(ts,calcfc)" in G98,=
 but
you can perform a two-step job in which the first step uses=
 "freq" and
the second job step uses "opt=3D(ts,rcfc)". You might also=
 consider
performing an "opt=3Dqst3" calculation in which you use your=
 Onsager
model optimized TS as the initial guess structure for the CPCM
transition state. 


Regards,

Jim Hess


On Thursday, April 24, 2003, at 01:13 AM, zjwu wrote:


<< excerpt> Dear Dr. Hess,


?/DIV> 


I mean the job failing because the structure is not the TS=
 structure
anymore. The calculation may converge but goes to different=
 geometry
which I did not want. I have tried to read force constants at=
 cpcm
calculation from either gas phase frequency calculation or=
 Onsager
frequency calculation (these frequencies are obtained based on=
 the
optimized geometry) (calculation using Onsager model works well=
 for
the TS calculation).=A0In addition, I also tried opt=3D(ts,calcfc),=
 but as
you know,=A0calcfc does not exist for=A0cpcm.=A0It seems g03 is=
 possible to
calculate fc at cpcm level.


?/DIV> 


Hope I have made myself clear.


?/DIV> 


Thank you very much for your answer.


?/DIV> 


Best regards,


?/DIV> 


Zhijian Wu


?/DIV> 




<< /excerpt> < < image.tiff> 

<< excerpt> 

Dear=A0Dr.=A0Zhijian=A0Wu,

=A0=A0=A0=A0Is=A0this=A0job=A0failing=A0because=A0it=A0runs=A0out=A0of=A0optimization=A0cycle=
s?=A0I'd?/DIV> 

need=A0to=A0know=A0more=A0details=A0about=A0what=A0is=A0going=A0wrong=A0before=A0I=A0make=
?/DIV> 

detailed=A0suggestions,=A0but=A0one=A0possible=A0way=A0to=A0improve=A0this=A0calcul=
ation?/DIV> 

is=A0to=A0calculate=A0the=A0force=A0constants=A0in=A0the=A0solution=A0phase,=A0then=A0u=
se?/DIV> 

these=A0force=A0constants=A0to=A0start=A0the=A0transition=A0state=A0search..=A0Usua=
lly=A0the?/DIV> 

gas-phase=A0Hessian=A0is=A0a=A0good=A0enough=A0approximation,=A0but=A0in=A0some=A0cas=
es?/DIV> 

where=A0the=A0gas-phase=A0and=A0solution-phase=A0potential=A0energy=A0surfaces=A0=
are?/DIV> 

different=A0enough,=A0explicitly=A0calculating=A0the=A0second=A0derivatives=A0i=
n=A0the?/DIV> 

solution=A0phase=A0can=A0be=A0helpful.=A0Incidentally,=A0if=A0you=A0are=A0using=A0G98=
,=A0the?/DIV> 

CPCM=A0second=A0derivatives=A0will=A0be=A0performed=A0by=A0numerical=A0differenti=
ation?/DIV> 

of=A0the=A0analytic=A0gradients=A0and=A0if=A0you=A0are=A0using=A0G03,=A0the=A0second?/D=
IV> 

derivatives=A0will=A0be=A0calculated=A0analytically.

?/DIV> 

Regards,

Jim=A0Hess

?/DIV> 

++++++++++++++++++++++++++

James=A0Hess,=A0Ph.D.

Customer=A0Support=A0Scientist

Gaussian,=A0Inc.

e-mail:=A0help@gaussian.com

++++++++++++++++++++++++++

?/DIV> 

?/DIV> 

On=A0Tuesday,=A0April?2,?003,=A0at?8:29=A0PM,=A0zjwu=A0wrote:

?/DIV> 

>> >  =A0Dear=A0members,

>> > 

>> >  ?/DIV> 

>> > 

>> > =
 =A0I=A0am=A0trying=A0to=A0locate=A0the=A0transition=A0state=A0using=A0cpcm=A0model.=A0Th=
e?/DIV> 

>> > =
 =A0initial=A0structure=A0is=A0from=A0gas=A0phase=A0optimized=A0transition=A0struct=
ure?/DIV> 

