From owner-chemistry@ccl.net Sun Jul 10 00:02:00 2022 From: "Sachin Ramesh sachinadityaramesh() gmail.com" To: CCL Subject: CCL: [CCL] CCL: Negative frequencies with C1 symmetry (Orca) Message-Id: <-54751-220710000019-32717-6ox8xG5l2oCIGlZBth2CVg*server.ccl.net> X-Original-From: Sachin Ramesh Content-Type: multipart/alternative; boundary="000000000000f29cb005e36b78e1" Date: Sun, 10 Jul 2022 09:30:02 +0530 MIME-Version: 1.0 Sent to CCL by: Sachin Ramesh [sachinadityaramesh**gmail.com] --000000000000f29cb005e36b78e1 Content-Type: text/plain; charset="UTF-8" Hi, Imaginary modes under '-10 cm-1' if not many can be safely ignored. You could try to get rid of the imaginary mode by distorting the structure along the bond, angle or dihedral which is causing the imaginary mode. I should add that imaginary modes are tricky to get rid of when the solvent correction is used. The optimization could be done using solvent correction and frequency can be computed in gas phase. 'TightSCF TightOpt Grid7 Gridx9' seems to work for all of our systems upto 200 atoms, producing accurate results in good agreement with experimental observations. Hope this helps with best - Sachin On Sat, Jul 9, 2022 at 7:32 PM Grigoriy Zhurko reg_zhurko.:. chemcraftprog.com wrote: > > Sent to CCL by: "Grigoriy Zhurko" [reg_zhurko()chemcraftprog.com] > Hello, > I compute some molecules with Orca 5.0.3, and the computation sometimes > produces small negative frequencies, despite the symmetry of the molecules > is > C1. If I repeat the computation with another starting point, with some > probability all frequencies are positive. > I found that this problem arises when two additions to the model are > added: > the solvent model (!CPCM(Water)) and additions of some explicit water > molecules to the whole model. I understand that these water molecules > produce > very small frequencies along the h-bonds, and these frequencies can become > negative because of some problems with numerical integration. I tried the > combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still > sometimes the negative frequencies are produced. Maybe I need to further > increase the computational accuracy with options like "!VeryTightOpt", > "!DefGrid9", UltraTightSCF? I suppose you understand what I mean; > currently > I didn't find the information in the manual, how to further decrease the > optimization convergence threshold or increase the accuracy of DFT grid. > Please suggest how to do that. > In my work I can avoid using the frequencies since I need mainly the > energies; however I need to explain this somehow in the paper. I suppose, > it > is not good to compute the entropy of molecules with my keywords, because > small frequencies produce big errors with vibrational entropy. So, please > suggest me, what should I write in my papers, to explain that it is not > good > to compute the Gibbs energy of my molecules, but it is correct to compute > and > use the common energy. > > Grigoriy Zhurko > https://chemcraftprog.com> > > --000000000000f29cb005e36b78e1 Content-Type: text/html; charset="UTF-8" Content-Transfer-Encoding: quoted-printable
Hi,

=C2=A0 =C2=A0Imagi= nary modes under '-10 cm-1' if not many can be safely ignored. You = could try to get rid=C2=A0
of the imaginary mode by distorting th= e structure along the bond, angle or dihedral which is=C2=A0
caus= ing the imaginary mode.=C2=A0

=C2=A0 =C2=A0I shoul= d add that imaginary modes are tricky to get rid of when the solvent correc= tion is used.=C2=A0
The optimization could be done using solvent = correction and frequency can be computed in gas phase.=C2=A0

=
=C2=A0 'TightSCF TightOpt Grid7 Gridx9' seems to work fo= r all of our systems upto 200 atoms, producing=C2=A0
accurate res= ults in good agreement with experimental observations. =C2=A0
Hope this helps=C2=A0

with best=C2= =A0
- Sachin=C2=A0

=
On Sat, Ju= l 9, 2022 at 7:32 PM Grigoriy Zhurko reg_zhurko.:.chemcraftprog.com <owner-chemistry^_^ccl.net> wrote:

Sent to CCL by: "Grigoriy=C2=A0 Zhurko" [reg_zhurko()chemcraftprog= .com]
Hello,
I compute some molecules with Orca 5.0.3, and the computation sometimes produces small negative frequencies, despite the symmetry of the molecules = is
C1. If I repeat the computation with another starting point, with some
probability all frequencies are positive.
I found that this problem arises when two additions to the model are added:=
the solvent model (!CPCM(Water)) and additions of some explicit water
molecules to the whole model. I understand that these water molecules produ= ce
very small frequencies along the h-bonds, and these frequencies can become =
negative because of some problems with numerical integration. I tried the <= br> combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still
sometimes the negative frequencies are produced. Maybe I need to further increase the computational accuracy with options like "!VeryTightOpt&q= uot;,
"!DefGrid9", UltraTightSCF? I suppose you understand what I mean;= currently
I didn't find the information in the manual, how to further decrease th= e
optimization convergence threshold or increase the accuracy of DFT grid. Please suggest how to do that.
In my work I can avoid using the frequencies since I need mainly the
energies; however I need to explain this somehow in the paper. I suppose, i= t
is not good to compute the entropy of molecules with my keywords, because <= br> small frequencies produce big errors with vibrational entropy. So, please <= br> suggest me, what should I write in my papers, to explain that it is not goo= d
to compute the Gibbs energy of my molecules, but it is correct to compute a= nd
use the common energy.

Grigoriy Zhurko
= https://chemcraftprog.com



-=3D This is automatically added to each message by the mailing script =3D-=
E-mail to subscribers: CHEMISTRY^_^ccl.net or use:
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/cgi-bin/ccl/s= end_ccl_message

E-mail to administrators: CHEMISTRY-REQUEST^_^ccl.net or use
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/cgi-bin/ccl/s= end_ccl_message
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/chemistry/sub_un= sub.shtml

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

Job: http://www.ccl.net/jobs
Conferences: http://server.ccl.net/chemist= ry/announcements/conferences/

Search Messages: http://www.ccl.net/chemistry/sear= chccl/index.shtml
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/spammers.txt

RTFI: http://www.ccl.net/chemistry/aboutccl/ins= tructions/


--000000000000f29cb005e36b78e1-- From owner-chemistry@ccl.net Sun Jul 10 02:38:01 2022 From: "Alejandro Pisanty apisanty]|[gmail.com" To: CCL Subject: CCL: [External] CCL: Negative frequencies with C1 symmetry (Orca) Message-Id: <-54752-220710022452-26239-3e7b5ZZ+GUO2rkFqeRYjGA[*]server.ccl.net> X-Original-From: Alejandro Pisanty Content-Type: multipart/alternative; boundary="000000000000d9456605e36d7d5a" Date: Sun, 10 Jul 2022 01:24:18 -0500 MIME-Version: 1.0 Sent to CCL by: Alejandro Pisanty [apisanty!^!gmail.com] --000000000000d9456605e36d7d5a Content-Type: text/plain; charset="UTF-8" Content-Transfer-Encoding: quoted-printable Hi, indeed - the mix of expert and novice, and of disciplines and approaches, was unique for this list since its start in 1991 with 100 members and the initiative and smarts of Jan Labanowski. Our community has been exemplary in its self-governance, pioneering in issues like handling commercial announcements, the tone of interaction, handling controversies, staying secure, waves of technology change from a closed, ASCII-based mailing list many of us read and wrote on with Pine, to the Web and social media.. See Hocquet, Weber, and Pisanty, https://jcheminf.biomedcentral.com/articles/10.1186/s13321-018-0322-7 Not even the person who combines the most breadth and depth will be the ultimate expert in everything, and people may choose wisely to ask before delving deep into literature and manuals. The mix of theory and practice is also distinctive of the CCL like few other virtual communities - and very few are as mature as this one in which, as described by other members, utter novices became authoritative experts over time and never stopped the flow of good advice. Cheers, Alejandro Pisanty On Sat, Jul 9, 2022 at 8:48 PM Steve Williams willsd*appstate.edu < owner-chemistry]=[ccl.net> wrote: > Thank you Soren, for reminding me why Gregoriy has a familiar name .... I > have been retired for a few years and no longer do computational chemistr= y > anymore. But I used chemcraft for many years and convinced collaborators > who were not computational chemists to buy copies also, so we could > communicate well. So, yes, it is never wrong to be polite and helpful, a= nd > it is never wrong to NOT respond if polite and helpful is not your thing = at > the moment. > Steve Williams > > On Sat, Jul 9, 2022, 6:49 PM Soren Eustis soreneustis|-|gmail.com ccl.net> wrote: > >> Hey, be respectful and open to questions from newcomers or established >> scientists. I understood exactly what Grigoriy was talking about. In th= is >> case Grigoriy, happens to have made massive contributions to our communi= ty- >> including coding ChemCraft. >> >> If I were to try to discuss the complexities of the field in any other >> language than my native tongue, I=E2=80=99d be at a loss. >> >> Primarily, let=E2=80=99s be better to people here. In this case, Grigori= y is a >> world class scientist who deserves respect. Most importantly, even the >> brightest minds need to start somewhere. I spent a lot of time trying to >> have questions answered here as a new scientist and some people were pre= tty >> harsh. Some weren=E2=80=99t. Now I have published many papers and traine= d many >> scientists in the field. Be kind. >> >> Soren >> On Jul 9, 2022, 15:01 -0400, Anatoli Korkin korkin_-_nanoandgiga.com > ccl.net>, wrote: >> >> >> Sent to CCL by: Anatoli Korkin [korkin##nanoandgiga.com] >> You should not write a scientific paper without basic understanding of >> what you are doing! >> >> Sent from my iPhone >> >> On Jul 9, 2022, at 6:52 AM, Grigoriy Zhurko reg_zhurko.:. >> chemcraftprog.com wrote: >> >> =EF=BB=BF >> Sent to CCL by: "Grigoriy Zhurko" [reg_zhurko()chemcraftprog.com] >> Hello, >> I compute some molecules with Orca 5.0.3, and the computation sometimes >> produces small negative frequencies, despite the symmetry of the >> molecules is >> C1. If I repeat the computation with another starting point, with some >> probability all frequencies are positive. >> I found that this problem arises when two additions to the model are >> added: >> the solvent model (!CPCM(Water)) and additions of some explicit water >> molecules to the whole model. I understand that these water molecules >> produce >> very small frequencies along the h-bonds, and these frequencies can beco= me >> negative because of some problems with numerical integration. I tried th= e >> combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still >> sometimes the negative frequencies are produced. Maybe I need to further >> increase the computational accuracy with options like "!VeryTightOpt", >> "!DefGrid9", UltraTightSCF? I suppose you understand what I mean; >> currently >> I didn't find the information in the manual, how to further decrease the >> optimization convergence threshold or increase the accuracy of DFT grid. >> Please suggest how to do that. >> In my work I can avoid using the frequencies since I need mainly the >> energies; however I need to explain this somehow in the paper. I suppose= , >> it >> is not good to compute the entropy of molecules with my keywords, becaus= e >> small frequencies produce big errors with vibrational entropy. So, pleas= e >> suggest me, what should I write in my papers, to explain that it is not >> good >> to compute the Gibbs energy of my molecules, but it is correct to comput= e >> and >> use the common energy. >> >> Grigoriy Zhurko >> https://chemcraftprog.com> >> >> >> >> >> -=3D This is automatically added to each message by the mailing script = =3D- >> E-mail to subscribers: CHEMISTRY() ccl.net or use:>> >> E-mail to administrators: CHEMISTRY-REQUEST() ccl.net or use>> >> >> --=20 - - - - - - - - - - - - - - - - - - - - - - - - - - - Dr. Alejandro Pisanty Facultad de Qu=C3=ADmica UNAM Av. Universidad 3000, 04510 Mexico DF Mexico +525541444475 Blog: http://pisanty.blogspot.com LinkedIn: http://www.linkedin.com/in/pisanty Unete al grupo UNAM en LinkedIn, http://www.linkedin.com/e/gis/22285/4A106C0C8614 Twitter: http://twitter.com/apisanty ---->> Unete a ISOC Mexico, http://www.isoc.org . . . . . . . . . . . . . . . . --000000000000d9456605e36d7d5a Content-Type: text/html; charset="UTF-8" Content-Transfer-Encoding: quoted-printable
Hi,

indeed - the mix of expert and novi= ce, and of disciplines and approaches, was unique for this list since its s= tart in 1991 with 100 members and the initiative and smarts of Jan Labanows= ki.=C2=A0

Our community has been exemplary in its = self-governance, pioneering in issues like handling commercial announcement= s, the tone of interaction, handling controversies, staying secure, waves o= f technology change from a closed, ASCII-based mailing list many of us read= and wrote on with Pine, to the Web and social media.. See Hocquet, Weber, = and Pisanty,=C2=A0https://jcheminf.biomedcentral.com/articles/10.118= 6/s13321-018-0322-7=C2=A0

Not even the person = who combines the most breadth and depth will be the ultimate expert in ever= ything, and people may choose wisely to ask before delving deep into litera= ture and manuals. The mix of theory and practice is also distinctive of the= CCL like few other virtual communities - and very few are as mature=C2=A0a= s this one in which, as described by other members, utter novices became au= thoritative experts over time and never stopped the flow of good advice.

Cheers,

Alejandro Pisanty

On Sat, Jul 9, 2022 at 8:48 PM Steve Williams willsd*appstate.edu <owner-chemistry]=[ccl.net> wrote:
Thank you Soren, for reminding = me why Gregoriy has a familiar name .... I have been retired for a few year= s and no longer do computational chemistry anymore. But I used chemcraft fo= r many years and convinced collaborators who were not computational chemist= s to buy copies also, so we could communicate well.=C2=A0 So, yes, it is ne= ver wrong to be polite and helpful, and it is never wrong to NOT respond if= polite and helpful is not your thing at the moment.
Steve= Williams

On Sat, Jul 9, 2022, 6:49 PM Soren Eustis soreneustis|-|gmail.com <owner-chemistry() ccl.net= > wrote:
Hey, be respectful and open to questions from newcomers o= r established scientists.=C2=A0=C2=A0I understood exactly what Grigoriy was= talking about. In this case Grigoriy, happens to have made massive contrib= utions to our community- including coding ChemCraft.=C2=A0=C2=A0

If I were to try to discuss the complexities of the field in any other lang= uage than my native tongue, I=E2=80=99d be at a loss.

Primarily, let=E2=80=99s be better to people here. In this case, Grigoriy i= s a world class scientist who deserves respect. Most importantly, even the = brightest minds need to start somewhere. I spent a lot of time trying to ha= ve questions answered here as a new scientist and some people were pretty h= arsh. Some weren=E2=80=99t. Now I have published many papers and trained ma= ny scientists in the field. Be kind.

Soren=C2=A0
On Jul 9, 2022, 15:01 -0400, Anatoli Kork= in korkin_-_nanoandgiga.com <owner-chemistry() ccl.net<= /a>>, wrote:

Sent to CCL by: Anatoli Korkin [korkin##
nanoandgiga.com]
You should not write a scientific paper without basic understanding of what= you are doing!

