From owner-chemistry@ccl.net Wed Apr 8 07:49:01 2015 From: "J D Whitfield jdwhitfield-.-gmail.com" To: CCL Subject: CCL: Announcement of "Novel Computing Approaches to Quantum Chemistry" workshop (8/10 - 8/14) Message-Id: <-51221-150408073129-20802-eJ9s/Mp8/sWLLLm7VN7KNw%%server.ccl.net> X-Original-From: J D Whitfield Content-Type: multipart/alternative; boundary=f46d04428288e20927051334de64 Date: Wed, 8 Apr 2015 13:31:22 +0200 MIME-Version: 1.0 Sent to CCL by: J D Whitfield [jdwhitfield{=}gmail.com] --f46d04428288e20927051334de64 Content-Type: text/plain; charset=UTF-8 We are pleased to announce the "Novel Computing Approaches to Quantum Chemistry" workshop, to be held at the Telluride Science Research Center, Colorado, 10-14 August 2015. The workshop will provide a forum for researchers in the fields of Quantum Chemistry, Quantum Simulation, Tensor Network Methods and Hamiltonian Complexity Theory with the aim of exchanging recent results and ideas of joint interest, along with a discussion on future research strategies. More information of the workshop can be found on its homepage: http://www.telluridescience.org/meetings/workshop-details?wid=557 The registration link is here: https://www.telluridescience.org/for-scientists/for-participants/register/ Further queries can be addressed to us at james.whitfield*o*univie.ac.at *z.zimboras*o*ucl.ac.uk * We look forward seeing you at the Telluride Research Center! James Whitfield and Zoltan Zimboras -- Dr. J. D. Whitfield VCQ Postdoctoral Fellow Vienna Center for Quantum Science and Technology email: james.whitfield*o*univie.ac.at web: homepage.univie.ac.at/james.whitfield --f46d04428288e20927051334de64 Content-Type: text/html; charset=UTF-8 Content-Transfer-Encoding: quoted-printable
We are pleas= ed to announce the "Novel Computing Approaches to Quantum Chemistry&qu= ot;
workshop, to be= held at the Telluride Science Research Center, Colorado, 10-14 August 2015= .

The workshop will provide a for= um for researchers in the fields of Quantum Chemistry,
Quantum Simulation, Tensor Network Meth= ods and Hamiltonian Complexity Theory with
the aim of exchanging recent results and ideas of j= oint interest, along with a discussion
on future research strategies.

More information of the workshop can be found on its home= page:

The registration link is here:
https://w= ww.telluridescience.org/for-scientists/for-participants/register/
Further queries can be addressed to us at

z.zimboras*o*ucl.ac.uk

We look forward seeing you at the Telluride Research Center!
James Whitfield a= nd=C2=A0Zoltan Zimboras
--

Dr. = J. D. Whitfield
VCQ Postdoctoral Fellow
Vienna Center f= or Quantum Science and Technology