>> > 
?with=A0correct=A0vibrational=A0mode).=A0The=A0optimization=A0at=A0cpcm=A0level=A0f=
ails?/DIV> 

>> >  =A0by=A0the=A0following=A0keywords

>> > 

>> >  ?/DIV> 

>> > 

>> > 
?b3lyp/6-31g(d,p)=A0opt=3D(ts,=A0readfc,=A0noeigen)=A0scrf=3D(cpcm,solvent=3Dwa=
ter)

>> > 

>> >  ?/DIV> 

>> > 

>> > =
 =A0Do=A0anybody=A0has=A0experience=A0in=A0cpcm=A0transition=A0structure=A0calculat=
ion?

>> > 

>> >  ?/DIV> 

>> > 

>> >  =A0Thanks=A0a=A0lot.

>> > 

>> >  ?/DIV> 

>> > 

>> >  =A0Best=A0regards,

>> > 

>> >  ?/DIV> 

>> > 

>> >  =A0Zhijian=A0Wu

>> > 

<< /excerpt> 

--=====002_Dragon120100783831_=====
Content-Type: text/html;
      charset="GB2312"
Content-Transfer-Encoding: quoted-printable

<!DOCTYPE HTML PUBLIC "-//W3C//DTD HTML 4.0 Transitional//EN">
<HTML><HEAD>
<META http-equiv=3DContent-Type content=3D"text/html;=
 charset=3Dgb2312">
<META content=3D"MSHTML 6.00.2462.0" name=3DGENERATOR></HEAD>
<BODY>
<P>Dear Dr. Hess,</P>
<P>&nbsp;</P>
<P>Do you know any publications&nbsp;containing cpcm ts structure=
 calculations? 
I do find some papers on local minima optimizations using cpcm,=
 but did not see 
any paper on transition state calculation using cpcm model?</P>
<P>&nbsp;</P>
<P>Any papers on this aspect are appreaciated.</P>
<P>&nbsp;</P>
<P>Best wishes,</P>
<P>&nbsp;</P>
<P>Zhijian Wu</P>
<P>
<HR>
</P>
<DIV>Dear&nbsp;Dr.&nbsp;Zhijian&nbsp;Wu,</DIV>
<DIV>&nbsp;&nbsp;&nbsp;&nbsp;You&nbsp;have&nbsp;performed&nbsp;th=
e&nbsp;steps&nbsp;I'd&nbsp;recommend,&nbsp;i.e.&nbsp;using&nbsp;t=
he&nbsp;gas-phase&nbsp;&nbsp;</DIV>
<DIV>Hessian&nbsp;or&nbsp;the&nbsp;Hessian&nbsp;from&nbsp;an&nbsp=
;Onsager&nbsp;calculation.&nbsp;Since&nbsp;these&nbsp;options&nbs=
p;&nbsp;</DIV>
<DIV>did&nbsp;not&nbsp;work,&nbsp;it&nbsp;might&nbsp;be&nbsp;nece=
ssary&nbsp;to&nbsp;calculate&nbsp;the&nbsp;CPCM&nbsp;Hessian.&nbs=
p;You&nbsp;&nbsp;</DIV>
<DIV>cannot&nbsp;do&nbsp;this&nbsp;with&nbsp;"opt=3D(ts,calcfc)"&nb=
sp;in&nbsp;G98,&nbsp;but&nbsp;you&nbsp;can&nbsp;perform&nbsp;a&nb=
sp;&nbsp;</DIV>
<DIV>two-step&nbsp;job&nbsp;in&nbsp;which&nbsp;the&nbsp;first&nbs=
p;step&nbsp;uses&nbsp;"freq"&nbsp;and&nbsp;the&nbsp;second&nbsp;j=
ob&nbsp;&nbsp;</DIV>
<DIV>step&nbsp;uses&nbsp;"opt=3D(ts,rcfc)".&nbsp;You&nbsp;might&nbs=
p;also&nbsp;consider&nbsp;performing&nbsp;an&nbsp;&nbsp;</DIV>
<DIV>"opt=3Dqst3"&nbsp;calculation&nbsp;in&nbsp;which&nbsp;you&nbsp=
;use&nbsp;your&nbsp;Onsager&nbsp;model&nbsp;optimized&nbsp;TS&nbs=
p;&nbsp;</DIV>
<DIV>as&nbsp;the&nbsp;initial&nbsp;guess&nbsp;structure&nbsp;for&=
nbsp;the&nbsp;CPCM&nbsp;transition&nbsp;state.</DIV>
<DIV>&nbsp;</DIV>
<DIV>Regards,</DIV>
<DIV>Jim&nbsp;Hess</DIV>
<DIV>&nbsp;</DIV>
<DIV>On&nbsp;Thursday,&nbsp;April&nbsp;24,&nbsp;2003,&nbsp;at&nbs=
p;01:13&nbsp;AM,&nbsp;zjwu&nbsp;wrote:</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &nbsp;Dear&nbsp;Dr.&nbsp;Hess,</DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; 
&nbsp;I&nbsp;mean&nbsp;the&nbsp;job&nbsp;failing&nbsp;because&nbs=
p;the&nbsp;structure&nbsp;is&nbsp;not&nbsp;the&nbsp;TS&nbsp;struc=
ture&nbsp;&nbsp;</DIV>
<DIV>&gt;&gt; 
&nbsp;anymore.&nbsp;The&nbsp;calculation&nbsp;may&nbsp;converge&n=
bsp;but&nbsp;goes&nbsp;to&nbsp;different&nbsp;geometry&nbsp;&nbsp=
;</DIV>
<DIV>&gt;&gt; 
&nbsp;which&nbsp;I&nbsp;did&nbsp;not&nbsp;want.&nbsp;I&nbsp;have&=
nbsp;tried&nbsp;to&nbsp;read&nbsp;force&nbsp;constants&nbsp;at&nb=
sp;cpcm&nbsp;&nbsp;</DIV>
<DIV>&gt;&gt; 
&nbsp;calculation&nbsp;from&nbsp;either&nbsp;gas&nbsp;phase&nbsp;=
frequency&nbsp;calculation&nbsp;or&nbsp;Onsager&nbsp;&nbsp;</DIV>=