Sent from my iPhone

On Jul 9, 2022, at 6:52 AM, Grigoriy Zhurko reg_z= hurko.:.chemcraftprog.com <owner-chemistry*_*ccl.net> wrote:

=EF=BB=BF
Sent to CCL by: "Grigoriy Zhurko" [reg_zhurko()chemcraftprog.com]
Hello,
I compute some molecules with Orca 5.0.3, and the computation sometimes
produces small negative frequencies, despite the symmetry of the molecules = is
C1. If I repeat the computation with another starting point, with some
probability all frequencies are positive.
I found that this problem arises when two additions to the model are added:=
the solvent model (!CPCM(Water)) and additions of some explicit water
molecules to the whole model. I understand that these water molecules produ= ce
very small frequencies along the h-bonds, and these frequencies can become<= br> negative because of some problems with numerical integration. I tried the combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still
sometimes the negative frequencies are produced. Maybe I need to further increase the computational accuracy with options like "!VeryTightOpt&q= uot;,
"!DefGrid9", UltraTightSCF? I suppose you understand what I mean;= currently
I didn't find the information in the manual, how to further decrease th= e
optimization convergence threshold or increase the accuracy of DFT grid. Please suggest how to do that.
In my work I can avoid using the frequencies since I need mainly the
energies; however I need to explain this somehow in the paper. I suppose, i= t
is not good to compute the entropy of molecules with my keywords, because small frequencies produce big errors with vibrational entropy. So, please suggest me, what should I write in my papers, to explain that it is not goo= d
to compute the Gibbs energy of my molecules, but it is correct to compute a= nd
use the common energy.

Grigoriy Zhurko
= https://chemcraftprog.com>




-=3D This is automatically added to each message by the mailing script =3D-=
E-mail to subscribers: CHEMISTRY() ccl.net or use:
http://www.ccl.net/cgi-bin/ccl/send_ccl_message
E-mail to administrators: CHEMISTRY-REQUEST() ccl.net or use http://www.ccl.net/cgi-bin/ccl/send_ccl_message
Subscribe/Unsubscribe:
http://www.ccl.net/chemistry/sub_unsub.shtml