<= div>
--f46d04428288e20927051334de64-- From owner-chemistry@ccl.net Wed Apr 8 09:39:00 2015 From: "Sergio Manzetti sergio.manzetti\a/outlook.com" To: CCL Subject: CCL: Broken symmetry Message-Id: <-51222-150408093808-6924-IhkElAoyyukVXAuG7gkWDQ###server.ccl.net> X-Original-From: "Sergio Manzetti" Date: Wed, 8 Apr 2015 09:38:06 -0400 Sent to CCL by: "Sergio Manzetti" [sergio.manzetti::outlook.com] Dear All, while doing ab initio calculations, I experienced a limitation for a quintet state, where it seems impossible to resolve the symmetry of the system. This system was originally optimized using M06-2X and subequently subjected to ab initio with BCCD. The quintet state does not result, and only singlet and triplet can be resolved. Is there any approach to try to solve this? Thanks From owner-chemistry@ccl.net Wed Apr 8 10:43:01 2015 From: "ashika torikora ashika.torikora(_)gmail.com" To: CCL Subject: CCL:G: Understanding restricted vs unrestricted calculations Message-Id: <-51223-150408102343-23573-Tixf4Kam84fPqpXBXzr6kg:server.ccl.net> X-Original-From: ashika torikora Content-Type: multipart/alternative; boundary=001a1136dc9ee741f405133746a2 Date: Wed, 8 Apr 2015 16:23:37 +0200 MIME-Version: 1.0 Sent to CCL by: ashika torikora [ashika.torikora[a]gmail.com] --001a1136dc9ee741f405133746a2 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: quoted-printable Hello everyone, I am trying to understand the difference between restricted and unrestricted calculations. So far I have somewhat understood the basic difference (in restricted calculations consider the calculation is restricted to having two electrons per occupied orbital whereas for unrestricted calculations there are two complete sets of orbitals, one for the alpha electrons and one for the beta electrons). My question is more of a practical one. When should one use an unrestricted calculation? When is restricted or unrestricted used by default in gaussian(09) and when should one specify it? All answers welcome, ( =C2=B4 =E2=96=BD ` )=EF=BE=89 --001a1136dc9ee741f405133746a2 Content-Type: text/html; charset=UTF-8 Content-Transfer-Encoding: quoted-printable
Hello everyone,

I am trying to understa= nd the difference between restricted and unrestricted calculations. So far = I have somewhat understood the basic difference (in restricted calculations= consider the calculation is restricted to having two electrons per occupie= d orbital whereas for unrestricted calculations=C2=A0there are two complete= sets of orbitals, one for the alpha electrons and one for the beta electro= ns).=C2=A0
My question is more of a practical one.=C2=A0
When should one use an unrestricted calculation?
When is restri= cted or unrestricted used by default in gaussian(09) and when should one sp= ecify it?