<DIV>&gt;&gt; 
&nbsp;frequency&nbsp;calculation&nbsp;(these&nbsp;frequencies&nbs=
p;are&nbsp;obtained&nbsp;based&nbsp;on&nbsp;the&nbsp;&nbsp;</DIV>=

<DIV>&gt;&gt; 
&nbsp;optimized&nbsp;geometry)&nbsp;(calculation&nbsp;using&nbsp;=
Onsager&nbsp;model&nbsp;works&nbsp;well&nbsp;for&nbsp;&nbsp;</DIV=
>
<DIV>&gt;&gt; 
&nbsp;the&nbsp;TS&nbsp;calculation).=A0In&nbsp;addition,&nbsp;I&nbs=
p;also&nbsp;tried&nbsp;opt=3D(ts,calcfc),&nbsp;but&nbsp;as&nbsp;&nb=
sp;</DIV>
<DIV>&gt;&gt; 
&nbsp;you&nbsp;know,=A0calcfc&nbsp;does&nbsp;not&nbsp;exist&nbsp;fo=
r=A0cpcm.=A0It&nbsp;seems&nbsp;g03&nbsp;is&nbsp;possible&nbsp;to&nbsp=
;&nbsp;</DIV>
<DIV>&gt;&gt;=
 &nbsp;calculate&nbsp;fc&nbsp;at&nbsp;cpcm&nbsp;level.</DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; 
&nbsp;Hope&nbsp;I&nbsp;have&nbsp;made&nbsp;myself&nbsp;clear.</DI=
V>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; 
&nbsp;Thank&nbsp;you&nbsp;very&nbsp;much&nbsp;for&nbsp;your&nbsp;=
answer.</DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;Best&nbsp;regards,</DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;Zhijian&nbsp;Wu</DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&lt;&lt; image.tiff&gt; </DIV>
<DIV>&gt;&gt; </DIV>
<DIV>&gt;&gt; &nbsp;Dear=A0Dr.=A0Zhijian=A0Wu,</DIV>
<DIV>&gt;&gt; 
&nbsp;=A0=A0=A0=A0Is=A0this=A0job=A0failing=A0because=A0it=A0runs=A0out=A0of=A0optimization=
=A0cycles?=A0I'd&nbsp;</DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;need=A0to=A0know=A0more=A0details=A0about=A0what=A0is=A0going=A0wrong=A0before=A0=
I=A0make?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;detailed=A0suggestions,=A0but=A0one=A0possible=A0way=A0to=A0improve=A0this=A0=
calculation?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;is=A0to=A0calculate=A0the=A0force=A0constants=A0in=A0the=A0solution=A0phase,=A0=
then=A0use?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;these=A0force=A0constants=A0to=A0start=A0the=A0transition=A0state=A0search.=
.=A0Usually=A0the&nbsp;</DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;gas-phase=A0Hessian=A0is=A0a=A0good=A0enough=A0approximation,=A0but=A0in=A0so=
me=A0cases?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;where=A0the=A0gas-phase=A0and=A0solution-phase=A0potential=A0energy=A0sur=
faces=A0are?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;different=A0enough,=A0explicitly=A0calculating=A0the=A0second=A0derivat=
ives=A0in=A0the?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;solution=A0phase=A0can=A0be=A0helpful.=A0Incidentally,=A0if=A0you=A0are=A0usi=
ng=A0G98,=A0the?/DIV&gt; 
<DIV>&gt;&gt; 
&nbsp;CPCM=A0second=A0derivatives=A0will=A0be=A0performed=A0by=A0numerical=A0diff=
erentiation?/DIV&gt; 
<DIV>&gt;&gt;=
 &nbsp;of=A0the=A0analytic=A0gradients=A0and=A0if=A0you=A0are=A0using=A0G03,=A0the=A0se=
cond?/DIV&gt; 