Job: http://www.ccl.net/jobs



RTFI: http://www.ccl.net/chemistry/aboutccl/ins= tructions/




--
- - - - - - - - - - - - - = - - - - - - - - - - - - - -
=C2=A0 =C2=A0 =C2=A0Dr. Alejandro PisantyFacultad de Qu=C3=ADmica UNAM
Av. Universidad 3000, 04510 Mexico DF Mex= ico
+525541444475
Blog: http://pisanty.blogspot.com
LinkedIn: http://www.linkedin.com/in/= pisanty
Unete al grupo UNAM en LinkedIn, http://www.linkedin.com= /e/gis/22285/4A106C0C8614
Twitter: http://twitter.com/apisanty
---->> Un= ete a ISOC Mexico, http:/= /www.isoc.org
. =C2=A0. =C2=A0. =C2=A0. =C2=A0. =C2=A0. =C2=A0. =C2= =A0. =C2=A0. =C2=A0. =C2=A0. =C2=A0. =C2=A0. =C2=A0. =C2=A0. =C2=A0.
<= /div>
--000000000000d9456605e36d7d5a-- From owner-chemistry@ccl.net Sun Jul 10 03:39:00 2022 From: "Neese, Frank neese]![kofo.mpg.de" To: CCL Subject: CCL: [CCL] CCL: Negative frequencies with C1 symmetry (Orca) Message-Id: <-54753-220710033645-22141-0N+2u+buI21hjmn5Exh+nA- -server.ccl.net> X-Original-From: "Neese, Frank" Content-Language: de-DE Content-Type: multipart/alternative; boundary="_000_65519CE448FC44939D162FD3717B9ADFkofompgde_" Date: Sun, 10 Jul 2022 07:36:32 +0000 MIME-Version: 1.0 Sent to CCL by: "Neese, Frank" [neese|a|kofo.mpg.de] --_000_65519CE448FC44939D162FD3717B9ADFkofompgde_ Content-Type: text/plain; charset="utf-8" Content-Transfer-Encoding: base64 SnVzdCB0byBicmllZmx5IGNsYXJpZnkNCg0KVGlnaHRTQ0YgVGlnaHRPcHQgR3JpZDcgR3JpZHg5 Jw0KDQpJcyBPUkNBIHByZSA1LjAuIHdpdGggNS4wIHRoZXNlIG9sZCBncmlkcyBhcmUgZ29uZSBh bmQgdGhlIG5ldyBncmlkcyBhcmUgbXVjaCBtb3JlIGFjY3VyYXRlIGFuZCBkb27igJh0IG5lZWQg YnVtcGluZyB1cC4NCg0KVGhlIE9QIGhhcyB0cmllZCB0aGVzZSB0aGluZ3MgYW5kIHRoZSBuZWdh dGl2ZSBmcmVxdWVuY2llcyByZW1haW5lZCwgbWVhbmluZyB0aGF0IHRoZXkgYXJlIG5vdCBudW1l cmljYWwgbm9pc2UuIFRoZSBPUCB3YXMgYWR2aXNlZCB0byBkaXNwbGFjZSB0aGUgbW9sZWN1bGUg YWxvbmcgdGhlIHJlc3BlY3RpdmUgcmVhbCBtb2Rlcy4gSXQgd2FzIGFsc28gcG9pbnRlZCBvdXQg dG8gaGltIHRoYXQgdGhlcmUgaXMgYSBjb21wb3VuZCBzY3JpcHQgdGhhdCBjb21lcyB3aXRoIE9S Q0EgNS4wIGFuZCBsYXRlciB0aGF0IGF1dG9tYXRpY2FsbHkgZGlzcGxhY2VzIHRoZSBtb2xlY3Vs ZSBhbG9uZyBhbnkgbmVnYXRpdmUgZnJlcXVlbmN5IG1vZGUgdW50aWwgYWxsIG5lZ2F0aXZlIGZy ZXF1ZW5jaWVzIGFyZSBnb25lLg0KDQpUaGF0IGlzIHRoZSBiZXN0IGFkdmlzZSBJIGFtIGFibGUg dG8gZ2l2ZS4NCg0KU2VudCBmcm9tIG15IGlQYWQNCg0KT24gMTAuIEp1bCAyMDIyLCBhdCAwNzo1 NiwgU2FjaGluIFJhbWVzaCBzYWNoaW5hZGl0eWFyYW1lc2goKSBnbWFpbC5jb20gPG93bmVyLWNo ZW1pc3RyeUBjY2wubmV0PiB3cm90ZToNCg0K77u/DQpIaSwNCg0KICAgSW1hZ2luYXJ5IG1vZGVz IHVuZGVyICctMTAgY20tMScgaWYgbm90IG1hbnkgY2FuIGJlIHNhZmVseSBpZ25vcmVkLiBZb3Ug Y291bGQgdHJ5IHRvIGdldCByaWQNCm9mIHRoZSBpbWFnaW5hcnkgbW9kZSBieSBkaXN0b3J0aW5n IHRoZSBzdHJ1Y3R1cmUgYWxvbmcgdGhlIGJvbmQsIGFuZ2xlIG9yIGRpaGVkcmFsIHdoaWNoIGlz DQpjYXVzaW5nIHRoZSBpbWFnaW5hcnkgbW9kZS4NCg0KICAgSSBzaG91bGQgYWRkIHRoYXQgaW1h Z2luYXJ5IG1vZGVzIGFyZSB0cmlja3kgdG8gZ2V0IHJpZCBvZiB3aGVuIHRoZSBzb2x2ZW50IGNv cnJlY3Rpb24gaXMgdXNlZC4NClRoZSBvcHRpbWl6YXRpb24gY291bGQgYmUgZG9uZSB1c2luZyBz b2x2ZW50IGNvcnJlY3Rpb24gYW5kIGZyZXF1ZW5jeSBjYW4gYmUgY29tcHV0ZWQgaW4gZ2FzIHBo YXNlLg0KDQogICdUaWdodFNDRiBUaWdodE9wdCBHcmlkNyBHcmlkeDknIHNlZW1zIHRvIHdvcmsg Zm9yIGFsbCBvZiBvdXIgc3lzdGVtcyB1cHRvIDIwMCBhdG9tcywgcHJvZHVjaW5nDQphY2N1cmF0 ZSByZXN1bHRzIGluIGdvb2QgYWdyZWVtZW50IHdpdGggZXhwZXJpbWVudGFsIG9ic2VydmF0aW9u cy4NCg0KSG9wZSB0aGlzIGhlbHBzDQoNCndpdGggYmVzdA0KLSBTYWNoaW4NCg0KT24gU2F0LCBK dWwgOSwgMjAyMiBhdCA3OjMyIFBNIEdyaWdvcml5IFpodXJrbyByZWdfemh1cmtvLjouY2hlbWNy YWZ0cHJvZy5jb208aHR0cDovL2NoZW1jcmFmdHByb2cuY29tPiA8b3duZXItY2hlbWlzdHJ5Kipj Y2wubmV0PG1haWx0bzpvd25lci1jaGVtaXN0cnkqKmNjbC5uZXQ+PiB3cm90ZToNCg0KU2VudCB0 byBDQ0wgYnk6ICJHcmlnb3JpeSAgWmh1cmtvIiBbcmVnX3podXJrbygpY2hlbWNyYWZ0cHJvZy5j b208aHR0cDovL2NoZW1jcmFmdHByb2cuY29tPl0NCkhlbGxvLA0KSSBjb21wdXRlIHNvbWUgbW9s ZWN1bGVzIHdpdGggT3JjYSA1LjAuMywgYW5kIHRoZSBjb21wdXRhdGlvbiBzb21ldGltZXMNCnBy b2R1Y2VzIHNtYWxsIG5lZ2F0aXZlIGZyZXF1ZW5jaWVzLCBkZXNwaXRlIHRoZSBzeW1tZXRyeSBv ZiB0aGUgbW9sZWN1bGVzIGlzDQpDMS4gSWYgSSByZXBlYXQgdGhlIGNvbXB1dGF0aW9uIHdpdGgg YW5vdGhlciBzdGFydGluZyBwb2ludCwgd2l0aCBzb21lDQpwcm9iYWJpbGl0eSBhbGwgZnJlcXVl bmNpZXMgYXJlIHBvc2l0aXZlLg0KSSBmb3VuZCB0aGF0IHRoaXMgcHJvYmxlbSBhcmlzZXMgd2hl biB0d28gYWRkaXRpb25zIHRvIHRoZSBtb2RlbCBhcmUgYWRkZWQ6DQp0aGUgc29sdmVudCBtb2Rl bCAoIUNQQ00oV2F0ZXIpKSBhbmQgYWRkaXRpb25zIG9mIHNvbWUgZXhwbGljaXQgd2F0ZXINCm1v bGVjdWxlcyB0byB0aGUgd2hvbGUgbW9kZWwuIEkgdW5kZXJzdGFuZCB0aGF0IHRoZXNlIHdhdGVy IG1vbGVjdWxlcyBwcm9kdWNlDQp2ZXJ5IHNtYWxsIGZyZXF1ZW5jaWVzIGFsb25nIHRoZSBoLWJv bmRzLCBhbmQgdGhlc2UgZnJlcXVlbmNpZXMgY2FuIGJlY29tZQ0KbmVnYXRpdmUgYmVjYXVzZSBv ZiBzb21lIHByb2JsZW1zIHdpdGggbnVtZXJpY2FsIGludGVncmF0aW9uLiBJIHRyaWVkIHRoZQ0K Y29tYmluYXRpb24gb2Ygb3B0aW9ucyAhRGVmR3JpZDMsICFUaWdodE9wdCwgIVZlcnlUaWdodFND RiwgYW5kIHN0aWxsDQpzb21ldGltZXMgdGhlIG5lZ2F0aXZlIGZyZXF1ZW5jaWVzIGFyZSBwcm9k dWNlZC4gTWF5YmUgSSBuZWVkIHRvIGZ1cnRoZXINCmluY3JlYXNlIHRoZSBjb21wdXRhdGlvbmFs IGFjY3VyYWN5IHdpdGggb3B0aW9ucyBsaWtlICIhVmVyeVRpZ2h0T3B0IiwNCiIhRGVmR3JpZDki LCBVbHRyYVRpZ2h0U0NGPyBJIHN1cHBvc2UgeW91IHVuZGVyc3RhbmQgd2hhdCBJIG1lYW47IGN1 cnJlbnRseQ0KSSBkaWRuJ3QgZmluZCB0aGUgaW5mb3JtYXRpb24gaW4gdGhlIG1hbnVhbCwgaG93 IHRvIGZ1cnRoZXIgZGVjcmVhc2UgdGhlDQpvcHRpbWl6YXRpb24gY29udmVyZ2VuY2UgdGhyZXNo b2xkIG9yIGluY3JlYXNlIHRoZSBhY2N1cmFjeSBvZiBERlQgZ3JpZC4NClBsZWFzZSBzdWdnZXN0 IGhvdyB0byBkbyB0aGF0Lg0KSW4gbXkgd29yayBJIGNhbiBhdm9pZCB1c2luZyB0aGUgZnJlcXVl bmNpZXMgc2luY2UgSSBuZWVkIG1haW5seSB0aGUNCmVuZXJnaWVzOyBob3dldmVyIEkgbmVlZCB0 byBleHBsYWluIHRoaXMgc29tZWhvdyBpbiB0aGUgcGFwZXIuIEkgc3VwcG9zZSwgaXQNCmlzIG5v dCBnb29kIHRvIGNvbXB1dGUgdGhlIGVudHJvcHkgb2YgbW9sZWN1bGVzIHdpdGggbXkga2V5d29y ZHMsIGJlY2F1c2UNCnNtYWxsIGZyZXF1ZW5jaWVzIHByb2R1Y2UgYmlnIGVycm9ycyB3aXRoIHZp YnJhdGlvbmFsIGVudHJvcHkuIFNvLCBwbGVhc2UNCnN1Z2dlc3QgbWUsIHdoYXQgc2hvdWxkIEkg d3JpdGUgaW4gbXkgcGFwZXJzLCB0byBleHBsYWluIHRoYXQgaXQgaXMgbm90IGdvb2QNCnRvIGNv bXB1dGUgdGhlIEdpYmJzIGVuZXJneSBvZiBteSBtb2xlY3VsZXMsIGJ1dCBpdCBpcyBjb3JyZWN0 IHRvIGNvbXB1dGUgYW5kDQp1c2UgdGhlIGNvbW1vbiBlbmVyZ3kuDQoNCkdyaWdvcml5IFpodXJr bw0KaHR0cHM6Ly9jaGVtY3JhZnRwcm9nLmNvbQ0KDQoNCg0KLT0gVGhpcyBpcyBhdXRvbWF0aWNh bGx5IGFkZGVkIHRvIGVhY2ggbWVzc2FnZSBieSB0aGUgbWFpbGluZyBzY3JpcHQgPS0NCkUtbWFp bCB0byBzdWJzY3JpYmVyczogQ0hFTUlTVFJZKipjY2wubmV0PG1haWx0bzpDSEVNSVNUUlkqKmNj bC5uZXQ+IG9yIHVzZToNCiAgICAgIGh0dHA6Ly93d3cuY2NsLm5ldC9jZ2ktYmluL2NjbC9zZW5k X2NjbF9tZXNzYWdlDQoNCkUtbWFpbCB0byBhZG1pbmlzdHJhdG9yczogQ0hFTUlTVFJZLVJFUVVF U1QqKmNjbC5uZXQ8bWFpbHRvOkNIRU1JU1RSWS1SRVFVRVNUKipjY2wubmV0PiBvciB1c2UNCiAg ICAgIGh0dHA6Ly93d3cuY2NsLm5ldC9jZ2ktYmluL2NjbC9zZW5kX2NjbF9tZXNzYWdlDQogICAg ICBodHRwOi8vd3d3LmNjbC5uZXQvY2hlbWlzdHJ5L3N1Yl91bnN1Yi5zaHRtbA0KDQpCZWZvcmUg cG9zdGluZywgY2hlY2sgd2FpdCB0aW1lIGF0OiBodHRwOi8vd3d3LmNjbC5uZXQNCg0KSm9iOiBo dHRwOi8vd3d3LmNjbC5uZXQvam9icw0KQ29uZmVyZW5jZXM6IGh0dHA6Ly9zZXJ2ZXIuY2NsLm5l dC9jaGVtaXN0cnkvYW5ub3VuY2VtZW50cy9jb25mZXJlbmNlcy8NCg0KU2VhcmNoIE1lc3NhZ2Vz OiBodHRwOi8vd3d3LmNjbC5uZXQvY2hlbWlzdHJ5L3NlYXJjaGNjbC9pbmRleC5zaHRtbA0KICAg ICAgaHR0cDovL3d3dy5jY2wubmV0L3NwYW1tZXJzLnR4dA0KDQpSVEZJOiBodHRwOi8vd3d3LmNj bC5uZXQvY2hlbWlzdHJ5L2Fib3V0Y2NsL2luc3RydWN0aW9ucy8NCg0KDQo= --_000_65519CE448FC44939D162FD3717B9ADFkofompgde_ Content-Type: text/html; charset="utf-8" Content-Transfer-Encoding: base64 PGh0bWw+DQo8aGVhZD4NCjxtZXRhIGh0dHAtZXF1aXY9IkNvbnRlbnQtVHlwZSIgY29udGVudD0i dGV4dC9odG1sOyBjaGFyc2V0PXV0Zi04Ij4NCjwvaGVhZD4NCjxib2R5IGRpcj0iYXV0byI+DQpK dXN0IHRvIGJyaWVmbHkgY2xhcmlmeQ0KPGRpdj48YnI+DQo8L2Rpdj4NCjxkaXY+DQo8YmxvY2tx dW90ZSB0eXBlPSJjaXRlIj4NCjxkaXYgZGlyPSJsdHIiPg0KPGRpdiBkaXI9Imx0ciI+DQo8ZGl2 IGRpcj0ibHRyIj5UaWdodFNDRiBUaWdodE9wdCBHcmlkNyBHcmlkeDknPC9kaXY+DQo8L2Rpdj4N CjwvZGl2Pg0KPC9ibG9ja3F1b3RlPg0KPGRpdj48YnI+DQo8L2Rpdj4NCklzIE9SQ0EgcHJlIDUu MC4gd2l0aCA1LjAgdGhlc2Ugb2xkIGdyaWRzIGFyZSBnb25lIGFuZCB0aGUgbmV3IGdyaWRzIGFy ZSBtdWNoIG1vcmUgYWNjdXJhdGUgYW5kIGRvbuKAmHQgbmVlZCBidW1waW5nIHVwLiZuYnNwOzwv ZGl2Pg0KPGRpdj48YnI+DQo8L2Rpdj4NCjxkaXY+VGhlIE9QIGhhcyB0cmllZCB0aGVzZSB0aGlu Z3MgYW5kIHRoZSBuZWdhdGl2ZSBmcmVxdWVuY2llcyByZW1haW5lZCwgbWVhbmluZyB0aGF0IHRo ZXkgYXJlIG5vdCBudW1lcmljYWwgbm9pc2UuIFRoZSBPUCB3YXMgYWR2aXNlZCB0byBkaXNwbGFj ZSB0aGUgbW9sZWN1bGUgYWxvbmcgdGhlIHJlc3BlY3RpdmUgcmVhbCBtb2Rlcy4gSXQgd2FzIGFs c28gcG9pbnRlZCBvdXQgdG8gaGltIHRoYXQgdGhlcmUgaXMgYSBjb21wb3VuZCBzY3JpcHQNCiB0 aGF0IGNvbWVzIHdpdGggT1JDQSA1LjAgYW5kIGxhdGVyIHRoYXQgYXV0b21hdGljYWxseSBkaXNw bGFjZXMgdGhlIG1vbGVjdWxlIGFsb25nIGFueSBuZWdhdGl2ZSBmcmVxdWVuY3kgbW9kZSB1bnRp bCBhbGwgbmVnYXRpdmUgZnJlcXVlbmNpZXMgYXJlIGdvbmUuJm5ic3A7PC9kaXY+DQo8ZGl2Pjxi cj4NCjwvZGl2Pg0KPGRpdj5UaGF0IGlzIHRoZSBiZXN0IGFkdmlzZSBJIGFtIGFibGUgdG8gZ2l2 ZS4mbmJzcDs8YnI+DQo8YnI+DQo8ZGl2IGRpcj0ibHRyIj5TZW50IGZyb20gbXkgaVBhZDwvZGl2 Pg0KPGRpdiBkaXI9Imx0ciI+PGJyPg0KPGJsb2NrcXVvdGUgdHlwZT0iY2l0ZSI+T24gMTAuIEp1 bCAyMDIyLCBhdCAwNzo1NiwgU2FjaGluIFJhbWVzaCBzYWNoaW5hZGl0eWFyYW1lc2goKSBnbWFp bC5jb20gJmx0O293bmVyLWNoZW1pc3RyeUBjY2wubmV0Jmd0OyB3cm90ZTo8YnI+DQo8YnI+DQo8 L2Jsb2NrcXVvdGU+DQo8L2Rpdj4NCjxibG9ja3F1b3RlIHR5cGU9ImNpdGUiPg0KPGRpdiBkaXI9 Imx0ciI+77u/DQo8ZGl2IGRpcj0ibHRyIj4NCjxkaXYgZGlyPSJsdHIiPkhpLA0KPGRpdj48YnI+ DQo8L2Rpdj4NCjxkaXY+Jm5ic3A7ICZuYnNwO0ltYWdpbmFyeSBtb2RlcyB1bmRlciAnLTEwIGNt LTEnIGlmIG5vdCBtYW55IGNhbiBiZSBzYWZlbHkgaWdub3JlZC4gWW91IGNvdWxkIHRyeSB0byBn ZXQgcmlkJm5ic3A7PC9kaXY+DQo8ZGl2Pm9mIHRoZSBpbWFnaW5hcnkgbW9kZSBieSBkaXN0b3J0 aW5nIHRoZSBzdHJ1Y3R1cmUgYWxvbmcgdGhlIGJvbmQsIGFuZ2xlIG9yIGRpaGVkcmFsIHdoaWNo IGlzJm5ic3A7PC9kaXY+DQo8ZGl2PmNhdXNpbmcgdGhlIGltYWdpbmFyeSBtb2RlLiZuYnNwOzwv ZGl2Pg0KPGRpdj48YnI+DQo8L2Rpdj4NCjxkaXY+Jm5ic3A7ICZuYnNwO0kgc2hvdWxkIGFkZCB0 aGF0IGltYWdpbmFyeSBtb2RlcyBhcmUgdHJpY2t5IHRvIGdldCByaWQgb2Ygd2hlbiB0aGUgc29s dmVudCBjb3JyZWN0aW9uIGlzIHVzZWQuJm5ic3A7PC9kaXY+DQo8ZGl2PlRoZSBvcHRpbWl6YXRp b24gY291bGQgYmUgZG9uZSB1c2luZyBzb2x2ZW50IGNvcnJlY3Rpb24gYW5kIGZyZXF1ZW5jeSBj YW4gYmUgY29tcHV0ZWQgaW4gZ2FzIHBoYXNlLiZuYnNwOzwvZGl2Pg0KPGRpdj48YnI+DQo8L2Rp dj4NCjxkaXY+Jm5ic3A7ICdUaWdodFNDRiBUaWdodE9wdCBHcmlkNyBHcmlkeDknIHNlZW1zIHRv IHdvcmsgZm9yIGFsbCBvZiBvdXIgc3lzdGVtcyB1cHRvIDIwMCBhdG9tcywgcHJvZHVjaW5nJm5i c3A7PC9kaXY+DQo8ZGl2PmFjY3VyYXRlIHJlc3VsdHMgaW4gZ29vZCBhZ3JlZW1lbnQgd2l0aCBl eHBlcmltZW50YWwgb2JzZXJ2YXRpb25zLiAmbmJzcDs8L2Rpdj4NCjxkaXY+PGJyPg0KPC9kaXY+ DQo8ZGl2PkhvcGUgdGhpcyBoZWxwcyZuYnNwOzxicj4NCjwvZGl2Pg0KPGRpdj48YnI+DQo8L2Rp dj4NCjxkaXY+d2l0aCBiZXN0Jm5ic3A7PC9kaXY+DQo8Zm9udCBjb2xvcj0iIzg4ODg4OCI+DQo8 ZGl2Pi0gU2FjaGluJm5ic3A7PC9kaXY+DQo8L2ZvbnQ+PC9kaXY+DQo8YnI+DQo8ZGl2IGNsYXNz PSJnbWFpbF9xdW90ZSI+DQo8ZGl2IGRpcj0ibHRyIiBjbGFzcz0iZ21haWxfYXR0ciI+T24gU2F0 LCBKdWwgOSwgMjAyMiBhdCA3OjMyIFBNIEdyaWdvcml5IFpodXJrbyByZWdfemh1cmtvLjouPGEg aHJlZj0iaHR0cDovL2NoZW1jcmFmdHByb2cuY29tIj5jaGVtY3JhZnRwcm9nLmNvbTwvYT4gJmx0 