All answers welcome,
( =C2=B4 =E2=96=BD ` )= =EF=BE=89
--001a1136dc9ee741f405133746a2-- From owner-chemistry@ccl.net Wed Apr 8 12:00:01 2015 From: "Safiya Amer amersaf85 ~~ yahoo.com" To: CCL Subject: CCL:G: =?UTF-8?Q?=D8=A8=D8=AE=D8=B5=D9=88=D8=B5:_CCL:G:_Ghost_atoms_(symbol_Bq)?= Message-Id: <-51224-150408114820-31983-M+yFSxZT+S8BcEcrsGC8IQ ~ server.ccl.net> X-Original-From: Safiya Amer Content-Type: multipart/alternative; boundary="----=_Part_2658080_1212069801.1428507928881" Date: Wed, 8 Apr 2015 15:45:28 +0000 (UTC) MIME-Version: 1.0 Sent to CCL by: Safiya Amer [amersaf85 ~~ yahoo.com] ------=_Part_2658080_1212069801.1428507928881 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: quoted-printable =C2=A0 =C2=A0 Thanks to reply=C2=A0Dr. Joshua Layfield. your Z-Matrix of H2= -Fe(OH)3 was very useful for me. I used DFT (B3LYP and B3PW91) method and s= ome basis set, also I used the same kayword that you used it in rout sectio= n "POPT(z-matrix)", but there is problem in results, they were not as expec= ted. I can not what is the reason. Can you advice me about any additional k= aywords to get better results? Thank you another=C2=A0Safiya AmerGraduate student =D9=85=D9=86: "Layfield, Joshua P. jlayfield**stthomas.edu" =D8=A5=D9=84=D9=89: "Amer, Safiya Ess " =20 =D8=AA=D8=A7=D8=B1=D9=8A=D8=AE =D8=A7=D9=84=D8=A5=D8=B1=D8=B3=D8=A7=D9=84:= =D8=A7=D9=84=D8=A3=D8=B1=D8=A8=D8=B9=D8=A7=D8=A1 25 =D9=85=D8=A7=D8=B1=D8= =B3=D8=8C 2015=E2=80=8F 12:21 =D8=B5 =D8=A7=D9=84=D9=85=D9=88=D8=B6=D9=88=D8=B9: CCL:G: Ghost atoms (symbol Bq) =20 Sent to CCL by: "Layfield, Joshua P." [jlayfield _ stthomas.edu] Safiya,=20 =C2=A0 If you want to do a partially optimized scan something like this sho= uld work.=C2=A0 (Please note that my method and geometry are not great).=C2=A0 = By defining the two hydrogen positions relative to the the dummy atom (xx) you can scan the h2 molecule as a unit.=C2=A0 Also, if you want to do a fro= zen scan you also freeze the additional degrees of freedom at a good geometry by adding the =C2=B3F=C2=B2 flag.=C2=A0 Hope this helps! #HF/6-31G=C2=A0 =C2=A0 POPT(z-matrix) Scanning the intermolecular distance between=C2=A0 Fe(OH)3 and H2 1 1 fe o=C2=A0 1 ofe2 o=C2=A0 =C2=A0 1 ofe3=C2=A0 =C2=A0 =C2=A0 =C2=A0 2 ofeo3 o=C2=A0 =C2=A0 1 ofe4=C2=A0 =C2=A0 =C2=A0 =C2=A0 2 ofeo4=C2=A0 =C2=A0 =C2= =A0 =C2=A0 3 dih4 xx=C2=A0 =C2=A0 1 xxfe5=C2=A0 =C2=A0 =C2=A0 2 xxfeo5=C2=A0 =C2=A0 =C2=A0 = =C2=A0 3 dih5 h=C2=A0 =C2=A0 2 ho6=C2=A0 =C2=A0 =C2=A0 =C2=A0 1 hofe6=C2=A0 =C2=A0 =C2= =A0 =C2=A0 3 dih6 h=C2=A0 =C2=A0 3 ho7=C2=A0 =C2=A0 =C2=A0 =C2=A0 1 hofe7=C2=A0 =C2=A0 =C2= =A0 =C2=A0 2 dih7 h=C2=A0 =C2=A0 4 ho8=C2=A0 =C2=A0 =C2=A0 =C2=A0 1 hofe8=C2=A0 =C2=A0 =C2= =A0 =C2=A0 2 dih8 h=C2=A0 =C2=A0 5 hxx9=C2=A0 =C2=A0 =C2=A0 =C2=A0 1 hxxfe9=C2=A0 =C2=A0 =C2= =A0 =C2=A0 2 dih9 h=C2=A0 =C2=A0 5 hxx10=C2=A0 =C2=A0 =C2=A0 1 hxxfe10 9 dih10 ofe2=C2=A0 =C2=A0 =C2=A0 =C2=A0 2.371600 ofe3=C2=A0 =C2=A0 =C2=A0 =C2=A0 2.371600 ofeo3=C2=A0 =C2=A0 =C2=A0 109.471 ofe4=C2=A0 =C2=A0 =C2=A0 =C2=A0 2.371600 ofeo4=C2=A0 =C2=A0 =C2=A0 109.471 dih4=C2=A0 =C2=A0 =C2=A0 =C2=A0 120.000 xxfe5=C2=A0 =C2=A0 =C2=A0 2.000000 S 19 0.05 xxfeo5=C2=A0 =C2=A0 =C2=A0 109.471 dih5=C2=A0 =C2=A0 =C2=A0 -120.000 ho6=C2=A0 =C2=A0 =C2=A0 =C2=A0 0.947000 hofe6=C2=A0 =C2=A0 =C2=A0 109.471 dih6=C2=A0 =C2=A0 =C2=A0 =C2=A0 180.000 ho7=C2=A0 =C2=A0 =C2=A0 =C2=A0 0.947000 hofe7=C2=A0 =C2=A0 =C2=A0 109.471 dih7=C2=A0 =C2=A0 =C2=A0 =C2=A0 =C2=A0 0.000 ho8=C2=A0 =C2=A0 =C2=A0 =C2=A0 0.947000 hofe8=C2=A0 =C2=A0 =C2=A0 109.471 dih8=C2=A0 =C2=A0 =C2=A0 -180.000 hxx9=C2=A0 =C2=A0 =C2=A0 =C2=A0 0.370000 f hxxfe9=C2=A0 =C2=A0 =C2=A0 90.000=C2=A0 f dih9=C2=A0 =C2=A0 =C2=A0 =C2=A0 180.000=C2=A0 f hxx10=C2=A0 =C2=A0 =C2=A0 0.370000 f hxxfe10=C2=A0 =C2=A0 =C2=A0 90.000=C2=A0 f dih10 180.000=C2=A0 f Dr. Joshua Layfield Assistant Professor, Department of Chemistry University of St. Thomas Maill # OSS 402 2115 Summit Ave.=20 St. Paul, MN 55105-1079 (651) 962-5577 On 3/24/15, 12:00 PM, "Safiya Ess Amer amersaf85]~[yahoo.com" wrote: > >Sent to CCL by: "Safiya Ess Amer" [amersaf85||yahoo.com] >Hello. >Please, how can I use ghost atom with Cartesian coordinates? >I have system of H2-Fe(OH)3 and use G03W for getting energy as function >of=C2=A0=20 >more distances (Z) from center of H2 to Fe atom. I am calculating now >each=20 >value of energy at some distance manually. I need to put ghost atom at >center=20 >of H2, how can I do that to get PES. > >Can anyone help me in input file? >I have geometry of the system. > >Thanks in advance=20 > >Safiya Amer >amersaf85]^[yahoo.com> > -=3D This is automatically added to each message by the mailing script =3D-=C2=A0 =C2=A0 =C2=A0=C2=A0 =C2=A0 =C2=A0Subscribe/Unsubscribe:=20 =C2=A0 =C2=A0 =C2=A0Job: http://www.ccl.net/jobs=20=C2=A0 =C2=A0 =C2=A0------=_Part_2658080_1212069801.1428507928881 Content-Type: text/html; charset=UTF-8 Content-Transfer-Encoding: quoted-printable
    Thanks to reply Dr. Joshua Layfield. your Z-Matrix of H2-Fe(OH= )3 was very useful for me. I used DFT (B3LYP and B3PW91) method and some ba= sis set, also I used the same kayword that you used it in rout section "POPT(z-matrix)"= , but there is problem in results, they were not as expected. I can not wha= t is the reason. Can you advice me about any additional kaywords to get bet= ter results?