<DIV>&gt;&gt;=
 &nbsp;derivatives=A0will=A0be=A0calculated=A0analytically.</DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; &nbsp;Regards,</DIV>
<DIV>&gt;&gt; &nbsp;Jim=A0Hess</DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; &nbsp;++++++++++++++++++++++++++</DIV>
<DIV>&gt;&gt; &nbsp;James=A0Hess,=A0Ph.D.</DIV>
<DIV>&gt;&gt; &nbsp;Customer=A0Support=A0Scientist</DIV>
<DIV>&gt;&gt; &nbsp;Gaussian,=A0Inc.</DIV>
<DIV>&gt;&gt; &nbsp;e-mail:=A0help@gaussian.com</DIV>
<DIV>&gt;&gt; &nbsp;++++++++++++++++++++++++++</DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt;=
 &nbsp;On=A0Tuesday,=A0April?2,?003,=A0at?8:29=A0PM,=A0zjwu=A0wrote:</DIV>
<DIV>&gt;&gt; &nbsp;?/DIV&gt; 
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;=A0Dear=A0members,</DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; 
&nbsp;=A0I=A0am=A0trying=A0to=A0locate=A0the=A0transition=A0state=A0using=A0cpcm=A0mode=
l.=A0The?/DIV&gt; 
<DIV>&gt;&gt; &nbsp;&gt; &gt; 
&nbsp;=A0initial=A0structure=A0is=A0from=A0gas=A0phase=A0optimized=A0transition=A0s=
tructure?/DIV&gt; 
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;&nbsp;</DIV>
<DIV>&gt;&gt; 
&nbsp;?with=A0correct=A0vibrational=A0mode).=A0The=A0optimization=A0at=A0cpcm=A0l=
evel=A0fails?/DIV&gt; 
<DIV>&gt;&gt; &nbsp;&gt; &gt;=
 &nbsp;=A0by=A0the=A0following=A0keywords</DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;&nbsp;</DIV>
<DIV>&gt;&gt; 
&nbsp;?b3lyp/6-31g(d,p)=A0opt=3D(ts,=A0readfc,=A0noeigen)=A0scrf=3D(cpcm,solv=
ent=3Dwater)</DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; 
&nbsp;=A0Do=A0anybody=A0has=A0experience=A0in=A0cpcm=A0transition=A0structure=A0cal=
culation?</DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;=A0Thanks=A0a=A0lot.</DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;=A0Best=A0regards,</DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; &nbsp;=A0Zhijian=A0Wu</DIV>
<DIV>&gt;&gt; &nbsp;&gt; &gt; </DIV>
<DIV>Dear&nbsp;Dr.&nbsp;Zhijian&nbsp;Wu,</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;&nbsp;&nbsp;You&nbsp;have&nbsp;performed&nbsp;the&nbsp=
;steps&nbsp;I'd&nbsp;recommend,&nbsp;i.e.&nbsp;using&nbsp;the</DI=
V>
<DIV>gas-phase&nbsp;Hessian&nbsp;or&nbsp;the&nbsp;Hessian&nbsp;fr=
om&nbsp;an&nbsp;Onsager&nbsp;calculation.&nbsp;Since</DIV>