OzxhIGhyZWY9Im1haWx0bzpvd25lci1jaGVtaXN0cnkqKmNjbC5uZXQiPm93bmVyLWNoZW1pc3Ry eSoqY2NsLm5ldDwvYT4mZ3Q7IHdyb3RlOjxicj4NCjwvZGl2Pg0KPGJsb2NrcXVvdGUgY2xhc3M9 ImdtYWlsX3F1b3RlIiBzdHlsZT0ibWFyZ2luOjBweCAwcHggMHB4IDAuOGV4O2JvcmRlci1sZWZ0 LXdpZHRoOjFweDtib3JkZXItbGVmdC1zdHlsZTpzb2xpZDtib3JkZXItbGVmdC1jb2xvcjpyZ2Io MjA0LDIwNCwyMDQpO3BhZGRpbmctbGVmdDoxZXgiPg0KPGJyPg0KU2VudCB0byBDQ0wgYnk6ICZx dW90O0dyaWdvcml5Jm5ic3A7IFpodXJrbyZxdW90OyBbcmVnX3podXJrbygpPGEgaHJlZj0iaHR0 cDovL2NoZW1jcmFmdHByb2cuY29tIiByZWw9Im5vcmVmZXJyZXIiIHRhcmdldD0iX2JsYW5rIj5j aGVtY3JhZnRwcm9nLmNvbTwvYT5dPGJyPg0KSGVsbG8sPGJyPg0KSSBjb21wdXRlIHNvbWUgbW9s ZWN1bGVzIHdpdGggT3JjYSA1LjAuMywgYW5kIHRoZSBjb21wdXRhdGlvbiBzb21ldGltZXMgPGJy Pg0KcHJvZHVjZXMgc21hbGwgbmVnYXRpdmUgZnJlcXVlbmNpZXMsIGRlc3BpdGUgdGhlIHN5bW1l dHJ5IG9mIHRoZSBtb2xlY3VsZXMgaXMgPGJyPg0KQzEuIElmIEkgcmVwZWF0IHRoZSBjb21wdXRh dGlvbiB3aXRoIGFub3RoZXIgc3RhcnRpbmcgcG9pbnQsIHdpdGggc29tZSA8YnI+DQpwcm9iYWJp bGl0eSBhbGwgZnJlcXVlbmNpZXMgYXJlIHBvc2l0aXZlLjxicj4NCkkgZm91bmQgdGhhdCB0aGlz IHByb2JsZW0gYXJpc2VzIHdoZW4gdHdvIGFkZGl0aW9ucyB0byB0aGUgbW9kZWwgYXJlIGFkZGVk OiA8YnI+DQp0aGUgc29sdmVudCBtb2RlbCAoIUNQQ00oV2F0ZXIpKSBhbmQgYWRkaXRpb25zIG9m IHNvbWUgZXhwbGljaXQgd2F0ZXIgPGJyPg0KbW9sZWN1bGVzIHRvIHRoZSB3aG9sZSBtb2RlbC4g SSB1bmRlcnN0YW5kIHRoYXQgdGhlc2Ugd2F0ZXIgbW9sZWN1bGVzIHByb2R1Y2UgPGJyPg0KdmVy eSBzbWFsbCBmcmVxdWVuY2llcyBhbG9uZyB0aGUgaC1ib25kcywgYW5kIHRoZXNlIGZyZXF1ZW5j aWVzIGNhbiBiZWNvbWUgPGJyPg0KbmVnYXRpdmUgYmVjYXVzZSBvZiBzb21lIHByb2JsZW1zIHdp dGggbnVtZXJpY2FsIGludGVncmF0aW9uLiBJIHRyaWVkIHRoZSA8YnI+DQpjb21iaW5hdGlvbiBv ZiBvcHRpb25zICFEZWZHcmlkMywgIVRpZ2h0T3B0LCAhVmVyeVRpZ2h0U0NGLCBhbmQgc3RpbGwg PGJyPg0Kc29tZXRpbWVzIHRoZSBuZWdhdGl2ZSBmcmVxdWVuY2llcyBhcmUgcHJvZHVjZWQuIE1h eWJlIEkgbmVlZCB0byBmdXJ0aGVyIDxicj4NCmluY3JlYXNlIHRoZSBjb21wdXRhdGlvbmFsIGFj Y3VyYWN5IHdpdGggb3B0aW9ucyBsaWtlICZxdW90OyFWZXJ5VGlnaHRPcHQmcXVvdDssIDxicj4N CiZxdW90OyFEZWZHcmlkOSZxdW90OywgVWx0cmFUaWdodFNDRj8gSSBzdXBwb3NlIHlvdSB1bmRl cnN0YW5kIHdoYXQgSSBtZWFuOyBjdXJyZW50bHkgPGJyPg0KSSBkaWRuJ3QgZmluZCB0aGUgaW5m b3JtYXRpb24gaW4gdGhlIG1hbnVhbCwgaG93IHRvIGZ1cnRoZXIgZGVjcmVhc2UgdGhlIDxicj4N Cm9wdGltaXphdGlvbiBjb252ZXJnZW5jZSB0aHJlc2hvbGQgb3IgaW5jcmVhc2UgdGhlIGFjY3Vy YWN5IG9mIERGVCBncmlkLiA8YnI+DQpQbGVhc2Ugc3VnZ2VzdCBob3cgdG8gZG8gdGhhdC48YnI+ DQpJbiBteSB3b3JrIEkgY2FuIGF2b2lkIHVzaW5nIHRoZSBmcmVxdWVuY2llcyBzaW5jZSBJIG5l ZWQgbWFpbmx5IHRoZSA8YnI+DQplbmVyZ2llczsgaG93ZXZlciBJIG5lZWQgdG8gZXhwbGFpbiB0 aGlzIHNvbWVob3cgaW4gdGhlIHBhcGVyLiBJIHN1cHBvc2UsIGl0IDxicj4NCmlzIG5vdCBnb29k IHRvIGNvbXB1dGUgdGhlIGVudHJvcHkgb2YgbW9sZWN1bGVzIHdpdGggbXkga2V5d29yZHMsIGJl Y2F1c2UgPGJyPg0Kc21hbGwgZnJlcXVlbmNpZXMgcHJvZHVjZSBiaWcgZXJyb3JzIHdpdGggdmli cmF0aW9uYWwgZW50cm9weS4gU28sIHBsZWFzZSA8YnI+DQpzdWdnZXN0IG1lLCB3aGF0IHNob3Vs ZCBJIHdyaXRlIGluIG15IHBhcGVycywgdG8gZXhwbGFpbiB0aGF0IGl0IGlzIG5vdCBnb29kIDxi cj4NCnRvIGNvbXB1dGUgdGhlIEdpYmJzIGVuZXJneSBvZiBteSBtb2xlY3VsZXMsIGJ1dCBpdCBp cyBjb3JyZWN0IHRvIGNvbXB1dGUgYW5kIDxicj4NCnVzZSB0aGUgY29tbW9uIGVuZXJneS48YnI+ DQo8YnI+DQpHcmlnb3JpeSBaaHVya288YnI+DQo8YSBocmVmPSJodHRwczovL2NoZW1jcmFmdHBy b2cuY29tIiByZWw9Im5vcmVmZXJyZXIiIHRhcmdldD0iX2JsYW5rIj5odHRwczovL2NoZW1jcmFm dHByb2cuY29tPC9hPjxicj4NCjxicj4NCjxicj4NCjxicj4NCi09IFRoaXMgaXMgYXV0b21hdGlj YWxseSBhZGRlZCB0byBlYWNoIG1lc3NhZ2UgYnkgdGhlIG1haWxpbmcgc2NyaXB0ID0tPGJyPGJy PXI8YnI+DQo8YnI+DQpFLW1haWwgdG8gc3Vic2NyaWJlcnM6IDxhIGhyZWY9Im1haWx0bzpDSEVN SVNUUlkqKmNjbC5uZXQiIHRhcmdldD0iX2JsYW5rIj5DSEVNSVNUUlkqKmNjbC5uZXQ8L2E+IG9y IHVzZTo8YnI+DQombmJzcDsgJm5ic3A7ICZuYnNwOyA8YSBocmVmPSJodHRwOi8vd3d3LmNjbC5u ZXQvY2dpLWJpbi9jY2wvc2VuZF9jY2xfbWVzc2FnZSIgcmVsPSJub3JlZmVycmVyIiB0YXJnZXQ9 Il9ibGFuayI+DQpodHRwOi8vd3d3LmNjbC5uZXQvY2dpLWJpbi9jY2wvc2VuZF9jY2xfbWVzc2Fn ZTwvYT48YnI+DQo8YnI+DQpFLW1haWwgdG8gYWRtaW5pc3RyYXRvcnM6IDxhIGhyZWY9Im1haWx0 bzpDSEVNSVNUUlktUkVRVUVTVCoqY2NsLm5ldCIgdGFyZ2V0PSJfYmxhbmsiPg0KQ0hFTUlTVFJZ LVJFUVVFU1QqKmNjbC5uZXQ8L2E+IG9yIHVzZTxicj4NCiZuYnNwOyAmbmJzcDsgJm5ic3A7IDxh IGhyZWY9Imh0dHA6Ly93d3cuY2NsLm5ldC9jZ2ktYmluL2NjbC9zZW5kX2NjbF9tZXNzYWdlIiBy ZWw9Im5vcmVmZXJyZXIiIHRhcmdldD0iX2JsYW5rIj4NCmh0dHA6Ly93d3cuY2NsLm5ldC9jZ2kt YmluL2NjbC9zZW5kX2NjbF9tZXNzYWdlPC9hPjxicj4NCjxicjxicj4mbmJzcDsgJm5ic3A7ICZu YnNwOyA8YSBocmVmPSJodHRwOi8vd3d3LmNjbC5uZXQvY2hlbWlzdHJ5L3N1Yl91bnN1Yi5zaHRt bCIgcmVsPSJub3JlZmVycmVyIiB0YXJnZXQ9Il9ibGFuayI+DQpodHRwOi8vd3d3LmNjbC5uZXQv Y2hlbWlzdHJ5L3N1Yl91bnN1Yi5zaHRtbDwvYT48YnI+DQo8YnI+DQpCZWZvcmUgcG9zdGluZywg Y2hlY2sgd2FpdCB0aW1lIGF0OiA8YSBocmVmPSJodHRwOi8vd3d3LmNjbC5uZXQiIHJlbD0ibm9y ZWZlcnJlciIgdGFyZ2V0PSJfYmxhbmsiPg0KaHR0cDovL3d3dy5jY2wubmV0PC9hPjxicj4NCjxi cj4NCkpvYjogPGEgaHJlZj0iaHR0cDovL3d3dy5jY2wubmV0L2pvYnMiIHJlbD0ibm9yZWZlcnJl ciIgdGFyZ2V0PSJfYmxhbmsiPmh0dHA6Ly93d3cuY2NsLm5ldC9qb2JzPC9hPg0KPGJyPg0KQ29u ZmVyZW5jZXM6IDxhIGhyZWY9Imh0dHA6Ly9zZXJ2ZXIuY2NsLm5ldC9jaGVtaXN0cnkvYW5ub3Vu Y2VtZW50cy9jb25mZXJlbmNlcy8iIHJlbD0ibm9yZWZlcnJlciIgdGFyZ2V0PSJfYmxhbmsiPg0K aHR0cDovL3NlcnZlci5jY2wubmV0L2NoZW1pc3RyeS9hbm5vdW5jZW1lbnRzL2NvbmZlcmVuY2Vz LzwvYT48YnI+DQo8YnI+DQpTZWFyY2ggTWVzc2FnZXM6IDxhIGhyZWY9Imh0dHA6Ly93d3cuY2Ns Lm5ldC9jaGVtaXN0cnkvc2VhcmNoY2NsL2luZGV4LnNodG1sIiByZWw9Im5vcmVmZXJyZXIiIHRh cmdldD0iX2JsYW5rIj4NCmh0dHA6Ly93d3cuY2NsLm5ldC9jaGVtaXN0cnkvc2VhcmNoY2NsL2lu ZGV4LnNodG1sPC9hPjxicj4NCjxicjxicj4mbmJzcDsgJm5ic3A7ICZuYnNwOyA8YSBocmVmPSJo dHRwOi8vd3d3LmNjbC5uZXQvc3BhbW1lcnMudHh0IiByZWw9Im5vcmVmZXJyZXIiIHRhcmdldD0i X2JsYW5rIj4NCmh0dHA6Ly93d3cuY2NsLm5ldC9zcGFtbWVycy50eHQ8L2E+PGJyPg0KPGJyPg0K UlRGSTogPGEgaHJlZj0iaHR0cDovL3d3dy5jY2wubmV0L2NoZW1pc3RyeS9hYm91dGNjbC9pbnN0 cnVjdGlvbnMvIiByZWw9Im5vcmVmZXJyZXIiIHRhcmdldD0iX2JsYW5rIj4NCmh0dHA6Ly93d3cu Y2NsLm5ldC9jaGVtaXN0cnkvYWJvdXRjY2wvaW5zdHJ1Y3Rpb25zLzwvYT48YnI+DQo8YnI+DQo8 YnI+DQo8L2JyPGJyPjwvYnI8YnI+PC9icjxicj1yPGJyPjwvYmxvY2txdW90ZT4NCjwvZGl2Pg0K PC9kaXY+DQo8L2Rpdj4NCjwvYmxvY2txdW90ZT4NCjwvZGl2Pg0KPC9ib2R5Pg0KPC9odG1sPg0K --_000_65519CE448FC44939D162FD3717B9ADFkofompgde_-- From owner-chemistry@ccl.net Sun Jul 10 06:20:00 2022 From: "Sachin Ramesh sachinadityaramesh!^!gmail.com" To: CCL Subject: CCL: [CCL] CCL: Negative frequencies with C1 symmetry (Orca) Message-Id: <-54754-220710061849-30613-kj4ukyes7vJPH4kXa4d9LQ*o*server.ccl.net> X-Original-From: Sachin Ramesh Content-Type: multipart/alternative; boundary="00000000000084e4c605e370c29f" Date: Sun, 10 Jul 2022 15:48:32 +0530 MIME-Version: 1.0 Sent to CCL by: Sachin Ramesh [sachinadityaramesh^gmail.com] --00000000000084e4c605e370c29f Content-Type: text/plain; charset="UTF-8" Content-Transfer-Encoding: quoted-printable Hi, Yes, Prof. Neese. I was referring to ORCA 4.2.1. I should have mentioned it. -Sachin On Sun, Jul 10, 2022 at 3:27 PM Neese, Frank neese]![kofo.mpg.de < owner-chemistry(-)ccl.net> wrote: > Just to briefly clarify > > TightSCF TightOpt Grid7 Gridx9' > > > Is ORCA pre 5.0. with 5.0 these old grids are gone and the new grids are > much more accurate and don=E2=80=98t need bumping up. > > The OP has tried these things and the negative frequencies remained, > meaning that they are not numerical noise. The OP was advised to displace > the molecule along the respective real modes. It was also pointed out to > him that there is a compound script that comes with ORCA 5.0 and later th= at > automatically displaces the molecule along any negative frequency mode > until all negative frequencies are gone. > > That is the best advise I am able to give. > > Sent from my iPad > > On 10. Jul 2022, at 07:56, Sachin Ramesh sachinadityaramesh() gmail.com < > owner-chemistry(-)ccl.net> wrote: > > =EF=BB=BF > Hi, > > Imaginary modes under '-10 cm-1' if not many can be safely ignored. Yo= u > could try to get rid > of the imaginary mode by distorting the structure along the bond, angle o= r > dihedral which is > causing the imaginary mode. > > I should add that imaginary modes are tricky to get rid of when the > solvent correction is used. > The optimization could be done using solvent correction and frequency can > be computed in gas phase. > > 'TightSCF TightOpt Grid7 Gridx9' seems to work for all of our systems > upto 200 atoms, producing > accurate results in good agreement with experimental observations. > > Hope this helps > > with best > - Sachin > > On Sat, Jul 9, 2022 at 7:32 PM Grigoriy Zhurko reg_zhurko.:. > chemcraftprog.com wrote: > >> >> Sent to CCL by: "Grigoriy Zhurko" [reg_zhurko()chemcraftprog.com] >> Hello, >> I compute some molecules with Orca 5.0.3, and the computation sometimes >> produces small negative frequencies, despite the symmetry of the >> molecules is >> C1. If I repeat the computation with another starting point, with some >> probability all frequencies are positive. >> I found that this problem arises when two additions to the model are >> added: >> the solvent model (!CPCM(Water)) and additions of some explicit water >> molecules to the whole model. I understand that these water molecules >> produce >> very small frequencies along the h-bonds, and these frequencies can >> become >> negative because of some problems with numerical integration. I tried th= e >> combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still >> sometimes the negative frequencies are produced. Maybe I need to further >> increase the computational accuracy with options like "!VeryTightOpt", >> "!DefGrid9", UltraTightSCF? I suppose you understand what I mean; >> currently >> I didn't find the information in the manual, how to further decrease the >> optimization convergence threshold or increase the accuracy of DFT grid. >> Please suggest how to do that. >> In my work I can avoid using the frequencies since I need mainly the >> energies; however I need to explain this somehow in the paper. I suppose= , >> it >> is not good to compute the entropy of molecules with my keywords, becaus= e >> small frequencies produce big errors with vibrational entropy. So, pleas= e >> suggest me, what should I write in my papers, to explain that it is not >> good >> to compute the Gibbs energy of my molecules, but it is correct to comput= e >> and >> use the common energy. >> >> Grigoriy Zhurko >> https://chemcraftprog.com >> >> >> >> -=3D This is automatically added to each message by the mailing script = =3D- >> E-mail to subscribers: CHEMISTRY**ccl.net or use:>> >> E-mail to administrators: CHEMISTRY-REQUEST**ccl.net or use>> >> >> --00000000000084e4c605e370c29f Content-Type: text/html; charset="UTF-8" Content-Transfer-Encoding: quoted-printable