Thank you anothe= r
 =
Safiya Amer
Graduate student



=D9=85=D9=86: "Layfield, Joshua P= . jlayfield**stthomas.edu" <owner-chemistry]![ccl.net>
=D8=A5=D9=84=D9=89: "Amer, Safiya Ess = " <amersaf85]![yahoo.com>
=D8=AA=D8=A7=D8=B1=D9=8A=D8=AE =D8=A7=D9=84=D8=A5=D8=B1=D8=B3=D8= =A7=D9=84: =D8=A7=D9=84=D8=A3=D8=B1=D8=A8=D8=B9=D8=A7=D8=A1 25 = =D9=85=D8=A7=D8=B1=D8=B3=D8=8C 2015=E2=80=8F 12:21 =D8=B5
=D8=A7=D9=84=D9=85=D9=88=D8=B6=D9=88=D8=B9: CCL:G: Ghost atoms (symbol Bq)


Sent to CCL by: "Layfield, Joshua P." [jlayfie= ld _ stthomas.edu]
Safiya,

&= nbsp; If you want to do a partially optimized scan something like this shou= ld
work.&n= bsp; (Please note that my method and geometry are not great).  By
<= /div>
defining the t= wo hydrogen positions relative to the the dummy atom (xx)
you can scan the h2 molecul= e as a unit.  Also, if you want to do a frozen
scan you also freeze the addition= al degrees of freedom at a good geometry
by adding the =C2=B3F=C2=B2 flag.  Hope= this helps!