<DIV>these&nbsp;options&nbsp;did&nbsp;not&nbsp;work,&nbsp;it&nbsp=
;might&nbsp;be&nbsp;necessary&nbsp;to&nbsp;calculate&nbsp;the</DI=
V>
<DIV>CPCM&nbsp;Hessian.&nbsp;You&nbsp;cannot&nbsp;do&nbsp;this&nb=
sp;with&nbsp;"opt=3D(ts,calcfc)"&nbsp;in&nbsp;G98,&nbsp;but</DIV>
<DIV>you&nbsp;can&nbsp;perform&nbsp;a&nbsp;two-step&nbsp;job&nbsp=
;in&nbsp;which&nbsp;the&nbsp;first&nbsp;step&nbsp;uses&nbsp;"freq=
"&nbsp;and</DIV>
<DIV>the&nbsp;second&nbsp;job&nbsp;step&nbsp;uses&nbsp;"opt=3D(ts,r=
cfc)".&nbsp;You&nbsp;might&nbsp;also&nbsp;consider</DIV>
<DIV>performing&nbsp;an&nbsp;"opt=3Dqst3"&nbsp;calculation&nbsp;in&=
nbsp;which&nbsp;you&nbsp;use&nbsp;your&nbsp;Onsager</DIV>
<DIV>model&nbsp;optimized&nbsp;TS&nbsp;as&nbsp;the&nbsp;initial&n=
bsp;guess&nbsp;structure&nbsp;for&nbsp;the&nbsp;CPCM</DIV>
<DIV>transition&nbsp;state.&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>Regards,</DIV>
<DIV>&nbsp;</DIV>
<DIV>Jim&nbsp;Hess</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>On&nbsp;Thursday,&nbsp;April&nbsp;24,&nbsp;2003,&nbsp;at&nbs=
p;01:13&nbsp;AM,&nbsp;zjwu&nbsp;wrote:</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>&lt;&lt; excerpt&gt; Dear&nbsp;Dr.&nbsp;Hess,</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>I&nbsp;mean&nbsp;the&nbsp;job&nbsp;failing&nbsp;because&nbsp=
;the&nbsp;structure&nbsp;is&nbsp;not&nbsp;the&nbsp;TS&nbsp;struct=
ure</DIV>
<DIV>anymore.&nbsp;The&nbsp;calculation&nbsp;may&nbsp;converge&nb=
sp;but&nbsp;goes&nbsp;to&nbsp;different&nbsp;geometry</DIV>
<DIV>which&nbsp;I&nbsp;did&nbsp;not&nbsp;want.&nbsp;I&nbsp;have&n=
bsp;tried&nbsp;to&nbsp;read&nbsp;force&nbsp;constants&nbsp;at&nbs=
p;cpcm</DIV>
<DIV>calculation&nbsp;from&nbsp;either&nbsp;gas&nbsp;phase&nbsp;f=
requency&nbsp;calculation&nbsp;or&nbsp;Onsager</DIV>
<DIV>frequency&nbsp;calculation&nbsp;(these&nbsp;frequencies&nbsp=
;are&nbsp;obtained&nbsp;based&nbsp;on&nbsp;the</DIV>
<DIV>optimized&nbsp;geometry)&nbsp;(calculation&nbsp;using&nbsp;O=
nsager&nbsp;model&nbsp;works&nbsp;well&nbsp;for</DIV>
<DIV>the&nbsp;TS&nbsp;calculation).=A0In&nbsp;addition,&nbsp;I&nbsp=
;also&nbsp;tried&nbsp;opt=3D(ts,calcfc),&nbsp;but&nbsp;as</DIV>
<DIV>you&nbsp;know,=A0calcfc&nbsp;does&nbsp;not&nbsp;exist&nbsp;for=
=A0cpcm.=A0It&nbsp;seems&nbsp;g03&nbsp;is&nbsp;possible&nbsp;to</DIV>=