Hi,

=C2=A0 Yes, Prof. Neese. I was referring=C2=A0to ORCA 4.2.1.=C2=A0
=
I should have mentioned it.=C2=A0

-Sachin
On S= un, Jul 10, 2022 at 3:27 PM Neese, Frank neese]![kofo.mpg.de <owner-c= hemistry(-)ccl.net> wrote:
Just to briefly clarify

TightSCF TightOpt Grid7 Gridx9'

Is ORCA pre 5.0. with 5.0 these old grids are gone and the new grids are mu= ch more accurate and don=E2=80=98t need bumping up.=C2=A0

The OP has tried these things and the negative frequencies remained, m= eaning that they are not numerical noise. The OP was advised to displace th= e molecule along the respective real modes. It was also pointed out to him = that there is a compound script that comes with ORCA 5.0 and later that automatically displaces the molecu= le along any negative frequency mode until all negative frequencies are gon= e.=C2=A0

That is the best advise I am able to give.=C2=A0

Sent from my iPad

On 10. Jul 2022, at 07:56, Sachin Ramesh sachinad= ityaramesh() gmail.com &= lt;owner-chemi= stry(-)ccl.net> wrote:

=EF=BB=BF
Hi,

=C2=A0 =C2=A0Imaginary modes under '-10 cm-1' if not many can = be safely ignored. You could try to get rid=C2=A0
of the imaginary mode by distorting the structure along the bond, angl= e or dihedral which is=C2=A0
causing the imaginary mode.=C2=A0

=C2=A0 =C2=A0I should add that imaginary modes are tricky to get rid o= f when the solvent correction is used.=C2=A0
The optimization could be done using solvent correction and frequency = can be computed in gas phase.=C2=A0

=C2=A0 'TightSCF TightOpt Grid7 Gridx9' seems to work for all = of our systems upto 200 atoms, producing=C2=A0
accurate results in good agreement with experimental observations. =C2= =A0

Hope this helps=C2=A0

with best=C2=A0
- Sachin=C2=A0

On Sat, Jul 9, 2022 at 7:32 PM Grigor= iy Zhurko reg_zhurko.:.chemcraftprog.com <owner-chemistry**ccl.net> wrote:

Sent to CCL by: "Grigoriy=C2=A0 Zhurko" [reg_zhurko()chemcraftprog= .com]
Hello,
I compute some molecules with Orca 5.0.3, and the computation sometimes produces small negative frequencies, despite the symmetry of the molecules = is
C1. If I repeat the computation with another starting point, with some
probability all frequencies are positive.
I found that this problem arises when two additions to the model are added:=
the solvent model (!CPCM(Water)) and additions of some explicit water
molecules to the whole model. I understand that these water molecules produ= ce
very small frequencies along the h-bonds, and these frequencies can become =
negative because of some problems with numerical integration. I tried the <= br> combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still
sometimes the negative frequencies are produced. Maybe I need to further increase the computational accuracy with options like "!VeryTightOpt&q= uot;,
"!DefGrid9", UltraTightSCF? I suppose you understand what I mean;= currently
I didn't find the information in the manual, how to further decrease th= e
optimization convergence threshold or increase the accuracy of DFT grid. Please suggest how to do that.
In my work I can avoid using the frequencies since I need mainly the
energies; however I need to explain this somehow in the paper. I suppose, i= t
is not good to compute the entropy of molecules with my keywords, because <= br> small frequencies produce big errors with vibrational entropy. So, please <= br> suggest me, what should I write in my papers, to explain that it is not goo= d
to compute the Gibbs energy of my molecules, but it is correct to compute a= nd
use the common energy.