#HF/6-31G =   POPT(z-matrix)


Scanning the intermolecular distance between=   Fe(OH)3 and H2


1 1
fe
=
o  1 ofe2
o  &nb= sp; 1 ofe3        2 ofeo3
o    1 ofe4    &n= bsp;   2 ofeo4        3 dih4
xx    1 xxfe5  =     2 xxfeo5        3 dih5
h    2 ho6 =       1 hofe6        3 dih6
=
h    3 h= o7        1 hofe7        2 dih7
h  &n= bsp; 4 ho8        1 hofe8        = 2 dih8
h&= nbsp;   5 hxx9        1 hxxfe9     =   2 dih9
h    5 hxx10      1 hxxfe10 9 dih10


ofe2        2.371600
ofe3        2.371600
ofeo3  =     109.471
ofe4        2.371600
ofeo4      109.471
dih4        120.000
xxfe5  &nb= sp;   2.000000 S 19 0.05
xxfeo5      109.471
dih5      -= 120.000
ho= 6        0.947000
hofe6      109.471
dih6        180.000
ho7        0.947000
ho= fe7      109.471
dih7          0.000
ho8    =     0.947000
hofe8     = 109.471
dih8      -180.000
<= /div>
hxx9  &nb= sp;     0.370000 f
hxxfe9      90.000  f
dih9     = ;   180.000  f
hxx10      0.370000 f
hxxfe10      90.0= 00  f
dih10 180.000  f



<= /div>
Dr. Joshua Lay= field
Assi= stant Professor, Department of Chemistry
University of St. Thomas
Maill # OSS 402
2115 Summit Ave.
=
St. Paul, MN = 55105-1079
(651) 962-5577




On 3/24/15, 12:00 PM, "Safiya Ess Amer amersaf85]~[= yahoo.com"
<owner-chemistry]*[ccl.net> wrote:

>
>Sent to CCL by: "Safiya Ess Amer" [amersaf85||yahoo.c= om]
>Hello.
>Plea= se, how can I use ghost atom with Cartesian coordinates?
>I have system of H2-Fe(OH)3 and use G03W for getting energy as= function
= >of 
>more distances (Z) from center = of H2 to Fe atom. I am calculating now
>each
>value = of energy at some distance manually. I need to put ghost atom at
<= div dir=3D"ltr" id=3D"yui_3_16_0_1_1428501633350_5667">>center
>of H2, how can= I do that to get PES.
>
>Can anyone help me in input file?
>I have geometry of the system.
=
>
>Thanks in adva= nce
><= br>
>Safiya Amer
>ame= rsaf85]^[yahoo.com>
>


=

-=3D This is automatically added to each message by the maili= ng script =3D-
To recover the email address of th= e author of the message, please change
the strang= e characters on the top line to the ]![ sign. You can also
look up the X-Original-From= : line in the mail header.

E-mail to subscribers: CHEMIS= TRY]![ccl.net or use:

E-mail to administrators: CH= EMISTRY-REQUEST]![ccl.net or use


Before = posting, check wait time at: http://www.ccl.net


If your mai= l bounces from CCL with 5.7.1 error, check:





------=_Part_2658080_1212069801.1428507928881-- From owner-chemistry@ccl.net Wed Apr 8 12:36:01 2015 From: "=?iso-8859-1?Q?V=EDctor_Lua=F1a?= Cabal victor_+_fluor.quimica.uniovi.es" To: CCL Subject: CCL:G: Understanding restricted vs unrestricted calculations Message-Id: <-51225-150408121644-11129-aCQCErtSYsEkiztLycb2MA~~server.ccl.net> X-Original-From: =?iso-8859-1?Q?V=EDctor_Lua=F1a?= Cabal Content-disposition: inline Content-transfer-encoding: 8BIT Content-type: text/plain; charset=iso-8859-1 Date: Wed, 08 Apr 2015 18:10:22 +0200 MIME-version: 1.0 Sent to CCL by: =?iso-8859-1?Q?V=EDctor_Lua=F1a?= Cabal [victor~~fluor.quimica.uniovi.es] On Wed, Apr 08, 2015 at 04:23:37PM +0200, ashika torikora ashika.torikora(_)gmail.com wrote: > Hello everyone, > > I am trying to understand the difference between restricted and > unrestricted calculations. So far I have somewhat understood the basic > difference (in restricted calculations consider the calculation is > restricted to having two electrons per occupied orbital whereas for > unrestricted calculations there are two complete sets of orbitals, one for > the alpha electrons and one for the beta electrons). > My question is more of a practical one. > When should one use an unrestricted calculation? > When is restricted or unrestricted used by default in gaussian(09) and when > should one specify it? There are many answers. The simplest is: in a restricted calculation the orbital description of alpha and beta spin electrons are forced to be equivalent. in an unrestricted calculation that equivalence is not enforced The difference between electron density of alpha and beta electrons produces information on the magnetism of the system, mainly but not only. There are other workers in this list that can provide a more complex and detailed answer. Best regards, Dr. Víctor Luaña -- . . DEEP THOUGHT in D. Adams; Hitchhikers Guide to the Galaxy: / `' \ "I think the problem, to be quite honest with you, /(o)(o)\ is that you have never actually known what the question is." /`. \/ .'\ / '`'` \ "Lo mediocre es peor que lo bueno, pero también es peor | \'`'`/ | que lo malo, porque la mediocridad no es un grado, es una | |'`'`| | actitud" \/`'`'`'\/ -- Jorge Wasenberg, 2015 ===(((==)))==================================+========================= ! Dr.Víctor Luaña ! Mediocre is worse than ! Departamento de Química Física y Analítica ! good, but it is also ! Universidad de Oviedo, 33006-Oviedo, Spain ! worse than bad, because ! e-mail: victor~~fluor.quimica.uniovi.es ! mediocrity is not a grade, ! phone: +34-985-103491 fax: +34-985-103125 ! it is an attitude +--------------------------------------------+ GroupPage : http://azufre.quimica.uniovi.es/ (being reworked) From owner-chemistry@ccl.net Wed Apr 8 13:11:00 2015 From: "Yingbin Ge yingbin.ge|-|gmail.com" To: CCL Subject: CCL:G: Understanding restricted vs unrestricted calculations Message-Id: <-51226-150408120627-7488-WH7Wy0qVOtcaqKHrypIjew~!~server.ccl.net> X-Original-From: Yingbin Ge Content-Type: multipart/alternative; boundary=001a113560183193c10513389993 Date: Wed, 8 Apr 2015 08:58:12 -0700 MIME-Version: 1.0 Sent to CCL by: Yingbin Ge [yingbin.ge]^[gmail.com] --001a113560183193c10513389993 Content-Type: text/plain; charset=UTF-8 Dear Ashika, When should one use an unrestricted calculation? A: when you suspect there is at least one spatial orbital that is occupied by 1 electron and you do not wish to do a restricted open-shell (RO) calculation. For example, Na, Mg+, the ground electronic state of Sc, Ti, V, Cr, Mn and most other transition metal atoms, the ground electronic state of O2, a molecule with a severely stretched bond, etc. When is restricted or unrestricted used by default in gaussian(09) and when should one specify it? I think the default is restricted whenever the system has an even number of electrons. But I always examine and change it if necessary. Sincerely, Yingbin -- Yingbin Ge, Associate Professor Science Building 207A Department of Chemistry Central Washington University 400 E University Way Ellensburg, WA 98926 Office Phone: 509-963-2817 Email: yingbin . cwu.edu --001a113560183193c10513389993 Content-Type: text/html; charset=UTF-8 Content-Transfer-Encoding: quoted-printable

Dear Ashika,


When should one use an unrestricted calculation?


A:= when you suspect there is at least one spatial orbital that is occupied by= 1 electron and you do not wish to do a restricted open-shell (RO) calculat= ion. For example,
Na,
Mg+,
the ground electronic stat= e of Sc, Ti, V, Cr, Mn and most other transition metal atoms,
the groun= d electronic state of O2,
a molecule with a severely stretched bond, etc.