<DIV>calculate&nbsp;fc&nbsp;at&nbsp;cpcm&nbsp;level.</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>Hope&nbsp;I&nbsp;have&nbsp;made&nbsp;myself&nbsp;clear.</DIV=
>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>Thank&nbsp;you&nbsp;very&nbsp;much&nbsp;for&nbsp;your&nbsp;a=
nswer.</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>Best&nbsp;regards,</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>Zhijian&nbsp;Wu</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>&nbsp;</DIV>
<DIV>&lt;&lt; /excerpt&gt; &lt; &lt; image.tiff&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&lt;&lt; excerpt&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>Dear=A0Dr.=A0Zhijian=A0Wu,</DIV>
<DIV>&nbsp;</DIV>
<DIV>=A0=A0=A0=A0Is=A0this=A0job=A0failing=A0because=A0it=A0runs=A0out=A0of=A0optimization=A0=
cycles?=A0I'd?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>need=A0to=A0know=A0more=A0details=A0about=A0what=A0is=A0going=A0wrong=A0before=A0I=
=A0make?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>detailed=A0suggestions,=A0but=A0one=A0possible=A0way=A0to=A0improve=A0this=A0c=
alculation?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>is=A0to=A0calculate=A0the=A0force=A0constants=A0in=A0the=A0solution=A0phase,=A0t=
hen=A0use?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>these=A0force=A0constants=A0to=A0start=A0the=A0transition=A0state=A0search..=
=A0Usually=A0the?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>gas-phase=A0Hessian=A0is=A0a=A0good=A0enough=A0approximation,=A0but=A0in=A0som=
e=A0cases?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>where=A0the=A0gas-phase=A0and=A0solution-phase=A0potential=A0energy=A0surf=
aces=A0are?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>different=A0enough,=A0explicitly=A0calculating=A0the=A0second=A0derivati=
ves=A0in=A0the?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>solution=A0phase=A0can=A0be=A0helpful.=A0Incidentally,=A0if=A0you=A0are=A0usin=
g=A0G98,=A0the?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>CPCM=A0second=A0derivatives=A0will=A0be=A0performed=A0by=A0numerical=A0diffe=
rentiation?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>of=A0the=A0analytic=A0gradients=A0and=A0if=A0you=A0are=A0using=A0G03,=A0the=A0seco=
nd?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>derivatives=A0will=A0be=A0calculated=A0analytically.</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>Regards,</DIV>
<DIV>&nbsp;</DIV>
<DIV>Jim=A0Hess</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>++++++++++++++++++++++++++</DIV>
<DIV>&nbsp;</DIV>
<DIV>James=A0Hess,=A0Ph.D.</DIV>
<DIV>&nbsp;</DIV>
<DIV>Customer=A0Support=A0Scientist</DIV>
<DIV>&nbsp;</DIV>
<DIV>Gaussian,=A0Inc.</DIV>
<DIV>&nbsp;</DIV>
<DIV>e-mail:=A0help@gaussian.com</DIV>
<DIV>&nbsp;</DIV>
<DIV>++++++++++++++++++++++++++</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>On=A0Tuesday,=A0April?2,?003,=A0at?8:29=A0PM,=A0zjwu=A0wrote:</DIV>
<DIV>&nbsp;</DIV>
<DIV>?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;=A0Dear=A0members,</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; 
&nbsp;=A0I=A0am=A0trying=A0to=A0locate=A0the=A0transition=A0state=A0using=A0cpcm=A0mode=
l.=A0The?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; 
&nbsp;=A0initial=A0structure=A0is=A0from=A0gas=A0phase=A0optimized=A0transition=A0s=
tructure?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>?with=A0correct=A0vibrational=A0mode).=A0The=A0optimization=A0at=A0cpcm=A0le=
vel=A0fails?/DIV&gt; 
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;=A0by=A0the=A0following=A0keywords</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>?b3lyp/6-31g(d,p)=A0opt=3D(ts,=A0readfc,=A0noeigen)=A0scrf=3D(cpcm,solve=
nt=3Dwater)</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; 
&nbsp;=A0Do=A0anybody=A0has=A0experience=A0in=A0cpcm=A0transition=A0structure=A0cal=
culation?</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;=A0Thanks=A0a=A0lot.</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;=A0Best=A0regards,</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;?/DIV&gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; &nbsp;=A0Zhijian=A0Wu</DIV>
<DIV>&nbsp;</DIV>
<DIV>&gt;&gt; &gt; </DIV>
<DIV>&nbsp;</DIV>
<DIV>&lt;&lt; /excerpt&gt; </DIV>
<HR>
</DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV=
></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DI=
V></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></D=
IV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></DIV></=
DIV></DIV></DIV></DIV></DIV></DIV></DIV></BODY></HTML>