Grigoriy Zhurko
= https://chemcraftprog.com



-=3D This is automatically added to each message by the mailing script =3D-=
E-mail to subscribers: CHEMISTRY**ccl.net or use:
=C2=A0 =C2=A0 =C2=A0

E-mail to administrators:
CHEMISTRY-REQUEST**ccl.net or use
=C2=A0 =C2=A0 =C2=A0
=C2=A0 =C2=A0 =C2=A0


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

Job: http://www.ccl.net/jobs
Conferences: http://server.ccl.net/chemistry/announcements/conferences/

Search Messages: http://www.ccl.net/chemistry/searchccl/index.shtml
=C2=A0 =C2=A0 =C2=A0

RTFI:
http://www.ccl.net/chemistry/aboutccl/instructions/


--00000000000084e4c605e370c29f-- From owner-chemistry@ccl.net Sun Jul 10 08:11:00 2022 From: "Peter Jarowski peterjarowski_-_gmail.com" To: CCL Subject: CCL: [CCL] CCL: Negative frequencies with C1 symmetry (Orca) Message-Id: <-54755-220710040741-10594-kO4Cxe7wRB1RAi0a1XOSiA=server.ccl.net> X-Original-From: Peter Jarowski Content-Type: multipart/alternative; boundary="0000000000007177df05e36eed71" Date: Sun, 10 Jul 2022 10:07:22 +0200 MIME-Version: 1.0 Sent to CCL by: Peter Jarowski [peterjarowski[*]gmail.com] --0000000000007177df05e36eed71 Content-Type: text/plain; charset="UTF-8" Content-Transfer-Encoding: quoted-printable Hi All: A few comments. Do we have a reference for this 10 cm-1 rule-of-thumb? Has anyone published a comparison study using different softwares? I know NWchem ignores lateral frequencies (=C2=AB imaginary frequencies =C2=BB). So careful the outcome m= ight vary even assuming the same implementation of the partition functions. I guess we are talking sub Kcal/mol (cal / mol K :298 K) variations in thermal corrections. For solvatation, its tricky. The hard and fast rule is that the frequencies must be evaluated at the same level as the optimization. Thus, if you optimize in PCM implicit solvent you must do the thermal corrections in solvo as well. It often makes no significant difference, but I imagine it would introduce some small lateral frequencies if you do it in gas phase. In NWChem it requires numerical integration and takes forever. Best regards, Peter On Sun, 10 Jul 2022 at 07:57, Sachin Ramesh sachinadityaramesh() gmail.com = < owner-chemistry:ccl.net> wrote: > Hi, > > Imaginary modes under '-10 cm-1' if not many can be safely ignored. Yo= u > could try to get rid > of the imaginary mode by distorting the structure along the bond, angle o= r > dihedral which is > causing the imaginary mode. > > I should add that imaginary modes are tricky to get rid of when the > solvent correction is used. > The optimization could be done using solvent correction and frequency can > be computed in gas phase. > > 'TightSCF TightOpt Grid7 Gridx9' seems to work for all of our systems > upto 200 atoms, producing > accurate results in good agreement with experimental observations. > > Hope this helps > > with best > - Sachin > > On Sat, Jul 9, 2022 at 7:32 PM Grigoriy Zhurko reg_zhurko.:. > chemcraftprog.com wrote: > >> >> Sent to CCL by: "Grigoriy Zhurko" [reg_zhurko()chemcraftprog.com] >> Hello, >> I compute some molecules with Orca 5.0.3, and the computation sometimes >> produces small negative frequencies, despite the symmetry of the >> molecules is >> C1. If I repeat the computation with another starting point, with some >> probability all frequencies are positive. >> I found that this problem arises when two additions to the model are >> added: >> the solvent model (!CPCM(Water)) and additions of some explicit water >> molecules to the whole model. I understand that these water molecules >> produce >> very small frequencies along the h-bonds, and these frequencies can >> become >> negative because of some problems with numerical integration. I tried th= e >> combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still >> sometimes the negative frequencies are produced. Maybe I need to further >> increase the computational accuracy with options like "!VeryTightOpt", >> "!DefGrid9", UltraTightSCF? I suppose you understand what I mean; >> currently >> I didn't find the information in the manual, how to further decrease the >> optimization convergence threshold or increase the accuracy of DFT grid. >> Please suggest how to do that. >> In my work I can avoid using the frequencies since I need mainly the >> energies; however I need to explain this somehow in the paper. I suppose= , >> it >> is not good to compute the entropy of molecules with my keywords, becaus= e >> small frequencies produce big errors with vibrational entropy. So, pleas= e >> suggest me, what should I write in my papers, to explain that it is not >> good >> to compute the Gibbs energy of my molecules, but it is correct to comput= e >> and >> use the common energy. >> >> Grigoriy Zhurko >> https://chemcraftprog.com >> >> >> >> -=3D This is automatically added to each message by the mailing script = =3D- >> E-mail to subscribers: CHEMISTRY**ccl.net or use:>> >> E-mail to administrators: CHEMISTRY-REQUEST**ccl.net or use>> >> >> --0000000000007177df05e36eed71 Content-Type: text/html; charset="UTF-8" Content-Transfer-Encoding: quoted-printable
Hi All:

A few comments.

Do we = have a reference for this 10 cm-1 rule-of-thumb? Has anyone published a com= parison study using different softwares? I know NWchem ignores lateral freq= uencies (=C2=AB imaginary frequencies =C2=BB). So careful the outcome might= vary even assuming the same implementation of the partition functions. I g= uess we are talking sub Kcal/mol (cal / mol K :298 K) variations in thermal= corrections.

For solvat= ation, its tricky. The hard and fast rule is that the frequencies must be e= valuated at the same level as the optimization. Thus, if you optimize in PC= M implicit solvent you must do the thermal corrections in solvo as well.=C2= =A0 It often makes no significant difference, but I imagine it would introd= uce some small lateral frequencies if you do it in gas phase. In NWChem it = requires numerical integration and takes forever.
Best regards,

Peter

On Sun, 10 Jul 2022 at 07:57, Sachin Ramesh sachi= nadityaramesh() gmail.com <owner-chemistry:ccl.net> wrote:
Hi,

=C2=A0 =C2=A0Imaginary modes under '-10 cm-1' if no= t many can be safely ignored. You could try to get rid=C2=A0
of t= he imaginary mode by distorting the structure along the bond, angle or dihe= dral which is=C2=A0
causing the imaginary mode.=C2=A0
<= br>
=C2=A0 =C2=A0I should add that imaginary modes are tricky to = get rid of when the solvent correction is used.=C2=A0
The optimiz= ation could be done using solvent correction and frequency can be computed = in gas phase.=C2=A0

=C2=A0 'TightSCF TightOpt = Grid7 Gridx9' seems to work for all of our systems upto 200 atoms, prod= ucing=C2=A0
accurate results in good agreement with experimental = observations. =C2=A0

Hope this helps=C2=A0

with best=C2=A0
- Sachin=C2=A0

On Sat, Jul 9, 2022 at 7:32 PM Grigo= riy Zhurko reg_zhurko.:.chemcraftprog.com <owner-chemistry**ccl.net> wrote:

Sent to CCL by: "Grigoriy=C2=A0 Zhurko" [reg_zhurko()chemcraftprog= .com]
Hello,
I compute some molecules with Orca 5.0.3, and the computation sometimes produces small negative frequencies, despite the symmetry of the molecules = is
C1. If I repeat the computation with another starting point, with some
probability all frequencies are positive.
I found that this problem arises when two additions to the model are added:=
the solvent model (!CPCM(Water)) and additions of some explicit water
molecules to the whole model. I understand that these water molecules produ= ce
very small frequencies along the h-bonds, and these frequencies can become =
negative because of some problems with numerical integration. I tried the <= br> combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still
sometimes the negative frequencies are produced. Maybe I need to further increase the computational accuracy with options like "!VeryTightOpt&q= uot;,
"!DefGrid9", UltraTightSCF? I suppose you understand what I mean;= currently
I didn't find the information in the manual, how to further decrease th= e
optimization convergence threshold or increase the accuracy of DFT grid. Please suggest how to do that.
In my work I can avoid using the frequencies since I need mainly the
energies; however I need to explain this somehow in the paper. I suppose, i= t
is not good to compute the entropy of molecules with my keywords, because <= br> small frequencies produce big errors with vibrational entropy. So, please <= br> suggest me, what should I write in my papers, to explain that it is not goo= d
to compute the Gibbs energy of my molecules, but it is correct to compute a= nd
use the common energy.

Grigoriy Zhurko
= https://chemcraftprog.com



-=3D This is automatically added to each message by the mailing script =3D-=
E-mail to subscribers: CHEMISTRY**ccl.net or use:
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/cgi-bin/ccl/s= end_ccl_message

E-mail to administrators: CHEMISTRY-REQUEST**ccl.net or use
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/cgi-bin/ccl/s= end_ccl_message
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/chemistry/sub_un= sub.shtml

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

Job: http://www.ccl.net/jobs
Conferences: http://server.ccl.net/chemist= ry/announcements/conferences/

Search Messages: http://www.ccl.net/chemistry/sear= chccl/index.shtml
=C2=A0 =C2=A0 =C2=A0 http://www.ccl.net/spammers.txt

RTFI: http://www.ccl.net/chemistry/aboutccl/ins= tructions/


--0000000000007177df05e36eed71-- From owner-chemistry@ccl.net Sun Jul 10 10:33:00 2022 From: "may abdelghani may01dz : yahoo.fr" To: CCL Subject: CCL: Negative frequencies with C1 symmetry (Orca) Message-Id: <-54756-220710102840-26100-pH5j07/vqVrXZ0xpRDmuqg]![server.ccl.net> X-Original-From: may abdelghani Content-Type: multipart/alternative; boundary="----=_Part_6818212_734716936.1657463311962" Date: Sun, 10 Jul 2022 14:28:31 +0000 (UTC) MIME-Version: 1.0 Sent to CCL by: may abdelghani [may01dz__yahoo.fr] ------=_Part_6818212_734716936.1657463311962 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: quoted-printable I was getting Negative frequencies=C2=A0 whenever I used more than one no= de in the calculations.=C2=A0One of the ORCA users told me that the issue= =C2=A0 with the appearance of the Negative frequencies=C2=A0 came from usin= g more than one node. Of course, those frequencies disappeared right after = I used one node... hope that's your problem. Le dimanche 10 juillet 2022 =C3=A0 09:44:36 UTC+1, Neese, Frank neese]!= [kofo.mpg.de a =C3=A9crit : =20 =20 Just to briefly clarify TightSCF TightOpt Grid7 Gridx9' Is ORCA pre 5.0. with 5.0 these old grids are gone and the new grids are mu= ch more accurate and don=E2=80=98t need bumping up.=C2=A0 The OP has tried these things and the negative frequencies remained, meanin= g that they are not numerical noise. The OP was advised to displace the mol= ecule along the respective real modes. It was also pointed out to him that = there is a compound script that comes with ORCA 5.0 and later that automati= cally displaces the molecule along any negative frequency mode until all ne= gative frequencies are gone.=C2=A0 That is the best advise I am able to give.=C2=A0 Sent from my iPad On 10. Jul 2022, at 07:56, Sachin Ramesh sachinadityaramesh() gmail.com wrote: =EF=BB=BFHi, =C2=A0 =C2=A0Imaginary modes under '-10 cm-1' if not many can be safely ign= ored. You could try to get rid=C2=A0of the imaginary mode by distorting the= structure along the bond, angle or dihedral which is=C2=A0causing the imag= inary mode.=C2=A0 =C2=A0 =C2=A0I should add that imaginary modes are tricky to get rid of whe= n the solvent correction is used.=C2=A0The optimization could be done using= solvent correction and frequency can be computed in gas phase.=C2=A0 =C2=A0 'TightSCF TightOpt Grid7 Gridx9' seems to work for all of our system= s upto 200 atoms, producing=C2=A0accurate results in good agreement with ex= perimental observations. =C2=A0 Hope this helps=C2=A0 with best=C2=A0- Sachin=C2=A0 On Sat, Jul 9, 2022 at 7:32 PM Grigoriy Zhurko reg_zhurko.:.chemcraftprog.c= om wrote: Sent to CCL by: "Grigoriy=C2=A0 Zhurko" [reg_zhurko()chemcraftprog.com] Hello, I compute some molecules with Orca 5.0.3, and the computation sometimes=20 produces small negative frequencies, despite the symmetry of the molecules = is=20 C1. If I repeat the computation with another starting point, with some=20 probability all frequencies are positive. I found that this problem arises when two additions to the model are added:= =20 the solvent model (!CPCM(Water)) and additions of some explicit water=20 molecules to the whole model. I understand that these water molecules produ= ce=20 very small frequencies along the h-bonds, and these frequencies can become= =20 negative because of some problems with numerical integration. I tried the= =20 combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still=20 sometimes the negative frequencies are produced. Maybe I need to further=20 increase the computational accuracy with options like "!VeryTightOpt",=20 "!DefGrid9", UltraTightSCF? I suppose you understand what I mean; currently= =20 I didn't find the information in the manual, how to further decrease the=20 optimization convergence threshold or increase the accuracy of DFT grid.=20 Please suggest how to do that. In my work I can avoid using the frequencies since I need mainly the=20 energies; however I need to explain this somehow in the paper. I suppose, i= t=20 is not good to compute the entropy of molecules with my keywords, because= =20 small frequencies produce big errors with vibrational entropy. So, please= =20 suggest me, what should I write in my papers, to explain that it is not goo= d=20 to compute the Gibbs energy of my molecules, but it is correct to compute a= nd=20 use the common energy. Grigoriy Zhurko https://chemcraftprog.com -=3D This is automatically added to each message by the mailing script =3D-= =20 E-mail to subscribers: CHEMISTRY**ccl.net or use: =C2=A0 =C2=A0 =C2=A0E-mail to administrators: CHEMISTRY-REQUEST**ccl.net or use =C2=A0 =C2=A0 =C2=A0=C2=A0 =C2=A0 =C2=A0=C2=A0 =C2=A0 =C2=A0=20 =20 ------=_Part_6818212_734716936.1657463311962 Content-Type: text/html; charset=UTF-8 Content-Transfer-Encoding: quoted-printable
I was getting Negativ= e frequencies  whenever I used more than one node in the calculations.=  
One of the = ORCA users told me that the issue  with the appearance of= the Negative frequencies  came from using more than one node. Of cour= se, those frequencies disappeared right after I used one node... hope that'= s your problem.