When is restricted or unrestricted = used by default in gaussian(09) and when should one specify it?
I think the default is restricted whenever the system has an even number= of electrons. But I always examine and change it if necessary.
Sincerely,
Yingbin

--
Yingbin Ge, A= ssociate Professor
Science Building 207A
Department of Chemistry
Central Washington University
400 E University Way
Ellensburg, WA 98926
Office Phone: 509-963-2817
--001a113560183193c10513389993-- From owner-chemistry@ccl.net Wed Apr 8 13:45:01 2015 From: "Igors Mihailovs igors.mihailovs0!^!gmail.com" To: CCL Subject: CCL:G: Understanding restricted vs unrestricted calculations Message-Id: <-51227-150408130922-7867-bCIx+G3ltLy1bhp6NBoEIA*o*server.ccl.net> X-Original-From: Igors Mihailovs Content-Transfer-Encoding: 8bit Content-Type: text/plain; charset=UTF-8 Date: Wed, 8 Apr 2015 20:09:15 +0300 MIME-Version: 1.0 Sent to CCL by: Igors Mihailovs [igors.mihailovs0/a\gmail.com] Hello Ashika, UNrestricted calculations are used for systems with odd number of electrons (free radicals, in particular radical cations and anions that occur upon ionization of a molecule / electron capture by it) and also for systems that have even number of electrons but unpaired: these are biradicals, e. g., oxygen molecule, or, most commonly, these are electronically excited species - singlet and triplet states. All this correspond to spin multiplicity of specie beig higher than 1. By default, Gaussian 09 sets calculation type to be unrestricted only if spin multiplicity is higher than one. However, the initial guess still has alpha and beta states coinciding in energy, so the optimization might not break the spin symmetry by its own, and the resulting wavefuction will be something like a "saddle point" between two unrestricted functions. Spin symmetry means that there is no biradical character of the full wavefunction of Your system, e.g., that alpha and beta electrons are distributed equally – in fact, sharing spatial parts of their wavefunctions, as in restricted calculation. To check if Your unrestricted wavefunction is really unrestricted, You ought to run the same calculation with "Stable=Opt" keyword. This requires a bit more resources than plain single point, as it have to diagonalize configuration interaction (CI) matrices. Personally I appeared at questioning about this when I noticed that values for closed-shell molecules in my unrestricted calculations (not only Kohn–Sham, but even Hartree–Fock) were surprisingly equal to 0.000, with no spin contamination. The last one is "the beast" of unrestricted calculations: those wavefunctions that we obtain by solving Schroedinger equation are not neccessarily eigenfunctions of spin-squared operator, S**2, but in reality they should be; so, in fact unrestricted wavefunction contain some spurious contribution from energetically higher-laying states with greater spin than we have set up in the calculation parameters (electronically "more excited" states). This means that we have somewhat incorrect wavefunction and, as a concequence, somewhat incorrect energy. Spin contamination is usually relatively high for Hartree–Fock and correlated methods (MPn, etc.) based upon it, but particularily less for unrestricted Kohn–Sham DFT calculations. There is one more alternative: restricted open-shell calculations (RO). Here, all spatial shells that in the reality contain two electrons (usually inner shells) are forced to stay together, as in restricted calculation, whereas those containing only one electron are computed as they are. This method should give more reasonable results, but it requires more computational resources, because we now have not only one Slater determinant as in unrestricted calculation, double that of restricted one, but several (multiple) determinants, a bit like in CI. Hope this will be useful, Igors Mihailovs (engineer) Institute of Solid State Physics University of Latvia 2015-04-08 17:23 GMT+03:00, ashika torikora ashika.torikora(_)gmail.com : > Hello everyone, > > I am trying to understand the difference between restricted and > unrestricted calculations. So far I have somewhat understood the basic > difference (in restricted calculations consider the calculation is > restricted to having two electrons per occupied orbital whereas for > unrestricted calculations there are two complete sets of orbitals, one for > the alpha electrons and one for the beta electrons). > My question is more of a practical one. > When should one use an unrestricted calculation? > When is restricted or unrestricted used by default in gaussian(09) and when > should one specify it? > > All answers welcome, > ( ´ ▽ ` )ノ >