--=====002_Dragon120100783831_=====--




From chemistry-request@server.ccl.net Sun Apr 27 19:15:49 2003
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  charset="us-ascii"
From: Matt Challacombe <MChalla@LANL.Gov>
Reply-To: MChalla@LANL.Gov
Organization: Group T-12, Los Alamos National Lab
To: CHEMISTRY@ccl.net
Subject: xyz->zmat->xyz
Date: Sun, 27 Apr 2003 17:07:14 -0600
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Hi,

Is there a simple program for converting from xyz to 
z-matrix and back?  I've spent quite a while examining 
different versions of babel, but none of them seem to 
work in this capacity...

Thx, Matt

-- 
Matt Challacombe       
Theoretical Division, Los Alamos           
http://www.t12.lanl.gov/~mchalla/ 
 


From chemistry-request@server.ccl.net Sun Apr 27 07:53:41 2003
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Date: Sun, 27 Apr 2003 13:53:46 +0200
From: "Jeremy R. Greenwood" <jeremy@compchem.dfh.dk>
To: CHEMISTRY@ccl.net
Subject: Ab initio prediction of time-averaged NMR shifts
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Dear CCL,

Question: can someone provide a reference/suggestion/theory/method/example
for extending ab initio NMR chemical shift prediction to the reproduction 
of time-averaged shifts for systems in rapid equilibrium?

--

My problem:

I have characterised a potential energy surface (to basis set 
convergence with B3LYP) of a strained system as 
[1] -- TS1,2 -- [2] -- TS2,3 -- [3]
Where the transitions involve (et al.) ca. 60 degree 
torsional sweeps about RCH2--N-oxide(RR')--CH2R bonds.

The barriers are modest, and at normal temperatures the interchange 
is rapid, thus the NMR spectrum gives a sharp-line average.

I have calculated magnetic shielding tensors for minima and transition
states, and could in principle do it for points along the path. 
The 1H proton shifts vary dramatically over the energy surface as
the protons move in the shadow of the chiral N-O. I doubt a naive 
approach of linearly combining the shifts of the minima according 
to relative energy will tell the story of the time-averaged structure
and its magnetic properties.

Thanks in advance for any suggestions.

Jeremy
----------------------------------------------------------------------
Jeremy Greenwood                                  jeremy@greenwood.net
Department of Medicinal Chemistry                      bh +45 35306117
The Danish University of Pharmaceutical Sciences       fx +45 35306040
Universitetsparken 2, DK-2100 Copenhagen, Denmark      ah +45 32598030
----------------------------------------------------------------------