=20
=20
Le dimanche 10 juillet 2022 =C3=A0 09:44:36 UTC+1, Nees= e, Frank neese]![kofo.mpg.de <owner-chemistry|*|ccl.net> a =C3=A9crit :


Just to briefly clarify

TightSCF TightOpt Grid7 Gridx9'

Is ORCA pre 5.0. with 5.0 these old grids are gone and the new grids are mu= ch more accurate and don=E2=80=98t need bumping up. 

The OP has tried these things and the negative frequencies remained, m= eaning that they are not numerical noise. The OP was advised to displace th= e molecule along the respective real modes. It was also pointed out to him = that there is a compound script that comes with ORCA 5.0 and later that automatically displaces the molecu= le along any negative frequency mode until all negative frequencies are gon= e. 

That is the best advise I am able to give. 

Sent from my iPad

On 10. Jul 2022, at 07:56, Sachin Ramesh sachinad= ityaramesh() gmail.com <owner-chemistry|*|ccl.net> wrote:

=EF=BB=BF
Hi,

   Imaginary modes under '-10 cm-1' if not many can be safel= y ignored. You could try to get rid 
of the imaginary mode by distorting the structure along the bond, angl= e or dihedral which is 
causing the imaginary mode. 

   I should add that imaginary modes are tricky to get rid o= f when the solvent correction is used. 
The optimization could be done using solvent correction and frequency = can be computed in gas phase. 

  'TightSCF TightOpt Grid7 Gridx9' seems to work for all of our s= ystems upto 200 atoms, producing 
accurate results in good agreement with experimental observations. &nb= sp;

Hope this helps 

with best 
- Sachin 

On Sat, Jul 9= , 2022 at 7:32 PM Grigoriy Zhurko reg_zhurko.:.chemcraftprog.co= m <owner-chemistry**ccl.net> wrote:

Sent to CCL by: "Grigoriy  Zhurko" [reg_zhurko()chemcraftp= rog.com]
Hello,
I compute some molecules with Orca 5.0.3, and the computation sometimes produces small negative frequencies, despite the symmetry of the molecules = is
C1. If I repeat the computation with another starting point, with some
probability all frequencies are positive.
I found that this problem arises when two additions to the model are added:=
the solvent model (!CPCM(Water)) and additions of some explicit water
molecules to the whole model. I understand that these water molecules produ= ce
very small frequencies along the h-bonds, and these frequencies can become =
negative because of some problems with numerical integration. I tried the <= br clear=3D"none"> combination of options !DefGrid3, !TightOpt, !VeryTightSCF, and still
sometimes the negative frequencies are produced. Maybe I need to further increase the computational accuracy with options like "!VeryTightOpt",
"!DefGrid9", UltraTightSCF? I suppose you understand what I mean; currently=
I didn't find the information in the manual, how to further decrease the optimization convergence threshold or increase the accuracy of DFT grid. Please suggest how to do that.
In my work I can avoid using the frequencies since I need mainly the
energies; however I need to explain this somehow in the paper. I suppose, i= t
is not good to compute the entropy of molecules with my keywords, because <= br clear=3D"none"> small frequencies produce big errors with vibrational entropy. So, please <= br clear=3D"none"> suggest me, what should I write in my papers, to explain that it is not goo= d
to compute the Gibbs energy of my molecules, but it is correct to compute a= nd
use the common energy.

Grigoriy Zhurko
https://chemcraftprog.com



-=3D This is automatically added to each message by the mailing script =3D-= =20
E-mail to subscribers: CHEMISTRY**ccl.net or use:
     

E-mail to administrators:
CHEMISTRY-REQUEST**ccl.net or use
     
     


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

Job: http://www.ccl.net/jobs
Conferences: http://server.ccl.net/chemistry/announcements/conferences/

Search Messages: http://www.ccl.net/chemistry/searchccl/index.shtml
     

RTFI:
http://www.ccl.net/chemistry/aboutccl/instructions/


=20
------=_Part_6818212_734716936.1657463311962-- From owner-chemistry@ccl.net Sun Jul 10 11:28:01 2022 From: "Neese, Frank neese]^[kofo.mpg.de" To: CCL Subject: CCL: [CCL] CCL: Negative frequencies with C1 symmetry (Orca) Message-Id: <-54757-220710100406-21912-brNGcuyqZb4KfyR2R1BrMA/a\server.ccl.net> X-Original-From: "Neese, Frank" Content-Language: de-DE Content-Type: multipart/alternative; boundary="_000_52054C25769F4B0A9E379E9B7316DECEkofompgde_" Date: Sun, 10 Jul 2022 14:03:58 +0000 MIME-Version: 1.0 Sent to CCL by: "Neese, Frank" [neese~!~kofo.mpg.de] --_000_52054C25769F4B0A9E379E9B7316DECEkofompgde_ Content-Type: text/plain; charset="utf-8" Content-Transfer-Encoding: base64 U29sdmF0aW9uIGlzIGRvbmUgYW5hbHl0aWNhbGx5IGluIE9SQ0EgaW5jbHVkaW5nIEhlc3NpYW5z IGFuZCBlbXBsb3lpbmcgdGhlIEdhdXNzaWFuIGNoYXJnZSBzY2hlbWUuIEl0IGlzIGVmZmljaWVu dCwgbnVtZXJpY2FsbHkgc21vb3RoIGFuZCBzdGFibGUuDQoNClZvbiBtZWluZW0gaVBob25lIGdl c2VuZGV0DQoNCkFtIDEwLjA3LjIwMjIgdW0gMTU6NTcgc2NocmllYiBQZXRlciBKYXJvd3NraSBw ZXRlcmphcm93c2tpXy1fZ21haWwuY29tIDxvd25lci1jaGVtaXN0cnlAY2NsLm5ldD46DQoNCu+7 vw0KSGkgQWxsOg0KDQpBIGZldyBjb21tZW50cy4NCg0KRG8gd2UgaGF2ZSBhIHJlZmVyZW5jZSBm b3IgdGhpcyAxMCBjbS0xIHJ1bGUtb2YtdGh1bWI/IEhhcyBhbnlvbmUgcHVibGlzaGVkIGEgY29t cGFyaXNvbiBzdHVkeSB1c2luZyBkaWZmZXJlbnQgc29mdHdhcmVzPyBJIGtub3cgTldjaGVtIGln bm9yZXMgbGF0ZXJhbCBmcmVxdWVuY2llcyAowqsgaW1hZ2luYXJ5IGZyZXF1ZW5jaWVzIMK7KS4g U28gY2FyZWZ1bCB0aGUgb3V0Y29tZSBtaWdodCB2YXJ5IGV2ZW4gYXNzdW1pbmcgdGhlIHNhbWUg aW1wbGVtZW50YXRpb24gb2YgdGhlIHBhcnRpdGlvbiBmdW5jdGlvbnMuIEkgZ3Vlc3Mgd2UgYXJl IHRhbGtpbmcgc3ViIEtjYWwvbW9sIChjYWwgLyBtb2wgSyBbYV0yOTggSykgdmFyaWF0aW9ucyBp biB0aGVybWFsIGNvcnJlY3Rpb25zLg0KDQpGb3Igc29sdmF0YXRpb24sIGl0cyB0cmlja3kuIFRo ZSBoYXJkIGFuZCBmYXN0IHJ1bGUgaXMgdGhhdCB0aGUgZnJlcXVlbmNpZXMgbXVzdCBiZSBldmFs dWF0ZWQgYXQgdGhlIHNhbWUgbGV2ZWwgYXMgdGhlIG9wdGltaXphdGlvbi4gVGh1cywgaWYgeW91 IG9wdGltaXplIGluIFBDTSBpbXBsaWNpdCBzb2x2ZW50IHlvdSBtdXN0IGRvIHRoZSB0aGVybWFs IGNvcnJlY3Rpb25zIGluIHNvbHZvIGFzIHdlbGwuICBJdCBvZnRlbiBtYWtlcyBubyBzaWduaWZp Y2FudCBkaWZmZXJlbmNlLCBidXQgSSBpbWFnaW5lIGl0IHdvdWxkIGludHJvZHVjZSBzb21lIHNt YWxsIGxhdGVyYWwgZnJlcXVlbmNpZXMgaWYgeW91IGRvIGl0IGluIGdhcyBwaGFzZS4gSW4gTldD aGVtIGl0IHJlcXVpcmVzIG51bWVyaWNhbCBpbnRlZ3JhdGlvbiBhbmQgdGFrZXMgZm9yZXZlci4N Cg0KQmVzdCByZWdhcmRzLA0KDQpQZXRlcg0KDQpPbiBTdW4sIDEwIEp1bCAyMDIyIGF0IDA3OjU3 LCBTYWNoaW4gUmFtZXNoIHNhY2hpbmFkaXR5YXJhbWVzaCgpIGdtYWlsLmNvbTxodHRwOi8vZ21h aWwuY29tPiA8b3duZXItY2hlbWlzdHJ5W2FdY2NsLm5ldDxtYWlsdG86b3duZXItY2hlbWlzdHJ5 W2FdY2NsLm5ldD4+IHdyb3RlOg0KSGksDQoNCiAgIEltYWdpbmFyeSBtb2RlcyB1bmRlciAnLTEw IGNtLTEnIGlmIG5vdCBtYW55IGNhbiBiZSBzYWZlbHkgaWdub3JlZC4gWW91IGNvdWxkIHRyeSB0 byBnZXQgcmlkDQpvZiB0aGUgaW1hZ2luYXJ5IG1vZGUgYnkgZGlzdG9ydGluZyB0aGUgc3RydWN0 dXJlIGFsb25nIHRoZSBib25kLCBhbmdsZSBvciBkaWhlZHJhbCB3aGljaCBpcw0KY2F1c2luZyB0 aGUgaW1hZ2luYXJ5IG1vZGUuDQoNCiAgIEkgc2hvdWxkIGFkZCB0aGF0IGltYWdpbmFyeSBtb2Rl cyBhcmUgdHJpY2t5IHRvIGdldCByaWQgb2Ygd2hlbiB0aGUgc29sdmVudCBjb3JyZWN0aW9uIGlz IHVzZWQuDQpUaGUgb3B0aW1pemF0aW9uIGNvdWxkIGJlIGRvbmUgdXNpbmcgc29sdmVudCBjb3Jy ZWN0aW9uIGFuZCBmcmVxdWVuY3kgY2FuIGJlIGNvbXB1dGVkIGluIGdhcyBwaGFzZS4NCg0KICAn VGlnaHRTQ0YgVGlnaHRPcHQgR3JpZDcgR3JpZHg5JyBzZWVtcyB0byB3b3JrIGZvciBhbGwgb2Yg b3VyIHN5c3RlbXMgdXB0byAyMDAgYXRvbXMsIHByb2R1Y2luZw0KYWNjdXJhdGUgcmVzdWx0cyBp biBnb29kIGFncmVlbWVudCB3aXRoIGV4cGVyaW1lbnRhbCBvYnNlcnZhdGlvbnMuDQoNCkhvcGUg dGhpcyBoZWxwcw0KDQp3aXRoIGJlc3QNCi0gU2FjaGluDQoNCk9uIFNhdCwgSnVsIDksIDIwMjIg YXQgNzozMiBQTSBHcmlnb3JpeSBaaHVya28gcmVnX3podXJrby46LmNoZW1jcmFmdHByb2cuY29t PGh0dHA6Ly9jaGVtY3JhZnRwcm9nLmNvbT4gPG93bmVyLWNoZW1pc3RyeSoqY2NsLm5ldDxtYWls dG86b3duZXItY2hlbWlzdHJ5KipjY2wubmV0Pj4gd3JvdGU6DQoNClNlbnQgdG8gQ0NMIGJ5OiAi R3JpZ29yaXkgIFpodXJrbyIgW3JlZ196aHVya28oKWNoZW1jcmFmdHByb2cuY29tPGh0dHA6Ly9j aGVtY3JhZnRwcm9nLmNvbT5dDQpIZWxsbywNCkkgY29tcHV0ZSBzb21lIG1vbGVjdWxlcyB3aXRo IE9yY2EgNS4wLjMsIGFuZCB0aGUgY29tcHV0YXRpb24gc29tZXRpbWVzDQpwcm9kdWNlcyBzbWFs bCBuZWdhdGl2ZSBmcmVxdWVuY2llcywgZGVzcGl0ZSB0aGUgc3ltbWV0cnkgb2YgdGhlIG1vbGVj dWxlcyBpcw0KQzEuIElmIEkgcmVwZWF0IHRoZSBjb21wdXRhdGlvbiB3aXRoIGFub3RoZXIgc3Rh cnRpbmcgcG9pbnQsIHdpdGggc29tZQ0KcHJvYmFiaWxpdHkgYWxsIGZyZXF1ZW5jaWVzIGFyZSBw b3NpdGl2ZS4NCkkgZm91bmQgdGhhdCB0aGlzIHByb2JsZW0gYXJpc2VzIHdoZW4gdHdvIGFkZGl0 aW9ucyB0byB0aGUgbW9kZWwgYXJlIGFkZGVkOg0KdGhlIHNvbHZlbnQgbW9kZWwgKCFDUENNKFdh dGVyKSkgYW5kIGFkZGl0aW9ucyBvZiBzb21lIGV4cGxpY2l0IHdhdGVyDQptb2xlY3VsZXMgdG8g dGhlIHdob2xlIG1vZGVsLiBJIHVuZGVyc3RhbmQgdGhhdCB0aGVzZSB3YXRlciBtb2xlY3VsZXMg cHJvZHVjZQ0KdmVyeSBzbWFsbCBmcmVxdWVuY2llcyBhbG9uZyB0aGUgaC1ib25kcywgYW5kIHRo ZXNlIGZyZXF1ZW5jaWVzIGNhbiBiZWNvbWUNCm5lZ2F0aXZlIGJlY2F1c2Ugb2Ygc29tZSBwcm9i bGVtcyB3aXRoIG51bWVyaWNhbCBpbnRlZ3JhdGlvbi4gSSB0cmllZCB0aGUNCmNvbWJpbmF0aW9u IG9mIG9wdGlvbnMgIURlZkdyaWQzLCAhVGlnaHRPcHQsICFWZXJ5VGlnaHRTQ0YsIGFuZCBzdGls bA0Kc29tZXRpbWVzIHRoZSBuZWdhdGl2ZSBmcmVxdWVuY2llcyBhcmUgcHJvZHVjZWQuIE1heWJl IEkgbmVlZCB0byBmdXJ0aGVyDQppbmNyZWFzZSB0aGUgY29tcHV0YXRpb25hbCBhY2N1cmFjeSB3 aXRoIG9wdGlvbnMgbGlrZSAiIVZlcnlUaWdodE9wdCIsDQoiIURlZkdyaWQ5IiwgVWx0cmFUaWdo dFNDRj8gSSBzdXBwb3NlIHlvdSB1bmRlcnN0YW5kIHdoYXQgSSBtZWFuOyBjdXJyZW50bHkNCkkg ZGlkbid0IGZpbmQgdGhlIGluZm9ybWF0aW9uIGluIHRoZSBtYW51YWwsIGhvdyB0byBmdXJ0aGVy IGRlY3JlYXNlIHRoZQ0Kb3B0aW1pemF0aW9uIGNvbnZlcmdlbmNlIHRocmVzaG9sZCBvciBpbmNy ZWFzZSB0aGUgYWNjdXJhY3kgb2YgREZUIGdyaWQuDQpQbGVhc2Ugc3VnZ2VzdCBob3cgdG8gZG8g dGhhdC4NCkluIG15IHdvcmsgSSBjYW4gYXZvaWQgdXNpbmcgdGhlIGZyZXF1ZW5jaWVzIHNpbmNl IEkgbmVlZCBtYWlubHkgdGhlDQplbmVyZ2llczsgaG93ZXZlciBJIG5lZWQgdG8gZXhwbGFpbiB0 aGlzIHNvbWVob3cgaW4gdGhlIHBhcGVyLiBJIHN1cHBvc2UsIGl0DQppcyBub3QgZ29vZCB0byBj b21wdXRlIHRoZSBlbnRyb3B5IG9mIG1vbGVjdWxlcyB3aXRoIG15IGtleXdvcmRzLCBiZWNhdXNl DQpzbWFsbCBmcmVxdWVuY2llcyBwcm9kdWNlIGJpZyBlcnJvcnMgd2l0aCB2aWJyYXRpb25hbCBl bnRyb3B5LiBTbywgcGxlYXNlDQpzdWdnZXN0IG1lLCB3aGF0IHNob3VsZCBJIHdyaXRlIGluIG15 IHBhcGVycywgdG8gZXhwbGFpbiB0aGF0IGl0IGlzIG5vdCBnb29kDQp0byBjb21wdXRlIHRoZSBH aWJicyBlbmVyZ3kgb2YgbXkgbW9sZWN1bGVzLCBidXQgaXQgaXMgY29ycmVjdCB0byBjb21wdXRl IGFuZA0KdXNlIHRoZSBjb21tb24gZW5lcmd5Lg0KDQpHcmlnb3JpeSBaaHVya28NCmh0dHBzOi8v Y2hlbWNyYWZ0cHJvZy5jb20NCg0KDQoNCi09IFRoaXMgaXMgYXV0b21hdGljYWxseSBhZGRlZCB0 byBlYWNoIG1lc3NhZ2UgYnkgdGhlIG1haWxpbmcgc2NyaXB0ID0tDQpFLW1haWwgdG8gc3Vic2Ny aWJlcnM6IENIRU1JU1RSWSoqY2NsLm5ldDxtYWlsdG86Q0hFTUlTVFJZKipjY2wubmV0PiBvciB1 c2U6DQogICAgICBodHRwOi8vd3d3LmNjbC5uZXQvY2dpLWJpbi9jY2wvc2VuZF9jY2xfbWVzc2Fn ZQ0KDQpFLW1haWwgdG8gYWRtaW5pc3RyYXRvcnM6IENIRU1JU1RSWS1SRVFVRVNUKipjY2wubmV0 PG1haWx0bzpDSEVNSVNUUlktUkVRVUVTVCoqY2NsLm5ldD4gb3IgdXNlDQogICAgICBodHRwOi8v d3d3LmNjbC5uZXQvY2dpLWJpbi9jY2wvc2VuZF9jY2xfbWVzc2FnZQ0KICAgICAgaHR0cDovL3d3 dy5jY2wubmV0L2NoZW1pc3RyeS9zdWJfdW5zdWIuc2h0bWwNCg0KQmVmb3JlIHBvc3RpbmcsIGNo ZWNrIHdhaXQgdGltZSBhdDogaHR0cDovL3d3dy5jY2wubmV0DQoNCkpvYjogaHR0cDovL3d3dy5j Y2wubmV0L2pvYnMNCkNvbmZlcmVuY2VzOiBodHRwOi8vc2VydmVyLmNjbC5uZXQvY2hlbWlzdHJ5 L2Fubm91bmNlbWVudHMvY29uZmVyZW5jZXMvDQoNClNlYXJjaCBNZXNzYWdlczogaHR0cDovL3d3 dy5jY2wubmV0L2NoZW1pc3RyeS9zZWFyY2hjY2wvaW5kZXguc2h0bWwNCiAgICAgIGh0dHA6Ly93 d3cuY2NsLm5ldC9zcGFtbWVycy50eHQNCg0KUlRGSTogaHR0cDovL3d3dy5jY2wubmV0L2NoZW1p c3RyeS9hYm91dGNjbC9pbnN0cnVjdGlvbnMvDQoNCg0K --_000_52054C25769F4B0A9E379E9B7316DECEkofompgde_ Content-Type: text/html; charset="utf-8" Content-Transfer-Encoding: base64 PGh0bWw+DQo8aGVhZD4NCjxtZXRhIGh0dHAtZXF1aXY9IkNvbnRlbnQtVHlwZSIgY29udGVudD0i dGV4dC9odG1sOyBjaGFyc2V0PXV0Zi04Ij4NCjwvaGVhZD4NCjxib2R5IGRpcj0iYXV0byI+DQpT b2x2YXRpb24gaXMgZG9uZSBhbmFseXRpY2FsbHkgaW4gT1JDQSBpbmNsdWRpbmcgSGVzc2lhbnMg YW5kIGVtcGxveWluZyB0aGUgR2F1c3NpYW4gY2hhcmdlIHNjaGVtZS4gSXQgaXMgZWZmaWNpZW50 LCBudW1lcmljYWxseSBzbW9vdGggYW5kIHN0YWJsZS48YnI+DQo8YnI+DQo8ZGl2IGRpcj0ibHRy Ij5Wb24gbWVpbmVtIGlQaG9uZSBnZXNlbmRldDwvZGl2Pg0KPGRpdiBkaXI9Imx0ciI+PGJyPg0K PGJsb2NrcXVvdGUgdHlwZT0iY2l0ZSI+QW0gMTAuMDcuMjAyMiB1bSAxNTo1NyBzY2hyaWViIFBl dGVyIEphcm93c2tpIHBldGVyamFyb3dza2lfLV9nbWFpbC5jb20gJmx0O293bmVyLWNoZW1pc3Ry eUBjY2wubmV0Jmd0Ozo8YnI+DQo8YnI+DQo8L2Jsb2NrcXVvdGU+DQo8L2Rpdj4NCjxibG9ja3F1 b3RlIHR5cGU9ImNpdGUiPg0KPGRpdiBkaXI9Imx0ciI+77u/DQo8ZGl2IGRpcj0iYXV0byI+SGkg QWxsOjwvZGl2Pg0KPGRpdiBkaXI9ImF1dG8iPjxicj4NCjwvZGl2Pg0KPGRpdiBkaXI9ImF1dG8i PkEgZmV3IGNvbW1lbnRzLjwvZGl2Pg0KPGRpdiBkaXI9ImF1dG8iPjxicj4NCjwvZGl2Pg0KPGRp diBkaXI9ImF1dG8iPkRvIHdlIGhhdmUgYSByZWZlcmVuY2UgZm9yIHRoaXMgMTAgY20tMSBydWxl LW9mLXRodW1iPyBIYXMgYW55b25lIHB1Ymxpc2hlZCBhIGNvbXBhcmlzb24gc3R1ZHkgdXNpbmcg ZGlmZmVyZW50IHNvZnR3YXJlcz8gSSBrbm93IE5XY2hlbSBpZ25vcmVzIGxhdGVyYWwgZnJlcXVl bmNpZXMgKMKrIGltYWdpbmFyeSBmcmVxdWVuY2llcyDCuykuIFNvIGNhcmVmdWwgdGhlIG91dGNv bWUgbWlnaHQgdmFyeSBldmVuIGFzc3VtaW5nDQogdGhlIHNhbWUgaW1wbGVtZW50YXRpb24gb2Yg dGhlIHBhcnRpdGlvbiBmdW5jdGlvbnMuIEkgZ3Vlc3Mgd2UgYXJlIHRhbGtpbmcgc3ViIEtjYWwv bW9sIChjYWwgLyBtb2wgSyBbYV0yOTggSykgdmFyaWF0aW9ucyBpbiB0aGVybWFsIGNvcnJlY3Rp b25zLjwvZGl2Pg0KPGRpdiBkaXI9ImF1dG8iPjxicj4NCjwvZGl2Pg0KPGRpdiBkaXI9ImF1dG8i PkZvciBzb2x2YXRhdGlvbiwgaXRzIHRyaWNreS4gVGhlIGhhcmQgYW5kIGZhc3QgcnVsZSBpcyB0 aGF0IHRoZSBmcmVxdWVuY2llcyBtdXN0IGJlIGV2YWx1YXRlZCBhdCB0aGUgc2FtZSBsZXZlbCBh cyB0aGUgb3B0aW1pemF0aW9uLiBUaHVzLCBpZiB5b3Ugb3B0aW1pemUgaW4gUENNIGltcGxpY2l0 IHNvbHZlbnQgeW91IG11c3QgZG8gdGhlIHRoZXJtYWwgY29ycmVjdGlvbnMgaW4gc29sdm8gYXMg d2VsbC4mbmJzcDsgSXQgb2Z0ZW4NCiBtYWtlcyBubyBzaWduaWZpY2FudCBkaWZmZXJlbmNlLCBi dXQgSSBpbWFnaW5lIGl0IHdvdWxkIGludHJvZHVjZSBzb21lIHNtYWxsIGxhdGVyYWwgZnJlcXVl bmNpZXMgaWYgeW91IGRvIGl0IGluIGdhcyBwaGFzZS4gSW4gTldDaGVtIGl0IHJlcXVpcmVzIG51 bWVyaWNhbCBpbnRlZ3JhdGlvbiBhbmQgdGFrZXMgZm9yZXZlci48L2Rpdj4NCjxkaXYgZGlyPSJh dXRvIj48YnI+DQo8L2Rpdj4NCjxkaXYgZGlyPSJhdXRvIj5CZXN0IHJlZ2FyZHMsPC9kaXY+DQo8 ZGl2IGRpcj0iYXV0byI+PGJyPg0KPC9kaXY+DQo8ZGl2IGRpcj0iYXV0byI+UGV0ZXI8L2Rpdj4N CjxkaXY+PGJyPg0KPGRpdiBjbGFzcz0iZ21haWxfcXVvdGUiPg0KPGRpdiBkaXI9Imx0ciIgY2xh c3M9ImdtYWlsX2F0dHIiPk9uIFN1biwgMTAgSnVsIDIwMjIgYXQgMDc6NTcsIFNhY2hpbiBSYW1l c2ggc2FjaGluYWRpdHlhcmFtZXNoKCkNCjxhIGhyZWY9Imh0dHA6Ly9nbWFpbC5jb20iPmdtYWls LmNvbTwvYT4gJmx0OzxhIGhyZWY9Im1haWx0bzpvd25lci1jaGVtaXN0cnlbYV1jY2wubmV0Ij5v d25lci1jaGVtaXN0cnlbYV1jY2wubmV0PC9hPiZndDsgd3JvdGU6PGJyPg0KPC9kaXY+DQo8Ymxv Y2txdW90ZSBjbGFzcz0iZ21haWxfcXVvdGUiIHN0eWxlPSJtYXJnaW46MHB4IDBweCAwcHggMC44 ZXg7Ym9yZGVyLWxlZnQtd2lkdGg6MXB4O2JvcmRlci1sZWZ0LXN0eWxlOnNvbGlkO3BhZGRpbmct bGVmdDoxZXg7Ym9yZGVyLWxlZnQtY29sb3I6cmdiKDIwNCwyMDQsMjA0KSI+DQo8ZGl2IGRpcj0i bHRyIj4NCjxkaXYgZGlyPSJsdHIiPkhpLA0KPGRpdj48YnI+DQo8L2Rpdj4NCjxkaXYgZGlyPSJh dXRvIj4mbmJzcDsgJm5ic3A7SW1hZ2luYXJ5IG1vZGVzIHVuZGVyICctMTAgY20tMScgaWYgbm90 IG1hbnkgY2FuIGJlIHNhZmVseSBpZ25vcmVkLiBZb3UgY291bGQgdHJ5IHRvIGdldCByaWQmbmJz cDs8L2Rpdj4NCjxkaXY+b2YgdGhlIGltYWdpbmFyeSBtb2RlIGJ5IGRpc3RvcnRpbmcgdGhlIHN0 cnVjdHVyZSBhbG9uZyB0aGUgYm9uZCwgYW5nbGUgb3IgZGloZWRyYWwgd2hpY2ggaXMmbmJzcDs8 L2Rpdj4NCjxkaXY+Y2F1c2luZyB0aGUgaW1hZ2luYXJ5IG1vZGUuJm5ic3A7PC9kaXY+DQo8ZGl2 Pjxicj4NCjwvZGl2Pg0KPGRpdj4mbmJzcDsgJm5ic3A7SSBzaG91bGQgYWRkIHRoYXQgaW1hZ2lu YXJ5IG1vZGVzIGFyZSB0cmlja3kgdG8gZ2V0IHJpZCBvZiB3aGVuIHRoZSBzb2x2ZW50IGNvcnJl Y3Rpb24gaXMgdXNlZC4mbmJzcDs8L2Rpdj4NCjxkaXY+VGhlIG9wdGltaXphdGlvbiBjb3VsZCBi ZSBkb25lIHVzaW5nIHNvbHZlbnQgY29ycmVjdGlvbiBhbmQgZnJlcXVlbmN5IGNhbiBiZSBjb21w dXRlZCBpbiBnYXMgcGhhc2UuJm5ic3A7PC9kaXY+DQo8ZGl2Pjxicj4NCjwvZGl2Pg0KPGRpdj4m bmJzcDsgJ1RpZ2h0U0NGIFRpZ2h0T3B0IEdyaWQ3IEdyaWR4OScgc2VlbXMgdG8gd29yayBmb3Ig YWxsIG9mIG91ciBzeXN0ZW1zIHVwdG8gMjAwIGF0b21zLCBwcm9kdWNpbmcmbmJzcDs8L2Rpdj4N CjxkaXY+YWNjdXJhdGUgcmVzdWx0cyBpbiBnb29kIGFncmVlbWVudCB3aXRoIGV4cGVyaW1lbnRh bCBvYnNlcnZhdGlvbnMuICZuYnNwOzwvZGl2Pg0KPGRpdj48YnI+DQo8L2Rpdj4NCjxkaXY+SG9w ZSB0aGlzIGhlbHBzJm5ic3A7PGJyPg0KPC9kaXY+DQo8ZGl2Pjxicj4NCjwvZGl2Pg0KPGRpdj53 aXRoIGJlc3QmbmJzcDs8L2Rpdj4NCjxmb250IHN0eWxlPSJjb2xvcjpyZ2IoMTM2LDEzNiwxMzYp Ij4NCjxkaXY+LSBTYWNoaW4mbmJzcDs8L2Rpdj4NCjwvZm9udD48L2Rpdj4NCjxicj4NCjxkaXYg Y2xhc3M9ImdtYWlsX3F1b3RlIj4NCjxkaXYgZGlyPSJsdHIiIGNsYXNzPSJnbWFpbF9hdHRyIj5P biBTYXQsIEp1bCA5LCAyMDIyIGF0IDc6MzIgUE0gR3JpZ29yaXkgWmh1cmtvIHJlZ196aHVya28u Oi48YSBocmVmPSJodHRwOi8vY2hlbWNyYWZ0cHJvZy5jb20iIHRhcmdldD0iX2JsYW5rIj5jaGVt Y3JhZnRwcm9nLmNvbTwvYT4gJmx0OzxhIGhyZWY9Im1haWx0bzpvd25lci1jaGVtaXN0cnkqKmNj bC5uZXQiIHRhcmdldD0iX2JsYW5rIj5vd25lci1jaGVtaXN0cnkqKmNjbC5uZXQ8L2E+Jmd0OyB3 cm90ZTo8YnI+DQo8L2Rpdj4NCjxibG9ja3F1b3RlIGNsYXNzPSJnbWFpbF9xdW90ZSIgc3R5bGU9 Im1hcmdpbjowcHggMHB4IDBweCAwLjhleDtib3JkZXItbGVmdC13aWR0aDoxcHg7Ym9yZGVyLWxl ZnQtc3R5bGU6c29saWQ7cGFkZGluZy1sZWZ0OjFleDtib3JkZXItbGVmdC1jb2xvcjpyZ2IoMjA0 LDIwNCwyMDQpIj4NCjxicj4NClNlbnQgdG8gQ0NMIGJ5OiAmcXVvdDtHcmlnb3JpeSZuYnNwOyBa aHVya28mcXVvdDsgW3JlZ196aHVya28oKTxhIGhyZWY9Imh0dHA6Ly9jaGVtY3JhZnRwcm9nLmNv bSIgcmVsPSJub3JlZmVycmVyIiB0YXJnZXQ9Il9ibGFuayI+Y2hlbWNyYWZ0cHJvZy5jb208L2E+ XTxicj4NCkhlbGxvLDxicj4NCkkgY29tcHV0ZSBzb21lIG1vbGVjdWxlcyB3aXRoIE9yY2EgNS4w LjMsIGFuZCB0aGUgY29tcHV0YXRpb24gc29tZXRpbWVzIDxicj4NCnByb2R1Y2VzIHNtYWxsIG5l Z2F0aXZlIGZyZXF1ZW5jaWVzLCBkZXNwaXRlIHRoZSBzeW1tZXRyeSBvZiB0aGUgbW9sZWN1bGVz IGlzIDxicj4NCkMxLiBJZiBJIHJlcGVhdCB0aGUgY29tcHV0YXRpb24gd2l0aCBhbm90aGVyIHN0 YXJ0aW5nIHBvaW50LCB3aXRoIHNvbWUgPGJyPg0KcHJvYmFiaWxpdHkgYWxsIGZyZXF1ZW5jaWVz IGFyZSBwb3NpdGl2ZS48YnI+DQpJIGZvdW5kIHRoYXQgdGhpcyBwcm9ibGVtIGFyaXNlcyB3aGVu IHR3byBhZGRpdGlvbnMgdG8gdGhlIG1vZGVsIGFyZSBhZGRlZDogPGJyPg0KdGhlIHNvbHZlbnQg bW9kZWwgKCFDUENNKFdhdGVyKSkgYW5kIGFkZGl0aW9ucyBvZiBzb21lIGV4cGxpY2l0IHdhdGVy IDxicj4NCm1vbGVjdWxlcyB0byB0aGUgd2hvbGUgbW9kZWwuIEkgdW5kZXJzdGFuZCB0aGF0IHRo ZXNlIHdhdGVyIG1vbGVjdWxlcyBwcm9kdWNlIDxicj4NCnZlcnkgc21hbGwgZnJlcXVlbmNpZXMg YWxvbmcgdGhlIGgtYm9uZHMsIGFuZCB0aGVzZSBmcmVxdWVuY2llcyBjYW4gYmVjb21lIDxicj4N Cm5lZ2F0aXZlIGJlY2F1c2Ugb2Ygc29tZSBwcm9ibGVtcyB3aXRoIG51bWVyaWNhbCBpbnRlZ3Jh dGlvbi4gSSB0cmllZCB0aGUgPGJyPg0KY29tYmluYXRpb24gb2Ygb3B0aW9ucyAhRGVmR3JpZDMs ICFUaWdodE9wdCwgIVZlcnlUaWdodFNDRiwgYW5kIHN0aWxsIDxicj4NCnNvbWV0aW1lcyB0aGUg bmVnYXRpdmUgZnJlcXVlbmNpZXMgYXJlIHByb2R1Y2VkLiBNYXliZSBJIG5lZWQgdG8gZnVydGhl ciA8YnI+DQppbmNyZWFzZSB0aGUgY29tcHV0YXRpb25hbCBhY2N1cmFjeSB3aXRoIG9wdGlvbnMg bGlrZSAmcXVvdDshVmVyeVRpZ2h0T3B0JnF1b3Q7LCA8YnI+DQomcXVvdDshRGVmR3JpZDkmcXVv dDssIFVsdHJhVGlnaHRTQ0Y/IEkgc3VwcG9zZSB5b3UgdW5kZXJzdGFuZCB3aGF0IEkgbWVhbjsg Y3VycmVudGx5IDxicj4NCkkgZGlkbid0IGZpbmQgdGhlIGluZm9ybWF0aW9uIGluIHRoZSBtYW51 YWwsIGhvdyB0byBmdXJ0aGVyIGRlY3JlYXNlIHRoZSA8YnI+DQpvcHRpbWl6YXRpb24gY29udmVy Z2VuY2UgdGhyZXNob2xkIG9yIGluY3JlYXNlIHRoZSBhY2N1cmFjeSBvZiBERlQgZ3JpZC4gPGJy Pg0KUGxlYXNlIHN1Z2dlc3QgaG93IHRvIGRvIHRoYXQuPGJyPg0KSW4gbXkgd29yayBJIGNhbiBh dm9pZCB1c2luZyB0aGUgZnJlcXVlbmNpZXMgc2luY2UgSSBuZWVkIG1haW5seSB0aGUgPGJyPg0K ZW5lcmdpZXM7IGhvd2V2ZXIgSSBuZWVkIHRvIGV4cGxhaW4gdGhpcyBzb21laG93IGluIHRoZSBw YXBlci4gSSBzdXBwb3NlLCBpdCA8YnI+DQppcyBub3QgZ29vZCB0byBjb21wdXRlIHRoZSBlbnRy b3B5IG9mIG1vbGVjdWxlcyB3aXRoIG15IGtleXdvcmRzLCBiZWNhdXNlIDxicj4NCnNtYWxsIGZy ZXF1ZW5jaWVzIHByb2R1Y2UgYmlnIGVycm9ycyB3aXRoIHZpYnJhdGlvbmFsIGVudHJvcHkuIFNv LCBwbGVhc2UgPGJyPg0Kc3VnZ2VzdCBtZSwgd2hhdCBzaG91bGQgSSB3cml0ZSBpbiBteSBwYXBl cnMsIHRvIGV4cGxhaW4gdGhhdCBpdCBpcyBub3QgZ29vZCA8YnI+DQp0byBjb21wdXRlIHRoZSBH aWJicyBlbmVyZ3kgb2YgbXkgbW9sZWN1bGVzLCBidXQgaXQgaXMgY29ycmVjdCB0byBjb21wdXRl IGFuZCA8YnI+DQp1c2UgdGhlIGNvbW1vbiBlbmVyZ3kuPGJyPg0KPGJyPg0KR3JpZ29yaXkgWmh1 cmtvPGJyPg0KPGEgaHJlZj0iaHR0cHM6Ly9jaGVtY3JhZnRwcm9nLmNvbSIgcmVsPSJub3JlZmVy cmVyIiB0YXJnZXQ9Il9ibGFuayI+aHR0cHM6Ly9jaGVtY3JhZnRwcm9nLmNvbTwvYT48YnI+DQo8 YnI+DQo8YnI+DQo8YnI+DQotPSBUaGlzIGlzIGF1dG9tYXRpY2FsbHkgYWRkZWQgdG8gZWFjaCBt ZXNzYWdlIGJ5IHRoZSBtYWlsaW5nIHNjcmlwdCA9LTx1PjwvdT4gPGJyPg0KRS1tYWlsIHRvIHN1 YnNjcmliZXJzOiA8YSBocmVmPSJtYWlsdG86Q0hFTUlTVFJZKipjY2wubmV0IiB0YXJnZXQ9Il9i bGFuayI+Q0hFTUlTVFJZKipjY2wubmV0PC9hPiBvciB1c2U6PGJyPg0KJm5ic3A7ICZuYnNwOyAm bmJzcDsgPGEgaHJlZj0iaHR0cDovL3d3dy5jY2wubmV0L2NnaS1iaW4vY2NsL3NlbmRfY2NsX21l c3NhZ2UiIHJlbD0ibm9yZWZlcnJlciIgdGFyZ2V0PSJfYmxhbmsiPg0KaHR0cDovL3d3dy5jY2wu bmV0L2NnaS1iaW4vY2NsL3NlbmRfY2NsX21lc3NhZ2U8L2E+PGJyPg0KPGJyPg0KRS1tYWlsIHRv IGFkbWluaXN0cmF0b3JzOiA8YSBocmVmPSJtYWlsdG86Q0hFTUlTVFJZLVJFUVVFU1QqKmNjbC5u ZXQiIHRhcmdldD0iX2JsYW5rIj4NCkNIRU1JU1RSWS1SRVFVRVNUKipjY2wubmV0PC9hPiBvciB1 c2U8YnI+DQombmJzcDsgJm5ic3A7ICZuYnNwOyA8YSBocmVmPSJodHRwOi8vd3d3LmNjbC5uZXQv Y2dpLWJpbi9jY2wvc2VuZF9jY2xfbWVzc2FnZSIgcmVsPSJub3JlZmVycmVyIiB0YXJnZXQ9Il9i bGFuayI+DQpodHRwOi8vd3d3LmNjbC5uZXQvY2dpLWJpbi9jY2wvc2VuZF9jY2xfbWVzc2FnZTwv YT48YnI+DQo8dT48L3U+Jm5ic3A7ICZuYnNwOyAmbmJzcDsgPGEgaHJlZj0iaHR0cDovL3d3dy5j Y2wubmV0L2NoZW1pc3RyeS9zdWJfdW5zdWIuc2h0bWwiIHJlbD0ibm9yZWZlcnJlciIgdGFyZ2V0 PSJfYmxhbmsiPg0KaHR0cDovL3d3dy5jY2wubmV0L2NoZW1pc3RyeS9zdWJfdW5zdWIuc2h0bWw8 L2E+PGJyPg0KPGJyPg0KQmVmb3JlIHBvc3RpbmcsIGNoZWNrIHdhaXQgdGltZSBhdDogPGEgaHJl Zj0iaHR0cDovL3d3dy5jY2wubmV0IiByZWw9Im5vcmVmZXJyZXIiIHRhcmdldD0iX2JsYW5rIj4N Cmh0dHA6Ly93d3cuY2NsLm5ldDwvYT48YnI+DQo8YnI+DQpKb2I6IDxhIGhyZWY9Imh0dHA6Ly93 d3cuY2NsLm5ldC9qb2JzIiByZWw9Im5vcmVmZXJyZXIiIHRhcmdldD0iX2JsYW5rIj5odHRwOi8v d3d3LmNjbC5uZXQvam9iczwvYT4NCjxicj4NCkNvbmZlcmVuY2VzOiA8YSBocmVmPSJodHRwOi8v c2VydmVyLmNjbC5uZXQvY2hlbWlzdHJ5L2Fubm91bmNlbWVudHMvY29uZmVyZW5jZXMvIiByZWw9 Im5vcmVmZXJyZXIiIHRhcmdldD0iX2JsYW5rIj4NCmh0dHA6Ly9zZXJ2ZXIuY2NsLm5ldC9jaGVt aXN0cnkvYW5ub3VuY2VtZW50cy9jb25mZXJlbmNlcy88L2E+PGJyPg0KPGJyPg0KU2VhcmNoIE1l c3NhZ2VzOiA8YSBocmVmPSJodHRwOi8vd3d3LmNjbC5uZXQvY2hlbWlzdHJ5L3NlYXJjaGNjbC9p bmRleC5zaHRtbCIgcmVsPSJub3JlZmVycmVyIiB0YXJnZXQ9Il9ibGFuayI+DQpodHRwOi8vd3d3 LmNjbC5uZXQvY2hlbWlzdHJ5L3NlYXJjaGNjbC9pbmRleC5zaHRtbDwvYT48YnI+DQo8dT48L3U+ Jm5ic3A7ICZuYnNwOyAmbmJzcDsgPGEgaHJlZj0iaHR0cDovL3d3dy5jY2wubmV0L3NwYW1tZXJz LnR4dCIgcmVsPSJub3JlZmVycmVyIiB0YXJnZXQ9Il9ibGFuayI+DQpodHRwOi8vd3d3LmNjbC5u ZXQvc3BhbW1lcnMudHh0PC9hPjxicj4NCjxicj4NClJURkk6IDxhIGhyZWY9Imh0dHA6Ly93d3cu Y2NsLm5ldC9jaGVtaXN0cnkvYWJvdXRjY2wvaW5zdHJ1Y3Rpb25zLyIgcmVsPSJub3JlZmVycmVy IiB0YXJnZXQ9Il9ibGFuayI+DQpodHRwOi8vd3d3LmNjbC5uZXQvY2hlbWlzdHJ5L2Fib3V0Y2Ns L2luc3RydWN0aW9ucy88L2E+PGJyPg0KPGJyPg0KPGJyPg0KPC9ibG9ja3F1b3RlPg0KPC9kaXY+ DQo8L2Rpdj4NCjwvYmxvY2txdW90ZT4NCjwvZGl2Pg0KPC9kaXY+DQo8L2Rpdj4NCjwvYmxvY2tx dW90ZT4NCjwvYm9keT4NCjwvaHRtbD4NCg== --_000_52054C25769F4B0A9E379E9B7316DECEkofompgde_--